Hard Probes 2018: International Conference on Hard & Electromagnetic Probes of High-Energy Nuclear Collisions

Session

PLENARY

1 Oct 2018, 08:45

Aix-Les-Bains, Savoie, France

Conveners

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• Andreas Morsch (CERN)

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• Giulia Manca (Universita` degli studi di Cagliari and INFN, Cagliari, IT)

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• Jean-Paul Blaizot (CEA)

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• Ramona Vogt (LLNL)

PLENARY: Jets & high-pT: Radiation and fragmentation

• Raju Venugopalan (Brookhaven National Laboratory)

PLENARY: Futures of Heavy-Ion Physics (Hard Probes)

• David d'Enterria (CERN)

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• Marco Van Leeuwen (Nikhef National institute for subatomic physics (NL))

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• Marta Verweij (Vanderbilt University (US))

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• Christina Markert (University of Texas at Austin (US))

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• Christina Markert (University of Texas at Austin (US))

90. Conference Welcome (CERN Research Director)

Eckhard Elsen (CERN)

01/10/2018, 08:45

91. ALICE

Torsten Dahms (Technische Universitaet Muenchen (DE))

01/10/2018, 09:05

92. ATLAS

Alexander Milov (Weizmann Institute of Science (IL))

01/10/2018, 09:30

589. CMS

Yen-Jie Lee (Massachusetts Inst. of Technology (US))

01/10/2018, 09:55

94. LHCb

Emilie Amandine Maurice (Centre National de la Recherche Scientifique (FR))

01/10/2018, 10:40

96. PHENIX

Takao Sakaguchi (BNL)

01/10/2018, 11:00

95. STAR

Sooraj Krishnan Radhakrishnan (State University of New York (US))

01/10/2018, 11:20

388. Photon and weak probes of QCD matter (theory)

Jacopo Ghiglieri (CERN)

01/10/2018, 11:40

97. Parton Saturation

Prof. Alfred Müller (Columbia University)

01/10/2018, 14:00

98. Nuclear Parton Distribution Functions

Hannu Paukkunen (University of Jyväskylä)

01/10/2018, 14:25

99. Early time dynamics and hard probes in heavy-ion collisions (theory)

Soeren Schlichting (University of Washington)

01/10/2018, 14:50

101. Jet substructure in high-energy hadron collisions

Felix Ringer (Lawrence Berkeley National Laboratory)

01/10/2018, 15:40

102. Jets in QCD matter: Monte Carlo approaches

Liliana Apolinario (LIP (PT))

01/10/2018, 16:05

103. Jet-medium interactions in QCD matter (theory)

Dr Tan Luo (CCNU)

01/10/2018, 16:30

100. Lattice and EFT approaches for hard probes in QCD matter

Miguel Angel Escobedo Espinosa (University of Jyväskylä)

01/10/2018, 16:55

104. Open heavy-flavour probes of QCD matter (theory)

Shanshan Cao (Wayne State University)

01/10/2018, 17:20

105. Quarkonia probes of QCD matter (theory)

Marzia Nardi (Unknown)

01/10/2018, 17:45

228. Vacuum-like jet fragmentation in a dense QCD medium

Mr Paul Caucal (IPhT)

04/10/2018, 14:00

2a) Jets and high-pT hadrons (TALK)

A main difficulty in understanding the dynamics of jets produced in the high-density environment of ultrarelativistic heavy ion collision, is to provide a unified description for the two sources of radiation that are a priori expected: the "vacuum-like" emissions responsible for the parton shower from large virtualities (of the order of the hard scale) down to the hadronisation scale and the...

277. Jet fragmentation and charged particle angular distribution within and around jets in Pb+Pb collisions with ATLAS

Akshat Puri (Univ. Illinois at Urbana Champaign (US))

04/10/2018, 14:20

2a) Jets and high-pT hadrons (TALK)

Abstract: In this talk, we present the latest measurements of the jet fragmentation and the angular distributions of charged particles within and around jets, as performed with the ATLAS detector in Pb+Pb collisions at the LHC. Jets are direct probes of the QCD medium created in these collisions, and studying jet fragmentation provides insight into the strength and mechanism of jet quenching....

295. Exploring the phase space of jet splittings at ALICE in pp and Pb-Pb collisions using jet shapes and grooming techniques

Nima Zardoshti (University of Birmingham (GB))

04/10/2018, 14:40

2a) Jets and high-pT hadrons (TALK)

Recent results in jet substructure measurements in pp and Pb--Pb collisions are presented at $\sqrt{s} = 7$ TeV and $\sqrt{s_{\rm NN}}= 2.76$ TeV respectively. The jet shapes discussed focus on the splitting process of jets either by quantifying the 2-prongness of the jet (τ2/τ1) or by parameterising the splitting process itself (zg and Rg). The Nsubjettiness of a jet could be sensitive to a...

