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    Modern Physics

    The current, editable version of this book is available in Wikibooks, the open-content textbooks collection, at
    https://en.wikibooks.org/wiki/Modern_Physics

    Permission is granted to copy, distribute, and/or modify this document under the terms of the Creative Commons Attribution-ShareAlike 3.0 License.

    Introduction


    Welcome

    Welcome to Modern Physics. This book has a lot of information, but it also needs a lot of work. Feel free to read all the material that we have, and edit the material that needs editing. If you want to do a lot of work on this book, it is recommended that you read the note for contributors.

    Who This Book is For

    This book is for an introductory undergraduate study of calculus-based physics. The material covered in this book frequently is spread out over two or three semesters in an average undergraduate curriculum, if not more. This book will rely heavily on Calculus, including differential and integral calculus, multivariable calculus, and differential equations. Also, some topics of Linear Algebra will be considered and utilized. Students without the necessary background in mathematics will have a difficult time reading and following the material.

    What This Book Will Cover

    This book will cover the topic of waves first, because they are a predominant part of modern physical theory. Next, this book will cover the basics of motion. Next, the theory of Special Relativity and Quantum Mechanics are introduced. In the later sections, we cover a number of disjointed topics, including Gravity, Electromagnetism, Fluid dynamics, Thermodynamics, and Nuclear Physics. Additional topics may be added later, as needed. Many of the sections in this book are incomplete, and many pages are stubs. Readers are encouraged to help expand sections that need help.

    Where To Go From Here

    At the present time, there are no materials on Wikibooks that cover material that is more advanced than this. More material on future subjects may be added, however.


    For Contributors


    This page is going to be a brief introduction to editing this book, as well as a general style guide for new contributors.

    A Radically Modern Approach to Introductory Physics

    This book was published under the GFDL, and is a good resource. Since it is under the GFDL, material can be harvested from it, and adapted for this wikibook:

    This textbook aims to cover every aspect of modern physics at an undergraduate level in such a manner that anyone who is literate, and not frightened of math, should be able to understand and use it. It can be used to add new material to the Modern Physics book.

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    Page List


    This is a page listing for the Modern Physics book. Entries in italics are redirects and can probably be deleted.

    Page Listing For: Modern Physics




    Annus Mirabilis of Albert Einstein

    The term "Annus Mirabilis" is Latin for "Miracle Year," and it refers to the year 1905 when Albert Einstein, a relatively unknown physicist at the time, published four groundbreaking papers in the field of theoretical physics. These papers had a profound and lasting impact on our understanding of the fundamental laws of the universe and marked a turning point in the history of science. Here are the four papers that make up Einstein's Annus Mirabilis:

    • Special Theory of Relativity: In this paper, titled "On the Electrodynamics of Moving Bodies," Einstein introduced his special theory of relativity. He presented the theory's two key postulates: the principle of relativity (physical laws are the same for observers in non-accelerated motion) and the constancy of the speed of light in a vacuum for all observers. From these postulates, he derived the famous equation E=mc², which relates energy (E) to mass (m) and the speed of light (c). Special relativity revolutionized our understanding of space, time, and energy.
    • Photoelectric Effect: In the paper "On a Heuristic Point of View Concerning the Production and Transformation of Light," Einstein explained the photoelectric effect, in which light shining on a material causes it to emit electrons. He proposed that light consists of discrete packets of energy called photons, and the energy of each photon is proportional to its frequency. This paper provided strong evidence for the quantum nature of light, which was a departure from classical wave theory.
    • Brownian Motion: Einstein's paper "On the Movement of Small Particles Suspended in a Stationary Liquid as Required by the Molecular Kinetic Theory of Heat" addressed the random motion of small particles suspended in a liquid, known as Brownian motion. He showed that the motion could be explained by the kinetic theory of gases and provided experimental predictions that could be tested. This work provided further evidence for the existence of atoms and molecules.
    • Mass-Energy Equivalence: In a short paper titled "Does the Inertia of a Body Depend upon its Energy Content?" Einstein explored the concept of mass-energy equivalence, which was later expressed in the famous equation E=mc². He proposed that the mass of an object is equivalent to its energy content, suggesting that mass can be converted into energy and vice versa. This concept laid the foundation for nuclear physics and the understanding of nuclear reactions.

    Einstein's papers from 1905 were published in the journal "Annalen der Physik" (Annals of Physics) and had a profound impact on the scientific community. They fundamentally reshaped our understanding of the physical world and paved the way for later developments in modern physics, including the theory of general relativity and quantum mechanics. Einstein's work during his Annus Mirabilis marked him as one of the most influential physicists of the 20th century and earned him the Nobel Prize in Physics in 1921 for his explanation of the photoelectric effect.

    Special Theory of Relativity

    The Special Theory of Relativity, often simply referred to as the Theory of Relativity, is a fundamental theory in physics developed by Albert Einstein in 1905. This groundbreaking theory transformed our understanding of space, time, and the relationship between matter and energy. It consists of two main postulates and has had a profound impact on many areas of science and technology. Here are the key principles and implications of the Special Theory of Relativity:

    • Postulate 1 - The Principle of Relativity:
      • The laws of physics are the same for all observers, regardless of their motion.
      • This principle implies that there is no "absolute" state of rest or motion in the universe. The laws of physics remain consistent for observers in both uniform motion and at rest.
    • Postulate 2 - The Speed of Light:
      • The speed of light in a vacuum, denoted as "c," is the same for all observers, regardless of their relative motion.
      • This postulate implies that the speed of light is a universal constant, approximately equal to 299,792,458 meters per second (or about 186,282 miles per second).

    Key Implications and Concepts of the Special Theory of Relativity:

    • Time Dilation:
      • According to the theory, time is relative and depends on the observer's motion. An observer in motion relative to another will perceive time passing more slowly. This effect is known as time dilation.
      • The famous equation associated with time dilation is:
              
    
      • Time dilation has been experimentally confirmed in particle accelerators and other high-speed experiments.
    • Length Contraction:
      • Objects in motion appear to contract along their direction of motion from the perspective of a stationary observer. This phenomenon is known as length contraction.
      • The equation for length contraction is:
    • Relativistic Mass:
      • As an object's velocity approaches the speed of light, its relativistic mass increases according to the equation: , where is the relativistic mass, is the rest mass, is the velocity, and is the speed of light.
      • This concept highlights that as an object accelerates, it becomes more massive and requires more energy to continue accelerating.
    • E=mc² - Mass-Energy Equivalence:
      • Einstein's famous equation, , states that mass and energy are interchangeable. It means that mass can be converted into energy and vice versa.
      • This principle underlies nuclear reactions, such as those occurring in the sun, nuclear power plants, and atomic bombs.
    • Relativity of Simultaneity:
      • In special relativity, events that are simultaneous in one frame of reference may not be simultaneous in another frame of reference moving at a relative velocity.
      • This leads to the conclusion that there is no universal "now" across all frames of reference.
    • Lorentz Transformation:
      • The Lorentz transformation equations are mathematical formulas that relate space and time coordinates between two relatively moving observers. They describe how measurements of length, time, and other quantities differ between inertial frames.
    • Causality and the Speed of Light Limit:
      • The theory upholds causality, meaning that cause and effect relationships cannot be violated. No information, matter, or influence can travel faster than the speed of light.

    The Special Theory of Relativity has been rigorously tested and confirmed through numerous experiments and observations. It has far-reaching implications for our understanding of the physical universe and has played a pivotal role in the development of modern physics, including the theory of general relativity, which extends these principles to include gravitation. Special relativity has also influenced technology, particularly in the design of high-speed particle accelerators and the development of the Global Positioning System (GPS).

    Photoelectric Effect

    The photoelectric effect is a phenomenon in physics where electrons are emitted from a material when it is exposed to electromagnetic radiation, typically in the form of visible or ultraviolet light. This effect was one of the key pieces of experimental evidence that contributed to the development of quantum mechanics and the understanding of the dual nature of light.

    Here are the main features and principles of the photoelectric effect:

    • Emission of Electrons: When electromagnetic radiation, such as light, is incident on a material surface, it can cause the emission of electrons from that material. These emitted electrons are called photoelectrons.
    • Quantized Energy: The photoelectric effect provided experimental evidence for the quantization of energy, a fundamental concept in quantum mechanics. Electrons in a material are bound by discrete energy levels, and to be emitted, an electron must absorb a photon (a particle of light) with energy equal to or greater than the energy required to overcome the binding energy of the electron.
    • Threshold Frequency: There is a minimum frequency of incident light, called the threshold frequency (), below which no photoelectrons are emitted, regardless of the intensity (brightness) of the light. Photoelectron emission only occurs when the frequency of the incident light exceeds this threshold.
    • Einstein's Explanation: Albert Einstein provided a theoretical explanation of the photoelectric effect in 1905. He proposed that light is composed of discrete packets of energy called photons. When a photon is absorbed by an electron in the material, it imparts its energy to the electron, allowing it to overcome the binding energy and escape the material's surface as a photoelectron. The energy of a photon () is directly proportional to its frequency (), as given by the equation , where is Planck's constant.
    • Intensity and Electron Kinetic Energy: Increasing the intensity of the incident light (the number of photons per unit time) results in more photoelectrons being emitted, but it does not affect their maximum kinetic energy. The maximum kinetic energy of the emitted photoelectrons depends only on the frequency of the incident light and is given by the equation , where is the work function, representing the minimum energy required to remove an electron from the material.
    • Wave-Particle Duality: The photoelectric effect is a clear example of the wave-particle duality of light. Although light is typically described as a wave, the photoelectric effect demonstrates its particle-like behavior, where photons of discrete energy interact with electrons in a quantized manner.

    The photoelectric effect has practical applications in devices like photodetectors and photovoltaic cells (solar cells) and has been crucial in developing our understanding of quantum mechanics and the fundamental nature of light. It played a significant role in the development of the concept of quantization of energy and contributed to Albert Einstein receiving the Nobel Prize in Physics in 1921.

    Brownian Motion

    Brownian motion, also known as Brownian movement or pedesis, is the random and continuous motion of microscopic particles suspended in a fluid (liquid or gas) resulting from their collision with fast-moving atoms or molecules in the surrounding medium. This phenomenon was first observed and explained by the Scottish scientist Robert Brown in 1827, although it wasn't fully understood until Albert Einstein provided a theoretical explanation in 1905, which helped establish the concept of atoms and molecules.

    Key characteristics and principles of Brownian motion include:

    • Random Motion: Brownian motion is characterized by the erratic, zigzagging, and unpredictable paths taken by the particles. The motion appears to be chaotic because it results from the cumulative effect of countless collisions with much smaller, faster-moving particles (atoms or molecules) in the fluid.
    • Microscopic Scale: Brownian motion is most noticeable at microscopic scales, such as when observing tiny particles like pollen grains, dust, or colloidal particles suspended in a liquid. At macroscopic scales, the effects of Brownian motion are not typically observable.
    • Continuous Nature: Brownian motion is a continuous, ongoing process. It continues as long as the particles are suspended in the fluid and there are thermal fluctuations (random movements) of the surrounding molecules.
    • Thermal Motion: Brownian motion is driven by thermal energy. The fast, random motion of the surrounding fluid molecules is a manifestation of their thermal energy. When these fast-moving molecules collide with the suspended particles, they impart momentum, causing the particles to move randomly.
    • Einstein's Explanation: Albert Einstein's 1905 paper on the theory of Brownian motion provided a mathematical explanation for this phenomenon, which supported the idea that matter is composed of discrete atoms and molecules. Einstein's equations describe the mean square displacement of a Brownian particle over time.
    • Diffusion: Brownian motion is related to the process of diffusion, where particles tend to move from regions of higher concentration to regions of lower concentration. Diffusion is the net result of the random motion of particles due to Brownian motion.
    • Applications: Brownian motion has numerous practical applications and implications in various fields, including physics, chemistry, biology, and engineering. It is used to explain phenomena such as the diffusion of molecules in gases and liquids, the behavior of colloids, and the motion of small particles in biological systems.
    • Statistical Properties: Brownian motion is often analyzed statistically. The mean square displacement of a particle over time follows a linear relationship with time, and this relationship is used to determine diffusion coefficients and other properties of the suspended particles.
    • Brownian Motion Simulations: Computer simulations and models of Brownian motion have been developed to study the behavior of particles in complex systems. These simulations have applications in areas like materials science and drug delivery.

    In summary, Brownian motion is a fundamental phenomenon that occurs at the microscopic scale and results from the continuous, random motion of particles suspended in a fluid. It has played a crucial role in our understanding of the kinetic theory of matter and the behavior of atoms and molecules in gases and liquids.

    Mass-Energy Equivalence

    Mass-energy equivalence is a fundamental principle in physics that describes the relationship between mass and energy. This concept is most famously encapsulated by Albert Einstein's equation, , which states that energy () is equal to mass () times the speed of light () squared. Here are key points about mass-energy equivalence:

    • The Equation :
      • The equation is one of the most famous equations in physics, and it relates mass and energy. It asserts that a given amount of mass can be converted into a corresponding amount of energy and vice versa.
      • represents energy in joules (J), represents mass in kilograms (kg), and represents the speed of light in a vacuum, approximately meters per second (m/s).
    • Origin:
      • Albert Einstein proposed the mass-energy equivalence principle in his special theory of relativity, which was published in 1905. This theory revolutionized physics by demonstrating that mass and energy are interconnected.
    • Consequences:
      • The mass-energy equivalence principle has profound consequences. It implies that mass is a form of energy, and any mass can be converted into energy and released in various processes, such as nuclear reactions.
      • Conversely, energy can be converted into mass, as observed in particle accelerators where high-energy collisions can create new particles with mass.
    • Nuclear Reactions:
      • The most famous application of mass-energy equivalence is in nuclear reactions, such as those occurring in the sun and nuclear power plants. In these reactions, a small amount of mass is converted into a large amount of energy, as described by .
      • The energy released in nuclear reactions is harnessed for electricity generation and other applications.
    • Atomic Bombs:
      • The destructive power of atomic bombs is a result of mass-energy equivalence. In nuclear explosions, a small amount of nuclear material undergoes a chain reaction, releasing a massive amount of energy as the mass is converted into energy.
    • Particle Physics:
      • Particle accelerators, like the Large Hadron Collider (LHC), accelerate particles to high speeds and collide them to study fundamental particles and their interactions. These experiments take advantage of mass-energy equivalence to create and study particles.
    • Cosmological Implications:
      • Mass-energy equivalence also has implications for cosmology and the study of the universe's early moments, particularly during the Big Bang. It helps explain how particles and radiation behaved in the early universe.
    • Practical Applications:
      • Mass-energy equivalence is applied in technologies like positron emission tomography (PET) scanners, where antimatter annihilation reactions are used to produce gamma rays for medical imaging.

    In summary, mass-energy equivalence is a fundamental concept in physics that shows that mass and energy are interchangeable. It is a cornerstone of modern physics and has numerous practical applications in energy production, nuclear physics, and particle physics. Albert Einstein's equation, , succinctly captures this profound relationship.


    Gravity

    Newtons Law of Gravitation

    1. The Law of Gravitation
    2. Gravitational Field
    3. Gravitational Flux
    4. Flux from Multiple Masses
    5. Kepler's Laws
    6. Use of Conservation Laws
    7. Effects of Relativity
    Problems

    Modern theories of Gravitation

    1. General relativity

    Speculative theories

    1. Brans-Dicke theory

    Further Reading


    Space Physics

    Space physics, also known as space plasma physics or astrophysical plasma physics, is a branch of space science and physics that focuses on the study of charged particles and electromagnetic fields in space environments. It seeks to understand the behavior of plasmas (ionized gases) and the physical processes that occur in space, ranging from the Earth's magnetosphere to the broader universe. Here are key aspects of space physics:

    • Plasma in Space: Space is filled with plasmas, which consist of charged particles (ions and electrons) that interact with electromagnetic fields. These plasmas can be found in various space environments, including the solar wind, planetary magnetospheres, and interstellar and intergalactic space.
    • Solar-Terrestrial Physics: A significant portion of space physics is devoted to studying the interaction between the solar wind (a stream of charged particles from the Sun) and the Earth's magnetic field. This interaction gives rise to phenomena such as geomagnetic storms, auroras, and the Van Allen radiation belts.
    • Magnetospheres: Space physics investigates the magnetospheres of planets and celestial bodies. These protective magnetic fields influence the behavior of charged particles in space and play a crucial role in shielding planets from harmful solar and cosmic radiation.
    • Space Weather: Space physicists study space weather, which includes the conditions in space that can affect technology and systems on Earth and in space. Space weather phenomena include solar flares, coronal mass ejections, and their impact on satellite communications, navigation systems, and power grids.
    • Astrophysical Plasmas: Beyond our solar system, space physics explores the behavior of plasmas in astrophysical environments. This includes the study of accretion disks around black holes, the interstellar medium, and the behavior of plasmas in galaxies and galaxy clusters.
    • Cosmic Rays: Space physics investigates cosmic rays, which are high-energy charged particles originating from various sources in the universe, including the Sun and distant astrophysical phenomena. Understanding cosmic rays can provide insights into astrophysical processes.
    • Satellite Missions: Space physicists often utilize space-based observatories and satellite missions to collect data and conduct experiments in space. These missions enable the direct measurement of space plasmas, electromagnetic fields, and other space phenomena.
    • Numerical Modeling: Numerical simulations and computer modeling play a significant role in space physics. Researchers use mathematical models to simulate the behavior of plasmas and electromagnetic fields in various space environments, helping to predict and understand complex space phenomena.
    • Interdisciplinary Field: Space physics is highly interdisciplinary, involving elements of plasma physics, astrophysics, magnetohydrodynamics (MHD), and geophysics. Researchers collaborate across disciplines to address complex questions related to space and plasma physics.
    • Scientific Questions: Key scientific questions in space physics include understanding the origin and evolution of planetary magnetospheres, the acceleration of charged particles in space, the dynamics of solar and astrophysical plasmas, and the impact of space weather on human activities and technology.

    Space physics is a dynamic field that continues to advance our understanding of the complex and interconnected processes that occur in space environments. It has practical applications in space exploration, satellite technology, and space weather prediction, contributing to our ability to navigate and utilize space resources effectively.



    Constants

    Constants

    1. Constants of Nature
    2. Miscellaneous Conversions


    Table of nuclides

    {split}

    A table with the basic properties of all nuclides.

    Legend

    α Alpha decay
    β- Beta decay
    β+ Positron emission
    K+ Electron capture
    IT Internal conversion
    SF Spontaneous fission
    p Proton emission
    n Neutron emission


    Neutron

    Isotope Half-life Spin Parity Mode(s) or Abundance
    0n 614.6s 1/2+ %β-=100

    Hydrogen

    Isotope Half-life Spin Parity Mode(s) or Abundance
    1H stable 1/2+ %Abundance=99.985
    2H stable 1+ %Abundance=0.015
    3H 12.33 a 1/2+ %β-=100
    4H 2-

    Helium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    3He stable 1/2+ %Abundance=0.000137
    4He stable 0+ %Abundance=99.999863
    5He 0.60 MeV 3/2- %n=100
    6He 806.7 ms 0+ %β-=100
    7He 160 keV (3/2)- %n=100
    8He 119.0 ms 0+ %β-=100, %β-n=16
    9He 0.30 MeV (1/2-) %n=100
    10He 0.3 MeV 0+ %n=100

    Lithium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    4Li 2-
    5Li 1.5 MeV 3/2- %p=100
    6Li stable 1+ 1+ %Abundance=7.5
    7Li stable 3/2- %Abundance=92.5
    8Li 838 ms 2+ %β-=100, %β-2α=100
    9Li 178.3 ms 3/2- %β-=100, %β-n2α=49.5
    10Li 1.2 MeV %n=100
    11Li 8.5 ms 3/2- %β-=100, %β-n=85 , %β-2n=4.1 , %β-2α3n=1.9

    Beryllium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    6Be 92 keV 0+ %2pα=100
    7Be 53.12 d 3/2- %K=100
    8Be 6.8 eV 0+ %2α=100
    9Be stable 3/2- 3/2- %Abundance=100
    10Be 1510000 a 0+ %β-=100
    11Be 13.81 s 1/2+ %β-=100, %β-α=3.1
    12Be 23.6 ms 0+ %β-=100
    13Be 0.9 MeV (1/2,5/2)+ %n=100
    14 Be 4.35 ms 0+ %β-=100, %β-n=81 , %β-2n=5

    Boron

    Isotope Half-life Spin Parity Mode(s) or Abundance
    7B 1.4 MeV (3/2-) %XP=100
    8B 770 ms 2+ %K+%β+=100, %K2α=100
    9B 0.54 keV 3/2- %2αP=100
    10B stable 3+ %Abundance=19.9
    11B stable 3/2- %Abundance=80.1
    12B 20.20 ms 1+ %β-=100, %β-3α=1.58
    13B 17.36 ms 3/2- %β-=100, %β-n=0.28
    14B 13.8 ms 2- %β-=100
    15B 10.5 ms %β-=100
    16B 200 ps (0-) %n=100
    17B 5.08 ms (3/2-) %β-=100, %β-n=?

    Carbon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    8C 230 keV 0+ %Xp=100
    9C 126,5 ms (3/2-) %K+%β+=100, %Kp2α=?
    10C 19.255 s 0+ %K+%β+=100
    11C 20.39 m 3/2- %K+%β+=100
    12C stable 0+ %Abundance=98.90
    13C stable 1/2- %Abundance=1.10
    14C 5730 a 0+ %β-=100
    15C 2.449 s 1/2+ %β-=100
    16C 0.747 s 0+ %β-=100, %β-n > 98.8
    17C 0.193 s %β-=100, %β-n=32
    18C 0.095 s 0+ %β-=100, %β-n ~ 25
    19C 0.046 s %β-=100, %β-n=47
    20C 0.014 s 0+ %β-=100, %β-n=72

    Nitrogen

    Isotope Half-life Spin Parity Mode(s) or Abundance
    11N 740 keV 1/2+ %p=?
    12N 11.000 ms 1+ %K+%β+=100, %K3α=3.5
    13N 9.965 m 1/2- %K+%β+=100
    14N stable 1+ %Abundance=99.634
    15N stable 1/2- %Abundance=0.366
    16N 7.13 s 2- %β-=100, %β-α=0.00120
    17N 4.173 s 1/2- %β-=100, %β-n=95.1
    18N 624 ms 1- %β-=100, %β-α=12.2 , %β-n=14.3
    19N 0.304 s (1/2-) %β-=100, %β-n=62.4
    20N 100 ms %β-=100, %β-n ~ 61
    21N 85 ms %β-=100, %β-n=84
    22N 24 ms %β-=100, %β-n=35

    Oxygen

    Isotope Half-life Spin Parity Mode(s) or Abundance
    12O 0.40 MeV 0+ %2p=60
    13O 8.58 ms (3/2-) %K+%β+=100, %Kp=12
    14O 70.606 s 0+ %K+%β+=100
    15O 122.24 s 1/2- %K+%β+=100
    16O stable 0+ %Abundance=99.762
    17O stable 5/2+ %Abundance=0.038
    18O stable 0+ %Abundance=0.200
    19O 26.91 s 5/2+ %β-=100
    20O 13.51 s 0+ %β-=100
    21O 3.42 s (1/2,3/2,5/2)+ %β-=100
    22O 2.25 s 0+ %β-=100
    23O 82 ms %β-=100, %β-n=31
    24O 61 ms 0+ %β-=100, %β-n=58

    Fluorine

    Isotope Half-life Spin Parity Mode(s) or Abundance
    F (2-) %p=100
    F 1.0 MeV (1/2+) %p=100
    F 40 keV 0- %p=100
    F 64.49 s 5/2+ %K+%β+=100
    F 109.77 m 1+ %K+%β+=100
    F stable 1/2+ %Abundance=100
    F 11.00 s 2+ %β-=100
    F 4.158 s 5/2+ %β-=100
    F 4.23 s 4+,(3+) %β-=100
    F 2.23 s (3/2,5/2)+ %β-=100
    F 0.34 s (1,2,3)+ %β-=100
    F 59 ms uo

    Neon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    16Ne 122 keV 0+ %2p=100
    17Ne 109.2 ms 1/2- %K+%β+=100, %Kp=95.8 , %Kα=2.7
    18Ne 1672 ms 0+ %K+%β+=100
    19Ne 17.22 s 1/2+ %K+%β+=100
    20Ne stable 0+ %Abundance=90.48
    21Ne stable 3/2+ %Abundance=0.27
    22Ne stable 0+ %Abundance=9.25
    23Ne 37.24 s 5/2+ %β-=100
    24Ne 3.38 m 0+ %β-=100
    25Ne 602 ms (1/2,3/2)+ %β-=100
    26Ne 197 ms 0+ %β-=100, %β-n=0.13
    27Ne 32 ms %β-=100, %β-n=2.0
    28Ne 17 ms 0+ %β-=100, %β-n=22
    29Ne 0.2 s %β-=100

    Sodium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    19Na %p=?
    20Na 447.9 ms 2+ %K+%β+=100, %Kα=20.5
    21Na 22.49 s 3/2+ %K+%β+=100
    22Na 2.6019 a 3+ %K+%β+=100
    23Na stable 3/2+ %Abundance=100
    24Na 14.9590 s 4+ %β-=100
    24m1Na 20.20 ms 1+ %IT=99.95, %β-=0.05
    25Na 59.1 s 5/2+ %β-=100
    26Na 1.072 s 3+ %β-=100
    27Na 301 ms 5/2+ %β-=100 , %β-n=0.13
    28Na 30.5 ms 1+ %β-=100 , %β-n=0.58
    29Na 44.9 ms 3/2 %β-=100 , %β-n=21.5
    30Na 48 ms 2+ %β-=100 , %β-n=30 , %β-2n=1.17 , %β-α=5.5E-5
    31Na 17.0 ms 3/2+ %β-=100, %β-n=37 , %β-2n=0.9
    32Na 13.2 ms (3-,4-) %β-=100 , %β-n=24 , %β-2n=8.3
    33Na 8.2 ms %β-=100, %β-n=52 , %β-2n=12
    34Na 5.5 ms %β-=100, %β-n=?, %β-2n=?
    35Na 1.5 ms %β-=100, %β-n=?

    Magnesium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    20Mg 95 ms 0+ %K+%β+=100, %Kp ~ 3
    21Mg 122 ms (3/2,5/2)+ %K+%β+=100 , %Kp=29.3
    22Mg 3.857 s 0+ %K+%β+=100
    23Mg 11.317 s 3/2+ %K+%β+=100
    24Mg stable 0+ %Abundance=78.99
    25Mg stable 5/2+ %Abundance=10.00
    26Mg stable 0+ %Abundance=11.01
    27Mg 9.458 m 1/2+ %β-=100
    28Mg 20.91 h 0+ %β-=100
    29Mg 1.30 s 3/2+ %β-=100
    30Mg 335 ms 0+ %β-=100
    31Mg 230 ms %β-=100 , %β-n=1.7
    32Mg 120 ms 0+ %β-=100 , %β-n=2.4
    33Mg 90 ms %β-=100, %β-n=17
    34Mg 20 ms 0+ %β-=100, %β-n=?

