Exclusive dielectron production in ultraperipheral Pb plus Pb collisions at ?sNN=5.02 TeV with ATLAS
dc.contributor.author | Aad G. | |
dc.contributor.author | Abbott B. | |
dc.contributor.author | Abbott D. C. | |
dc.contributor.author | Abeling K. | |
dc.contributor.author | Abidi S. H. | |
dc.contributor.author | Aboulhorma A. | |
dc.contributor.author | Abramowicz H. | |
dc.contributor.author | Abreu H. | |
dc.contributor.author | Abulaiti Y. | |
dc.contributor.author | Abusleme Hoffman A. C. | |
dc.contributor.author | Acharya B. S. | |
dc.contributor.author | Achkar B. | |
dc.contributor.author | Adam L. | |
dc.contributor.author | Adam Bourdarios C. | |
dc.contributor.author | Adamczyk L. | |
dc.contributor.author | Adamek L. | |
dc.contributor.author | Addepalli S. V. | |
dc.contributor.author | Adelman J. | |
dc.contributor.author | Adiguzel A. | |
dc.contributor.author | Adorni S. | |
dc.contributor.author | Adye T. | |
dc.contributor.author | Affolder A. A. | |
dc.contributor.author | Afik Y. | |
dc.contributor.author | Agaras M. N. | |
dc.contributor.author | Agarwala J. | |
dc.contributor.author | Aggarwal A. | |
dc.contributor.author | Agheorghiesei C. | |
dc.contributor.author | Aguilar-Saavedra J. A. | |
dc.contributor.author | Ahmad A. | |
dc.contributor.author | Ahmadov F. | |
dc.contributor.author | Ahmed W. S. | |
dc.contributor.author | Ai X. | |
dc.contributor.author | Aielli G. | |
dc.contributor.author | Aizenberg I. | |
dc.contributor.author | Akbiyik M. | |
dc.contributor.author | Akesson T. P. A. | |
dc.contributor.author | Akimov A. V. | |
dc.contributor.author | Al Khoury K. | |
dc.contributor.author | Alberghi G. L. | |
dc.contributor.author | Albert J. | |
dc.date.accessioned | 2025-05-19T16:37:53Z | |
dc.date.available | 2025-05-19T16:37:53Z | |
dc.date.issued | 2023/06/27 | |
dc.description.abstract | Exclusive production of dielectron pairs, gamma gamma -> e(+) e(-), is studied using L-int = 1.72 nb(-1) of data from ultraperipheral collisions of lead nuclei at root s(NN) = 5.02TeV recorded by the ATLAS detector at the LHC. The process of interest proceeds via photon-photon interactions in the strong electromagnetic fields of relativistic lead nuclei. Dielectron production is measured in the fiducial region defined by following requirements: electron transverse momentum p(T)(e) > 2.5 GeV, absolute electron pseudorapidity |eta(e)| < 2.5, dielectron invariant mass m(ee) > 5 GeV, and dielectron transverse momentum p(T)(ee) < 2 GeV. Differential cross-sections are measured as a function of mee, average peT, absolute dielectron rapidity |y(ee)|, and scattering angle in the dielectron rest frame, | cos theta* |, in the inclusive sample, and also with a requirement of no activity in the forward direction. The total integrated fiducial cross-section is measured to be 215 +/- 1(stat.) (+23)(-20)(syst.) +/- 4(lumi.) mu b. Within experimental uncertainties the measured integrated cross-section is in good agreement with the QED predictions from the Monte Carlo programs Starlight and SuperChic, confirming the broad features of the initial photon fluxes. The differential cross-sections show systematic differences from these predictions which are more pronounced at high |y(ee)| and | cos theta* | values. | |
dc.identifier.doi | http://dx.doi.org/10.1007/JHEP06(2023)182 | |
dc.identifier.issn | 1029-8479 | |
dc.identifier.uri | https://publicacionesabiertas.userena.cl/handle/123456789/295 | |
dc.language | English | |
dc.publisher | SPRINGER | |
dc.title | Exclusive dielectron production in ultraperipheral Pb plus Pb collisions at ?sNN=5.02 TeV with ATLAS | |
dc.type | Article |