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Probing the nucleus with linearly polarized photons

James Brandenburg · CERN

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The intense electromagnetic fields produced by ultra-relativistic heavy nuclei have been proposed as a source of quasi-real photons i.e. in the Weizsacker-Williams equivalent photon method. A photon from one nucleus can fluctuate into a quark antiquark pair and interact directly with the other nucleus to produce a vector meson (e.g. $\rho^0$). Recent STAR measurements of the Breit-Wheeler pair poduction process - $\gamma\gamma \rightarrow e^+e^-$ have demonstrated that the interacting photons are linearly polarized, and that photon polarization induces angular modulations in the final state particle distribution.

In this talk we present STAR measurements of diffractive photo-production of the $\rho^0$-meson (and direct $\pi^+\pi^-$ pairs) in ultra-peripheral Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. We measure azimuthal angular distributions of the final state $\pi^+\pi^-$ pairs and observe $\cos 2\Delta\phi$ and $\cos 4\Delta\phi$ modulations (where $\Delta\phi = \Delta\phi[ (\pi^++\pi^-), (\pi^+-\pi^-)]$. Theoretical predictions suggest that such modulations may provide new insight into nuclear structure and may shed light on the transverse momentum dependent (TMD) distributions of gluons within large nuclei - a topic of great interest both at existing experiments and at a future Electron Ion Collider.

[1] C. Weizsäcker, Zeitschrift für Physik 88 (1934): 612–25. [2] H. Xing, C. Zhang, J. Zhou, and Y.-J. Zhou, ArXiv:2006.06206 [Hep-Ph] (2020). [3] A. Metz, and J. Zhou. Physical Review D 84 5 (2011)..

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The talk

  1. Probing the nucleus with linearly polarized photons 2021-01-13 · 26 min · CERN's player

Credits and licence

Institution
CERN
Department
Conferences
Speaker
James Brandenburg
Year
2021
Language
English
Source
CERN
Licence
CERN, as CERN states it. CERN's terms
Attribution
© CERN. CERN provides its audiovisual media free of charge for educational and informational use, credited to CERN; this lecture is shown in CERN's own player.
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