    Aluminium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    22Al 70 ms %K+%β+=100 , %Kp+%K2p ~ 2.9
    23Al 0.47 s %K+%β+=100, %Kp=?
    24Al 2.053 s 4+ %K+%β+=100, %Kα=0.035
    24m1Al 131.3 ms 1+ %IT=82 , %K+%β+=18 , %Kα=0.028
    25Al 7.183 s 5/2+ %K+%β+=100
    26Al 7.17e+5 a 5+ %K+%β+=100
    26m1Al 6.3452 s 0+ %K+%β+=100
    27Al stable 5/2+ %Abundance=100
    28Al 2.2414 m 3+ %β-=100
    29Al 6.56 m 5/2+ %β-=100
    30Al 3.60 s 3+ %β-=100
    31Al 644 ms (3/2,5/2)+ %β-=100
    32Al 33 ms 1+ %β-=100

    Silicon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    22Si 6 ms 0+ %K+%β+=100, %Kp=?
    23Si
    24Si 102 ms 0+ %K+%β+=100, %Kp ~ 7
    25Si 220 ms 5/2+ %K+%β+=100, %Kp=?
    26Si 2.234 s 0+ %K+%β+=100
    27Si 4.16 s 5/2+ %K+%β+=100
    28Si stable 0+ %Abundance=92.23
    29Si stable 1/2+ %Abundance=4.67
    30Si stable 0+ %Abundance=3.10
    31Si 157.3 m 3/2+ %β-=100
    32Si 150 a 0+ %β-=100
    33Si 6.18 s %β-=100
    34Si 2.77 s 0+ %β-=100
    35Si 0.78 s %β-=100
    36Si 0.45 s 0+ %β-=100, %β-n < 10

    Phosphorus

    Isotope Half-life Spin Parity Mode(s) or Abundance
    26P 20 ms (3+) %K+%β+=100, %Kp+%K2p ~ 1.9
    27P 260 ms 1/2+ %K+%β+=100, %Kp ~ 0.05
    28P 270.3 ms 3+ %K+%β+=100, %Kp=0.0013 , %Kα=0.00086
    29P 4.140 s 1/2+ %K+%β+=100
    30P 2.498 m 1+ %K+%β+=100
    31P stable 1/2+ %Abundance=100
    32P 14.262 d 1+ %β-=100
    33P 25.34 d 1/2+ %β-=100
    34P 12.43 s 1+ %β-=100
    35P 47.3 s 1/2+ %β-=100
    36P 5.6 s %β-=100
    37P 2.31 s %β-=100
    38P 0.64 s %β-=100, %β-n < 10
    39P 0.16 s %β-=100, %β-n=41
    40P 260 ms %β-=100, %β-n=30
    41P 120 ms %β-=100, %β-n=30
    42P 110 ms %β-=100, %β-n=50
    43P 33 ms %β-=100, %β-n=100


    Sulphur

    Isotope Half-life Spin Parity Mode(s) or Abundance
    27S 21 ms %K+%β+=100, %K2p=2.0, %Kp=?
    28S 125 ms 0+ %K+%β+=100, %Kp=21
    29S 187 ms 5/2+ %K+%β+=100, %Kp=47
    30S 1.178 s 0+ %K+%β+=100
    31S 2.572 s 1/2+ %K+%β+=100
    32S stable 0+ %Abundance=95.02
    33S stable 3/2+ %Abundance=0.75
    34S stable 0+ %Abundance=4.21
    35S 87.32 d 3/2+ %β-=100
    36S stable 0+ %Abundance=0.02
    37S 5.05 m 7/2- %β-=100
    38S 170.3 m 0+ %β-=100
    39S 11.5 s (3/2,5/2,7/2) - %β-=100
    40S 8.8 s 0+ %β-=100
    41S
    42S 0.56 s 0+ %β-=100, %β-n < 4
    43S 220 ms %β-=100, %β-n=40
    44S 123 ms 0+ %β-=100, %β-n=18
    45S 82 ms %β-=100, %β-n=54

    Chlorine

    Isotope Half-life Spin Parity Mode(s) or Abundance
    31Cl 150 ms %K+%β+=100, %Kp=0.44
    32Cl 298 ms 1+ %K+%β+=100 , %Kα=0.054 , %Kp=0.026
    33Cl 2.511 s 3/2+ %K+%β+=100
    34Cl 1.5264 s 0+ %K+%β+=100
    34m1Cl 32.00 m 3+ %K+%β+=55.4 , %IT=44.6
    35Cl stable 3/2+ %Abundance=75.77
    36Cl 3.01e+5 a 2+ %β-=98.10 , %K+%β+=1.90
    37Cl stable 3/2+ %Abundance=24.23
    38Cl 37.24 m 2- %β-=100
    38m1Cl 715 ms 5- %IT=100
    39Cl 55.6 m 3/2+ %β-=100
    40Cl 1.35 m 2- %β-=100
    41Cl 38.4 s (1/2,3/2)+ %β-=100
    42Cl 6.8 s %β-=100
    43Cl 3.3 s %β-=100
    44Cl 434 ms %β-=100, %β-n < 8
    45Cl 400 ms %β-=100, %β-n=24
    46Cl 223 ms %β-=100, %β-n=60
    47Cl %β-=100, %β-n < 3

    Argon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    30Ar 20 ns 0+ %p=?
    31Ar 15.1 ms %K+%β+=100, %Kp=42 , %K2p=2.48 , %K3p=2.1
    32Ar 98 ms 0+ %K+%β+=100, %Kp=43
    33Ar 173.0 ms 1/2+ %K+%β+=100, %Kp=38.7
    34Ar 844.5 ms 0+ %K+%β+=100
    35Ar 1.775 s 3/2+ %K+%β+=100
    36Ar stable 0+ %Abundance=0.337
    37Ar 35.04 d 3/2+ %K=100
    38Ar stable 0+ %Abundance=0.063
    39Ar 269 a 7/2- %β-=100
    40Ar stable 0+ %Abundance=99.600
    41Ar 109.34 m 7/2- %β-=100
    42Ar 32.9 a 0+ %β-=100
    43Ar 5.37 m (3/2,5/2) %β-=100
    44Ar 11.87 m 0+ %β-=100
    45Ar 21.48 s %β-=100
    46Ar 8.4 s 0+ %β-=100
    47Ar 700 ms %β-=100, %β-n < 1

    Potassium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    35K 190 ms 3/2+ %K+%β+=100, %Kp=0.37
    36K 342 ms 2+ %K+%β+=100, %Kp=0.048 , %Kα=0.0034
    37K 1.226 s 3/2+ %K+%β+=100
    38K 7.636 m 3+ %K+%β+=100
    38m1K 923.9 ms 0+ %K+%β+=100
    39K stable 3/2+ %Abundance=93.2581
    40K 1.277e+9 a 4- %Abundance=0.0117, %β-=89.28 , %K+%β+=10.72
    41K stable 3/2+ %Abundance=6.7302
    42K 12.360 h 2- %β-=100
    43K 22.3 h 3/2+ %β-=100
    44K 22.13 m 2- %β-=100
    45K 17.3 m 3/2+ %β-=100
    46K 105 s (2-) %β-=100
    47K 17.50 s 1/2+ %β-=100
    48K 6.8 s (2-) %β-=100, %β-n=1.14
    49K 1.26 s (3/2+) %β-=100, %β-n=86
    50K 472 ms (0-,1,2-) %β-=100, %β-n=29
    51K 365 ms (1/2+,3/2+) %β-=100 , %β-n=47
    52K 105 ms %β-=100, %β-n=91
    53K 30 ms (3/2+) %β-=100, %β-n=85
    54K 10 ms %β-=100, %β-n=?

    Calcium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    35Ca 50 ms %K+%β+=100, %K2p=?
    36Ca 102 ms 0+ %K+%β+=100, %Kp=57
    37Ca 181.1 ms 3/2+ %K+%β+=100, %Kp=76
    38Ca 440 ms 0+ %K+%β+=100
    39Ca 859.6 ms 3/2+ %K+%β+=100
    40Ca stable 0+ %Abundance=96.941
    41Ca 1.03e+5 a 7/2- %K=100
    42Ca stable 0+ %Abundance=0.647
    43Ca stable 7/2- %Abundance=0.135
    44Ca stable 0+ %Abundance=2.086
    45Ca 162.61 d 7/2- %β-=100
    46Ca stable 0+ %Abundance=0.004
    47Ca 4.536 d 7/2- %β-=100
    48Ca 6e+18 a 0+ %Abundance=0.187, %β-=?, %ββ=?
    49Ca 8.718 m 3/2- %β-=100
    50Ca 13.9 s 0+ %β-=100
    51Ca 10.0 s ( 3/2- ) %β-=100, %β-n=?
    52Ca 4.6 s 0+ %β-=100
    53Ca 90 ms ( 3/2- ,5/2-) %β-=100, %β-n+%β-2n > 30

    Scandium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    40Sc 182.3 ms 4- %K+%β+=100, %Kα=0.017 , %Kp=0.44
    41Sc 596.3 ms 7/2- %K+%β+=100
    42Sc 681.3 ms 0+ %K+%β+=100
    42m1Sc 61.7 s 7+,(5+,6+) %K+%β+=100
    43Sc 3.891 h 7/2- %K+%β+=100
    44Sc 3.927 h 2+ %K+%β+=100
    44m1Sc 58.6 h 6+ %IT=98.80 , %K+%β+=1.20
    45Sc stable 7/2- %Abundance=100
    45m1Sc 318 ms 3/2+ %IT=100
    46Sc 83.79 d 4+ %β-=100
    46m1Sc 18.75 s 1- %IT=100
    47Sc 3.3492 d 7/2- %β-=100
    48Sc 43.67 h 6+ %β-=100
    49Sc 57.2 m 7/2- %β-=100
    50Sc 102.5 s 5+ %β-=100
    50m1Sc 0.35 s 2+,3+ %IT > 97.5 < 100, %β-<2.5
    51Sc 12.4 s (7/2)- %β-=100
    52Sc 8.2 s 3+ %β-=100

    Titanium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    39Ti 26 ms ( 3/2+ ) %K=100, %Kp+%K2p ~ 14
    40Ti 50 ms 0+ %K+%β+=100
    41Ti 80 ms 3/2+ %K+%β+=100, %Kp ~ 100
    42Ti 199 ms 0+ %K+%β+=100
    43Ti 509 ms 7/2- %K+%β+=100
    44Ti 63 a 0+ %K=100
    45Ti 184.8 m 7/2- %K+%β+=100
    46Ti stable 0+ %Abundance=8.0
    47Ti stable 5/2- %Abundance=7.3
    48Ti stable 0+ %Abundance=73.8
    49Ti stable 7/2- %Abundance=5.5
    50Ti stable 0+ %Abundance=5.4
    51Ti 5.76 m 3/2- %β-=100
    52Ti 1.7 m 0+ %β-=100
    53Ti 32.7 s (3/2)- %β-=100
    54Ti 0+
    55Ti 320 ms ( 3/2- ) %β-=100
    56Ti 160 ms 0+ %β-=100, %β-n=0.06 s ys
    57Ti 180 ms (5/2-) %β-=100, %β-n=0.04 sys
    58Ti 0+
    59Ti (5/2-) %β-=?
    60Ti 0+ %β-=?
    61Ti (1/2-) %β-=?, %β-n=?

    Vanadium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    43V 800 ms ( 7/2- ) %K+%β+=100
    44V 90 ms (2+) %K+%β+=100, %Kα=?
    44m1V 150 ms (6+) %K+%β+=100
    45V 547 ms 7/2- %K+%β+=100
    46V 422.37 ms 0+ %K+%β+=100
    46m1V 1.02 ms 3+ %IT=100
    47V 32.6 m 3/2- %K+%β+=100
    48V 15.9735 d 4+ %K+%β+=100
    49V 330 d 7/2- %K=100
    50V 1.4e+17 a 6+ %Abundance=0.250, %K+%β+=83 , %β-=17
    51V stable 7/2- %Abundance=99.750
    52V 3.743 m 3+ %β-=100
    53V 1.61 m 7/2- %β-=100
    54V 49.8 s 3+ %β-=100
    55V 6.54 s ( 7/2- ) %β-=100
    56V 230 ms (3+) %β-=100
    57V 320 ms ( 7/2- ) %β-=100, %β-n=?
    58V 200 ms (3+) %β-=100
    59V 130 ms ( 7/2- ) %β-=100
    60V 200 ms (3+) %β-=100, %β-n=0.03 sys
    61V
    62V (3+) %β-=?
    63V ( 7/2- ) %β-=?
    64V %β-=?

    Chromium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    43Cr 21 ms ( 3/2+ ) %K+%β+=100, %Kp=?, %Kα=?
    44Cr 53 ms 0+ %K+%β+=100, %Kp<10
    45Cr 50 ms %K+%β+=100, %Kp ~ 27
    46Cr 0.26 s 0+ %K+%β+=100
    47Cr 500 ms 3/2- %K+%β+=100
    48Cr 21.56 h 0+ %K+%β+=100
    49Cr 42.3 m 5/2- %K+%β+=100
    50Cr 1.8e+17 a 0+ %Abundance=4.345, %KK=?
    51Cr 27.7025 d 7/2- %K=100
    52Cr stable 0+ %Abundance=83.789
    53Cr stable 3/2- %Abundance=9.501
    54Cr stable 0+ %Abundance=2.365
    55Cr 3.497 m 3/2- %β-=100
    56Cr 5.94 m 0+ %β-=100
    57Cr 21.1 s 3/2-,5/2-, 7/2- %β-=100
    58Cr 7.0 s 0+ %β-=100
    59Cr 0.74 s %β-=100
    60Cr 0.57 s 0+ %β-=100
    61Cr 270 ms (5/2-) %β-=100, %β-n=0.6 sys
    62Cr 190 ms 0+ %β-=100, %β-n=1.0 sys
    63Cr 110 ms (1/2-) %β-=100, %β-n=1.4 sys
    64Cr 0+
    65Cr (1/2-) %β-=?
    66Cr 0+ %β-=100
    67Cr (1/2-) %β-=?

    Manganese

    Isotope Half-life Spin Parity Mode(s) or Abundance
    46Mn 41 ms %K=100, %Kp=32
    47Mn 100 ms %K+%β+=100, %Kp > 3.4
    48Mn 158.1 ms 4+ %K+%β+=100, %Kp=0.28 , %Kα<6E-4
    49Mn 382 ms 5/2- %K+%β+=100
    50Mn 283.88 ms 0+ %K+%β+=100
    50m1Mn 1.75 m 5+ %K+%β+=100
    51Mn 46.2 m 5/2- %K+%β+=100
    52Mn 5.591 d 6+ %K+%β+=100
    52m1Mn 21.1 m 2+ %K+%β+=98.25 , %IT=1.75
    53Mn 3.74e+6 a 7/2- %K=100
    54Mn 312.3 d 3+ %K+%β+=100, %β- < 2.9E-4
    55Mn stable 5/2- %Abundance=100
    56Mn 2.5785 h 3+ %β-=100
    57Mn 85.4 s 5/2- %β-=100
    58Mn 3.0 s 1+ %β-=100
    58m1Mn 65.2 s (4)+ %β- ~ 80, %IT ~ 20
    59Mn 4.6 s 3/2-,5/2- %β-=100
    60Mn 51 s 0+ %β-=100
    60m1Mn 1.77 s 3+ %β-=88.5 , %IT=11.5
    61Mn 0.71 s (5/2-) %β-=100
    62Mn 0.88 s (3+) %β-=100
    63Mn 0.25 s %β-=100
    64Mn 140 ms (3+) %β-=100, %β-n=1.4 sys
    65Mn 110 ms (5/2-) %β-=100, %β-n=6.9 sys
    66Mn 90 ms %β-=100, %β-n=11 sys

    Iron

    Isotope Half-life Spin Parity Mode(s) or Abundance
    46Fe 20 ms 0+ %K=100, %Kp=?
    47Fe 27 ms %K+%β+=100, %Kp=?
    48Fe 44 ms 0+ %K+%β+=100, %Kp > 3.6
    49Fe 70 ms ( 7/2- ) %K+%β+=100, %Kp > 62
    50Fe 150 ms 0+ %K+%β+=100, %β+P ~ 0
    51Fe 305 ms 5/2- %K+%β+=100
    52Fe 8.275 h 0+ %K+%β+=100
    52m1Fe 45.9 s (12+) %K+%β+=100
    53Fe 8.51 m 7/2- %K+%β+=100
    53m1Fe 2.58 m 19/2- %IT=100
    54Fe stable 0+ %Abundance=5.8
    55Fe 2.73 a 3/2- %K=100
    56Fe stable 0+ %Abundance=91.72
    57Fe stable 1/2- %Abundance=2.2
    58Fe stable 0+ %Abundance=0.28
    59Fe 44.503 d 3/2- %β-=100
    60Fe 1.5e+6 a 0+ %β-=100
    61Fe 5.98 m 3/2-,5/2- %β-=100
    62Fe 68 s 0+ %β-=100
    63Fe 6.1 s (5/2)- %β-=100
    64Fe 2.0 s 0+ %β-=100
    65Fe 0.4 s %β-=100
    66Fe 440 ms 0+ %β-=100
    67Fe 470 ms (1/2-) %β-=100, %β-n=1.1 s ys
    68Fe 0.10 s 0+ %β-=100
    69Fe 170 ms (1/2-) %β-=100, %β-n=6.9 sys

    Cobalt

    Isotope Half-life Spin Parity Mode(s) or Abundance
    50Co 44 ms (6+) %K+%β+=100, %Kp > 42
    51Co ( 7/2- )
    52Co 18 ms %K+%β+=100
    53Co 240 ms ( 7/2- ) %K+%β+=100
    53m1Co 247 ms (19/2-) %K+%β+ ~ 98.5, %p ~ 1.5
    54Co 193.23 ms 0+ %K+%β+=100
    54m1Co 1.48 m (7)+ %K+%β+=100
    55Co 17.53 h 7/2- %K+%β+=100
    56Co 77.27 d 4+ %K+%β+=100
    57Co 271.79 d 7/2- %K=100
    58Co 70.86 d 2+ %K+%β+=100
    58m1Co 9.04 h 5+ %IT=100
    59Co stable 7/2- %Abundance=100
    60Co 5.2714 a 5+ %β-=100
    60m1Co 10.467 m 2+ %IT=99.76 , %β-=0.24
    61Co 1.650 h 7/2- %β-=100
    62Co 1.50 m 2+ %β-=100
    62m1Co 13.91 m 5+ %β- ~ 100, %IT < 1
    63Co 27.4 s (7/2)- %β-=100
    64Co 0.30 s 1+ %β-=100
    65Co 1.20 s (7/2)- %β-=100
    66Co 0.233 s (3+) %β-=100
    67Co 0.42 s ( 7/2- ) %β-=100
    68Co 0.18 s %β-=100
    69Co 0.27 s %β-=100
    70Co 150 ms %β-=100, %β-n=2.5 sys
    71Co 210 ms ( 7/2- ) %β-=100, %β-n=2.6 sys
    72Co 90 ms %β-=100, %β-n=4.8 sys
    73Co ( 7/2- ) %β-=?
    74Co %β-=?
    75Co ( 7/2- ) %β-=?

    Nickel

    Isotope Half-life Spin Parity Mode(s) or Abundance
    52Ni 38 ms 0+ %K+%β+=100, %Kp=17
    53Ni 45 ms ( 7/2- ) %K+%β+=100, %Kp ~ 45
    54Ni 0+ %K+%β+=100
    55Ni 212.1 ms 7/2- %K+%β+=100
    56Ni 6.077 d 0+ %K+%β+=100
    57Ni 35.60 h 3/2- %K+%β+=100
    58Ni stable 0+ %Abundance=68.077
    59Ni 7.6e+4 a 3/2- %K+%β+=100
    60Ni stable 0+ %Abundance=26.223
    61Ni stable 3/2- %Abundance=1.140
    62Ni stable 0+ %Abundance=3.634
    63Ni 100.1 a 1/2- %β-=100
    64Ni stable 0+ %Abundance=0.926
    65Ni 2.5172 h 5/2- %β-=100
    66Ni 54.6 h 0+ %β-=100
    67Ni 21 s (1/2-) %β-=100
    68Ni 19 s 0+ %β-=100
    69Ni 11.4 s %β-=100
    70Ni 0+
    71Ni 1.86 s %β-=100
    72Ni 2.1 s 0+ %β-=100
    73Ni 0.70 s (7/2+) %β-=100, %β-n=0.3 sys
    74Ni 0.54 s 0+ %β-=100, %β-n=4.5 sys
    75Ni 0.6 s (7/2+) %β-=100, %β-n=8.4 sys
    76Ni 0.24 s 0+ %β-=100, %β-n=?

    Copper

    Isotope Half-life Spin Parity Mode(s) or Abundance
    57Cu 199.4 ms 3/2- %K+%β+=100
    58Cu 3.204 s 1+ %K+%β+=100
    59Cu 81.5 s 3/2- %K+%β+=100
    60Cu 23.7 m 2+ %K+%β+=100
    61Cu 3.333 h 3/2- %K+%β+=100
    62Cu 9.74 m 1+ %K+%β+=100
    63Cu stable 3/2- %Abundance=69.17
    64Cu 12.700 h 1+ %K+%β+=61.0 , %β-=39.0
    65Cu stable 3/2- %Abundance=30.83
    66Cu 5.120 m 1+ %β-=100
    67Cu 61.83 h 3/2- %β-=100
    68Cu 31.1 s 1+ %β-=100
    68m1Cu 3.75 m (6-) %IT=84 , %β-=16
    69Cu 2.85 m 3/2- %β-=100
    70Cu 4.5 s (1+) %β-=100
    70m1Cu 47 s (4)- %β-=100
    71Cu 19.5 s ( 3/2- ) %β-=100
    72Cu 6.6 s (1+) %β-=100
    73Cu 3.9 s %β-=100
    74Cu 1.594 s (1+,3+) %β-=100
    75Cu 1.224 s %β-=100, %β-n=3.5
    76Cu 0.641 s %β-=100, %β-n=3
    76m1Cu 1.27 s %β-=100
    77Cu 469 ms %β-=100, %β-n=?
    78Cu 342 ms %β-=100
    79Cu 188 ms %β-=100, %β-n=55

    Zinc

    Isotope Half-life Spin Parity Mode(s) or Abundance
    57Zn 40 ms ( 7/2- ) %K+%β+=100, %Kp > 65
    58Zn 65 ms 0+ %K+%β+=100
    59Zn 182.0 ms 3/2- %K+%β+=100, %Kp=0.10
    60Zn 2.38 m 0+ %K+%β+=100
    61Zn 89.1 s 3/2- %K+%β+=100
    62Zn 9.186 h 0+ %K+%β+=100
    63Zn 38.47 m 3/2- %K+%β+=100
    64Zn stable 0+ %Abundance=48.6
    65Zn 244.26 d 5/2- %K+%β+=100
    66Zn stable 0+ %Abundance=27.9
    67Zn stable 5/2- %Abundance=4.1
    68Zn stable 0+ %Abundance=18.8
    69Zn 56.4 m 1/2- %β-=100
    69m1Zn 13.76 h 9/2+ %IT=99.967 , %β-=0.033
    70Zn 5e+14 a 0+ %Abundance=0.6
    71Zn 2.45 m 1/2- %β-=100
    71m1Zn 3.96 h 9/2+ %β-=100, %IT < 0.05
    72Zn 46.5 h 0+ %β-=100
    73Zn 23.5 s (1/2)- %β-=100
    73m1Zn 5.8 s (7/2+) %β-=?, %IT=?
    74Zn 95.6 s 0+ %β-=100
    75Zn 10.2 s (7/2+) %β-=100
    76Zn 5.7 s 0+ %β-=100
    77Zn 2.08 s (7/2+) %β-=100
    77m1Zn 1.05 s (1/2-) %IT > 50, %β- < 50
    78Zn 1.47 s 0+ %β-=100
    79Zn 995 ms (9/2+) %β-=100, %β-n=1.3
    80Zn 0.545 s 0+ %β-=100, %β-n=1.0
    81Zn 0.29 s %β-=100, %β-n=7.5

    Gallium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    61Ga 0.15 s (3/2- ) %K+%β+=100
    62Ga 116.12 ms 0+ %K+%β+=100
    63Ga 32.4 s 3/2- ,5/2- %K+%β+=100
    64Ga 2.627 m 0+ %K+%β+=100
    65Ga 15.2 m 3/2- %K+%β+=100
    66Ga 9.49 h 0+ %K+%β+=100
    67Ga 3.2612 d 3/2- %K=100
    68Ga 67.629 m 1+ %K+%β+=100
    69Ga stable 3/2- %Abundance=60.108
    70Ga 21.14 m 1+ %β-=99.59 , %K=0.41
    71Ga stable 3/2- %Abundance=39.892
    72Ga 14.10 h 3- %β-=100
    72m1Ga 39.68 ms ( 0+) %IT=100
    73Ga 4.86 h 3/2- %β-=100
    74Ga 8.12 m (3-) %β-=100
    74m1Ga 9.5 s (0) %IT > 50, %β- < 50
    75Ga 126 s 3/2- %β-=100
    76Ga 32.6 s (2+,3+) %β-=100
    77Ga 13.2 s (3/2- ) %β-=100
    78Ga 5.09 s (3+) %β-=100
    79Ga 2.847 s (3/2- ) %β-=100, %β-n=0.089
    80Ga 1.697 s (3) %β-=100, %β-n=0.89
    81Ga 1.217 s (5/2- ) %β-=100 , %β-n=11.9
    82Ga 0.599 s (1,2,3) %β-=100, %β-n=22.3
    83Ga 0.31 s %β-=100, %β-n=40
    84Ga 85 ms %β-=100, %β-n=70


    Germanium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    61Ge 40 ms (3/2- ) %K+%β+=100, %Kp ~ 80
    62Ge 0+ %K+%β+=100
    63Ge 95 ms %K+%β+=100
    64Ge 63.7 s 0+ %K+%β+=100
    65Ge 30.9 s (3/2) - %K+%β+=100, %Kp=0.011
    66Ge 2.26 h 0+ %K+%β+=100
    67Ge 18.9 m 1/2- %K+%β+=100
    68Ge 270.8 d 0+ %K=100
    69Ge 39.05 h 5/2- %K+%β+=100
    70Ge stable 0+ %Abundance=21.23
    71Ge 11.43 d 1/2- %K=100
    71m1Ge 20.40 ms 9/2+ %IT=100
    72Ge stable 0+ %Abundance=27.66
    73Ge stable 9/2+ %Abundance=7.73
    73m1Ge 0.499 s 1/2- %IT=100
    74Ge stable 0+ %Abundance=35.94
    75Ge 82.78 m 1/2- %β-=100
    75m1Ge 47.7 s 7/2+ %IT=99.970 , %β-=0.030
    76Ge stable 0+ %Abundance=7.44
    77Ge 11.30 h 7/2+ %β-=100
    77m1Ge 52.9 s 1/2- %β-=81 , %IT=19
    78Ge 88.0 m 0+ %β-=100
    79Ge 18.98 s (1/2 ) - %β-=100
    79m1Ge 39.0 s (7/2+) %β-=96 , %IT=4
    80Ge 29.5 s 0+ %β-=100
    81Ge 7.6 s (9/2+) %β-=100
    81m1Ge 7.6 s (1/2+) %β-=100
    82Ge 4.60 s 0+ %β-=100
    83Ge 1.85 s (5/2+) %β-=100

    Arsenic

    Isotope Half-life Spin Parity Mode(s) or Abundance
    65As 0.19 s %K+%β+=100
    66As 95.77 ms %K+%β+=100
    67As 42.5 s (5/2- ) %K+%β+=100
    68As 151.6 s 3+ %K+%β+=100
    69As 15.2 m 5/2- %K+%β+=100
    70As 52.6 m 4(+) %K+%β+=100
    71As 65.28 h 5/2- %K+%β+=100
    72As 26.0 h 2- %K+%β+=100
    73As 80.30 d 3/2- %K=100
    74As 17.77 d 2- %β-=34 , %K+%β+=66
    75As stable 3/2- %Abundance=100
    75m1As 16.79 ms 9/2+ %IT=100
    76As 1.0778 d 2- %β-=100
    77As 38.83 h 3/2- %β-=100
    78As 90.7 m 2- %β-=100
    79As 9.01 m 3/2- %β-=100
    80As 15.2 s 1+ %β-=100
    81As 33.3 s 3/2- %β-=100
    82As 19.1 s (1+) %β-=100
    82m1As 13.6 s (5-) %β-=100
    83As 13.4 s (5/2- ,3/2- ) %β-=100
    84As 4.5 s (3-) %β-=100, %β-n=0.28
    85As 2.021 s (3/2- ) %β-=100, %β-n=59.4
    86As 0.945 s %β-=100, %β-n=33
    87As 0.48 s (3/2- ) %β-=100, %β-n=15.4