340. Probing properties of the QCD Medium using jet substructure techniques in pp and PbPb collisions at 5.02 TeV at CMS

Dhanush Anil Hangal (University of Illinois at Chicago (US))

04/10/2018, 15:00

2a) Jets and high-pT hadrons (TALK)

We present recent results on measurements of inclusive jet substructures using grooming techniques and constituent correlations with pp and PbPb data collected with the CMS detector at a center-of-mass energy of 5.02 TeV per nucleon pair. Jet grooming techniques are used to focus on the hard structure of the jet by extracting the two subjets corresponding to the hardest parton splitting. The...

601. Intro: Futures of Heavy-Ion Physics (Hard Probes)

David d'Enterria (CERN)

04/10/2018, 15:50

136. Future heavy-ion facilities: sPHENIX experiment

Gunther Roland (Massachusetts Inst. of Technology (US))

04/10/2018, 15:55

137. Future heavy-ion facilities: Electron-Ion Collider (EIC)

Abhay Deshpande (Stony Brook University)

04/10/2018, 16:15

138. Future heavy-ion facilities: Fixed-target LHC (AFTER)

Jean-Philippe Lansberg (Centre National de la Recherche Scientifique (FR))

04/10/2018, 16:35

139. Future heavy-ion facilities: LHeC/FCC-eh

Max Klein (University of Liverpool (GB))

04/10/2018, 16:55

140. Future heavy-ion facilities: FCC-AA

Andrea Dainese (INFN - Padova (IT))

04/10/2018, 17:15

141. Round-table discussion: Future of hard probes & heavy-ion collisions

Abhay Deshpande (Stony Brook University), Andrea Dainese (INFN - Padova (IT)), Gunther Roland (Massachusetts Inst. of Technology (US)), Jean-Philippe Lansberg (Centre National de la Recherche Scientifique (FR)), Nestor Armesto Perez (Universidade de Santiago de Compostela (ES))

04/10/2018, 17:35

142. Direct-photon and heavy-flavour production in proton-proton collisions at $\sqrt{s}$ = 7 TeV with ALICE

Horst Sebastian Scheid (Johann-Wolfgang-Goethe Univ. (DE))

05/10/2018, 09:00

143. The problem of overlapping formation times

Shahin Iqbal (National Centre for Physics)

05/10/2018, 09:05

144. Heavy flavour dynamics in event-by-event viscous hydrodynamic backgrounds

Roland Katz (University of São Paulo)

05/10/2018, 09:10

145. Measurement of the azimuthal anisotropy of charged particles in 5.02 TeV Pb+Pb and 5.44 TeV Xe+Xe collisions with ATLAS

Klaudia Burka (Polish Academy of Sciences (PL))

05/10/2018, 09:15

146. Measurements of Bottomonium production in pp, pPb and PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV

Geonhee Oh (Chonnam National University (KR))

05/10/2018, 09:20

147. Initial-state in heavy-ion collisions at colliders: Theory summary

Vladimir Skokov (Brookhaven national laboratory)

05/10/2018, 09:25

591. Initial-state in heavy-ion collisions at colliders : Experimental summary

Émilien Chapon (CERN)

05/10/2018, 09:55

155. Ultraperipheral collisions: Summary

Janet Elizabeth Seger (Creighton University (US))

05/10/2018, 10:40

149. Jets in QCD matter: Experimental summary

Michael Linus Knichel (CERN)

05/10/2018, 11:05

150. Jets in QCD matter: Theory summary

Korinna Christine Zapp (LIP Laboratorio de Instrumentacao e Fisica Experimental de Part)

05/10/2018, 11:30

151. Open heavy flavour: Experimental summary

Deepa Thomas (University of Texas at Austin (US))

05/10/2018, 11:55

152. Quarkonia: Experimental summary

Hugo Denis Antonio Pereira Da Costa (Université Paris-Saclay (FR))

05/10/2018, 14:00

153. Open heavy flavour and quarkonia: Theoretical summary

Ralf Rapp (Texas A&M University)

05/10/2018, 14:25

154. Electroweak observables: Summary

Friederike Bock (CERN)

05/10/2018, 14:50

157. HP'20 Austin presentation

Christina Markert (University of Texas at Austin (US))

05/10/2018, 15:45

158. Talk (closing)

Andreas Morsch (CERN), David d'Enterria (CERN), Philippe Crochet (Univ. Blaise Pascal Clermont-Fe. II (FR))

05/10/2018, 16:00

148. Initial-state in heavy-ion collisions at colliders: Experimental summary

Émilien Chapon (CERN)