19–23 Dec 2024
Swatantrata Bhavan, Banaras Hindu University, Varanasi
Asia/Kolkata timezone

Heavy quark energy loss in Proton-Lead Collisions at $\sqrt{s_{NN}}$ = 5.02 TeV

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20m
Swatantrata Bhavan, Banaras Hindu University, Varanasi

Swatantrata Bhavan, Banaras Hindu University, Varanasi

Department of Physics, I.Sc., Banaras Hindu University, 221005 Varanasi, India
Postar Heavy ion and QCD

Speaker

Dr Kapil Saraswat (Institute of Physics, Academia Sinica, Taipei, Taiwan)

Description

In the current work, We calculate the heavy quark (charm and bottom) energy loss due to elastic collisions and gluon radiation in proton-Lead (pPb) collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV. We use the Peigne and Peshier formalism to calculate the collisional energy loss and generalised dead cone approach and DGLV formalism to calculate the radiative energy loss. We also calculate the fluctuations.
Nuclear modification factors including shadowing, energy loss and fluctuations are calculated for $B$ and $D$ mesons in pPb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV and are compared with the measured CMS and ALICE data.

References :
(1) Kapil Saraswat et. al., Nucl. Phys. A 1022 (2022) 122441.
(2) CMS Collaboration, CMS-PAS-HIN-14-004.
(3) CMS Collaboration, Phys. Rev. Lett. 116 (2016) 032301.
(4) ALICE Collaboration, Phys. Rev. C 94 (2016) 054908.

Field of contribution Phenomenology

Authors

Dr Deependra Singh Rawat (School of Allied Sciences (Physics), Graphic Era Hill University, Bhimtal Campus, Sattal Road, Nainital, India.) Prof. Harish Chandra Chandola (Department of Physics (UGC-CAS), Kumaun University, Nainital-263001, India.) Dr Kapil Saraswat (Institute of Physics, Academia Sinica, Taipei, Taiwan) Dr Manoj Kumar Singh (Institute of Physics, Academia Sinica, Taipei, Taiwan) Prof. Prashanta Kumar Khandai (Department of Physics, Ewing Christain College, Prayagraj - 212003, India.) Prof. Venktesh Singh (Department of Phyics, School of Physical & Chemical Science, Central University of South Bihar, Gaya - 428236, India.)

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