    Selenium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    67Se 60 ms %K+%β+=100, %Kp=0.5
    68Se 35.5 s 0+ %K+%β+=100
    69Se 27.4 s (3/2- ) %K+%β+=100, %Kp=0.045
    70Se 41.1 m 0+ %K+%β+=100
    71Se 4.74 m 3/2- ,5/2- %K+%β+=100
    72Se 8.40 d 0+ %K=100
    73Se 7.15 h 9/2+ %K+%β+=100
    73m1Se 39.8 m 3/2- %K+%β+=27.4 , %IT=72.6
    74Se stable 0+ %Abundance=0.89
    75Se 119.779 d 5/2+ %K=100
    76Se stable 0+ %Abundance=9.36
    77Se stable 1/2- %Abundance=7.63
    77m1Se 17.36 s 7/2+ %IT=100
    78Se stable 0+ %Abundance=23.78
    79Se 1.13e6 a 7/2+ %β-=100
    79m1Se 3.92 m 1/2- %IT=99.944 , %β-=0.056
    80Se stable 0+ %Abundance=49.61
    81Se 18.45 m 1/2- %β-=100
    81m1Se 57.28 m 7/2+ %IT=99.948 , %β-=0.052
    82Se 1.08e+20 a 0+ %Abundance=8.73, %ββ=100
    83Se 22.3 m 9/2+ %β-=100
    83m1Se 70.1 s 1/2- %β-=100
    84Se 3.10 m 0+ %β-=100
    85Se 31.7 s (5/2+) %β-=100
    86Se 15.3 s 0+ %β-=100
    87Se 5.29 s (5/2+) %β-=100, %β-n=0.36
    88Se 1.53 s 0+ %β-=100, %β-n=0.99
    89Se 0.41 s (5/2+) %β-=100, %β-n=7.8
    90Se 0+
    91Se 0.27 s %β-=100, %β-n=21

    Bromine

    Isotope Half-life Spin Parity Mode(s) or Abundance
    70Br 79.1 ms %K+%β+=100
    70m1Br 2.2 s %K+%β+=100
    71Br 21.4 s 5/2- %K+%β+=100
    72Br 78.6 s 3+ %K+%β+=100
    72m1Br 10.6 s 1- %IT ~ 100, %K+%β+=?
    73Br 3.4 m 1/2- %K+%β+=100
    74Br 25.4 m (0-) %K+%β+=100
    74m1Br 46 m 4(+) %K+%β+=100
    75Br 96.7 m 3/2- %K+%β+=100
    76Br 16.2 h 1- %K+%β+=100
    76m1Br 1.31 s (4) + %IT > 99.4, %K+%β+ < 0.6
    77Br 57.036 h 3/2- %K+%β+=100
    77m1Br 4.28 m 9/2+ %IT=100
    78Br 6.46 m 1+ %K+%β+=100, %β- < 0.01
    78m1Br 119.2 μs (4+)
    79Br stable 3/2- %Abundance=50.69
    79m1Br 4.86 s 9/2+ %IT=100
    80Br 17.68 m 1+ %β-=91.7 , %K+%β+=8.3
    80m1Br 4.4205 h 5- %IT=100
    81Br stable 3/2- %Abundance=49.31
    82Br 35.30 h 5- %β-=100
    82m1Br 6.13 m 2- %IT=97.6 , %β-=2.4
    83Br 2.40 h 3/2- %β-=100
    84Br 31.80 m 2- %β-=100
    84m1Br 6.0 m 6- %β-=100
    85Br 2.90 m 3/2- %β-=100
    86Br 55.1 s (2- ) %β-=100
    87Br 55.60 s 3/2- %β-=100, %β-n=2.52
    88Br 16.34 s (1,2- ) %β-=100, %β-n=6.58
    89Br 4.348 s (3/2- ,5/2- ) %β-=100, %β-n=13.8
    90Br 1.91 s %β-n=25.2 , %β-=100
    91Br 0.541 s %β-=100, %β-n=18.3
    92Br 0.343 s (2- ) %β-=100, %β-n=33
    93Br 102 ms (5/2- ) %β-=100, %β-n=10 +5-3
    94Br 70 ms %β-=100, %β-n=30

    Krypton

    Isotope Half-life Spin Parity Mode(s) or Abundance
    71Kr 64 ms %K+%β+=100, %Kp=5.2
    72Kr 17.2 s 0+ %K+%β+=100
    73Kr 27.0 s 5/2- %K+%β+=100, %Kp=0.68
    74Kr 11.50 m 0+ %K+%β+=100
    75Kr 4.3 m (5/2) + %K+%β+=100
    76Kr 14.8 h 0+ %K+%β+=100
    77Kr 74.4 m 5/2+ %K+%β+=100
    78Kr stable 0+ %Abundance=0.35
    79Kr 35.04 h 1/2- %K+%β+=100
    79m1Kr 50 s 7/2+ %IT=100
    80Kr stable 0+ %Abundance=2.25
    81Kr 2.29e+5 a 7/2+ %K=100
    81m1Kr 13.10 s 1/2- %IT=99.9975 , %K=2.5E-3
    82Kr stable 0+ %Abundance=11.6
    83Kr stable 9/2+ %Abundance=11.5
    83m1Kr 1.83 h 1/2- %IT=100
    84Kr stable 0+ %Abundance=57.0
    85Kr 10.756 a 9/2+ %β-=100
    85m1Kr 4.480 h 1/2- %IT=21.4 , %β-=78.6
    86Kr stable 0+ %Abundance=17.3
    87Kr 76.3 m 5/2+ %β-=100
    88Kr 2.84 h 0+ %β-=100
    89Kr 3.15 m (3/2+,5/2+) %β-=100
    90Kr 32.32 s 0+ %β-=100
    91Kr 8.57 s (5/2+) %β-=100
    92Kr 1.840 s 0+ %β-=100, %β-n=0.033
    93Kr 1.286 s (1/2+) %β-=100, %β-n=1.95
    94Kr 0.20 s 0+ %β-=100, %β-n=5.7
    95Kr 0.78 s 1/2 %β-=100

    Rubidium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    74Rb 64.9 ms (0+) %K+%β+=100
    75Rb 19.0 s (3/2- ,5/2-) %K+%β+=100
    76Rb 36.5 s 1(-) %K+%β+=100
    77Rb 3.77 m 3/2- %K+%β+=100
    78Rb 17.66 m 0(+) %K+%β+=100
    78m1Rb 5.74 m 4(-) %K+%β+=90 , %IT=10
    79Rb 22.9 m 5/2+ %K+%β+=100
    80Rb 34 s 1+ %K+%β+=100
    81Rb 4.576 h 3/2- %K+%β+=100
    81m1Rb 30.5 m 9/2+ %IT=97.6 , %K+%β+ =2.4
    82Rb 1.273 m 1+ %K+%β+=100
    82m1Rb 6.472 h 5- %K+%β+=100, %IT<0.33
    83Rb 86.2 d 5/2- %K=100
    83m1Rb 7.8 ms 9/2+ %IT=?, %K+%β+=?
    84Rb 32.77 d 2- %β-=3.8 , %K+%β+=96.2
    84m1Rb 20.26 m 6- %IT=100
    85Rb stable 5/2- %Abundance=72.165
    86Rb 18.631 d 2- %β-=99.9948 , %K=0.0052
    86m1Rb 1.017 m 6- %IT=100
    87Rb 4.75e10 a 3/2- %Abundance=27.835, %β-=100
    88Rb 17.78 m 2- %β-=100
    89Rb 15.15 m 3/2- %β-=100
    90Rb 158 s 0- %β-=100
    90m1Rb 258 s 3- %β-=97.4 , %IT=2.6
    91Rb 58.4 s 3/2(-) %β-=100
    92Rb 4.492 s 0- %β-=100, %β-n=0.0107
    93Rb 5.84 s 5/2- %β-=100, %β-n=1.39
    94Rb 2.702 s 3(-) %β-=100, %β-n=10.4
    95Rb 377.5 ms 5/2- %β-=100, %β-n=8.73
    96Rb 0.199 s 2+ %β-=100, %β-n=13.8
    97Rb 169.9 ms 3/2(+) %β-=100, %β-n=25.1
    98Rb 114 ms (1,0) %β-=100, %β-n=13.6 , %β-2n=0.051
    98m1Rb 96 ms (4,5) %β-=100
    99Rb 50.3 ms (5/2+ ) %β-=100, %β-n=20.7
    100Rb 51 ms %β-=100, %β-n=6 , %β-2n=0.16
    101Rb 32 ms (3/2+ ) %β-=100, %β-n=28
    102Rb 37 ms %β-=100 , %β-n=18

    Strontium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    75Sr 71 ms %K+%β+=100, %Kp=6.5
    76Sr 8.9 s 0+ %K+%β+=100
    77Sr 9.0 s 5/2+ %K+%β+=100 , %Kp < 0.25
    78Sr 2.5 m 0+ %K+%β+=100
    79Sr 2.25 m 3/2(-) %K+%β+=100
    80Sr 106.3 m 0+ %K+%β+=100
    81Sr 22.3 m 1/2- %K+%β+=100
    82Sr 25.55 d 0+ %K=100
    83Sr 32.41 h 7/2+ %K+%β+=100
    83m1Sr 4.95 s 1/2- %IT=100
    84Sr stable 0+ %Abundance=0.56
    85Sr 64.84 d 9/2+ %K=100
    85m1Sr 67.63 m 1/2- %IT=86.6 , %K+%β+=13.4
    86Sr stable 0+ %Abundance=9.86
    87Sr stable 9/2+ %Abundance=7.00
    87m1Sr 2.803 h 1/2- %K=0.30 , %IT=99.70
    88Sr stable 0+ %Abundance=82.58
    89Sr 50.53 d 5/2+ %β-=100
    90Sr 28.79 a 0+ %β-=100
    91Sr 9.63 h 5/2+ %β-=100
    92Sr 2.71 h 0+ %β-=100
    93Sr 7.423 m 5/2+ %β-=100
    94Sr 75.3 s 0+ %β-=100
    95Sr 23.90 s 1/2+ %β-=100
    96Sr 1.07 s 0+ %β-=100
    97Sr 426 ms 1/2+ %β-=100, %β-n=0.005
    98Sr 0.653 s 0+ %β-=100, %β-n=0.18
    99Sr 0.269 s 3/2+ %β-=100, %β-n=0.100
    100Sr 202 ms 0+ %β-=100, %β-n=0.78
    101Sr 118 ms (5/2-) %β-=100, %β-n=2.37

    Yttrium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    79Y 14.8 s (5/2+ ) %K+%β+=100, %Kp=?
    80Y 35 s (3,4,5) %K+%β+=100
    81Y 70.4 s (5/2+ ) %K+%β+=100
    82Y 9.5 s 1+ %K+%β+=100
    83Y 7.08 m (9/2+ ) %K+%β+=100
    83m1Y 2.85 m (3/2-) %K+%β+=60 , %IT=40
    84Y 4.6 s 1+ %K+%β+=100
    84m1Y 39.5 m (5-) %K+%β+=100
    85Y 2.68 h (1/2) - %K+%β+=100
    85m1Y 4.86 h 9/2+ %K+%β+=100, %IT < 2E-3
    86Y 14.74 h 4- %K+%β+=100
    86m1Y 48 m (8+ ) %IT=99.31 , %K+%β+=0.69
    87Y 79.8 h 1/2- %K+%β+=100
    87m1Y 13.37 h 9/2+ %IT=98.43 , %K+%β+=1.57
    88Y 106.65 d 4- %K+%β+=100
    88m1Y 13.9 ms (8) + %IT=100
    89Y stable 1/2- %Abundance=100
    89m1Y 16.06 s 9/2+ %IT=100
    90Y 64.00 h 2- %β-=100
    90m1Y 3.19 h 7+ %IT=99.9982 , %β-=0.0018
    91Y 58.51 d 1/2- %β-=100
    91m1Y 49.71 m 9/2+ %IT=100, %β-<1.5
    92Y 3.54 h 2- %β-=100
    93Y 10.18 h 1/2- %β-=100
    93m1Y 0.82 s 7/2+ %IT=100
    94Y 18.7 m 2- %β-=100
    95Y 10.3 m 1/2- %β-=100
    96Y 5.34 s 0- %β-=100
    96m1Y 9.6 s (8+ ) %β- ~ 100
    97Y 3.75 s (1/2-) %β-=100, %β-n=0.055

    Zirconium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    81Zr 15 s %K+%β+=100, %Kp=?
    82Zr 32 s 0+ %K+%β+=100
    83Zr 44 s (1/2-) %K+%β+=100, %Kp=?
    84Zr 25.9 m 0+ %K+%β+=100
    85Zr 7.86 m 7/2+ %K+%β+=100
    85m1Zr 10.9 s (1/2-) %K+%β+ > 8, %IT < 92
    86Zr 16.5 h 0+ %K+%β+=100
    87Zr 1.68 h (9/2) + %K+%β+=100
    87m1Zr 14.0 s (1/2) - %IT=100
    88Zr 83.4 d 0+ %K=100
    89Zr 78.41 h 9/2+ %K+%β+=100
    89m1Zr 4.18 m 1/2- %K+%β+=6.23 , %IT=93.77
    90Zr stable 0+ %Abundance=51.45
    90m1Zr 809.2 ms 5- %IT=100
    91Zr stable 5/2+ %Abundance=11.22
    92Zr stable 0+ %Abundance=17.15
    93Zr 1.53e+6 a 5/2+ %β-=100
    94Zr stable 0+ %Abundance=17.38
    95Zr 64.02 d 5/2+ %β-=100
    96Zr 3.8e19 a 0+ %Abundance=2.80, %β- β-=100
    97Zr 16.91 h 1/2+ %β-=100
    98Zr 30.7 s 0+ %β-=100
    99Zr 2.1 s (1/2+ ) %β-=100
    100Zr 7.1 s 0+ %β-=100
    101Zr 2.3 s (3/2+ ) %β-=100
    102Zr 2.9 s 0+ %β-=100
    103Zr 1.3 s (5/2-) %β-=100
    104Zr 1.2 s 0+ %β-=100

    Niobium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    83Nb 4.1 s (5/2+ ) %K+%β+=100
    84Nb 12 s 3+ %K+%β+=100, %Kp=?
    85Nb 20.9 s (9/2+ ) %K+%β+=100
    86Nb 88 s (5+ ) %K+%β+=100
    86m1Nb 56 s %K+%β+=100
    87Nb 2.6 m (9/2+ ) %K+%β+=100
    87m1Nb 3.7 m (1/2-) %K+%β+=100
    88Nb 14.5 m (8+ ) %K+%β+=100
    88m1Nb 7.8 m (4-) %K+%β+=100
    89Nb 1.9 h (9/2+ ) %K+%β+=100
    89m1Nb 1.18 h (1/2) - %K+%β+=100
    90Nb 14.60 h 8+ %K+%β+=100
    90m1Nb 18.81 s 4- %IT=100
    90m2Nb 6.19 ms 1+ %IT=100
    91Nb 680 a 9/2+ %K+%β+=100
    91m1Nb 60.86 d 1/2- %IT=93 , %K+%β+=7
    92Nb 3.47e+7 a (7) + %K+%β+=100, %β- < 0.05
    92m1Nb 10.15 d (2) + %K+%β+=100
    93Nb stable 9/2+ %Abundance=100
    93m1Nb 16.13 a 1/2- %IT=100
    94Nb 2.03e+4 a (6) + %β-=100
    94m1Nb 6.263 m 3+ %IT=99.50 , %β-=0.50
    95Nb 34.975 d 9/2+ %β-=100
    95m1Nb 86.6 h 1/2- %β-=5.6 , %IT=94.4
    96Nb 23.35 h 6+ %β-=100
    97Nb 72.1 m 9/2+ %β-=100
    97m1Nb 52.7 s 1/2- %IT=100
    98Nb 2.86 s 1+ %β-=100
    98m1Nb 51.3 m (5+ ) %β-=99.9 , %IT < 0.2
    99Nb 15.0 s 9/2+ %β-=100

    Molybdenium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    86Mo 19.6 s 0+ %K+%β+=100
    87Mo 13.4 s (7/2+ ) %K+%β+=100, %β+P=?
    88Mo 8.0 m 0+ %K+%β+=100
    89Mo 2.04 m (9/2+ ) %K+%β+=100
    89m1Mo 190 ms (1/2-) %IT=100
    90Mo 5.56 h 0+ %K+%β+=100
    91Mo 15.49 m 9/2+ %K+%β+=100
    91m1Mo 65.0 s 1/2- %K+%β+=49.9 , %IT=50.1
    92Mo stable 0+ %Abundance=14.84
    93Mo 4.0e+3 a 5/2+ %K=100
    93m1Mo 6.85 h 21/2+ %IT=99.88 , %K+%β+=0.12
    94Mo stable 0+ %Abundance=9.25
    95Mo stable 5/2+ %Abundance=15.92
    96Mo stable 0+ %Abundance=16.68
    97Mo stable 5/2+ %Abundance=9.55
    98Mo stable 0+ %Abundance=24.13
    99Mo 65.94 h 1/2+ %β-=100
    100Mo 1.00e+19 a 0+ %Abundance=9.63, %ββ=100
    101Mo 14.61 m 1/2+ %β-=100
    102Mo 11.3 m 0+ %β-=100
    103Mo 67.5 s (3/2+ ) %β-=100
    104Mo 60 s 0+ %β-=100
    105Mo 35.6 s (5/2-) %β-=100
    106Mo 8.4 s 0+ %β-=100
    107Mo 3.5 s %β-=100
    108Mo 1.09 s 0+ %β-=100
    109Mo 0.53 s %β-=100
    110Mo 0.30 s 0+ %β-=100

    Technetium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    88Tc 6.4 s (6,7,8) %K+%β+=100
    88m1Tc 5.8 s (2,3) %K+%β+=100
    89Tc 12.8 s (9/2+ ) %K+%β+=100
    89m1Tc 12.9 s (1/2-) %K+%β+=100
    90Tc 49.2 s (8+ ) %K+%β+=100
    90m1Tc 8.7 s 1+ %K+%β+=100
    91Tc 3.14 m (9/2) + %K+%β+=100
    91m1Tc 3.3 m (1/2) - %K+%β+=100, %IT<1
    92Tc 4.23 m (8) + %K+%β+=100
    93Tc 2.75 h 9/2+ %K+%β+=100
    93m1Tc 43.5 m 1/2- %IT=76.6 , %K+%β+=23.4
    94Tc 293 m 7+ %K+%β+=100
    94m1Tc 52.0 m (2) + %K+%β+=100, %IT<0.1
    95Tc 20.0 h 9/2+ %K+%β+=100
    95m1Tc 61 d 1/2- %K+%β+=96.12 , %IT=3.88
    96Tc 4.28 d 7+ %K+%β+=100
    96m1Tc 51.5 m 4+ %IT=98.0 , %K+%β+=2.0
    97Tc 2.6e6 a 9/2+ %K=100
    97m1Tc 90.1 d 1/2- %IT=100, %K<0.34
    98Tc 4.2e+6 a (6) + %β-=100
    99Tc 2.111e+5 a 9/2+ %β-=100
    99m1Tc 6.01 h 1/2- %IT=99.9963 , %β-=0.0037
    100Tc 15.8 s 1+ %β-=99.9982 , %K=0.0018
    101Tc 14.22 m 9/2+ %β-=100
    102Tc 5.28 s 1+ %β-=100
    102m1Tc 4.35 m (4,5) %β-=98 , %IT=2
    103Tc 54.2 s 5/2+ %β-=100
    104Tc 18.3 m (3+ ) %β-=100
    105Tc 7.6 m (3/2-) %β-=100


    Ruthenium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    90Ru 11 s 0+ %K+%β+=100
    91Ru 9 s (9/2+ ) %K+%β+=100
    91m1Ru 7.6 s (1/2-) %K+%β+=?, %Kp=?, %IT=?
    92Ru 3.65 m 0+ %K+%β+=100
    93Ru 59.7 s (9/2) + %K+%β+=100
    93m1Ru 10.8 s (1/2) - %IT=22.0 , %K+%β+=78.0 , %Kp=0.027
    94Ru 51.8 m 0+ %K+%β+=100
    95Ru 1.643 h 5/2+ %K+%β+=100
    96Ru stable 0+ %Abundance=5.52
    97Ru 2.9 d 5/2+ %K=100
    98Ru stable 0+ %Abundance=1.88
    99Ru stable 5/2+ %Abundance=12.7
    100Ru stable 0+ %Abundance=12.6
    101Ru stable 5/2+ %Abundance=17.0
    102Ru stable 0+ %Abundance=31.6
    103Ru 39.26 d 3/2+ %β-=100
    103m1Ru 1.69 ms 11/2- %IT=100
    104Ru stable 0+ %Abundance=18.7
    105Ru 4.44 h 3/2+ %β-=100
    106Ru 373.59 d 0+ %β-=100
    107Ru 3.75 m (5/2) + %β-=100
    108Ru 4.55 m 0+ %β-=100
    109Ru 34.5 s (5/2+ ) %β-=100
    110Ru 14.6 s 0+ %β-=100
    111Ru 2.12 s %β-=100
    112Ru 1.75 s 0+ %β-=100
    113Ru 0.80 s %β-=100
    114Ru 0.53 s 0+ %β-=100
    115Ru 0.40 s %β-=100, %β-n=?

    Rhodium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    94Rh 70.6 s (3+ ) %K+%β+=100, %Kp=1.8
    94m1Rh 25.8 s (8+ ) %K+%β+=100
    95Rh 5.02 m (9/2) + %K+%β+=100
    95m1Rh 1.96 m (1/2) - %K+%β+=12 , %IT=88
    96Rh 9.90 m 6+ %K+%β+=100
    96m1Rh 1.51 m 3+ %IT=60 , %K+%β+=40
    97Rh 30.7 m (9/2) + %K+%β+=100
    97m1Rh 46.2 m (1/2) - %K+%β+=94.4 , %IT=5.6
    98Rh 8.7 m (2) + %K+%β+=100
    98m1Rh 3.5 m (5+ ) %K+%β+>0, %IT=?
    99Rh 16.1 d 1/2- %K+%β+=100
    99m1Rh 4.7 h 9/2+ %K+%β+ > 99.84 , %IT<0.16
    100Rh 20.8 h 1- %K+%β+=100
    100m1Rh 4.6 m (5+ ) %IT ~ 98.3, %K+%β+ ~ 1.7
    101Rh 3.3 a 1/2- %K=100
    101m1Rh 4.34 d 9/2+ %K=92.80 , %IT=7.20
    102Rh 207 d (1- ,2-) %β-=20 , %K+%β+=80
    102m1Rh 2.9 a 6(+) %K+%β+=99.767 , %IT=0.233
    103Rh stable 1/2- %Abundance=100
    103m1Rh 56.12 m 7/2+ %IT=100
    104Rh 42.3 s 1+ %β-= 99.55 , %K+%β+= 0.45
    104m1Rh 4.34 m 5+ %IT=99.87 , %β-=0.13
    105Rh 35.36 h 7/2+ %β-=100
    105m1Rh 45 s 1/2- %IT=100
    106Rh 29.80 s 1+ %β-=100
    106m1Rh 131 m (6) + %β-=100
    107Rh 21.7 m 7/2+ %β-=100
    108Rh 16.8 s 1+ %β-=100
    108m1Rh 6.0 m (5+ ) %β-=100
    109Rh 80 s 7/2+ %β-=100

    Palladium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    96Pd 122 s 0+ %K+%β+=100
    97Pd 3.10 m (5/2+ ) %K+%β+=100
    98Pd 17.7 m 0+ %K+%β+=100
    99Pd 21.4 m (5/2) + %K+%β+=100
    100Pd 3.63 d 0+ %K=100
    101Pd 8.47 h 5/2+ %K+%β+=100
    102Pd stable 0+ %Abundance=1.02
    103Pd 16.991 d 5/2+ %K=100
    104Pd stable 0+ %Abundance=11.14
    105Pd stable 5/2+ %Abundance=22.33
    106Pd stable 0+ %Abundance=27.33
    107Pd 6.5e+6 a 5/2+ %β-=100
    107m1Pd 21.3 s 11/2- %IT=100
    108Pd stable 0+ %Abundance=26.46
    109Pd 13.7012 h 5/2+ %β-=100
    109m1Pd 4.696 m 11/2- %IT=100
    110Pd stable 0+ %Abundance=11.72
    111Pd 23.4 m 5/2+ %β-=100
    111m1Pd 5.5 h 11/2- %IT=73 , %β-=27
    112Pd 21.03 h 0+ %β-=100
    113Pd 93 s (5/2+ ) %β-=100
    113m1Pd 100 s %β-=?
    113m2Pd 0.3 s (9/2-) %IT=100
    114Pd 2.42 m 0+ %β-=100
    115Pd 25 s (5/2+ ) %β-=100
    115m1Pd 50 s (11/2-) %β-=92.0 , %IT=8.0
    116Pd 11.8 s 0+ %β-=100
    117Pd 4.3 s (5/2+ ) %β-=100
    117m1Pd 19.1 ms (11/2-) %IT=100
    118Pd 1.9 s 0+ %β-=100
    119Pd 0.92 s %β-=100
    120Pd 0.5 s 0+ %β-=100

    Silver

    Isotope Half-life Spin Parity Mode(s) or Abundance
    94Ag 10 ms 0+ %K+%β+=100
    94m1Ag 0.42 s (9+ ) %K+%β+=100, %Kp=?
    95Ag 2.0 s %K+%β+=100, %Kp=?
    96Ag 5.1 s (8+ , 9+ ) %K+%β+=100, %Kp=8.0
    97Ag 19 s (9/2+ ) %K+%β+=100
    98Ag 46.7 s (5+ ) %K+%β+=100
    99Ag 124 s (9/2) + %K+%β+=100
    99m1Ag 10.5 s (1/2-) %IT=100
    100Ag 2.01 m (5) + %K+%β+=100
    100m1Ag 2.24 m (2) + %K+%β+=?, %IT=?
    101Ag 11.1 m 9/2+ %K+%β+=100
    101m1Ag 3.10 s (1/2) - %IT=100
    102Ag 12.9 m 5+ %K+%β+=100
    102m1Ag 7.7 m 2+ %IT=49 , %K+%β+=51
    103Ag 65.7 m 7/2+ %K+%β+=100
    103m1Ag 5.7 s 1/2- %IT=100
    104Ag 69.2 m 5+ %K+%β+=100
    104m1Ag 33.5 m 2+ %K+%β+=100, %IT < 0.07
    105Ag 41.29 d 1/2- %K+%β+=100
    105m1Ag 7.23 m 7/2+ %IT=99.66 , %K+%β+=0.34
    106Ag 23.96 m 1+ %K+β+=99.5 , %β- < 1
    106m1Ag 8.28 d 6+ %K+β+=100
    107Ag stable 1/2- %Abundance=51.839
    107m1Ag 44.3 s 7/2+ %IT=100
    108Ag 2.37 m 1+ %β-=97.15 , %K+%β+=2.85
    108m1Ag 418 a 6+ %IT=8.7 , %K+%β+=91.3
    109Ag stable 1/2- %Abundance=48.161
    109m1Ag 39.6 s 7/2+ %IT=100
    110Ag 24.6 s 1+ %β-=99.70 , %K=0.30
    110m1Ag 249.79 d 6+ %β-=98.64 , %IT=1.36
    111Ag 7.45 d 1/2- %β-=100
    111m1Ag 64.8 s 7/2+ %IT=99.3, %β-=0.7
    112Ag 3.130 h 2(-) %β-=100
    113Ag 5.37 h 1/2- %β-=100
    113m1Ag 68.7 s 7/2+ %IT= 64 , %β-=36
    114Ag 4.6 s 1+ %β-=100
    114m1Ag 1.50 ms (LE 6+ ) %IT=100
    115Ag 20.0 m 1/2- %β-=100
    115m1Ag 18.0 s 7/2+ %β-=79.0 , %IT=21.0
    116Ag 2.68 m (2) - %β-=100
    116m1Ag 8.6 s (5+ ) %IT=6.0 , %β-=94.0
    117Ag 72.8 s (1/2-) %β-=100
    117m1Ag 5.34 s (7/2+ ) %β-=94.0 , %IT=6.0
    118Ag 3.76 s (1) - %β-=100
    118m1Ag 2.0 s (4) + %β-=59, %IT=41
    119Ag 2.1 s (7/2+ ) %β-=100
    119m1Ag 6.0 s (1/2-) %β-=100
    120Ag 1.23 s (3+ ) %β-=100
    120m1Ag 0.32 s (6-) %β- ~ 63, %IT ~ 37
    121Ag 0.78 s (7/2+ ) %β-=100 , %β-n=0.080
    122Ag 0.48 s (3+ ) %β-=100, %β-n=?
    122m1Ag 1.5 s %β-=100
    123Ag 0.309 s (7/2+ ) %β-=100, %β-n=55
    124Ag 0.172 s %β-=100 , %β-n > 0.1
    125Ag 166 ms %β-=100, %β-n=?
    126Ag 107 ms %β-=100
    127Ag 109 ms %β-=100
    128Ag 58 ms %β-=100, %β-n=?

    Cadmium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    97Cd 3 s %K+%β+=100, %Kp=?
    98Cd 9.2 s 0+ %K+%β+=100
    99Cd 16 s (5/2+ ) %K+%β+=100, %Kp=0.17 +11-5, %Kα<1E-4
    100Cd 49.1 s 0+ %K+%β+=100
    101Cd 1.36 m (5/2+ ) %K+%β+=100
    102Cd 5.5 m 0+ %K+%β+=100
    103Cd 7.3 m (5/2+ ) %K+%β+=100
    104Cd 57.7 m 0+ %K+%β+=100
    105Cd 55.5 m 5/2+ %K+%β+ =100
    106Cd stable 0+ %Abundance=1.25
    107Cd 6.50 h 5/2+ %K+%β+=100
    108Cd stable 0+ %Abundance=0.89
    109Cd 462.6 d 5/2+ %K=100
    110Cd stable 0+ %Abundance=12.49
    111Cd stable 1/2+ %Abundance=12.80
    111m1Cd 48.54 m 11/2- %IT=100
    112Cd stable 0+ %Abundance=24.13
    113Cd 7.7e+15 a 1/2+ %Abundance=12.22, %β-=100
    113m1Cd 14.1 a 11/2- %β-=99.86, %IT=0.14
    114Cd stable 0+ %Abundance=28.73
    115Cd 53.46 h 1/2+ %β-=100
    115m1Cd 44.6 d 11/2- %β-=100
    116Cd stable 0+ %Abundance=7.49
    117Cd 2.49 h 1/2+ %β-=100
    117m1Cd 3.36 h (11/2) - %β-=100
    118Cd 50.3 m 0+ %β-=100
    119Cd 2.69 m 3/2+ %β-=100
    119m1Cd 2.20 m (11/2-) %β-=100
    120Cd 50.80 s 0+ %β-=100
    121Cd 13.5 s (3/2+ ) %β-=100
    121m1Cd 8.3 s (11/2-) %β-=100
    122Cd 5.24 s 0+ %β-=100
    123Cd 2.10 s (3/2) + %β-=100
    123m1Cd 1.82 s (11/2-) %β-=100
    124Cd 1.25 s 0+ %β-=100
    125Cd 0.65 s (3/2+ ) %β-=100
    125m1Cd 0.57 s (11/2-) %β-=100
    126Cd 0.506 s 0+ %β-=100
    127Cd 0.37 s (3/2+ ) %β-=100
    128Cd 0.34 s 0+ %β-=100
    129Cd 0.27 s (3/2+ ) %β-=100
    130Cd 0.20 s 0+ %β-=100 , %β-n ~ 4

    Indium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    100In 7.0 s %K+%β+=100, %Kp>3.9
    101In 15.1 s %K+%β+ ~ 100, %Kp=?
    102In 22 s (6+ ) %K+%β+=100, %Kp=0.0093
    103In 65 s (9/2) + %K+%β+=100
    103m1In 34 s (1/2-) %K+%β+=67, %IT=33
    104In 1.80 m (6+ ) %K+%β+=100
    104m1In 15.7 s (3+ ) %IT=80, %K+%β+=20
    105In 5.07 m (9/2) + %K+%β+=100
    105m1In 48 s (1/2) - %IT=100
    106In 6.2 m 7+ %K+%β+=100
    106m1In 5.2 m (3+ ) %K+%β+=100
    107In 32.4 m 9/2+ %K+%β+=100
    107m1In 50.4 s 1/2- %IT=100
    108In 58.0 m 7+ %K+%β+=100
    108m1In 39.6 m 2+ %K+%β+=100
    109In 4.2 h 9/2+ %K+%β+=100
    109m1In 1.34 m 1/2- %IT=100
    109m2In 0.209 s (19/2+ ) %IT=100
    110In 4.9 h 7+ %K+%β+=100
    110m1In 69.1 m 2+ %K+%β+=100
    111In 2.8047 d 9/2+ %K=100
    111m1In 7.7 m 1/2- %IT=100
    112In 14.97 m 1+ %β-=44 , %K+%β+=56
    112m1In 20.56 m 4+ %IT=100
    113In stable 9/2+ %Abundance=4.3
    113m1In 1.6582 h 1/2- %IT=100
    114In 71.9 s 1+ %β-=99.50 , %K+%β+=0.50
    114m1In 49.51 d 5+ %IT=96.75 , %K+%β+=3.25
    114m2In 43.1 ms 8- %IT=100
    115In 4.41e+14 a 9/2+ %Abundance=95.7, %β-=100
    115m1In 4.486 h 1/2- %IT=95.0 , %β-=5.0
    116In 14.10 s 1+ %β- > 99.94 , %K < 0.06
    116m1In 54.29 m 5+ %β-=100
    116m2In 2.18 s 8- %IT=100
    117In 43.2 m 9/2+ %β-=100
    117m1In 116.2 m 1/2- %β-=52.9 , %IT=47.1
    118In 5.0 s 1+ %β-=100
    118m1In 4.45 m 5+ %β-=100
    118m2In 8.5 s 8- %β-=1.4 , %IT=98.6
    119In 2.4 m 9/2+ %β-=100
    119m1In 18.0 m 1/2- %β-=94.4 , %IT=5.6
    120In 3.08 s 1+ %β-=100
    120m1In 46.2 s (3,4,5) + %β-=100
    120m2In 47.3 s (8-) %β-=100
    121In 23.1 s 9/2+ %β-=100
    121m1In 3.88 m 1/2- %β-=98.8 , %IT=1.2
    122In 1.5 s 1+ %β-=100
    122m1In 10.3 s 5+ %β-=100
    122m2In 10.8 s 8- %β-=100
    123In 5.98 s 9/2+ %β-=100
    123m1In 47.8 s 1/2- %β-=100
    124In 3.11 s 3+ %β-=100
    124m1In 3.7 s (8-) %β-=100
    125In 2.36 s 9/2(+) %β-=100
    125m1In 12.2 s 1/2(-) %β-=100
    126In 1.60 s 3(+) %β-=100
    126m1In 1.64 s 7- ,8- ,9- %β-=100
    127In 1.09 s (9/2+ ) %β-=100, %β-n < 0.03
    127m1In 3.67 s (1/2-) %β-=100, %β-n=0.69
    128In 0.84 s (3+ ) %β-=100, %β-n < 0.04
    128m1In 0.72 s (8-) %β-=100, %β-n < 0.04
    129In 0.61 s (9/2+ ) %β-=100, %β-n=0.25
    129m1In 1.23 s (1/2-) %β- > 99.7, %β-n=2.5 , %IT < 0.3
    130In 0.32 s 1(-) %β-=100 , %β-n=0.90
    130m1In 0.55 s (10- ) %β-=100 , %β-n < 1.67
    130m2In 0.55 s (5+ ) %β-=100 , %β-n < 1.67
    131In 0.282 s (9/2+ ) %β-=100, %β-n < 2.2
    131m1In 0.35 s (1/2-) %β-=100, %β-n < 2.2 , %IT < 0.04
    131m2In 0.32 s (21/2+ ) %β-=100, %β-n < 2.2
    132In 0.201 s (7-) %β-=100 , %β-n=6.2
    133In 180 ms (9/2+ ) %β-=100, %β-n=85
    134In 138 ms %β-=100, %β-n=65

    Tin

    Isotope Half-life Spin Parity Mode(s) or Abundance
    100Sn 0.94 s 0+ %K+%β+=100, %Kp < 17
    101Sn 3 s %K+%β+=100, %Kp=?
    102Sn 4.5 s 0+ %K+%β+=100
    103Sn 7 s %K+%β+=100
    104Sn 20.8 s 0+ %K+%β+=100
    105Sn 31 s %K+%β+=100, %β+P=?
    106Sn 115 s 0+ %K+%β+=100
    107Sn 2.90 m (5/2+ ) %K+%β+=100
    108Sn 10.30 m 0+ %K+%β+=100
    109Sn 18.0 m 5/2(+) %K+%β+=100
    110Sn 4.11 h 0+ %K=100
    111Sn 35.3 m 7/2+ %K+%β+=100
    112Sn stable 0+ %Abundance=0.97
    113Sn 115.09 d 1/2+ %K+%β+=100
    113m1Sn 21.4 m 7/2+ %IT=91.1 , %K+%β+=8.9
    114Sn stable 0+ %Abundance=0.65
    115Sn stable 1/2+ %Abundance=0.34
    116Sn stable 0+ %Abundance=14.53
    117Sn stable 1/2+ %Abundance=7.68
    117m1Sn 13.60 d 11/2- %IT=100
    118Sn stable 0+ %Abundance=24.23
    119Sn stable 1/2+ %Abundance=8.59
    119m1Sn 293.1 d 11/2- %IT=100
    120Sn stable 0+ %Abundance=32.59
    121Sn 27.06 h 3/2+ %β-=100
    121m1Sn 55 a 11/2- %IT=77.6 , %β-=22.4
    122Sn stable 0+ %Abundance=4.63
    123Sn 129.2 d 11/2- %β-=100
    123m1Sn 40.06 m 3/2+ %β-=100
    124Sn stable 0+ %Abundance=5.79
    125Sn 9.64 d 11/2- %β-=100
    125m1Sn 9.52 m 3/2+ %β-=100
    126Sn 1e+5 a 0+ %β-=100
    127Sn 2.10 h (11/2-) %β-=100
    127m1Sn 4.13 m (3/2+ ) %β-=100
    128Sn 59.07 m 0+ %β-=100
    128m1Sn 6.5 s (7-) %IT=100
    129Sn 2.23 m (3/2+ ) %β-=100
    129m1Sn 6.9 m (11/2-) %β-=100, %IT ~ 2E-4
    130Sn 3.72 m 0+ %β-=100
    130m1Sn 1.7 m (7-) %β-=100
    131Sn 56.0 s (3/2+ ) %β-=100
    131m1Sn 58.4 s (11/2-) %β-=100, %IT < 0.009
    132Sn 39.7 s 0+ %β-=100
    133Sn 1.45 s (7/2-) %β-=100, %β-n=0.08
    134Sn 1.12 s 0+ %β-=100, %β-n=17

    Antimony

    Isotope Half-life Spin Parity Mode(s) or Abundance
    108Sb 7.4 s (4+ ) %K+%β+=100, %Kp=?
    109Sb 17.0 s (5/2+ ) %K+%β+=100
    110Sb 23.0 s 3+ %K+%β+=100
    111Sb 75 s (5/2+ ) %K+%β+=100
    112Sb 51.4 s 3+ %K+%β+=100
    113Sb 6.67 m 5/2+ %K+%β+=100
    114Sb 3.49 m 3+ %K+%β+=100
    115Sb 32.1 m 5/2+ %K+%β+=100
    116Sb 15.8 m 3+ %K+%β+=100
    116m1Sb 60.3 m 8- %K+%β+=100
    117Sb 2.80 h 5/2+ %K+%β+=100
    118Sb 3.6 m 1+ %K+%β+=100
    118m1Sb 5.00 h 8- %K+%β+=100
    119Sb 38.19 h 5/2+ %K=100
    119m1Sb 0.85 s (25/2+ ) %IT=100
    120Sb 15.89 m 1+ %K+%β+=100
    120m1Sb 5.76 d 8- %K+%β+=100
    121Sb stable 5/2+ %Abundance=57.36
    122Sb 2.7238 d 2- %β-=97.59 , %K+%β+=2.41
    122m1Sb 4.191 m (8) - %IT=100
    123Sb stable 7/2+ %Abundance=42.64
    124Sb 60.20 d 3- %β-=100
    124m1Sb 93 s 5+ %IT=75 , %β-=25
    124m2Sb 20.2 m (8) - %IT=100
    125Sb 2.7582 a 7/2+ %β-=100
    126Sb 12.46 d (8) - %β-=100
    126m1Sb 19.15 m (5) + %β-=86 , %IT=14
    126m2Sb 11 s (3) - %IT=100
    127Sb 3.85 d 7/2+ %β-=100
    128Sb 9.01 h 8- %β-=100
    128m1Sb 10.4 m 5+ %β-=96.4 , %IT=3.6
    129Sb 4.40 h 7/2+ %β-=100
    129m1Sb 17.7 m (19/2-) %β-=85, %IT=15
    130Sb 39.5 m (8-) %β-=100
    130m1Sb 6.3 m (5) + %β-=100
    131Sb 23.03 m (7/2+ ) %β-=100
    132Sb 2.79 m (4+ ) %β-=100
    132m1Sb 4.10 m (8-) %β-=100
    133Sb 2.5 m (7/2+ ) %β-=100
    134Sb 0.78 s (0- ) %β-=100
    134m1Sb 10.23 s (7-) %β-=100, %β-n=0.091
    135Sb 1.71 s (7/2+ ) %β-=100 , %β-n=16.4
    136Sb 0.82 s %β-=100, %β-n=24.0, %β-2n=?

    Tellurium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    106Te 60 μs 0+ %α=100
    107Te 3.1 ms %α > 70, %K+%β+ < 30
    108Te 2.1 s 0+ %K+%β+=51 , %α=49 , %β+P=2.4
    109Te 4.6 s %K+%β+=96.1 , %α=3.9 , %Kp=?
    110Te 18.6 s 0+ %K+%β+ ~ 100, %α ~ 0.003
    111Te 19.3 s (5/2+ ) %K+%β+=100, %Kp=?
    112Te 2.0 m 0+ %K+%β+=100
    113Te 1.7 m (7/2+ ) %K+%β+=100
    114Te 15.2 m 0+ %K+%β+=100
    115Te 5.8 m 7/2+ %K+%β+=100
    115m1Te 6.7 m (1/2) + %K+%β+ < 100, %IT=?
    116Te 2.49 h 0+ %K+%β+=100
    117Te 62 m 1/2+ %K+%β+=100
    117m1Te 103 ms 11/2- %IT=100
    118Te 6.00 d 0+ %K=100
    119Te 16.03 h 1/2+ %K+%β+=100
    119m1Te 4.70 d 11/2- %K+%β+=100, %IT < 0.008
    120Te stable 0+ %Abundance=0.096
    121Te 16.78 d 1/2+ %K+%β+=100
    121m1Te 154 d 11/2- %IT=88.6 , %K+%β+=11.4
    122Te stable 0+ %Abundance=2.603
    123Te 1e+13 a 1/2+ %Abundance=0.908, %K=100
    123m1Te 119.7 d 11/2- %IT=100
    124Te stable 0+ %Abundance=4.816
    125Te stable 1/2+ %Abundance=7.139
    125m1Te 57.40 d 11/2- %IT=100
    126Te stable 0+ %Abundance=18.95
    127Te 9.35 h 3/2+ %β-=100
    127m1Te 109 d 11/2- %IT=97.6 , %β-=2.4
    128Te 2.2e24 a 0+ %Abundance=31.69, %ββ=100
    129Te 69.6 m 3/2+ %β-=100
    129m1Te 33.6 d 11/2- %IT=63 , %β-=37
    130Te 7.9e20 a 0+ %Abundance=33.80, %β- β -=100
    131Te 25.0 m 3/2+ %β-=100
    131m1Te 30 h 11/2- %β-=77.8 , %IT=22.2
    132Te 3.204 d 0+ %β-=100
    133Te 12.5 m (3/2+ ) %β-=100
    133m1Te 55.4 m (11/2-) %IT=17.5 , %β-=82.5
    134Te 41.8 m 0+ %β-=100
    135Te 19.0 s (7/2-) %β-=100
    136Te 17.5 s 0+ %β-=100, %β-n=1.1
    137Te 2.49 s (7/2-) %β-=100, %β-n=2.69
    138Te 1.4 s 0+ %β-=100, %β-n=6.3

    Iodine

    Isotope Half-life Spin Parity Mode(s) or Abundance
    108I 36 ms (1) %α=91 , %p < 1
    109I 100 μs %p ~ 100
    110I 0.65 s %K+%β+=83 , %α=17 , %Kp=11 , %Kα=1.1
    111I 2.5 s (5/2+ ) %K+%β+=99.9, %α ~ 0.1
    112I 3.42 s %K+%β+=100, %α ~ 0.0012
    113I 6.6 s (5/2+ ) %K+%β+=100, %Kα=?, %α =3.310E-7
    114I 2.1 s 1+ %K+%β+= 100, %Kp=?
    114m1I 6.2 s (7) %K+%β+=?, %IT=?
    115I 1.3 m (5/2+ ) %K+%β+=100
    116I 2.91 s 1+ %K+%β+=100
    116m1I 3.27 μs (7-)
    117I 2.22 m (5/2) + %K+%β+=100
    118I 13.7 m 2- %K+%β+=100
    118m1I 8.5 m (7-) %K+%β+<100, %IT>0
    119I 19.1 m 5/2+ %K+%β+=100
    120I 81.0 m 2- %K+%β+=100
    120m1I 53 m 4 to 8 %K+%β+=100
    121I 2.12 h 5/2+ %K+%β+=100
    122I 3.63 m 1+ %K+%β+=100
    122m1I 80 μs
    123I 13.27 h 5/2+ %K+%β+=100
    124I 4.1760 d 2- %K+%β+=100
    125I 59.408 d 5/2+ %K=100
    126I 13.11 d 2- %K+%β+=56.3 , %β-=43.7
    127I stable 5/2+ %Abundance=100
    128I 24.99 m 1+ %β-=93.1 , %K+%β+=6.9
    129I 1.57e7 a 7/2+ %β-=100
    130I 12.36 h 5+ %β-=100
    130m1I 9.0 m 2+ %IT=84 , %β-=16
    131I 8.02070 d 7/2+ %β-=100
    132I 2.295 h 4+ %β-=100
    132m1I 1.387 h (8-) %IT=86 , %β-=14
    133I 20.8 h 7/2+ %β-=100
    133m1I 9 s (19/2-) %IT=100
    134I 52.5 m (4) + %β-=100
    134m1I 3.60 m (8) - %IT=97.7 , %β-=2.3
    135I 6.57 h 7/2+ %β-=100
    136I 83.4 s (1-) %β-=100
    136m1I 46.9 s (6-) %β-=100
    137I 24.5 s (7/2+ ) %β-=100, %β-n=6.97
    138I 6.49 s (2-) %β-=100, %β-n=5.5
    139I 2.29 s (7/2+ ) %β-=100, %β-n=9.9
    140I 0.86 s (4) %β-=100 , %β-n=9.3
    141I 0.43 s %β-=100, %β-n=21.2

    Xenon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    110Xe 0.60 μs 0+ %K+β+=?, %α=?
    111Xe 0.74 s %K+%β+=?, %α=?
    112Xe 2.7 s 0+ %K+%β+=99.2, %α=0.8 +11- 5
    113Xe 2.74 s %K+%β+ ~ 100, %α ~ 0.011, %Kp=7 , %Kα ~ 0.007
    114Xe 10.0 s 0+ %K+%β+=100
    115Xe 18 s (5/2+ ) %K+%β+=100, %Kp=0.34 , %Kα=0.0003
    116Xe 59 s 0+ %K+%β+=100
    117Xe 61 s 5/2(+) %K+%β+=100, %Kp=0.0029
    118Xe 3.8 m 0+ %K+%β+=100
    119Xe 5.8 m (5/2+ ) %K+%β+=100
    120Xe 40 m 0+ %K+%β+=100
    121Xe 40.1 m 5/2(+) %K+%β+=100
    122Xe 20.1 h 0+ %K=100
    123Xe 2.08 h (1/2) + %K+%β+=100
    124Xe 1.6e+14 a 0+ %Abundance=0.10, %KEC=100
    125Xe 16.9 h (1/2) + %K+%β+=100
    125m1Xe 57 s (9/2) - %IT=100
    126Xe stable 0+ %Abundance=0.09
    127Xe 36.4 d 1/2+ %K=100
    127m1Xe 69.2 s 9/2- %IT=100
    128Xe stable 0+ %Abundance=1.91
    129Xe stable 1/2+ %Abundance=26.4
    129m1Xe 8.88 d 11/2- %IT=100
    130Xe stable 0+ %Abundance=4.1
    131Xe stable 3/2+ %Abundance=21.2
    131m1Xe 11.84 d 11/2- %IT=100
    132Xe stable 0+ %Abundance=26.9
    132m1Xe 8.39 ms (10+) %IT=100
    133Xe 5.243 d 3/2+ %β-=100
    133m1Xe 2.19 d 11/2- %IT=100
    134Xe stable 0+ %Abundance=10.4
    134m1Xe 290 ms 7- %IT=100
    135Xe 9.14 h 3/2+ %β-=100
    135m1Xe 15.29 m 11/2- %IT=99.996 , %β-=0.004
    136Xe 2.36e21 a 0+ %Abundance=8.9
    137Xe 3.818 m 7/2- %β-=100
    138Xe 14.08 m 0+ %β-=100
    139Xe 39.68 s 3/2- %β-=100
    140Xe 13.60 s 0+ %β-=100
    141Xe 1.73 s 5/2(-) %β-=100, %β-n=0.044
    142Xe 1.22 s 0+ %β-=100, %β-n=0.406
    143Xe 0.30 s 5/2- %β-=100
    144Xe 1.15 s 0+ %β-=100
    145Xe 0.9 s %β-=100, %β-n=?
    146Xe 0+ %β-=100

    Caesium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    113Cs 17 μs (5/2+ ) %p ~ 100, %K+%β+ ~ 0.03
    114Cs 0.57 s (1+ ) %K+%β+ ~ 100, %α=0.018 , %Kp=7 , %Kα=0.16
    115Cs 1.4 s %K+%β+=100, %Kp ~ 0.07
    116Cs 3.84 s >4+ %K+%β+=100, %Kp=0.44 , %Kα=0.08
    116m1Cs 0.70 s (1+ ) %K+%β+=100, %Kp=0.28 , %Kα=0.049
    117Cs 8.4 s (9/2+ ) %K+%β+=100
    117m1Cs 6.5 s (3/2+ ) %K+%β+=100
    118Cs 14 s 2 %K+%β+=100, %Kp<4.2E-2 , %Kα<2.4E-3
    118m1Cs 17 s (7-) %K+%β+=100, %Kp<4.2E-2 , %Kα<2.4E-3
    119Cs 43.0 s 9/2+ %K+%β+=100
    119m1Cs 30.4 s 3/2(+) %K+%β+=100
    120Cs 64 s 2 %K+%β+=100
    120m1Cs 57 s %K+%β+=100, %Kp=7E-6 , %Kα=2.0E-5
    121Cs 155 s 3/2(+) %K+%β+=100
    121m1Cs 122 s 9/2(+) %K+%β+=83, %IT=17
    122Cs 21.0 s 1+ %K+%β+=100
    122m1Cs 3.70 m 8- %K+%β+=100
    122m2Cs 0.36 s (5) - %IT=100
    123Cs 5.94 m 1/2+ %K+%β+=100
    123m1Cs 1.64 s (11/2) - %IT=100
    124Cs 30.8 s 1+ %K+%β+=100
    124m1Cs 6.3 s (7) + %IT=100
    125Cs 45 m (1/2+ ) %K+%β+=100
    126Cs 1.64 m 1+ %K+%β+=100
    127Cs 6.25 h 1/2+ %K+%β+=100
    128Cs 3.66 m 1+ %K+%β+=100
    129Cs 32.06 h 1/2+ %K+%β+=100
    130Cs 29.21 m 1+ %K+%β+=98.4, %β-=1.6
    130m1Cs 3.46 m 5- %IT=99.84 , %K+%β+=0.16
    131Cs 9.689 d 5/2+ %K=100
    132Cs 6.479 d 2+ %K+%β+=98.13 , %β-=1.87
    133Cs stable 7/2+ %Abundance=100
    134Cs 2.0648 a 4+ %β-=99.9997 , %K=0.0003
    134m1Cs 2.903 h 8- %IT=100
    135Cs 2.3e+6 a 7/2+ %β-=100
    135m1Cs 53 m 19/2- %IT=100
    136Cs 13.16 d 5+ %β-=100
    136m1Cs 19 s 8- %IT=?, %β-=?
    137Cs 30.07 a 7/2+ %β-=100
    138Cs 33.41 m 3- %β-=100
    138m1Cs 2.91 m 6- %β-=19 , %IT=81
    139Cs 9.27 m 7/2+ %β-=100
    140Cs 63.7 s 1- %β-=100
    141Cs 24.94 s 7/2+ %β-=100, %β-n=0.029
    142Cs 1.70 s 0- %β-=100, %β-n=0.091
    143Cs 1.78 s 3/2+ %β-=100, %β-n=1.62
    144Cs 1.01 s 1 %β-=100, %β-n=3.17
    144m1Cs 1 s (GE 4) %β-=?
    145Cs 0.594 s 3/2+ %β-=100, %β-n=13.8
    146Cs 0.321 s 1- %β-=100 , %β-n=14.2
    147Cs 0.225 s (3/2+ ) %β-=100, %β-n=43
    148Cs 158 ms %β-=100, %β-n=25

    Barium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    114Ba 0.43 s 0+ %K+%β+ ~ 100, %α=?, %12C ~ 3E-5
    115Ba 0.4 s %K+%β+=100
    116Ba 0.3 s 0+ %K+%β+=100
    117Ba 1.75 s (3/2) %K+%β+=100, %Kp=?, %Kα=?
    118Ba 5.5 s 0+ %K+%β+=100
    119Ba 5.4 s (5/2+ ) %K+%β+=100, %Kp < 25
    120Ba 32 s 0+ %K+%β+=100
    121Ba 29.7 s 5/2(+) %K+%β+=100, %Kp=0.02
    122Ba 1.95 m 0+ %K+%β+=100
    123Ba 2.7 m 5/2+ %K+%β+=100
    124Ba 11.0 m 0+ %K+%β+=100
    125Ba 3.5 m 1/2(+) %K+%β+=100
    126Ba 100 m 0+ %K+%β+ =100
    127Ba 12.7 m 1/2+ %K+%β+=100
    127m1Ba 1.9 s 7/2- %IT=100
    128Ba 2.43 d 0+ %K=100
    129Ba 2.23 h 1/2+ %K+%β+=100
    129m1Ba 2.16 h 7/2+ %K+%β+ < 100, %IT=?
    130Ba stable 0+ %Abundance=0.106
    130m1Ba 11 ms 8- %IT=100
    131Ba 11.50 d 1/2+ %K+%β+=100
    131m1Ba 14.6 m 9/2- %IT=100
    132Ba stable 0+ %Abundance=0.101
    133Ba 10.51 a 1/2+ %K=100
    133m1Ba 38.9 h 11/2- %K=0.0096 , %IT=99.9904
    134Ba stable 0+ %Abundance=2.417
    134m1Ba 2.63 μs (10+)
    135Ba stable 3/2+ %Abundance=6.592
    135m1Ba 28.7 h 11/2- %IT=100
    136Ba stable 0+ %Abundance=7.854
    136m1Ba 0.3084 s 7- %IT=100
    137Ba stable 3/2+ %Abundance=11.23
    137m1Ba 2.552 m 11/2- %IT=100
    138Ba stable 0+ %Abundance=71.70
    139Ba 83.06 m 7/2- %β-=100
    140Ba 12.752 d 0+ %β-=100
    141Ba 18.27 m 3/2- %β-=100
    142Ba 10.6 m 0+ %β-=100
    143Ba 14.33 s 5/2- %β-=100
    144Ba 11.5 s 0+ %β-=100, %β-n=3.6
    145Ba 4.31 s 5/2- %β-=100
    146Ba 2.22 s 0+ %β-=100
    147Ba 0.893 s (3/2+ ) %β-=100, %β-n=0.06
    148Ba 0.607 s 0+ %β-=100, %β-n=0.4
    149Ba 0.344 s %β-=100, %β-n=0.43
    150Ba 0.3 s 0+ %β-=100, %β-n=?

    Lanthanum

    Isotope Half-life Spin Parity Mode(s) or Abundance
    120La 2.8 s %K+%β+=100
    121La 5.3 s %K+%β+=100, %Kp=?
    122La 8.7 s %K+%β+=100, %Kp=?
    123La 17 s %K+%β+=100
    124La 29 s %K+%β+=100
    124m1La 1 s %K+%β+=100
    125La 76 s (11/2-) %K+%β+=100
    126La 54 s %K+%β+=100
    127La 5.1 m (11/2-) %K+%β+=100
    127m1La 3.7 m (3/2+ ) %K+%β+=100, %IT=?
    128La 5.0 m (5+ ) %K+%β+=100
    128m1La 560 ms (1+ , 2+ ) %K+%β+=100
    129La 11.6 m 3/2+ %K+%β+=100
    129m1La 0.56 s 11/2- %IT=100
    130La 8.7 m 3(+) %K+%β+=100
    131La 59 m 3/2+ %K+%β+=100
    132La 4.8 h 2- %K+%β+=100
    132m1La 24.3 m 6- %IT=76, %K+%β+=24
    133La 3.912 h 5/2+ %K+%β+=100
    134La 6.45 m 1+ %K+%β+=100
    135La 19.5 h 5/2+ %K+%β+=100
    136La 9.87 m 1+ %K+%β+=100
    136m1La 114 ms %IT=100
    137La 6e4 a 7/2+ %K=100
    138La 1.05e+11 a 5+ %Abundance=0.0902, %β-=33.6 , %K+%β+=66.4
    139La stable 7/2+ %Abundance=99.9098
    140La 1.6781 d 3- %β-=100
    141La 3.92 h (7/2+ ) %β-=100
    142La 91.1 m 2- %β-=100
    143La 14.2 m (7/2) + %β-=100
    144La 40.8 s (3-) %β-=100
    145La 24.8 s (5/2+ ) %β-=100
    146La 6.27 s 2- %β-=100
    146m1La 10.0 s (6-) %β-=100
    147La 4.015 s (5/2+ ) %β-=100, %β-n=0.035
    148La 1.05 s (2-) %β-=100 , %β-n=0.11
    149La 1.05 s %β-=100, %β-n=1.43
    150La 0.86 s %β-=100, %β-n=2.7

    Cerium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    123Ce 3.2 s (5/2) %K+%β+=100, %Kp=?
    124Ce 6 s 0+ %K+%β+=100
    125Ce 9.0 s (5/2+ ) %K+%β+=100, %Kp=?
    126Ce 50 s 0+ %K+%β+=100
    127Ce 31 s (5/2+ ) %K+%β+=100
    128Ce 4.1 s 0+ %K+%β+=100
    129Ce 3.5 m 5/2+ %K+%β+=100
    130Ce 25 m 0+ %K+%β+=100
    131Ce 10.2 m (7/2+ ) %K+%β+=100
    131m1Ce 5.0 m (1/2+ ) %K+%β+=100
    132Ce 3.51 h 0+ %K+%β+=100
    132m1Ce 13 ms (8- ,9-) %IT=100
    133Ce 97 m 1/2+ %K+%β+=100
    133m1Ce 4.9 h 9/2- %K+%β+=100
    134Ce 3.16 d 0+ %K=100
    135Ce 17.7 h 1/2(+) %K+%β+=100
    135m1Ce 20 s 11/2(-) %IT=100
    136Ce stable 0+ %Abundance=0.19
    137Ce 9.0 h 3/2+ %K+%β+=100
    137m1Ce 34.4 h 11/2- %IT=99.22 , %K+%β+=0.78
    138Ce stable 0+ %Abundance=0.25
    138m1Ce 8.65 ms 7- %IT=100
    139Ce 137.640 d 3/2+ %K=100
    139m1Ce 54.8 s 11/2- %IT=100
    140Ce stable 0+ %Abundance=88.48
    141Ce 32.501 d 7/2- %β-=100
    142Ce 5e+16 a 0+ %Abundance=11.08
    143Ce 33.039 h 3/2- %β-=100
    144Ce 284.893 d 0+ %β-=100
    145Ce 3.01 m (3/2) - %β-=100
    146Ce 13.52 m 0+ %β-=100
    147Ce 56.4 s (5/2-) %β-=100
    148Ce 56 s 0+ %β-=100
    149Ce 5.3 s (3/2-) %β-=100
    150Ce 4.0 s 0+ %β-=100
    151Ce 1.02 s %β-=100
    152Ce 1.4 s 0+ %β-=100

    Praesodymium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    124Pr 1.2 s %K+%β+=100, %Kp=?
    125Pr 3.3 s %K+%β+=100
    126Pr 3.14 s (3,4,5) %K+%β+=100, %Kp=?
    127Pr 4.2 s (11/2-) %K+%β+=100
    128Pr 3.1 s 4,5,6 %K+%β+=100, %Kp=?
    129Pr 30 s (3/2+ ) %K+%β+=100
    130Pr 40.0 s %K+%β+=100
    131Pr 1.53 m (3/2+ ) %K+%β+=100
    131m1Pr 5.7 s (11/2-) %IT=95 , %K+%β+=5
    132Pr 1.6 m %K+%β+=100
    133Pr 6.5 m (3/2+ ) %K+%β+=100
    134Pr 17 m 2- %K+%β+=100
    134m1Pr 11 m (5-) %K+%β+=100
    135Pr 24 m 3/2(+) %K+%β+=100
    136Pr 13.1 m 2+ %K+%β+=100
    137Pr 1.28 h 5/2+ %K+%β+=100
    138Pr 1.45 m 1+ %K+%β+=100
    138m1Pr 2.12 h 7- %K+%β+=100
    139Pr 4.41 h 5/2+ %K+%β+=100
    140Pr 3.39 m 1+ %K+β+=100
    141Pr stable 5/2+ %Abundance=100
    142Pr 19.12 h 2- %β-=99.9836 , %K=0.0164
    142m1Pr 14.6 m 5- %IT=100
    143Pr 13.57 d 7/2+ %β-=100
    144Pr 17.28 m 0- %β-=100
    144m1Pr 7.2 m 3- %IT=99.93, %β-=0.07
    145Pr 5.984 h 7/2+ %β-=100
    146Pr 24.15 m (2) - %β-=100
    147Pr 13.4 m (3/2+ ) %β-=100
    148Pr 2.27 m 1- %β-=100
    148m1Pr 2.0 m (4) %β-=100
    149Pr 2.26 m (5/2+ ) %β-=100
    150Pr 6.19 s (1) - %β-=100
    151Pr 18.90 s (3/2-) %β-=100
    152Pr 3.63 s (4-) %β-=100
    153Pr 4.28 s %β-=100
    154Pr 2.3 s (3+ , 2+ ) %β-=100

    Neodymium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    127Nd 1.8 s %K+%β+=100, %Kp=?
    128Nd 4 s 0+ %K+%β+=100, %Kp=?
    129Nd 7 s (5/2+ ) %K+%β+=100, %Kp=?
    130Nd 28 s 0+ %K+%β+=100
    131Nd 27 s (5/2) %K+%β+=100 , %Kp=?
    132Nd 1.75 m 0+ %β+=100
    133Nd 70 s (7/2+ ) %K+%β+=100
    133m1Nd 70 s (1/2) + %K+%β+=?, %IT=?
    134Nd 8.5 m 0+ %K+%β+=100
    134m1Nd 410 μs (8) -
    135Nd 12.4 m 9/2(-) %K+%β+=100
    135m1Nd 5.5 m (1/2+ ) %K+%β+=100
    136Nd 50.65 m 0+ %K+%β+=100
    137Nd 38.5 m 1/2+ %K+%β+=100
    137m1Nd 1.60 s 11/2- %IT=100
    138Nd 5.04 h 0+ %K=100
    139Nd 29.7 m 3/2+ %K+%β+=100
    139m1Nd 5.50 h 11/2- %K+%β+=88.2 , %IT=11.8
    140Nd 3.37 d 0+ %K=100
    141Nd 2.49 h 3/2+ %K+%β+=100
    141m1Nd 62.0 s 11/2- %IT > 99.95, %K+%β+ < 0.05
    142Nd stable 0+ %Abundance=27.13
    143Nd stable 7/2- %Abundance=12.18
    144Nd 2.29e+15 a 0+ %Abundance=23.80, %α=100
    145Nd stable 7/2- %Abundance=8.30
    146Nd stable 0+ %Abundance=17.19
    147Nd 10.98 d 5/2- %β-=100
    148Nd stable 0+ %Abundance=5.76
    149Nd 1.728 h 5/2- %β-=100
    150Nd 1.1e19 a 0+ %Abundance=5.64, %β- β-=?
    151Nd 12.44 m 3/2+ %β-=100
    152Nd 11.4 m 0+ %β-=100
    153Nd 31.6 s (3/2) - %β-=100
    154Nd 25.9 s 0+ %β-=100
    155Nd 8.9 s %β-=100
    156Nd 5.47 s 0+ %β-=100

    Promethium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    132Pm 6.3 s (3+ ) %K+%β+=100 , %Kp ~ 5E-5
    133Pm 3/2+ %K+%β+=100
    133m1Pm 15 s 11/2- %K+%β+=100, %IT=?
    134Pm 5 s (2+ ) %K+%β+=100
    134m1Pm 22 s (5+ ) %K+%β+=100
    135Pm 45 s (11/2-) %K+%β+=100
    135m1Pm 49 s (3/2+ , 5/2+ ) %K+%β+=100
    136Pm 47 s (2+ ) %K+%β+=100
    136m1Pm 107 s (5-) %K+%β+=100
    137Pm 2.4 m 11/2- %K+%β+=100
    138Pm 10 s 1+ %K+%β+=100
    138m1Pm 3.24 m (5-) %K+%β+=?, %IT=?
    139Pm 4.15 m (5/2) + %K+%β+=100
    139m1Pm 180 ms (11/2) - %IT=99.94 +5-20, %K+%β+=0.06 +20-5
    140Pm 9.2 s 1+ %K+%β+=100
    140m1Pm 5.95 m 7- %K+%β+=100
    140m2Pm 5.95 m 8- %K+%β+=100
    141Pm 20.90 m 5/2+ %K+%β+=100
    142Pm 40.5 s 1+ %K+%β+=100
    142m1Pm 2.0 ms (8) - %IT=100
    143Pm 265 d 5/2+ %K+%β+=100
    144Pm 363 d 5- %K+%β+=100
    145Pm 17.7 a 5/2+ %K=100, %α=2.8E-7
    146Pm 5.53 a 3- %K=66.0 , %β-=34.0
    147Pm 2.6234 a 7/2+ %β-=100
    148Pm 5.370 d 1- %β-=100
    148m1Pm 41.29 d 6- %β-=95.0 , %IT=5.0
    149Pm 53.08 h 7/2+ %β-=100
    150Pm 2.68 h (1-) %β-=100
    151Pm 28.40 h 5/2+ %β-=100
    152Pm 4.12 m 1+ %β-=100
    152m1Pm 7.52 m 4- %β-=100
    152m2Pm 13.8 m (8) %β- < 100, %IT > 0
    153Pm 5.25 m 5/2- %β-=100
    154Pm 1.73 m (0,1) %β-=100
    154m1Pm 2.68 m (3,4) %β-=100
    155Pm 41.5 s (5/2-) %β-=100
    156Pm 26.70 s 4(-) %β-=100
    157Pm 10.56 s (5/2-) %β-=100
    158Pm 4.8 s %β-=100

    Samarium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    131Sm 1.2 s %K+%β+=100, %Kp=?
    132Sm 4.0 s 0+ %K+%β+=100 , %Kp=?
    133Sm 3.7 s (5/2+ ) %K+%β+=100, %Kp=?
    134Sm 10 s 0+ %K+%β+=100
    135Sm 10.3 s (7/2+ ) %K+%β+=100, %Kp=0.02
    136Sm 47 s 0+ %K+%β+=100
    137Sm 45 s (9/2-) %K+%β+=100
    138Sm 3.1 m 0+ %K+%β+=100
    139Sm 2.57 m (1/2) + %K+%β+=100
    139m1Sm 10.7 s (11/2) - %IT=93.7 , %K+%β+=6.3
    140Sm 14.82 m 0+ %K+%β+=100
    141Sm 10.2 m 1/2+ %K+%β+=100
    141m1Sm 22.6 m 11/2- %K+%β+=99.69 , %IT=0.31
    142Sm 72.49 m 0+ %K+%β+=100
    143Sm 8.83 m 3/2+ %K+%β+=100
    143m1Sm 66 s 11/2- %IT=99.76 , %K+%β+=0.24
    143m2Sm 30 ms 23/2(-) %IT=100
    144Sm stable 0+ %Abundance=3.1
    145Sm 340 d 7/2- %K=100
    146Sm 1.03e8 a 0+ %α=100
    147Sm 1.06e+11 a 7/2- %Abundance=15.0, %α=100
    148Sm 7e+15 a 0+ %Abundance=11.3 , %α=100
    149Sm 2e+15 a 7/2- %Abundance=13.8
    150Sm stable 0+ %Abundance=7.4
    151Sm 90 a 5/2- %β-=100
    152Sm stable 0+ %Abundance=26.7
    153Sm 46.284 h 3/2+ %β-=100
    153m1Sm 10.6 ms 11/2- %IT=100
    154Sm stable 0+ %Abundance=22.7
    155Sm 22.3 m 3/2- %β-=100
    156Sm 9.4 h 0+ %β-=100
    157Sm 482 s (3/2-) %β-=100
    158Sm 5.30 m 0+ %β-=100
    159Sm 11.37 s (5/2-) %β-=100
    160Sm 9.6 s 0+ %β-=100

    Europium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    134Eu 0.5 s %K+%β+=100, %Kp > 0
    135Eu 1.5 s %K+%β+=100, %Kp=?
    136Eu 3.3 s (7+ ) %K+%β+=100, %Kp=0.09
    136m1Eu 3.7 s (3+ ) %K+%β+=100, %Kp=0.09
    137Eu 11 s (11/2-) %K+%β+=100
    138Eu 12.1 s (6-) %K+%β+=100
    139Eu 17.9 s (11/2) - %K+%β+=100
    140Eu 1.51 s 1+ %K+%β+=100
    140m1Eu 125 ms (5-) %IT=100 , %K+%β+ < 1
    141Eu 40.7 s 5/2+ %K+%β+=100
    141m1Eu 2.7 s 11/2- %K+%β+=13 +4-2 , %IT=87 +2-4
    142Eu 2.34 s 1+ %K+%β+=100
    142m1Eu 1.22 m 8- %K+%β+=100
    143Eu 2.63 m 5/2+ %K+%β+=100
    144Eu 10.2 s 1+ %K+%β+=100
    145Eu 5.93 d 5/2+ %K+%β+=100
    146Eu 4.61 d 4- %K+%β+=100
    147Eu 24.1 d 5/2+ %K+β+=100, %α=0.0022
    148Eu 54.5 d 5- %K+%β+=100, %α=9.4E-7
    149Eu 93.1 d 5/2+ %K=100
    150Eu 36.9 a 5(-) %K+%β+=100
    150m1Eu 12.8 h 0- %K+%β+=11 , %β-=89 , %IT < 5E-8
    151Eu stable 5/2+ %Abundance=47.8
    152Eu 13.537 a 3- %K=72.1 , %β-=27.9
    152m1Eu 9.3116 h 0- %K+%β+=28 , %β-=72
    152m2Eu 96 m 8- %IT=100
    153Eu stable 5/2+ %Abundance=52.2
    154Eu 8.593 a 3- %β-=99.98 , %K+%β+=0.02
    154m1Eu 46.3 m (8-) %IT=100
    155Eu 4.7611 a 5/2+ %β-=100
    156Eu 15.19 d 0+ %β-=100
    157Eu 15.18 h 5/2+ %β-=100
    158Eu 45.9 m (1-) %β-=100
    159Eu 18.1 m 5/2+ %β-=100
    160Eu 38 s 1(-) %β-=100
    161Eu 26 s %β-=100
    162Eu 10.6 s %β-=100

    Gadolinium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    139Gd 4.9 s 9/2- %K+%β+=?, %β+P=?
    140Gd 15.8 s 0+ %K+%β+=100
    141Gd 14 s (1/2+ ) %K+%β+=100, %Kp=0.03
    141m1Gd 24.5 s (11/2-) %K+%β+=89 , %IT=11
    142Gd 70.2 s 0+ %K+%β+=100
    143Gd 39 s (1/2) + %K+%β+=100, %Kp < 0.001
    143m1Gd 112 s (11/2-) %K+%β+=100
    144Gd 4.5 m 0+ %K+%β+=100
    145Gd 23.0 m 1/2+ %K+%β+=100
    145m1Gd 85 s 11/2- %IT=94.3 , %K+%β+=5.7
    146Gd 48.27 d 0+ %K=100
    147Gd 38.06 h 7/2- %K+%β+=100
    148Gd 74.6 a 0+ %α=100
    149Gd 9.28 d 7/2- %K+%β+=100, %α=4.3E-4
    150Gd 1.79e6 a 0+ %α=100
    151Gd 124 d 7/2- %K=100, %α ~ 8E-7
    152Gd 1.08e14 a 0+ %Abundance=0.20, %α=100
    153Gd 240.4 d 3/2- %K=100
    154Gd stable 0+ %Abundance=2.18
    155Gd stable 3/2- %Abundance=14.80
    155m1Gd 31.97 ms 11/2- %IT=100
    156Gd stable 0+ %Abundance=20.47
    157Gd stable 3/2- %Abundance=15.65
    158Gd stable 0+ %Abundance=24.84
    159Gd 18.479 h 3/2- %β-=100
    160Gd stable 0+ %Abundance=21.86
    161Gd 3.66 m 5/2- %β-=100
    162Gd 8.4 m 0+ %β-=100
    163Gd 68 s (5/2-) %β-=100
    164Gd 45 s 0+ %β-=100


    Terbium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    140Tb 2.4 s 5 %K+%β+=100, %p=0.26
    141Tb 3.5 s (5/2-) %K+%β+=100
    142Tb 597 ms 1+ %K+%β+=100 , %Kp=0.0022
    142m1Tb 303 ms (5-) %IT=100, %K+%β+ < 0.5
    143Tb 12 s (11/2-) %K+%β+=100
    143m1Tb 21 s (5/2+ )
    144Tb 1 s (1+ ) %K+%β+=100
    144m1Tb 4.25 s (6-) %IT=66 , %K+%β+=34
    145Tb (1/2+ )
    145m1Tb 29.5 s (11/2-) %K+%β+=100
    146Tb 8 s 1+ %K+%β+=100
    146m1Tb 23 s 5- %K+%β+=100
    146m2Tb 1.18 ms (10+) %IT=100
    147Tb 1.7 h (1/2+ ) %K+%β+=100
    147m1Tb 1.83 m (11/2) - %K+%β+=100
    148Tb 60 m 2- %K+%β+=100
    148m1Tb 2.20 m 9+ %K+%β+=100
    149Tb 4.118 h 1/2+ %K+%β+=83.3 , %α=16.7
    149m1Tb 4.16 m 11/2- %K+%β+=99.978 , %α=0.022
    150Tb 3.48 h (2-) %K+%β+=100, %α<0.05
    150m1Tb 5.8 m 9+ %K+%β+=100
    151Tb 17.609 h 1/2(+) %K+%β+=100 , %α=9.5E-3
    151m1Tb 25 s (11/2-) %IT=93.8 , %K+%β+=6.2
    152Tb 17.5 h 2- %K+%β+=100, %α < 7E-7
    152m1Tb 4.2 m 8+ %IT=78.8 , %K+%β+=21.2
    153Tb 2.34 d 5/2+ %K+%β+=100
    154Tb 21.5 h 0 %K+%β+=100, %β- < 0.1
    154m1Tb 9.4 h 3- %K+%β+=78.2 , %IT=21.8 , %β- < 0.1
    154m2Tb 22.7 h 7- %K+%β+=98.2 , %IT=1.8
    154m3Tb 513 ns
    155Tb 5.32 d 3/2+ %K=100
    156Tb 5.35 d 3- %K+%β+=100 , %β-=?
    156m1Tb 24.4 h (7-) %IT=100
    156m2Tb 5.3 h (0+) %IT=?, %K+%β+=?
    157Tb 71 a 3/2+ %K=100
    158Tb 180 a 3- %K+%β+=83.4 , %β-=16.6
    158m1Tb 10.70 s 0- %IT=100, %β- < 0.6, %K+%β+ < 0.01
    159Tb stable 3/2+ %Abundance=100
    160Tb 72.3 d 3- %β-=100
    161Tb 6.88 d 3/2+ %β-=100
    162Tb 7.60 m 1- %β-=100
    163Tb 19.5 m 3/2+ %β-=100
    164Tb 3.0 m (5+ ) %β-=100
    165Tb 2.11 m (3/2+ ) %β-=100

    Dysprosium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    141Dy 0.9 s (9/2-) %K+%β+=100 , %Kp=?
    142Dy 2.3 s 0+ %K+%β+=100, %Kp=0.06
    143Dy 4.1 s (1/2+ ) %K+%β+=100, %Kp=?
    144Dy 9.1 s 0+ %K+%β+=100, %Kp=?
    145Dy 10 s (1/2+ ) %K+%β+=100
    145m1Dy 13.6 s (11/2-) %K+%β+=100
    146Dy 29 s 0+ %K+%β+=100
    146m1Dy 150 ms (10+) %IT=100
    147Dy 40 s 1/2+ %K+%β+=100, %Kp=?
    147m1Dy 55 s 11/2- %K+%β+=65 , %IT=35
    148Dy 3.1 m 0+ %K+%β+=100
    149Dy 4.20 m (7/2-) %K+%β+=100
    149m1Dy 490 ms (27/2-) %IT=99.3 , %K+%β+=0.7
    150Dy 7.17 m 0+ %α=36 , %K+%β+=64
    151Dy 17.9 m 7/2(-) %K+%β+=94.4 , %α=5.6
    152Dy 2.38 h 0+ %α=0.100 , %K=99.900
    153Dy 6.4 h 7/2(-) %K+%β+=99.9906 , %α=0.0094
    154Dy 3.0e+6 a 0+ %α=100
    155Dy 9.9 h 3/2- %K+%β+=100
    156Dy stable 0+ %Abundance=0.06
    157Dy 8.14 h 3/2- %K+%β+=100
    157m1Dy 21.6 ms 11/2- %IT=100
    158Dy stable 0+ %Abundance=0.10
    159Dy 144.4 d 3/2- %K=100
    160Dy stable 0+ %Abundance=2.34
    161Dy stable 5/2+ %Abundance=18.9
    162Dy stable 0+ %Abundance=25.5
    163Dy stable 5/2- %Abundance=24.9
    164Dy stable 0+ %Abundance=28.2
    165Dy 2.334 h 7/2+ %β-=100
    165m1Dy 1.257 m 1/2- %IT=97.76 , %β-=2.24
    166Dy 81.6 h 0+ %β-=100
    167Dy 6.20 m (1/2-) %β-=100
    168Dy 8.7 m 0+ %β-=100
    169Dy 39 s (5/2-) %β-=100


    Holmium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    144Ho 0.7 s %K+%β+=100, %Kp=?
    145Ho 2.4 s (11/2-) %K+%β+=100
    146Ho 3.6 s (10+) %K+%β+=100, %Kp=?
    147Ho 5.8 s (11/2-) %K+%β+=100, %Kp=?
    148Ho 2.2 s 1+ %K+%β+=100
    148m1Ho 9.59 s 6- %K+%β+=100, %Kp=0.08
    148m2Ho 2.35 ms (10+) %IT=100
    149Ho 21.1 s (11/2-) %K+%β+=100
    149m1Ho 56 s (1/2+ ) %K+%β+=100
    150Ho 72 s 2- %K+%β+=100
    150m1Ho 23.3 s (9) + %K+%β+=100
    151Ho 35.2 s (11/2-) %K+%β+=78 , %α=22
    151m1Ho 47.2 s (1/2+ ) %α=80 +15-20, %K+%β+=20 +20- 15
    152Ho 161.8 s 2- %α=12 , %K+%β+=88
    152m1Ho 50.0 s 9+ %α=10.8 , %K+%β+=89.2
    153Ho 2.01 m 11/2- %K+%β+=99.949 , %α=0.051
    153m1Ho 9.3 m 1/2+ %K+%β+=99.82 , %α=0.18
    154Ho 11.76 m (2) - %K+%β+=99.981 , %α=0.019
    154m1Ho 3.10 m 8+ %K+%β+=100, %α < 0.001
    155Ho 48 m 5/2+ %K+%β+=100
    156Ho 56 m (4+ ) %K+%β+=100
    156m1Ho 9.5 s (1+ ) %IT=?, %K+%β+=?
    157Ho 12.6 m 7/2- %K+%β+=100
    158Ho 11.3 m 5+ %K+%β+=100
    158m1Ho 28 m 2- %K+%β+ < 19, %IT > 81
    158m2Ho 21.3 m (9+ ) %K+%β+ > 93, %IT < 7
    159Ho 33.05 m 7/2- %K+%β+=100
    159m1Ho 8.30 s 1/2+ %IT=100
    160Ho 25.6 m 5+ %K+%β+=100
    160m1Ho 5.02 h 2- %IT=65 , %K+%β+=35
    160m2Ho 3 s (9+ ) %IT=100
    161Ho 2.48 h 7/2- %K=100
    161m1Ho 6.76 s 1/2+ %IT=100
    162Ho 15.0 m 1+ %K+%β+=100
    162m1Ho 67.0 m 6- %IT=62, %K+%β+=38
    163Ho 4570 a 7/2- %K=100
    163m1Ho 1.09 s 1/2+ %IT=100
    164Ho 29 m 1+ %K=60 , %β-=40
    164m1Ho 37.5 m 6- %IT=100
    165Ho stable 7/2- %Abundance=100
    166Ho 26.83 h 0- %β-=100
    166m1Ho 1.20e3 a (7) - %β-=100
    167Ho 3.1 h 7/2- %β-=100
    168Ho 2.99 m 3+ %β-=100
    168m1Ho 132 s (6+ ) %IT > 99.5, %β- < 0.5
    169Ho 4.7 m 7/2- %β-=100
    170Ho 2.76 m (6+ ) %β-=100
    170m1Ho 43 s (1+ ) %β-=100
    171Ho 53 s (7/2-) %β-=100
    172Ho 25 s %β-=100

    Erbium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    145Er 0.9 s (11/2-) %K+%β+=100, %Kp=?
    146Er 1.7 s 0+ %K+%β+=100, %Kp=?
    147Er 2.5 s (11/2-) %K+%β+=100, %Kp=?
    147m1Er 2.5 s (1/2+ ) %K+%β+=100, %Kp=?
    148Er 4.6 s 0+ %K+%β+=100, %Kp ~ 0.15
    149Er 4 s (1/2+ ) %K+%β+=100, %Kp=7
    149m1Er 8.9 s (11/2-) %K+%β+=96.5 , %IT=3.5 , %Kp=0.18
    150Er 18.5 s 0+ %K+%β+=100
    151Er 23.5 s (7/2-) %K+%β+=100
    151m1Er 0.58 s (27/2-) %IT=95.3 , %K+%β+=4.7
    152Er 10.3 s 0+ %K+%β+=10 , %α=90
    153Er 37.1 s (7/2-) %α=53 , %K+%β+=47
    154Er 3.73 m 0+ %K+%β+=99.53 , %α=0.47
    155Er 5.3 m 7/2- %K+%β+=99.978 , %α=0.022
    156Er 19.5 m 0+ %K+%β+=100
    157Er 18.65 m 3/2- %K+%β+=100
    157m1Er 76 ms (9/2+ ) %IT=100
    158Er 2.29 h 0+ %K=100
    159Er 36 m 3/2- %K+%β+=100
    160Er 28.58 h 0+ %K=100
    161Er 3.21 h 3/2- %K+%β+=100
    162Er stable 0+ %Abundance=0.14
    163Er 75.0 m 5/2- %K+%β+=100
    164Er stable 0+ %Abundance=1.61
    165Er 10.36 h 5/2- %K=100
    166Er stable 0+ %Abundance=33.6
    167Er stable 7/2+ %Abundance=22.95
    167m1Er 2.269 s 1/2- %IT=100
    168Er stable 0+ %Abundance=26.8
    169Er 9.40 d 1/2- %β-=100
    170Er stable 0+ %Abundance=14.9
    171Er 7.516 h 5/2- %β-=100
    172Er 49.3 h 0+ %β-=100
    173Er 1.4 m (7/2-) %β-=100
    174Er 3.3 m 0+ %β-=100
    175Er 1.2 m (9/2+ ) %β-=100


    Thullium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    146Tm 235 ms (10+) %K+%β+ ~ 55, %p ~ 45
    146m1Tm 72 ms (5- ,6-) %p=100, %K+%β+=?
    147Tm 0.56 s (11/2-) %K+%β+ ~ 90, %p ~ 10
    147m1Tm 360 μs (1/2+,3/2+ )
    148Tm 0.7 s (10+ ) %K+%β+=100
    149Tm 0.9 s (11/2-) %K+%β+=100, %Kp=0.2 +2-1
    150Tm 2.2 s (6-) %K+%β+=100, %Kp=1.2
    150m1Tm 5.2 ms (10+) %IT=100
    151Tm 4.17 s (11/2-) %K+%β+=100
    151m1Tm 6.6 s (1/2+ ) %K+%β+=100
    152Tm 8.0 s (2) - %K+%β+=100
    152m1Tm 5.2 s (9) + %K+%β+=100
    153Tm 1.48 s (11/2-) %α=91 , %K+%β+=9
    153m1Tm 2.5 s (1/2+ ) %α=92 , %K+%β+=8
    154Tm 8.1 s (2-) %K+%β+=56 , %α=44
    154m1Tm 3.30 s (9+ ) %α=90 sys%K+%β+=10 sys%IT=?
    155Tm 21.6 s (11/2-) %K+%β+=98.1 , %α=1.9
    155m1Tm 45 s (1/2+ ) %K+%β+>92, %α<8
    156Tm 83.8 s 2- %K+%β+=99.936 , %α=0.064
    156m1Tm 19 s %α=?
    157Tm 3.63 m 1/2+ %K+%β+=100
    158Tm 3.98 m 2- %K+%β+=100
    158m1Tm 20 ns (5+ )
    158m2Tm 16 ns (9-)
    159Tm 9.13 m 5/2+ %K+%β+=100
    160Tm 9.4 m 1- %K+%β+=100
    160m1Tm 74.5 s 5 %K+%β+=15 , %IT=85
    161Tm 33 m 7/2+ %K+%β+=100
    162Tm 21.70 m 1- %K+%β+=100
    162m1Tm 24.3 s 5+ %IT=82 , %K+%β+=18
    163Tm 1.810 h 1/2+ %K+%β+=100
    164Tm 2.0 m 1+ %K+%β+=100
    164m1Tm 5.1 m 6- %IT ~ 80, %K+%β+ ~ 20
    165Tm 30.06 h 1/2+ %K+%β+=100
    166Tm 7.70 h 2+ %K+%β+=100
    166m1Tm 350 ms 6- %IT=100
    167Tm 9.25 d 1/2+ %K=100
    168Tm 93.1 d 3(+) %K+%β+=99.990 , %β-=0.010
    169Tm stable 1/2+ %Abundance=100
    170Tm 128.6 d 1- %K=0.131 , %β-=99.869
    171Tm 1.92 a 1/2+ %β-=100
    172Tm 63.6 h 2- %β-=100
    173Tm 8.24 h (1/2+ ) %β-=100
    174Tm 5.4 m (4) - %β-=100
    175Tm 15.2 m 1/2+ %β-=100
    176Tm 1.9 m (4+ ) %β-=100
    177Tm 85 s (1/2+ ) %β-=100

    Ytterbium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    151Yb 1.6 s (1/2+ ) %K+%β+=100, %Kp=?
    151m1Yb 1.6 s (11/2-) %K+%β+ ~ 100, %Kp=?
    152Yb 3.04 s 0+ %K+%β+=100, %Kp=?
    153Yb 4.2 s 7/2- %α=50 sys %K+%β+=50 sys
    154Yb 0.409 s 0+ %α=92.6 , %K+%β+=7.4
    155Yb 1.800 s (7/2-) %α=89 , %K+%β+=11
    156Yb 26.1 s 0+ %K+%β+=90 , %α=10
    157Yb 38.6 s 7/2- %K+%β+=99.5, %α=0.5
    158Yb 1.49 m 0+ %α ~ 0.0021 , %K+%β+=100
    159Yb 1.58 m 5/2(-) %K+%β+=100
    160Yb 4.8 m 0+ %K+%β+=100
    161Yb 4.2 m 3/2- %K+%β+=100
    162Yb 18.87 m 0+ %K+%β+=100
    163Yb 11.05 m 3/2- %K+%β+=100
    164Yb 75.8 m 0+ %K=100
    165Yb 9.9 m 5/2- %K+%β+=100
    166Yb 56.7 h 0+ %K=100
    167Yb 17.5 m 5/2- %K+%β+=100
    168Yb stable 0+ %Abundance=0.13
    169Yb 32.026 d 7/2+ %K=100
    169m1Yb 46 s 1/2- %IT=100
    170Yb stable 0+ %Abundance=3.05
    171Yb stable 1/2- %Abundance=14.3
    171m1Yb 5.25 ms 7/2+ %IT=100
    172Yb stable 0+ %Abundance=21.9
    173Yb stable 5/2- %Abundance=16.12
    174Yb stable 0+ %Abundance=31.8
    175Yb 4.185 d 7/2- %β-=100
    175m1Yb 68.2 ms 1/2- %IT=100
    176Yb stable 0+ %Abundance=12.7
    176m1Yb 11.4 s (8-) %IT > 90, %β- < 10
    177Yb 1.911 h (9/2+ ) %β-=100
    177m1Yb 6.41 s (1/2-) %IT=100
    178Yb 74 m 0+ %β-=100
    179Yb 8.0 m (1/2-) %β-=100
    180Yb 2.4 m 0+ %β-=100

    Lutetium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    150Lu 35 ms %p=80 , %K+%β+=20
    151Lu 88 ms (11/2-) %p=70
    152Lu 0.7 s (5- ,6-) %K+%β+=100, %Kp=15
    153Lu 0.9 s 11/2- %α ~ 70 , %K+%β+ ~ 30
    154Lu (2-)
    154m1Lu 1.12 s (9+ ) %K+%β+ ~ 100
    154m2Lu 35 μs (17+ )
    155Lu 140 ms (1/2+ , 3/2+ ) %α=?
    155m1Lu 68 ms (11/2-) %α=79 , %K+%β+=21
    155m2Lu 2.60 ms (25/2-) %α ~ 100
    156Lu 198 ms (9+ ) %α ~ 95 , %K+%β+=5
    156m1Lu 494 ms (2-) %α=79 , %K+%β+=21
    157Lu 6.8 s (1/2+ , 3/2+ ) %α > 0
    157m1Lu 4.79 s (11/2-) %α=6 , %K+%β+=94
    158Lu 10.6 s %α=0.91 , %K+%β+=99.09
    159Lu 12.1 s %K+%β+=99.96 sys%α=0.04 sys
    160Lu 36.1 s %K+%β+=100, %α < 1E-4
    160m1Lu 40 s %K+%β+ < 100, %α=?
    161Lu 77 s (5/2+ ) %K+%β+=100
    161m1Lu 7.3 ms (9/2-) %IT=100
    162Lu 1.37 m (1-) %K+%β+=100
    162m1Lu 1.5 m (4-) %K+%β+ < 100
    162m2Lu 1.9 m %K+%β+ < 100
    163Lu 238 s (1/2-) %K+%β+=100
    164Lu 3.14 m %K+%β+=100
    165Lu 10.74 m (7/2+ ) %K+%β+=100
    165m1Lu 12 m 1/2+
    166Lu 2.65 m (6-) %K+%β+=100
    166m1Lu 1.41 m (3-) %K+%β+=58 , %IT=42
    166m2Lu 2.12 m (0- ) %K+%β+>80, %IT<20
    167Lu 51.5 m 7/2+ %K+%β+=100
    168Lu 5.5 m (6-) %K+%β+=100
    168m1Lu 6.7 m 3+ %K+%β+ > 95, %IT < 5
    169Lu 34.06 h 7/2+ %K+%β+=100
    169m1Lu 160 s 1/2- %IT=100
    170Lu 2.012 d 0+ %K+%β+=100
    170m1Lu 0.67 s (4) - %IT=100
    171Lu 8.24 d 7/2+ %K+%β+=100
    171m1Lu 79 s 1/2- %IT=100
    172Lu 6.70 d 4- %K+%β+=100
    172m1Lu 3.7 m 1- %IT=100
    173Lu 1.37 a 7/2+ %K=100
    174Lu 3.31 a (1) - %K+%β+=100
    174m1Lu 142 d (6) - %IT=99.38 , %K=0.62
    175Lu stable 7/2+ %Abundance=97.41
    176Lu 3.78e10 a 7- %Abundance=2.59, %β-=100
    176m1Lu 3.635 h 1- %β-=99.905 , %K=0.095
    177Lu 6.734 d 7/2+ %β-=100
    177m1Lu 160.4 d 23/2- %β-=78.3 , %IT=21.7
    178Lu 28.4 m 1(+) %β-=100
    178m1Lu 23.1 m (9-) %β-=100
    179Lu 4.59 h 7/2(+) %β-=100
    179m1Lu 3.1 ms 1/2(+) %IT=100
    180Lu 5.7 m (5) + %β-=100
    181Lu 3.5 m (7/2+ ) %β-=100
    182Lu 2.0 m (0,1,2) %β-=100
    183Lu 58 s (7/2+ ) %β-=100
    184Lu 20 s (2+ ) %β-=100

    Hafnium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    154Hf 2 s 0+ %K+%β+=100
    155Hf 0.89 s %K+%β+=100, %α=?
    156Hf 25 ms 0+ %α > 81
    156m1Hf 444 μs
    157Hf 110 ms 7/2- %α=86 , %K+%β+=14
    158Hf 2.85 s 0+ %α=44 , %K+%β+=56
    159Hf 5.6 s %K+%β+=59 , %α=41
    160Hf 13.6 s 0+ %K+%β+=99.3 , %α=0.7
    161Hf 16.8 s (13/2+ ) %K+%β+=99.71 , %α=0.29
    162Hf 37.6 s 0+ %K+%β+=99.9937 , %α=0.0063
    163Hf 40.0 s %K+%β+=100
    164Hf 111 s 0+ %K+%β+=100
    165Hf 76 s (5/2-) %K+%β+=100
    166Hf 6.77 m 0+ %K+%β+=100
    167Hf 2.05 m (5/2-) %K+%β+=100
    168Hf 25.95 m 0+ %K+%β+=100
    169Hf 3.24 m (5/2) - %K+%β+=100
    170Hf 16.01 h 0+ %K=100
    171Hf 12.1 h (7/2+ ) %K+%β+=100
    172Hf 1.87 a 0+ %K=100
    173Hf 23.6 h 1/2- %K+%β+=100
    174Hf 2.0e15 a 0+ %Abundance=0.162, %α=100
    175Hf 70 d 5/2- %K=100
    176Hf stable 0+ %Abundance=5.206
    177Hf stable 7/2- %Abundance=18.606
    177m1Hf 1.08 s 23/2+ %IT=100
    177m2Hf 51.4 m 37/2- %IT=100
    178Hf stable 0+ %Abundance=27.297
    178m1Hf 4.0 s 8- %IT=100
    178m2Hf 31 a 16+ %IT=100
    179Hf stable 9/2+ %Abundance=13.629
    179m1Hf 18.67 s 1/2- %IT=100
    179m2Hf 25.05 d 25/2- %IT=100
    180Hf stable 0+ %Abundance=35.100
    180m1Hf 5.5 h 8- %IT=99.7 , %β-=0.3
    181Hf 42.39 d 1/2- %β-=100
    182Hf 9e6 a 0+ %β-=100
    182m1Hf 61.5 m 8- %β-=58 , %IT=42
    183Hf 1.067 h (3/2-) %β-=100
    184Hf 4.12 h 0+ %β-=100
    184m1Hf 48 s (8-) %IT=100
    185Hf 3.5 m %β-=100

    Tantalum

    Isotope Half-life Spin Parity Mode(s) or Abundance
    156Ta 144 ms (2-) %p ~ 100
    156m1Ta 375 ms (9+ ) %K+%β+=95.8 , %p=4.2
    157Ta 10.1 ms 1/2+ %α=96.6 , %p=3.4
    157m1Ta 4.3 ms 11/2- %K+%β+ ~ 5
    158Ta 36.5 ms (2-) %α=93 , %K+%β+=7
    158m1Ta 49 ms (9+ ) %α ~ 100
    159Ta 0.57 s %α=80 , %K+%β+=20
    160Ta 1.55 s (9+ ) %K+%β+=66, %α=34
    160m1Ta 1.7 s (2-) %α=?
    161Ta 2.7 s %K+%β+ ~ 95, %α ~ 5
    162Ta 3.52 s %K+%β+=99.926 , %α=0.074
    163Ta 10.6 s %K+%β+ ~ 99.8, %α ~ 0.2
    164Ta 14.2 s (3+ ) %K+%β+=100
    165Ta 31.0 s %K+%β+=100
    166Ta 34.4 s (2) + %K+%β+=100
    167Ta 1.4 m (3/2+ ) %K+%β+=100
    168Ta 2.0 m (3+ ) %K+%β+=100
    169Ta 4.9 m (5/2-) %K+%β+=100
    170Ta 6.76 m (3+ ) %K+%β+=100
    171Ta 23.3 m (5/2-) %K+%β+=100
    172Ta 36.8 m (3+ ) %K+%β+=100
    173Ta 3.14 h 5/2- %K+%β+=100
    174Ta 1.05 h 3+ %K+%β+=100
    174m1Ta 250 ns
    175Ta 10.5 h 7/2+ %K+%β+=100
    176Ta 8.09 h (1) - %K+%β+=100
    176m1Ta 1.1 ms (+) %IT=100
    176m2Ta 1.4 ms (20- )
    177Ta 56.56 h 7/2+ %K+%β+=100
    178Ta 9.31 m 1+ %K+%β+=100
    178m1Ta 2.36 h (7) - %K+%β+=100
    178m2Ta 60 ms (15-) %IT=100
    179Ta 1.82 a 7/2+ %K=100
    179m1Ta 9.0 ms (25/2+ )
    179m2Ta 52 ms (37/2+ )
    180Ta 8.152 h 1+ %Abundance=0.012, %K=86 , %β-=14
    180m1Ta 1.2e+15 a 9-
    181Ta stable 7/2+ %Abundance=99.988
    182Ta 114.43 d 3- %β-=100
    182m1Ta 283 ms 5+ %IT=100
    182m2Ta 15.84 m 10- %IT=100
    183Ta 5.1 d 7/2+ %β-=100
    184Ta 8.7 h (5-) %β-=100
    185Ta 49.4 m (7/2+ ) %β-=100
    186Ta 10.5 m (2- ,3-) %β-=100

    Tungsten

    Isotope Half-life Spin Parity Mode(s) or Abundance
    158W 0.9 ms 0+ %α=100
    158m1W 0.16 ms 8+
    159W 7.3 ms %α ~ 99.5, %K+%β+ ~ 0.5
    160W 91 ms 0+ %α=87 , %K+%β+=?
    161W 410 ms %α=82
    162W 1.39 s 0+ %K+%β+=53 , %α=47
    163W 2.75 s %K+%β+=59 , %α=41
    164W 6.0 s 0+ %K+%β+=95.6 , %α=4.4
    165W 5.1 s %K+%β+=100 , %α < 0.2
    166W 18.8 s 0+ %K+%β+=99.965 , %α=0.035
    167W 19.9 s (7/2-) %K+%β+=?, %α=?
    168W 53 s 0+ %K+%β+ ~ 100, %α=2.7E-3
    169W 76 s (5/2-) %K+%β+=100
    170W 2.42 m 0+ %K+%β+=100
    171W 2.38 m (5/2-) %K+%β+=100
    172W 6.6 m 0+ %K+%β+=100
    173W 7.6 m 5/2- %K+%β+=100
    174W 31 m 0+ %K+%β+=100
    175W 35.2 m (1/2-) %K+%β+=100
    176W 2.5 h 0+ %K=100
    177W 135 m (1/2-) %K+%β+=100
    178W 21.6 d 0+ %K=100
    179W 37.05 m (7/2) - %K+%β+=100
    179m1W 6.40 m (1/2) - %IT=99.72 , %K+%β+=0.28
    180W stable 0+ %Abundance=0.13
    180m1W 5.47 ms 8- %IT=100
    181W 121.2 d 9/2+ %K=100
    182W stable 0+ %Abundance=26.3
    183W 1.1e+17 a 1/2- %Abundance=14.3
    183m1W 5.2 s 11/2+ %IT=100
    184W 3e+17 a 0+ %Abundance=30.67
    185W 75.1 d 3/2- %β-=100
    185m1W 1.67 m 11/2+ %IT=100
    186W stable 0+ %Abundance=28.6
    187W 23.72 h 3/2- %β-=100
    188W 69.4 d 0+ %β-=100
    189W 11.5 m (3/2-) %β-=100
    190W 30.0 m 0+ %β-=100

    Rhenium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    160Re 0.79 ms %p=91 , %α=9
    161Re 0.37 ms (1/2+ ) %p=100
    161m1Re 16 ms (11/2-) %α=95.2 , %p=4.8
    162Re 107 ms (2-) %α=94
    162m1Re 75 ms (9+ ) %α=91
    163Re 260 ms %α=64 , %K+%β+=36
    164Re 0.38 s %K+%β+ ~ 100
    164m1Re 0.88 s %α=?
    165Re 2.4 s %K+%β+=87 , %α=13
    166Re 2.8 s %α < 8
    167Re 6.1 s %K+%β+ ~ 99.3, %α ~ 0.7
    168Re 4.4 s (6+ ) %K+%β+ ~ 100, %α ~ 5E-3
    169Re
    169m1Re 12.9 s %α ~ 0.2
    170Re 9.2 s (5+ ) %K+%β+=100
    171Re 15.2 s (9/2-) %K+%β+=100
    172Re 15 s (5) %K+%β+=100
    172m1Re 55 s (2) %K+%β+=100
    173Re 1.98 m (5/2-) %K+%β+=100
    174Re 2.40 m %K+%β+=100
    175Re 5.89 m (5/2-) %K+%β+=100
    176Re 5.3 m 3(+) %K+%β+=100
    177Re 14 m (5/2-) %K+%β+=100
    178Re 13.2 m (3+ ) %K+%β+=100
    179Re 19.5 m (5/2) + %K+%β+=100
    180Re 2.44 m (1) - %K+%β+=100
    181Re 19.9 h 5/2+ %K+%β+=100
    182Re 64.0 h 7+ %K+%β+=100
    182m1Re 12.7 h 2+ %K+%β+=100
    183Re 70.0 d 5/2+ %K=100
    183m1Re 1.04 ms (25/2) + %IT=100
    184Re 38.0 d 3(-) %K+%β+=100
    184m1Re 169 d 8(+) %IT=75.4 , %K=24.6
    185Re stable 5/2+ %Abundance=37.40
    186Re 3.7183 d 1- %K=7.47 , %β-=92.53
    186m1Re 2.0e+5 a (8+ ) %IT=100
    187Re 4.35e10 a 5/2+ %Abundance=62.60, %β-=100, %α < 0.0001
    188Re 17.005 h 1- %β-=100
    188m1Re 18.6 m (6) - %IT=100
    189Re 24.3 h 5/2+ %β-=100
    190Re 3.1 m (2) - %β-=100
    190m1Re 3.2 h (6-) %β-=54.4 , %IT=45.6
    191Re 9.8 m (3/2+ , 1/2+ ) %β-=100
    192Re 16 s %β-=100

    Osmium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    162Os 1.9 ms 0+ %α=100
    163Os %α=?, %K+%β+=?
    164Os 21 ms 0+ %α ~ 98 , %K+%β+ ~ 2
    165Os 71 ms (7/2-) %α > 60 , %K+%β+ < 40
    166Os 181 ms 0+ %α=72 , %K+%β+=28
    167Os 0.83 s %α=67 , %K+%β+=33
    168Os 2.1 s 0+ %K+%β+=56 , %α=44
    169Os 3.4 s %K+%β+=89 , %α=11
    170Os 7.3 s 0+ %K+%β+=88 , %α=12
    171Os 8.0 s (5/2-) %K+%β+=98.3 , %α=1.7
    172Os 19.2 s 0+ %K+%β+=99.0 , %α=1.0
    173Os 16 s (5/2-) %K+%β+=99.979 , %α=0.021
    174Os 44 s 0+ %K+%β+=99.980 +4-10, %α=0.020 +10-4
    175Os 1.4 m (5/2-) %K+%β+=100
    176Os 3.6 m 0+ %K+%β+=100
    177Os 2.8 m (1/2-) %K+%β+=100
    178Os 5.0 m 0+ %K+%β+=100
    179Os 6.5 m (1/2-) %K+%β+=100
    180Os 21.5 m 0+ %K+%β+=100
    181Os 105 m 1/2- %K+%β+=100
    181m1Os 2.7 m (7/2) - %K+%β+=100
    182Os 22.10 h 0+ %K=100
    183Os 13.0 h 9/2+ %K+%β+=100
    183m1Os 9.9 h 1/2- %K+%β+=85 , %IT=15
    184Os 5.6e13 a 0+ %Abundance=0.02
    185Os 93.6 d 1/2- %K=100
    186Os 2.0e15 a 0+ %Abundance=1.58, %α=100
    187Os stable 1/2- %Abundance=1.6
    188Os stable 0+ %Abundance=13.3
    189Os stable 3/2- %Abundance=16.1
    189m1Os 5.8 h 9/2- %IT=100
    190Os stable 0+ %Abundance=26.4
    190m1Os 9.9 m (10) - %IT=100
    191Os 15.4 d 9/2- %β-=100
    191m1Os 13.10 h 3/2- %IT=100
    192Os stable 0+ %Abundance=41.0
    192m1Os 5.9 s (10- ) %IT > 87, %β- < 13
    193Os 30.11 h 3/2- %β-=100
    194Os 6.0 a 0+ %β-=100
    195Os 6.5 m %β-=100
    196Os 34.9 m 0+ %β-=100

    Iridium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    165Ir 300 μs (11/2-) %p=87 , %α=13
    166Ir 10.5 ms (2-) %α=93 , %p=7
    166m1Ir 15.1 ms (9+ ) %α=98.2 , %p=1.8
    167Ir 5 ms %α=?
    168Ir 161 ms %α=?
    169Ir 0.4 s %α ~ 100, %K+%β+=?, %p=?
    170Ir 1.05 s %K+%β+=25 sys%α=75 sys
    171Ir 1.5 s %α ~ 100, %K+%β+=?, %p=?
    172Ir 4.4 s (3+ ) %α ~ 2, %K+%β+=98
    172m1Ir 2.0 s (7+ ) %α=23 , %K+%β+=77
    173Ir 9.0 s (3/2+ , 5/2+ ) %K+%β+ > 93, %α < 7
    173m1Ir 2.20 s (11/2-) %K+%β+=88 , %α=12
    174Ir 9 s (3+ ) %K+%β+=99.53 , %α=0.47
    174m1Ir 4.9 s (7+ ) %K+%β+=97.5 , %α=2.5
    175Ir 9 s (5/2-) %K+%β+=99.15 , %α=0.85
    176Ir 8 s %K+%β+=97.9 , %α=2.1
    177Ir 30 s (5/2-) %K+%β+=99.94 , %α=0.06
    178Ir 12 s %K+%β+=100
    179Ir 79 s (5/2) - %K+%β+=100
    180Ir 1.5 m %K+%β+=100
    181Ir 4.90 m (5/2) - %K+%β+=100
    182Ir 15 m (5+ ) %K+%β+=100
    183Ir 58 m 5/2- %K+%β+=100
    184Ir 3.09 h 5- %K+%β+=100
    185Ir 14.4 h 5/2- %K+%β+=100
    186Ir 16.64 h 5+ %K+%β+=100
    186m1Ir 1.90 h 2- %K+%β+ ~ 75, %IT ~ 25
    187Ir 10.5 h 3/2+ %K+%β+=100
    187m1Ir 30.3 ms 9/2- %IT=100
    188Ir 41.5 h 1- %K+%β+=100
    188m1Ir 4.2 ms
    189Ir 13.2 d 3/2+ %K=100
    189m1Ir 13.3 ms 11/2- %IT=100
    189m2Ir 3.7 ms (25/2) + %IT=100
    190Ir 11.78 d (4-) %K+%β+=100, %β- < 0.002
    190m1Ir 1.2 h (1-) %IT=100
    190m2Ir 3.25 h (11) - %K+%β+=94.4 , %IT=5.6
    191Ir stable 3/2+ %Abundance=37.3
    191m1Ir 4.94 s 11/2- %IT=100
    191m2Ir 5.5 s %IT=100
    192Ir 73.831 d 4(+) %β-=95.24 , %K=4.76
    192m1Ir 1.45 m 1(-) %IT=99.982, %β-=0.018
    192m2Ir 241 a (9) %IT=100
    193Ir stable 3/2+ %Abundance=62.7
    193m1Ir 10.53 d 11/2- %IT=100
    194Ir 19.28 h 1- %β-=100
    194m1Ir 31.85 ms (4+ ) %IT=100
    194m2Ir 171 d (10,11) %β-=100
    195Ir 2.5 h 3/2+ %β-=100
    195m1Ir 3.8 h 11/2- %β-=95 , %IT=5
    196Ir 52 s (0- ) %β-=100
    196m1Ir 1.40 h (10,11-) %β- ~ 100 , %IT < 0.3
    197Ir 5.8 m 3/2+ %β-=100
    197m1Ir 8.9 m 11/2- %β-=99.75 , %IT=0.25
    198Ir 8 s %β-=100

    Platinum

    Isotope Half-life Spin Parity Mode(s) or Abundance
    168Pt 2.0 ms 0+ %α=100
    169Pt 5 ms %α=?
    170Pt 6 ms 0+ %α=100
    171Pt 25 ms %α ~ 99, %K+%β+ ~ 1
    172Pt 0.096 s 0+ %α=94 +6-32 , %K+%β+=6 +32-6
    173Pt 342 ms %K+%β+=16 , %α=84
    174Pt 0.90 s 0+ %α=75 , %K+%β+=25
    175Pt 2.52 s %α=64 , %K+%β+=36
    176Pt 6.33 s 0+ %K+%β+=62 , %α=38
    177Pt 11 s (5/2-) %K+%β+=94.4 , %α=5.6
    178Pt 21.1 s 0+ %K+%β+=95.4 , %α=4.6
    179Pt 21.2 s 1/2- %K+%β+=99.76 , %α=0.24
    180Pt 52 s 0+ %K+%β+=100, %α ~ 0.3
    181Pt 51 s 1/2- %K+%β+=100, %α ~ 0.06
    182Pt 3.0 m 0+ %K+%β+=99.969 , %α=0.031
    183Pt 6.5 m 1/2- %K+%β+ ~ 100, %α ~ 0.0013
    183m1Pt 43 s (7/2) - %K+%β+=100, %α=?
    184Pt 17.3 m 0+ %K+%β+=100, %α ~ 0.001
    184m1Pt 1.01 ms 8- %IT=100
    184m2Pt 1.1 ms 8-
    185Pt 70.9 m 9/2+ %K+%β+=100, %α=0.0050
    185m1Pt 33.0 m 1/2- %K+%β+=99 , %IT < 2
    186Pt 2.2 h 0+ %K+%β+=100, %α ~ 0.00010
    187Pt 2.35 h 3/2- %K+%β+=100
    188Pt 10.2 d 0+ %K=100, %α=2.9E-5
    189Pt 10.87 h 3/2- %K+%β+=100
    190Pt 6.5e11 a 0+ %Abundance=0.01, %α=100
    191Pt 2.802 d 3/2- %K=100
    192Pt stable 0+ %Abundance=0.79
    193Pt 50 a 1/2- %K=100
    193m1Pt 4.33 d 13/2+ %IT=100
    194Pt stable 0+ %Abundance=32.9
    195Pt stable 1/2- %Abundance=33.8
    195m1Pt 4.02 d 13/2+ %IT=100
    196Pt stable 0+ %Abundance=25.3
    197Pt 19.8915 h 1/2- %β-=100
    197m1Pt 95.41 m 13/2+ %IT=96.7 , %β-=3.3
    198Pt stable 0+ %Abundance=7.2
    199Pt 30.80 m 5/2- %β-=100
    199m1Pt 13.6 s (13/2) + %IT=100
    200Pt 12.5 h 0+ %β-=100
    201Pt 2.5 m (5/2-) %β-=100
    202Pt 44 h 0+ %β-=100

    Gold

    Isotope Half-life Spin Parity Mode(s) or Abundance
    172Au 6.3 ms %α ~ 100, %p < 2
    173Au 59 ms %α < 100
    174Au 120 ms %α=?
    175Au 200 ms %α=94 +6-25, %K+%β+=6 +25-6
    176Au 1.08 s %α=?, %K+%β+=?
    177Au 1.18 s %α < 40
    178Au 2.6 s %K+%β+ < 60, %α > 40
    179Au 7.1 s %K+%β+=78.0 , %α=22.0
    180Au 8.1 s %K+%β+ < 98.2, %α > 1.8
    181Au 11.4 s 5/2- %K+%β+=98.7 , %α=1.3
    182Au 15.6 s %K+%β+=99.87 , %α=0.13
    183Au 42.0 s (5/2) - %K+%β+=99.70 , %α=0.30
    184Au 53.0 s 3+ %K+%β+=99.978, %α=0.022
    185Au 4.25 m 5/2- %K+%β+=99.74 , %α=0.26
    185m1Au 6.8 m %K+%β+ < 100, %IT=?
    186Au 10.7 m 3- %K+%β+=100, %α=8E-4
    187Au 8.4 m 1/2+ %K+%β+=100, %α=0.003 sys
    187m1Au 2.3 s 9/2- %IT=100
    188Au 8.84 m 1(-) %K+%β+=100
    189Au 28.7 m 1/2+ %K+%β+=100, %α < 3E-5
    189m1Au 4.59 m 11/2- %K+%β+ ~ 100, %IT > 0
    190Au 42.8 m 1- %K+%β+=100, %α < 1E-6
    190m1Au 125 ms (11-) %IT=?, %K+%β+=?
    191Au 3.18 h 3/2+ %K+%β+=100
    191m1Au 0.92 s (11/2-) %IT=100
    192Au 4.94 h 1- %K+%β+=100
    192m1Au 29 ms (5) + %IT=100
    192m2Au 160 ms (11-) %IT=100
    193Au 17.65 h 3/2+ %K+%β+=100
    193m1Au 3.9 s 11/2- %IT=99.97, %K+%β+ ~ 0.03
    194Au 38.02 h 1- %K+%β+=100
    194m1Au 600 ms (5+ ) %IT=100
    194m2Au 420 ms (11-) %IT=100
    195Au 186.09 d 3/2+ %K=100
    195m1Au 30.5 s 11/2- %IT=100
    196Au 6.183 d 2- %K+%β+=92.80 , %β- =7.20
    196m1Au 8.1 s 5+ %IT=100
    196m2Au 9.6 h 12- %IT=100
    197Au stable 3/2+ %Abundance=100
    197m1Au 7.73 s 11/2- %IT=100
    198Au 2.69517 d 2- %β-=100
    198m1Au 2.27 d (12-) %IT=100
    199Au 3.139 d 3/2+ %β-=100
    200Au 48.4 m 1(-) %β-=100
    200m1Au 18.7 h 12- %β-=82 , %IT=18
    201Au 26 m 3/2+ %β-=100
    202Au 28.8 s (1-) %β-=100
    203Au 53 s 3/2+ %β-=100
    204Au 39.8 s (2-) %β-=100
    205Au 31 s (3/2+ ) %β-=100

    Mercury

    Isotope Half-life Spin Parity Mode(s) or Abundance
    175Hg 20 ms %α=100
    176Hg 18 ms 0+ %α ~ 100
    177Hg 0.130 s %α=85, %K+%β+=15
    178Hg 266 ms 0+ %K+%β+=?, %α ~ 100
    179Hg 1.09 s %K+%β+ ~ 47, %α ~ 53, %Kp ~ 0.15
    180Hg 2.8 s 0+ %K+%β+=52 , %α=48
    181Hg 3.6 s 1/2(-) %K+%β+=64 , %α=36 , %Kp=0.014 , %Kα=9E-6
    182Hg 10.83 s 0+ %K+%β+=84.8 , %α=15.2
    183Hg 9.4 s 1/2- %K+%β+=88.3 , %α=11.7 , %Kp=0.00056
    184Hg 30.9 s 0+ %K+%β+=98.74 , %α=1.26
    185Hg 49.1 s 1/2- %K+%β+=94 , %α=6
    185m1Hg 21.6 s 13/2+ %IT=54 , %K+%β+=46 , %α ~ 0.03
    186Hg 1.38 m 0+ %K+%β+=99.982 , %α=0.018
    187Hg 2.4 m 13/2+ %K+%β+=100, %α>1.2E-4
    187m1Hg 1.9 m 3/2- %K+%β+=100, %α>2.5E-4
    188Hg 3.25 m 0+ %K+%β+=100, %α=4.0E-5
    189Hg 7.6 m 3/2- %K+%β+=100, %α < 3E-5
    189m1Hg 8.6 m 13/2+ %K+%β+=100, %α < 3E-5
    190Hg 20.0 m 0+ %K+%β+=100, %α < 5E-5
    191Hg 49 m (3/2-) %K+%β+=100
    191m1Hg 50.8 m 13/2+ %K+%β+=100
    192Hg 4.85 h 0+ %K=100, %α < 4E-6
    193Hg 3.80 h 3/2- %K+%β+=100
    193m1Hg 11.8 h 13/2+ %K+%β+=92.8 , %IT=7.2
    194Hg 444 a 0+ %K=100
    195Hg 9.9 h 1/2- %K+%β+=100
    195m1Hg 41.6 h 13/2+ %IT=54.2 , %K+%β+=45.8
    196Hg stable 0+ %Abundance=0.15
    197Hg 64.14 h 1/2- %K=100
    197m1Hg 23.8 h 13/2+ %K=8.6 , %IT=91.4
    198Hg stable 0+ %Abundance=9.97
    199Hg stable 1/2- %Abundance=16.87
    199m1Hg 42.6 m 13/2+ %IT=100
    200Hg stable 0+ %Abundance=23.10
    201Hg stable 3/2- %Abundance=13.18
    202Hg stable 0+ %Abundance=29.86
    203Hg 46.612 d 5/2- %β-=100
    204Hg stable 0+ %Abundance=6.87
    205Hg 5.2 m 1/2- %β-=100
    205m1Hg 1.10 ms (13/2+ ) %IT=100
    206Hg 8.15 m 0+ %β-=100
    207Hg 2.9 m (9/2+ ) %β-=100
    208Hg 42 m 0+ %β-=100

    Thallium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    179Tl 0.16 s %α ~ 100
    179m1Tl 1.4 ms (9/2-) %α ~ 100
    180Tl 0.70 s %K+%β+=?, %KSF ~ 1.0E-4
    181Tl (1/2+ )
    181m1Tl 3.4 s (9/2-) %α=?
    182Tl 3.1 s (7+ ) %K+%β+ > 96, %α < 4
    183Tl (1/2+ )
    183m1Tl 60 ms (9/2-) %α < 0.010
    184Tl 11 s %K+%β+=97.9 , %α=2.1
    185Tl 19.5 s (1/2+ ) %K+%β+=?
    185m1Tl 1.83 s (9/2-) %IT=?, %α=?
    186Tl 27.5 s (7+ ) %K+%β+=100, %α ~ 0.006
    186m1Tl 2.9 s (10- ) %IT=100
    187Tl 51 s (1/2+ ) %K+%β+=?, %α=?
    187m1Tl 15.60 s (9/2-) %α=?, %K+%β+=?, %IT=?
    188Tl 71 s (2-) %K+%β+=100
    188m1Tl 71 s (7+ ) %K+%β+=100
    188m2Tl 41 ms (9-) %IT=100
    189Tl 2.3 m (1/2+ ) %K+%β+=100
    189m1Tl 1.4 m (9/2-) %K+%β+=100, %IT<4
    190Tl 2.6 m (2) - %K+%β+=100
    190m1Tl 3.7 m (7+ ) %K+%β+=100
    191Tl (1/2+ )
    191m1Tl 5.22 m 9/2(-) %K+%β+=100
    192Tl 9.6 m (2-) %K+%β+=100
    192m1Tl 10.8 m (7+ ) %K+%β+=100
    193Tl 21.6 m 1/2+ %K+%β+=100
    193m1Tl 2.11 m 9/2- %IT=75, %K+%β+=25
    194Tl 33.0 m 2- %K+%β+=100 , %α < 1E-7
    194m1Tl 32.8 m (7+ ) %K+%β+=100
    195Tl 1.16 h 1/2+ %K+%β+=100
    195m1Tl 3.6 s 9/2- %IT=100
    196Tl 1.84 h 2- %K+%β+=100
    196m1Tl 1.41 h (7+ ) %K+%β+=95.5 , %IT=4.5
    197Tl 2.84 h 1/2+ %K+%β+=100
    197m1Tl 0.54 s 9/2- %IT=100
    198Tl 5.3 h 2- %K+%β+=100
    198m1Tl 1.87 h 7+ %IT=46 , %K+%β+=54
    198m2Tl 32.1 ms (10- ) %IT=100
    199Tl 7.42 h 1/2+ %K+%β+=100
    199m1Tl 28.4 ms 9/2- %IT=100
    200Tl 26.1 h 2- %K+%β+=100
    200m1Tl 34.3 ms 7+ %IT=100
    201Tl 72.912 h 1/2+ %K=100
    201m1Tl 2.035 ms (9/2-) %IT=100
    202Tl 12.23 d 2- %K+%β+=100
    202m1Tl 572 μs 7+
    203Tl stable 1/2+ %Abundance=29.524
    204Tl 3.78 a 2- %β-=97.10 , %K+%β+=2.90
    205Tl stable 1/2+ %Abundance=70.476
    206Tl 4.199 m 0- %β-=100
    206m1Tl 3.74 m (12-) %IT=100
    207Tl 4.77 m 1/2+ %β-=100
    207m1Tl 1.33 s 11/2- %IT=100, %β- < 0.1
    208Tl 3.053 m 5(+) %β-=100
    209Tl 2.20 m (1/2+ ) %β-=100
    210Tl 1.30 m (5+ ) %β-=100, %β-n=0.007 +7- 4



    Lead

    Isotope Half-life Spin Parity Mode(s) or Abundance
    181Pb 45 ms (13/2+ ) %α ~ 98
    182Pb 55 ms 0+ %α=?
    183Pb 300 ms (1/2-) %α ~ 94, %K+%β+ ~ 6
    184Pb 0.55 s 0+ %α=?
    185Pb 4.1 s %α < 100
    186Pb 4.83 s 0+ %α=54 , %K+%β+=46
    187Pb 18.3 s (13/2+ ) %K+%β+=98.0, %α=2.0
    187m1Pb 15.2 s %α=?, %K+%β+=?
    188Pb 24 s 0+ %K+%β+=91.5 , %α=8.5
    189Pb 51 s %K+%β+ > 99, %α ~ 0.4
    190Pb 1.2 m 0+ %K+%β+=99.79 , %α=0.21
    191Pb 1.33 m (3/2-) %K+%β+=99.987 , %α=0.013
    191m1Pb 2.18 m (13/2+ ) %K+%β+=100, %α ~ 0.02
    192Pb 3.5 m 0+ %K+%β+=99.9941 , %α=0.0059
    193Pb 2 m (3/2-) %K+%β+=?
    193m1Pb 5.8 m (13/2+ ) %K+%β+=100
    194Pb 12.0 m 0+ %K+%β+=100, %α=7.3E-6
    195Pb 15 m 3/2- %K+%β+=100
    195m1Pb 15.0 m 13/2+ %K+%β+=100
    196Pb 37 m 0+ %K+%β+=100, %α < 3E-5
    197Pb 8 m 3/2- %K+%β+=100
    197m1Pb 43 m 13/2+ %K+%β+=81 , %IT=19
    198Pb 2.40 h 0+ %K+%β+=100
    199Pb 90 m 3/2- %K+%β+=100
    199m1Pb 12.2 m 13/2+ %IT=93, %K+%β+=7
    200Pb 21.5 h 0+ %K=100
    201Pb 9.33 h 5/2- %K+%β+=100
    201m1Pb 61 s 13/2+ %IT>99, %K+%β+<1
    202Pb 5.25e4 a 0+ %K=100, %α<1
    202m1Pb 3.53 h 9- %IT=90.5 , %K+%β+=9.5
    203Pb 51.873 h 5/2- %K=100
    203m1Pb 6.3 s 13/2+ %IT=100
    203m2Pb 0.48 s 29/2- %IT=100
    204Pb 1.4e17 a 0+ %Abundance=1.4
    204m1Pb 67.2 m 9- %IT=100
    205Pb 1.53e+7 a 5/2- %K=100
    205m1Pb 5.54 ms 13/2+ %IT=100
    206Pb stable 0+ %Abundance=24.1
    207Pb stable 1/2- %Abundance=22.1
    207m1Pb 0.805 s 13/2+ %IT=100
    208Pb stable 0+ %Abundance=52.4
    209Pb 3.253 h 9/2+ %β-=100
    210Pb 22.3 a 0+ %β-=100, %α=1.9E-6
    211Pb 36.1 m 9/2+ %β- =100
    212Pb 10.64 h 0+ %β-=100
    213Pb 10.2 m (9/2+ ) %β-=100
    214Pb 26.8 m 0+ %β-=100
    215Pb 36 s (5/2+ ) %β-=100

    Bismuth

    Isotope Half-life Spin Parity Mode(s) or Abundance
    185Bi 44 μs (1/2+ ) %p ~ 100
    186Bi 15.0 ms (3+ ) %α ~ 100
    186m1Bi 9.8 ms (10- ) %α ~ 100
    187Bi 35 ms (9/2-) %α>50
    187m1Bi 0.8 ms (1/2+ )
    188Bi 0.21 s %α=?, %K+%β+=?
    188m1Bi 44 ms %α=?, %K+%β+=?
    189Bi 680 ms (9/2-) %α > 50, %K+%β+ < 50
    189m1Bi 5 ms (1/2+ ) %α > 50, %K+%β+ < 50
    190Bi 6.3 s (3+ ) %α=80 , %K+%β+=20
    190m1Bi 6.2 s (10- ) %α=70 , %K+%β+=30
    191Bi 12 s (9/2-) %α=60 , %K+%β+=40
    191m1Bi 150 ms (1/2+ ) %α > 50, %K+%β+ < 50
    192Bi 37 s (2+ , 3+ ) %K+%β+=82 , %α=18
    192m1Bi 39.6 s (10- ) %K+%β+=90.8 , %α=9.2
    193Bi 67 s (9/2-) %K+%β+=96.5 , %α=3.5
    193m1Bi 3.2 s (1/2+ ) %α=90 +10-20, %K+%β+=10 +20-10
    194Bi 95 s (3+ ) %K+%β+=99.54 , %α=0.46
    194m1Bi 115 s (10- ) %K+%β+=99.80 , %α=0.20
    194m2Bi 125 s (6+ , 7+ ) %K+%β+=100
    195Bi 183 s (9/2-) %K+%β+=99.967 , %α=0.033
    195m1Bi 87 s (1/2+ ) %K+%β+=67 , %α=33
    196Bi 308 s (3+ ) %K+%β+=100, %α=0.00115
    196m1Bi 0.6 s (7+ ) %IT=100
    196m2Bi 240 s (10- ) %K+%β+=74.2 , %IT=25.8 , %α=0.00038
    197Bi 9.33 m (9/2-) %K+%β+=100, %α=1E-4 sys
    197m1Bi 5.04 m (1/2+ ) %K+%β+=45 , %α=55 , %IT < 0.3
    198Bi 10.3 m (2+ , 3+ ) %K+%β+=100
    198m1Bi 11.6 m (7+ ) %K+%β+=100
    198m2Bi 7.7 s (10- ) %IT=100
    199Bi 27 m 9/2- %K+%β+=100
    199m1Bi 24.70 m (1/2+ ) %K+%β+=99 , %α ~ 0.01, %IT < 2
    200Bi 36.4 m 7+ %K+%β+=100
    200m1Bi 31 m (2+ ) %K+%β+ > 90, %IT < 10
    200m2Bi 0.40 s (10- ) %IT=100
    201Bi 108 m 9/2- %K+%β+=100, %α < 1E-4
    201m1Bi 59.1 m 1/2+ %K > 93, %IT < 6.8, %α ~ 0.3
    202Bi 1.72 h 5+ %K+%β+=100, %α<1E-5
    203Bi 11.76 h 9/2- %K+%β+=100, %α ~ 1E-5
    203m1Bi 303 ms 1/2+ %IT=100
    204Bi 11.22 h 6+ %K+%β+=100
    204m1Bi 13.0 ms 10- %IT=100
    204m2Bi 1.07 ms (17+ ) %IT=100
    205Bi 15.31 d 9/2- %K+%β+=100
    206Bi 6.243 d 6(+) %K+%β+=100
    207Bi 31.55 a 9/2- %K+%β+=100
    208Bi 3.68e+5 a (5) + %K+%β+=100
    208m1Bi 2.58 ms (10) - %IT=100
    Bi 1.910 yr 9/2- %α=100 , %Abundance=100
    210Bi 5.013 d 1- %β-=100, %α=1.32E-4
    210m1Bi 3.04e+6 a 9- %α=100
    211Bi 2.14 m 9/2- %α=99.724 , %β-=0.276
    212Bi 60.55 m 1(-) %β-=64.06 , %α=35.94 , %β-α=0.023
    212m1Bi 25.0 m (9-) %α=67 , %β-=33 , %β-α=30
    212m2Bi 7.0 m %β- ~ 100
    213Bi 45.59 m 9/2- %β-=97.91 , %α=2.09
    214Bi 19.9 m 1- %β-=99.979 , %α=0.021
    215Bi 7.6 m %β-=100
    216Bi 3.6 m (1-) %β- ~ 100
    217Bi 97 s (9/2-) %β-=100

    Polonium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    190Po 2.0 ms 0+ %α=100, %K+%β+=0.1 sys
    191Po 15.5 ms %α=?
    192Po 0.0332 s 0+ %α=100
    193Po 0.42 s (3/2- ) %α=?
    193m1Po 0.24 s (13/2+ ) %α=?
    194Po 0.392 s 0+ %α=93
    195Po 4.64 s (3/2- ) %α=75 , %K+%β+=25
    195m1Po 1.92 s (13/2+ ) %α ~ 90, %K+%β+ ~ 10, %IT < 0.01
    196Po 5.8 s 0+ %α ~ 98, %K+%β+ ~ 2
    197Po 53.6 s (3/2- ) %K+%β+=56 , %α=44
    197m1Po 25.8 s (13/2+ ) %α=84 , %K+%β+=16 , %IT=0.01 sys
    198Po 1.77 m 0+ %α=57 , %K+%β+=43
    199Po 5.48 m 3/2- %K+%β+=88 , %α=12
    199m1Po 4.13 m 13/2+ %K+%β+=59 , %α=39 , %IT=2.1
    200Po 11.5 m 0+ %α=11.1 , %K+%β+=88.9
    201Po 15.3 m 3/2- %K+%β+=98.4 , %α=1.6
    201m1Po 8.9 m 13/2+ %IT=56 , %K=41 , %α ~ 2.9
    202Po 44.7 m 0+ %K+%β+=98.08 , %α=1.92
    202m1Po 85 ns 8+
    202m2Po 200 ns 11-
    202m3Po 19 ns 12+
    202m4Po 11 ns (15-)
    203Po 36.7 m 5/2- %K+%β+=99.89 , %α=0.11
    203m1Po 45 s 13/2+ %IT ~ 100 , %α ~ 0.04 sys
    204Po 3.53 h 0+ %K+%β+=99.34 , %α=0.66
    205Po 1.66 h 5/2- %K+%β+=99.96 , %α=0.04
    205m1Po 58 ms 19/2- %IT=100
    206Po 8.8 d 0+ %K+%β+=94.55 , %α=5.45
    207Po 5.80 h 5/2- %K+%β+=99.979 , %α=0.021
    207m1Po 2.8 s 19/2- %IT=100
    208Po 2.898 a 0+ %α=99.9958 , %K+%β+=0.0042
    209Po 102 a 1/2- %α=99.52 , %K+%β+=0.48
    210Po 138.376 d 0+ %α=100
    211Po 0.516 s 9/2+ %α=100
    211m1Po 25.2 s (25/2+ ) %α=99.984 , %IT=0.016
    212Po 0.299 μs 0+ %α=100
    212m1Po 45.1 s (18+) %α=99.93 , %IT=0.07
    213Po 4.2 μs 9/2+ %α=100
    214Po 164.3 μs 0+ %α=100
    215Po 1.781 ms 9/2+ %α=99.99977 , %β-=2.3E-4
    216Po 0.145 s 0+ %α=100
    217Po 10 s %α > 95, %β- < 5
    218Po 3.10 m 0+ %α=99.980 , %β-=0.020

    Astatine

    Isotope Half-life Spin Parity Mode(s) or Abundance
    193At 40 ms %α=?
    194At 40 ms %α=?
    194m1At 250 ms %α=?
    195At 0.63 s %α > 75, %K+%β+ < 25
    196At 0.253 s %α ~ 100
    197At 0.35 s (9/2- ) %α=96 , %K+%β+=4
    197m1At 3.7 s (1/2+ ) %α=?, %K+%β+=?
    198At 4.2 s (3+ ) %α=90 , %K+%β+=10
    198m1At 1.0 s (10- ) %α=84 , %K+%β+=16
    199At 7.2 s (9/2- ) %α=90 , %K+%β+=10
    200At 43 s (3+ ) %α=57 , %K+%β+=43
    200m1At 47 s (7+) %α=43 , %K+%β+ < 57
    200m2At 3.5 s (10- ) %α ~ 10.5, %IT ~ 85, %K ~ 4.5
    201At 89 s (9/2- ) %α=71 , %K+%β+=29
    202At 184 s (2,3)+ %K+%β+=82 , %α=18
    202m1At 182 s (7+) %K+%β+=91.3, %α=8.7
    202m2At 0.46 s (10- ) %IT=99.7 , %K+%β+=0.25 sys %α=0.096
    203At 7.4 m 9/2- %K+%β+=69 , %α=31
    204At 9.2 m 7+ %K+%β+=96.2 , %α=3.8
    204m1At 108 ms (10- ) %IT=100
    205At 26.2 m 9/2- %K+%β+=90 , %α=10
    206At 30.0 m (5)+ %K+%β+=99.11 , %α=0.89
    207At 1.80 h 9/2- %K+%β+=91.4 , %α=8.6
    208At 1.63 h 6+ %K+%β+=99.45 , %α=0.55
    209At 5.41 h 9/2- %K+%β+=95.9 , %α=4.1
    210At 8.1 h (5)+ %K+%β+=99.825 , %α=0.175
    211At 7.214 h 9/2- %α=41.80 , %K=58.20
    212At 0.314 s (1- ) %α=100, %β- < 2E-6, %K+%β+ < 3E-2
    212m1At 0.119 s (9-) %α > 99, %IT < 1
    213At 125 ns 9/2- %α=100
    214At 558 ns 1- %α=100
    214m1At 265 ns
    214m2At 760 ns 9-
    215At 0.10 ms 9/2- %α=100
    216At 0.30 ms 1- %α=100, %K<3E-7, %β-<6E-3
    216m1At 0.1 ms (9-)
    217At 32.3 ms 9/2- %α=99.988 , %β-=0.012
    218At 1.5 s %α=99.9 , %β-=0.1
    219At 56 s %α ~ 97, %β- ~ 3
    220At 3.71 m 3 %α=8 , %β-=92
    221At 2.3 m %β-=100
    222At 54 s %β-=100
    223At 50 s %β-=100, %α=0.008 sys

    Radon

    Isotope Half-life Spin Parity Mode(s) or Abundance
    196Rn 3 ms 0+ %α ~ 100
    197Rn 65 ms (3/2- ) %α ~ 100
    197m1Rn 19 ms (13/2+ ) %α ~ 100
    198Rn 64 ms 0+ %α=100
    199Rn 0.62 s (3/2- ) %α=94 sys, %K+%β+=6 sys
    199m1Rn 0.32 s (13/2+ ) %α=97 sys, %K+%β+=3 sys
    200Rn 0.96 s 0+ %α=86 +14-4, %K+%β+<18
    201Rn 7.0 s (3/2- ) %α ~ 80 , %K+%β+ ~ 20
    201m1Rn 3.8 s (13/2+ ) %α ~ 90, %K+%β+ ~ 10, %IT ~ 0
    202Rn 10.0 s 0+ %α=86 , %K+%β+=14
    203Rn 45 s (3/2,5/2)- %α=66 , %K+%β+=34
    203m1Rn 28 s (13/2+ ) %α ~ 80 sys%K+%β+ ~ 20 sys
    204Rn 1.24 m 0+ %α=73 , %K+%β+=27
    205Rn 2.8 m 5/2- %K+%β+=77 , %α=23
    206Rn 5.67 m 0+ %α=63 , %K+%β+=37
    207Rn 9.25 m 5/2- %K+%β+=79 , %α=21
    208Rn 24.35 m 0+ %α=62 , %K+%β+=38
    209Rn 28.5 m 5/2- %K+%β+=83 , %α=17
    210Rn 2.4 h 0+ %α=96 , %K+%β+=4
    211Rn 14.6 h 1/2- %K=72.6 , %α=27.4
    212Rn 23.9 m 0+ %α=100
    213Rn 25.0 ms (9/2+ ) %α=100
    214Rn 0.27 μs 0+ %α=100
    214m1Rn 0.69 ns 6+
    214m2Rn 6.5 ns 8+
    215Rn 2.30 μs 9/2+ %α=100
    216Rn 45 μs 0+ %α=100
    217Rn 0.54 ms 9/2+ %α=100
    218Rn 35 ms 0+ %α=100
    219Rn 3.96 s 5/2+ %α=100
    220Rn 55.6 s 0+ %α=100
    221Rn 25 m 7/2(+) %β-=78 , %α=22
    222Rn 3.8235 d 0+ %α=100
    223Rn 23.2 m 7/2 %β-=100, %α=0.0004 sys
    224Rn 107 m 0+ %β-=100
    225Rn 4.5 m 7/2- %β-=100
    226Rn 7.4 m 0+ %β-=100
    227Rn 22.5 s %β-=100
    228Rn 65 s 0+ %β-=100

    Francium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    200Fr 19 ms (3+ ) %α=100
    200m1Fr 0.57 s (10- ) %α=100
    201Fr 48 ms (9/2- ) %α=100 , %K+%β+ < 1
    202Fr 0.34 s (3+ ) %α ~ 97 , %K+%β+ ~ 3
    202m1Fr 0.34 s (10- ) %α ~ 97 , %K+%β+ ~ 3
    203Fr 0.55 s (9/2- ) %α ~ 95 , %K+%β+ ~ 5
    204Fr 1.7 s (3+ ) %α ~ 80, %K+%β+ ~ 20
    204m1Fr 2.6 s (7+) %α=?
    204m2Fr 1 s (10- ) %α=?
    205Fr 3.85 s (9/2- ) %α > 99, %K+%β+ < 1
    206Fr 15.9 s (5+) %α=84 , %K+%β+=16
    206m1Fr 0.7 s (10- ) %α=0.3 , %IT=?
    207Fr 14.8 s 9/2- %α=95 , %K+%β+=5
    208Fr 59.1 s 7+ %α=90 , %K+%β+=10
    209Fr 50.0 s 9/2- %α=89 , %K+%β+=11
    210Fr 3.18 m 6+ %α=60 , %K+%β+=40
    211Fr 3.10 m 9/2- %α>80, %K<20
    212Fr 20.0 m 5+ %K+%β+=57 , %α=43
    213Fr 34.6 s 9/2- %α=99.45 , %K+%β+=0.55
    214Fr 5.0 ms (1- ) %α=100
    214m1Fr 3.35 ms (8-) %α=100
    215Fr 86 ns 9/2- %α=100
    215m1Fr 3.5 ns (23/2)-
    216Fr 0.70 μs (1- ) %α=100, %K<2E-7 sys
    217Fr 22 μs 9/2- %α=100
    218Fr 1.0 ms 1- %α=100
    218m1Fr 22.0 ms %α < 100 , %IT=?
    219Fr 20 ms 9/2- %α=100
    220Fr 27.4 s 1+ %α=99.65 , %β-=0.35
    221Fr 4.9 m 5/2- %α=100, %γ=8.8E-11
    222Fr 14.2 m 2- %β-=100
    223Fr 21.8 m 3/2(-) %β-=99.994, %α=0.006
    224Fr 3.33 m 1- %β-=100
    225Fr 4.0 m 3/2- %β-=100
    226Fr 49 s 1- %β-=100
    227Fr 2.47 m 1/2+ %β-=100
    228Fr 38 s 2- %β-=100
    229Fr 50 s %β-=100
    230Fr 19.1 s %β-=100
    231Fr 17.5 s %β-=100
    232Fr 5 s %β-=100

    Radium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    202Ra 0.7 ms 0+ %α=100
    203Ra 1.0 ms (3/2- ) %α ~ 100
    203m1Ra 33 ms (13/2+ ) %α ~ 100
    204Ra 59 ms 0+ %α ~ 100
    205Ra 210 ms (3/2- ) %α=?
    205m1Ra 170 ms (13/2+ ) %α=?
    206Ra 0.24 s 0+ %α ~ 100
    207Ra 1.3 s (5/2,3/2)- %α ~ 90, %K+%β+ ~ 10
    207m1Ra 55 ms (13/2+ ) %IT=85 sys%α=15 sys %K+%β+ ~ 0.55
    208Ra 1.3 s 0+ %α=95 sys %K+%β+=5 sys
    209Ra 4.6 s 5/2- %α ~ 90, %K+%β+ ~ 10
    210Ra 3.7 s 0+ %α ~ 96, %K+%β+ ~ 4
    211Ra 13 s 5/2(-) %α > 93, %K < 7
    212Ra 13.0 s 0+ %α ~ 85, %K+%β+ ~ 15
    213Ra 2.74 m 1/2- %α=80 , %K+%β+=20
    213m1Ra 2.1 ms %IT ~ 99, %α ~ 1
    214Ra 2.46 s 0+ %α=99.941 , %K=0.059
    215Ra 1.59 ms (9/2+ ) %α=100
    216Ra 182 ns 0+ %α=100, %K<1E-8
    217Ra 1.6 μs (9/2+ ) %α=100
    218Ra 25.6 μs 0+ %α=100
    219Ra 10 ms (7/2)+ %α=100
    220Ra 18 ms 0+ %α=100
    221Ra 28 s 5/2+ %α=100, %γ=1.2E-10
    222Ra 38.0 s 0+ %α=100, %14C=3.0E-8
    223Ra 11.435 d 3/2+ %α=100, %14C=6.4E-8
    224Ra 3.66 d 0+ %α=100, %14C=4.3E-9
    225Ra 14.9 d 1/2+ %β-=100
    226Ra 1600 a 0+ %α=100, %14C=3.2E-9
    227Ra 42.2 m 3/2+ %β-=100
    228Ra 5.75 a 0+ %β-=100
    229Ra 4.0 m 5/2(+) %β-=100
    230Ra 93 m 0+ %β-=100
    231Ra 103 s (7/2-,1/2+ ) %β-=100
    232Ra 250 s 0+ %β-=100
    233Ra 30 s %β-=100
    234Ra 30 s 0+ %β-=100

    Actinium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    206Ac 22 ms (3+ ) %α=?
    206m1Ac 33 ms (10- )
    207Ac 22 ms (9/2- ) %α ~ 100
    208Ac 95 ms (3+ ) %α=?
    208m1Ac 25 ms (10- ) %α=?
    209Ac 0.10 s (9/2- ) %α ~ 99, %K+%β+ ~ 1
    210Ac 0.35 s %α ~ 96, %K+%β+ ~ 4
    211Ac 0.25 s %α ~ 100
    212Ac 0.93 s %α ~ 97, %K+%β+ ~ 3
    213Ac 0.80 s %α < 100
    214Ac 8.2 s %α > 89 , %K < 11
    215Ac 0.17 s 9/2- %α=99.91 , %K+%β+=0.09
    216Ac 0.33 ms (1- ) %α=100
    216m1Ac 0.33 ms (9-)
    217Ac 69 ns 9/2- %α=100, %K+%β+ < 2
    217m1Ac 740 ns (29/2)+
    218Ac 1.08 μs (1- ) %α=100
    219Ac 11.8 μs 9/2- %α=100, %K+%β+ ~ 1E-6
    220Ac 26.4 ms (3-) %α=100
    221Ac 52 ms (3/2- ) %α=100
    222Ac 5.0 s 1- %α=99 , %K+%β+=1
    222m1Ac 63 s %α > 88, %IT < 10 , %K+%β+ < 2
    223Ac 2.10 m (5/2- ) %α=99, %K=1
    224Ac 2.78 h 0- %K=90.9 +14-20, %α=9.1 +20-14, %β- < 1.6 sys
    225Ac 10.0 d (3/2- ) %α=100, %14C=6.0E-10
    226Ac 29.37 h (1) %α=6E-3 , %β-=83 , %K=17
    227Ac 21.773 a 3/2- %β-=98.620 , %α=1.380
    228Ac 6.15 h 3+ %β-=100
    229Ac 62.7 m (3/2+ ) %β-=100
    230Ac 122 s (1+ ) %β-=100
    231Ac 7.5 m (1/2+ ) %β-=100
    232Ac 119 s (1+ ) %β-=100
    233Ac 145 s (1/2+ ) %β-=100
    234Ac 44 s %β-=100

    Thorium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    210Th 9 ms 0+ %α ~ 100
    211Th 37 ms %α=?, %K=?
    212Th 30 ms 0+ %α=100, %K+%β+ ~ 0.3
    213Th 140 ms %α < 100
    214Th 100 ms 0+ %α=100
    215Th 1.2 s (1/2- ) %α=100
    216Th 0.028 s 0+ %α=100, %K+%β+ ~ 0.01 sys
    216m1Th 180 μs (8+,11- )
    217Th 0.252 ms (9/2+ ) %α=100
    218Th 109 ns 0+ %α=100
    219Th 1.05 μs %α=100, %K+%β+ ~ 1E-7
    220Th 9.7 μs 0+ %α=100, %K=2E-7 sys
    221Th 1.68 ms (7/2+ ) %α=100
    222Th 2.8 ms 0+ %α=100
    223Th 0.60 s (5/2)+ %α=100
    224Th 1.05 s 0+ %α=100
    225Th 8.72 m (3/2)+ %α ~ 90, %K ~ 10
    226Th 30.57 m 0+ %α=100
    227Th 18.72 d (1/2+ ) %α=100
    228Th 1.9116 a 0+ %α=100, %20O=1.13E-11
    229Th 7340 a 5/2+ %α=100
    230Th 7.538e+4 a 0+ %α=100, %24NE=5.6E-11 , %SF < 3.8E-12
    231Th 25.52 h 5/2+ %β-=100, %α ~ 1E-8
    232Th 1.405e10 a 0+ %Abundance=100, %α=100 , %SF<1.8E-9
    233Th 22.3 m 1/2+ %β-=100
    234Th 24.10 d 0+ %β-=100
    235Th 7.1 m (1/2+ ) %β-=100
    236Th 37.5 m 0+ %β-=100
    237Th 5.0 m %β-=100

    Protactinium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    <212Pa 5.1 ms (3+ ) %α=?
    213Pa 5.3 ms %α=?
    214Pa 17 ms %α=?
    215Pa 14 ms %α=100
    216Pa 0.20 s %K ~ 2 sys %α ~ 98 sys
    217Pa 4.9 ms %α =100
    217m1Pa 1.6 ms %α < 100
    218Pa 0.12 ms %α=100
    219Pa 53 ns 9/2- %α=100, %K+%β+ ~ 5E-9
    220Pa 0.78 μs %α=100, %K+%β+=3E-7 sys
    221Pa 5.9 μs 9/2- %α=100
    222Pa 2.9 ms %α=100
    223Pa 6.5 ms %α=100, %K+%β+ < 1.0E-3
    224Pa 0.79 s %α=100
    225Pa 1.7 s %α=100
    226Pa 1.8 m %α=74 , %K+%β+=26
    227Pa 38.3 m (5/2- ) %α=85 , %K=15
    228Pa 22 h 3+ %K+%β+=98.0 , %α=2.0
    229Pa 1.50 d (5/2+ ) %K=99.52 , %α=0.48
    230Pa 17.4 d (2- ) %K+%β+=91.6 , %β-=8.4 , %α=0.0032
    231Pa 32760 a 3/2- %α=100, %SF < 1.6E-11
    232Pa 1.31 d (2- ) %β-=99.997 , %K=0.003
    233Pa 26.967 d 3/2- %β-=100
    234Pa 6.70 h 4+ %β-=100, %SF < 3E-10
    234m1Pa 1.17 m (0- ) %β-=99.84 , %IT=0.16 , %SF < 1E-9
    235Pa 24.5 m (3/2- ) %β-=100
    236Pa 9.1 m 1(-) %β-=100
    237Pa 8.7 m (1/2+ ) %β-=100
    238Pa 2.3 m (3-) %β-=100, %SF < 2.6E-6

    Uranium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    218U 1.5 ms 0+ %α=100
    219U 42 μs %α=?
    220U
    221U
    222U 1.0 μs 0+ %α=100
    223U 18 μs %α=?
    224U 0.9 ms 0+ %α=100
    225U 95 ms %α=100
    226U 0.35 s 0+ %α=100
    227U 1.1 m (3/2+ ) %α=100, %K+%β+ < 0.001
    228U 9.1 m 0+ %K<5, %α>95
    229U 58 m (3/2+ ) %K+%β+ ~ 80, %α ~ 20
    230U 20.8 d 0+ %α=100, %SF < 1.4E-10
    231U 4.2 d (5/2- ) %K=100, %α ~ 0.0055
    232U 68.9 a 0+ %α=100, %24NE=9E-11
    233U 1.592e+5 a 5/2+ %α=100, %SF < 6E-11, %24NE < 9.5E-11
    234U 2.455e+5 a 0+ %Abundance=0.0055, %α=100, %SF=1.64E-9 , %nE=9E-12 , %MG=1.4E-11
    235U 7.038e+8 a 7/2- %Abundance=0.7200, %α=100, %SF=7.0E-9 , %20NE=8E-10
    235m1U 25 m 1/2+ %IT=100
    236U 2.342e7 a 0+ %α=100, %SF=9.4E-8
    237U 6.75 d 1/2+ %β-=100
    238U 4.468e+9 a 0+ %Abundance=99.2745, %α=100, %SF=5.45E-5 , %ββ=2.2E-10
    238m1U 225 ns 0+
    238m2U 1 ns
    239U 23.45 m 5/2+ %β-=100
    240U 14.1 h 0+ %β-=100
    241U
    242U 16.8 m 0+ %β-=100

    Neptunium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    225Np 6 ms %α=?
    226Np 35 ms %α=100
    227Np 0.51 s %α=100, %K+%β+ ~ 0.05
    228Np 61.4 s %K=60 , %α=40 , %KSF=0.020
    229Np 4.0 m %α > 50, %K < 50
    230Np 4.6 m %K+%β+ < 97, %α > 3
    231Np 48.8 m (5/2) %K=98 , %α=2
    232Np 14.7 m (4+ ) %K+%β+=100
    233Np 36.2 m (5/2+ ) %K=100, %α < 0.001
    234Np 4.4 d (0+ ) %K+%β+=100
    235Np 396.1 d 5/2+ %K=99.99740 , %α=0.00260
    236Np 1.54e5 a (6-) %K=87.3 , %β-=12.5 , %α=0.16
    236m1Np 22.5 h 1 %K=52 , %β-=48
    237Np 2.144e+6 a 5/2+ %α=100, %SF < 2E-10
    237m1Np 45 ns
    238Np 2.117 d 2+ %β-=100
    238m1Np 112 ns
    239Np 2.3565 d 5/2+ %β-=100
    240Np 61.9 m (5+) %β-=100
    240m1Np 7.22 m 1(+) %β-=99.89 , %IT=0.11
    241Np 13.9 m (5/2+ ) %β-=100
    242Np 5.5 m (6) %β-=100
    242m1Np 2.2 m (1+ ) %β-=100
    243Np 1.8 m (5/2- ) %β-=100
    244Np 2.29 m (7-) %β-=100

    Plutonium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    228Pu 4 ms 0+ %α=100
    229Pu %α=?
    230Pu 0+ %α=?
    231Pu
    232Pu 34.1 m 0+ %K=77 , %α=23
    233Pu 20.9 m %K+%β+=99.88 , %α=0.12
    234Pu 8.8 h 0+ %K ~ 94, %α ~ 6
    234m1Pu 3 ns
    235Pu 25.3 m (5/2+ ) %K+%β+=99.9973 , %α=0.0027
    235m1Pu 25 ns
    236Pu 2.858 a 0+ %α=100, %SF=1.37E-7
    236m1Pu 37 ps (0+ )
    236m2Pu 34 ns
    237Pu 45.2 d 7/2- %α=0.0042 , %K=99.9958
    237m1Pu 0.18 s 1/2+ %IT=100
    237m2Pu 85 ns
    237m3Pu 1.1 μs
    238Pu 87.7 a 0+ %α=100, %SF=1.85E-7 , %MG ~ 6E-15, %SI ~ 1.4E-14
    238m1Pu 0.6 ns
    238m2Pu 6.0 ns (0+ )
    239Pu 24110 a 1/2+ %α=100, %SF=3.0E-10
    239m1Pu 7.5 μs (5/2+ )
    239m2Pu 2.6 ns (9/2- )
    240Pu 6563 a 0+ %α=100 , %SF=5.75E-6
    241Pu 14.35 a 5/2+ %β-=99.998, %α=0.00245 , %SF ~ 2.4E-14
    241m1Pu 21 μs
    241m2Pu 32 ns
    242Pu 3.733e+5 a 0+ %α=100 , %SF=5.54E-4
    243Pu 4.956 h 7/2+ %β-=100
    243m1Pu 45 ns
    244Pu 8.08e+7 a 0+ %α=99.879 , %SF=0.121 , %ββ < 3E-11
    245Pu 10.5 h (9/2- ) %β-=100
    245m1Pu 90 ns
    246Pu 10.84 d 0+ %β-=100
    247Pu 2.27 d %β-=100

    Americium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    232Am 79 s %K ~ 98, %α ~ 2, %KSF=0.069
    233Am
    234Am 2.32 m %K=99.961 , %α=0.039 , %KSF=0.0066
    235Am 15 m %K+%β+=?, %α=?
    236Am %K=?, %α=?
    237Am 73.0 m 5/2(-) %α=0.025 , %K=99.975
    237m1Am 5 ns
    238Am 98 m 1+ %K+%β+>99.99, %α=1.0E-4
    238m1Am 35 μs
    239Am 11.9 h (5/2)- %K=99.990 , %α=0.010
    239m1Am 163 ns (7/2+ )
    240Am 50.8 h (3-) %K=100, %α=1.9E-4
    241Am 432.2 a 5/2- %α=100, %SF=4.3E-10
    241m1Am 1.2 μs
    242Am 16.02 h 1- %β-=82.7 , %K=17.3
    242m1Am 141 a 5- %IT=99.541 , %α=0.459 , %SF < 4.7E-9
    242m2Am 14.0 ms %SF=?, %IT=?
    243Am 7370 a 5/2- %α=100, %SF=3.7E-9
    243m1Am 5.5 μs
    244Am 10.1 h (6-) %β-=100
    244m1Am 26 m 1+ %β-=99.9639 , %K=0.0361
    245Am 2.05 h (5/2)+ %β-=100
    245m1Am 0.64 μs
    246Am 39 m (7-) %β-=100
    246m1Am 25.0 m 2(-) %β-=100, %IT<0.01
    246m2Am 73 μs
    247Am 23.0 m (5/2) %β-=100

    Curium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    238Cm 2.4 h 0+ %K=96.16 , %α=3.84
    239Cm 2.9 h (7/2- ) %K= 100, %α < 0.1
    240Cm 27 d 0+ %α > 99.5 , %K < 0.5 , %SF=3.9E-6
    241Cm 32.8 d 1/2+ %K=99.0 , %α=1.0
    241m1Cm 15.3 ns
    242Cm 162.8 d 0+ %α=100, %SF=6.37E-6
    242m1Cm 40 ps
    242m2Cm 0.18 μs
    243Cm 29.1 a 5/2+ %α=99.71 , %K=0.29 , %SF=5.3E-9
    243m1Cm 42 ns
    244Cm 18.10 a 0+ %α=100, %SF=1.371E-4
    244m1Cm 34 ms 6+ %IT=100, %SF < 7.7E-10
    245Cm 8500 a 7/2+ %α=100, %SF=6.1E-7
    245m1Cm 13.2 ns
    246Cm 4730 a 0+ %α=99.9737 , %SF=0.0263
    247Cm 1.56e+7 a 9/2- %α=100
    248Cm 3.40e+5 a 0+ %α=91.61 , %SF=8.39
    249Cm 64.15 m 1/2(+) %β-=100
    250Cm 9000 a 0+ %SF ~ 86, %α ~ 8, %β- ~ 6
    251Cm 16.8 m (1/2+ ) %β-=100
    252Cm 2 d 0+ %β-=100

    Berkelium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    238Bk 144 s %K+%β+=100, %KSF=0.048
    239Bk (7/2+ )
    240Bk 4.8 m %K+%β+=100, %KSF=1E-3 sys
    241Bk (7/2+ )
    242Bk 7.0 m %K+%β+=100
    242m1Bk 9.5 ns
    242m2Bk 0.60 μs
    243Bk 4.5 h (3/2- ) %K ~ 99.85, %α ~ 0.15
    243m1Bk 5 ns
    244Bk 4.35 h (1- ) %K=99.994 , %α=0.006
    245Bk 4.94 d 3/2- %K=99.88 , %α=0.12
    245m1Bk 2 ns
    246Bk 1.80 d 2(-) %K=100, %α<0.2 sys
    247Bk 1380 a (3/2- ) %α < 100
    248Bk 9 a (6+) %α>70
    248m1Bk 23.7 h 1(-) %β-=70 , %K=30 , %α<0.001
    249Bk 320 d 7/2+ %β-=99.99855 , %α=0.00145 , %SF=4.76E-8
    250Bk 3.217 h 2- %β-=100
    251Bk 55.6 m (3/2- ) %β-=100, %α ~ 1E-5

    Californium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    237Cf 2.1 s %SF ~ 10 sys
    238Cf 21 ms 0+ %SF ~ 100 sys
    239Cf 39 s %α=?
    240Cf 1.06 m 0+ %α=87 , %SF ~ 13
    241Cf 3.78 m %K ~ 75, %α ~ 25
    242Cf 3.49 m 0+ %α=65 , %SF < 1.4E-2
    243Cf 10.7 m (1/2+ ) %K ~ 86, %α ~ 14
    244Cf 19.4 m 0+ %α=70
    245Cf 45.0 m (5/2+ ) %K=64 , %α=36
    246Cf 35.7 h 0+ %α=99.9996 , %SF=2.3E-4 , %K<5E-4
    246m1Cf 45 ns
    247Cf 3.11 h (7/2+ ) %K=99.965 , %α=0.035
    248Cf 333.5 d 0+ %α=99.9971 , %SF=0.0029
    249Cf 351 a 9/2- %α=100, %SF=4.4E-7
    250Cf 13.08 a 0+ %α=99.923 , %SF=0.077
    251Cf 898 a 1/2+ %α=100
    252Cf 2.645 a 0+ %α=96.908 , %SF=3.092
    253Cf 17.81 d (7/2+ ) %β-=99.69 , %α=0.31
    254Cf 60.5 d 0+ %SF=99.69 , %α=0.31
    255Cf 85 m (9/2+ ) %β-=100
    256Cf 12.3 m 0+ %SF=100, %β-<1 sys %α ~ 1E-6 sys

    Einsteinium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    241Es 9 s %α=100
    242Es 40 s %α ~ 100, %KSF=1.4
    243Es 21 s %K < 70, %α > 30
    244Es 37 s %K=96 , %α=4 , %KSF=0.01 sys
    245Es 1.1 m (3/2- ) %K=60 , %α=40
    246Es 7.7 m (4-,6+) %K=90.1 , %α=9.9 , %KSF=0.003 sys
    247Es 4.55 m (7/2+ ) %K ~ 93, %α ~ 7
    248Es 27 m (2-,0+ ) %K>99, %α ~ 0.25, %KSF=3E-5 sys
    249Es 102.2 m 7/2(+) %K=99.43 , %α=0.57
    250Es 8.6 h (6+) %K > 97, %α < 3 sys
    250m1Es 2.22 h 1(-) %K > 99, %α < 1 sys
    251Es 33 h (3/2- ) %K=99.51 , %α=0.49
    252Es 471.7 d (5-) %α=76 , %K=24 , %β- ~ 0.01
    253Es 20.47 d 7/2+ %α=100, %SF=8.9E-6
    254Es 275.7 d (7+) %α=100, %K<1E-4, %β-=1.74E-6 , %SF<3E-6
    254m1Es 39.3 h 2+ %β-=98 , %α=0.33 , %IT<3, %K=0.078 , %SF<0.045
    255Es 39.8 d (7/2+ ) %β-=92.0 , %α=8.0 , %SF=0.0045
    256Es 25.4 m (1+ ) %β-=100
    256m1Es 7.6 h (8+) %β- ~ 100, %β-SF=0.002

    Fermium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    242Fm 0.8 ms 0+ %SF=100
    243Fm 0.18 s %α < 100, %SF < 0.5, %K=?
    244Fm 3.3 ms 0+ %SF=100
    245Fm 4.2 s %α=100, %SF < 0.11
    246Fm 1.1 s 0+ %α=92 , %SF=7.3 , %K<1 sys
    247Fm 35 s %α > 50, %K+%β+ < 50
    247m1Fm 9.2 s %α < 100
    248Fm 36 s 0+ %α=93 , %K ~ 7, %SF=0.10
    249Fm 2.6 m (7/2+ ) %K ~ 85 sys %α ~ 15 sys
    250Fm 30 m 0+ %α>90, %K<10, %SF=0.0069
    250m1Fm 1.8 s %IT>80, %SF < 8E-5
    251Fm 5.30 h (9/2- ) %K=98.20 , %α=1.80
    252Fm 25.39 h 0+ %α=99.9977 , %SF=0.00232
    253Fm 3.00 d 1/2+ %K=88 , %α=12
    254Fm 3.240 h 0+ %α=99.9408 , %SF=0.0592
    255Fm 20.07 h 7/2+ %α=100, %SF=2.3E-5
    256Fm 157.6 m 0+ %SF=91.9 , %α=8.1
    257Fm 100.5 d (9/2+ ) %α=99.790 , %SF=0.210
    258Fm 370 μs 0+ %SF=100
    259Fm 1.5 s %SF=100

    Mendelevium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    245Md 0.35 s (7/2) %α=100
    245m1Md 0.90 ms (1/2- )
    246Md 1.0 s %α=100
    247Md 1.12 s %α=80 , %SF=20
    248Md 7 s %K=80 , %α=20 , %SF < 0.05
    249Md 24 s %K=80 , %α=20
    250Md 52 s %K=93 , %α=7 , %KSF=0.02 sys
    251Md 4.0 m %K > 90, %α < 10
    252Md 2.3 m %K>50, %α<50
    253Md 6 m %K+%β+=100
    254Md 10 m %K < 100
    254m1Md 28 m %K < 100
    255Md 27 m (7/2- ) %K=92 , %α=8 , %SF < 1.4
    256Md 78.1 m (0-,1- ) %K=90.7 , %α=9.3 , %SF < 2.8
    257Md 5.52 h (7/2- ) %K=85 , %α=15 , %SF<1
    258Md 51.5 d (8-) %α=100, %SF < 0.003, %β- < 0.003, %K < 0.003
    258m1Md 57.0 m (1- ) %K > 70, %SF < 30, %α < 1.2, %β- < 30
    259Md 96 m (7/2- ) %SF ~ 100, %α<1.3
    260Md 31.8 d %SF>73, %α < 25, %β- < 10

    Nobelium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    250No 0.25 ms 0+ %SF=100, %α ~ 0.05 sys
    251No 0.8 s %α ~ 100, %K ~ 1 sys%SF < 8
    252No 2.30 s 0+ %α=73.1 , %SF=26.9
    253No 1.7 m (9/2- ) %α ~ 80, %K ~ 20 sys
    254No 55 s 0+ %α=90 , %K=10 , %SF=0.17
    254m1No 0.28 s %IT>80
    255No 3.1 m (1/2+ ) %α=61.4 , %K=38.6
    256No 2.91 s 0+ %α=99.5 , %SF=0.53 +8-4
    257No 25 s (7/2+ ) %α ~ 100
    258No 1.2 ms 0+ %SF=100, %α ~ 1E-3 sys
    259No 58 m (9/2+ ) %α=75 , %K=25 , %SF<10
    260No 106 ms 0+ %SF=100
    261No
    262No 5 ms 0+ %SF=?

    Lawrencium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    253Lr 1.3 s %α=98 , %K ~ 1 sys%SF < 1
    254Lr 13 s %α=78 , %K=22 , %SF < 0.16
    255Lr 22 s %α=85 , %K<30, %SF<0.10
    256Lr 28 s %α>80, %K<20, %SF<0.026
    257Lr 0.646 s (9/2+ ) %α=100, %SF < 6.5E-4
    258Lr 3.9 s %α>95, %K<5, %SF < 5.0
    259Lr 6.3 s %α=77 , %SF=23 , %K<0.5
    260Lr 180 s %α=75 , %K=25
    261Lr 39 m %SF < 100
    262Lr 216 m %SF<10


    Rutherfordium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    253Rf 1.8 s %SF ~ 50, %α ~ 50
    253m1Rf 50 μs
    254Rf 0.5 ms 0+ %SF=100, %α ~ 0.3 sys
    254m1Rf 23 μs
    255Rf 1.5 s (9/2- ) %SF=52 , %α=48
    256Rf 6.7 ms 0+ %SF=98 +2- 7 , %α=2.2 +73-18
    257Rf 4.7 s (7/2+ ) %α=79.6 , %K=18 , %SF=2.4
    258Rf 12 ms 0+ %SF ~ 87, %α ~ 13
    259Rf 3.1 s %α=93 , %SF=7 , %K ~ 0.3
    260Rf 20.1 ms 0+ %SF=100
    261Rf 65 s %α>80, %SF<10, %K < 10 sys
    262Rf 2.1 s 0+ %SF=100
    262m1Rf 47 ms [2+ ]

    Dubnium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    255Db 1.6 s %α>47, %SF < 53
    256Db 2.6 s %SF < 40, %α ~ 70, %K ~ 10 sys
    257Db 1.3 s %α=82 , %SF=17 , %K=1 sys
    258Db 4.4 s %α=67 +5-9 , %K=33 +9-5, %SF<34
    258m1Db 20 s %K ~ 100
    259Db
    260Db 1.52 s %α > 90.4 , %SF ~ 9.6 , %K<2.5
    261Db 1.8 s %α>50, %SF<50
    262Db 34 s %α ~ 64, %SF ~ 33, %K ~ 3 sys
    263Db 27 s %SF=57 , %α=43

    Seaborgium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    258Sg 2.9 ms 0+ %SF=100
    259Sg 0.48 s (1/2+ ) %α=90 , %SF < 20
    260Sg 3.6 ms 0+ %α=50 +30-20 , %SF=50 +20-30
    261Sg 0.23 s %α=95 , %SF<10
    262Sg 0+
    263Sg 0.8 s %SF ~ 70, %α ~ 30
    263m1Sg 0.31 s [9/2+]
    264Sg 0+
    265Sg 10 s [1/2+ ] %α>50, %SF<50
    266Sg 21 s 0+ %α=50 , %SF=50

    Bohrium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    261Bh 11.8 ms %α=95 , %SF<10
    262Bh 102 ms %α > 80, %SF < 20
    262m1Bh 8.0 ms %α > 70, %SF < 30
    263Bh
    264Bh 0.44 s %α=100

    Hassium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    264Hs 0.85 ms 0+ %α ~ 100, %SF < 1.5
    265Hs 0.9 ms %α=?
    265m1Hs 1.55 ms [1/2+ ] %α ~ 100, %SF<9
    266Hs 0+
    267Hs 26 ms [9/2+ ] %α=100
    268Hs 0+
    269Hs 9 s [3/2+ ] %α=100

    Meitnerium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    266Mt 0.8 ms %α=100
    266m1Mt 3.8 ms %α=100, %SF < 5.5
    267Mt
    268Mt 0.07 s [5+,6+] %α=100

    Darmstadtium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    267Ds 3 μs [11/2- ] %α=100
    268Ds 0+
    269Ds 0.17 ms [1/2+ ] %α=100
    270Ds 0+
    271Ds 0.06 s [3/2+ ] %α=100
    271m1Ds 1.1 ms [9/2+ ] %α=100
    272Ds 0+
    273Ds 0.18 ms [3/2+ ] %α=100
    273m1Ds 120 ms [13/2- ] %α=100

    Roentgenium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    272Rg 1.5 ms [5+,6+] %α=100


    Copernicium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    277Cn 0.24 ms [3/2+ ]

    Flerovium

    Isotope Half-life Spin Parity Mode(s) or Abundance
    285Fl 0.58 ms %α=?