PPT-Longitudinal dynamics in heavy ion collisions

Author : yoshiko-marsland | Published Date : 2018-03-10

Jiangyong Jia BNL and Stony Brook University July 2023 2017 3D initial condition and final state dynamics 2 More dramatic at lower s due to stopping Collectivity

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Longitudinal dynamics in heavy ion collisions: Transcript


Jiangyong Jia BNL and Stony Brook University July 2023 2017 3D initial condition and final state dynamics 2 More dramatic at lower s due to stopping Collectivity is important bg in study of chirality criticality . interesting ?. Interaction of heavy quarks with the plasma. . - . our model (elastic and inelastic collisions, LPM). . - comparison with data. . - how far we are with our understanding. . Monoatomic i on Ion Name Ion Old Name New Name H + hydrogen ion /proton Cr 2+ chromous ion chromium (II) ion Li + lithium ion Cr 3+ chromic ion chromium (III) ion Na + sodium ion Mn 2+ manganous ion Will Witt. Introduction . –. Heavy Ion Physics. Heavy ion physics seeks to understand the behavior of strongly interacting matter (quarks and gluons) at extreme temperatures and densities.. Hadronic Matter. Inelastic vs. Elastic. Pg. 233 – 239. Pg. 240 - 248. Momentum vs. Energy. All interactions conserve momentum.. They do . not necessarily. conserve kinetic energy.. Obvious example: Explosions. Kinetic energy before is zero.. Statistics. “One out of every four accidents can be blamed on poor backing techniques”. - National Safety Council. …If only trucks would bend…. Statistics. The cost of “Property Damage Crash” (a typical backing up accident) is presently estimated at an average of $7,400 per event. Statistics. “One out of every four accidents can be blamed on poor backing techniques”. - National Safety Council. …If only trucks would bend…. Statistics. The cost of “Property Damage Crash” (a typical backing up accident) is presently estimated at an average of $7,400 per event. Law of Conservation of Momentum. With no external force, momentum doesn’t change. It’s the opposite of the impulse momentum relationship!. Ft = Δmv. Example. Consider a gun being fired.. A gun recoils when it is fired. . Shyamnath Gollakota. Dina Katabi. The Hidden Terminals Problem. Collision!. Alice. Bob. The Hidden Terminals Problem. Alice. Bob. More Collisions!. Retransmissions. Can’t get any useful. connections. Yuri . Kovchegov. The Ohio State University. based on work in collaboration with G. . Chirilli. . and D. . Wertepny. , . arXiv:1501.03106. [. hep-ph. ] . Outline. Introduction: classical gluon production problem in AA collisions and why it is important.. Collisions. @ LHC ++. 1. One. central ALICE event for . Pb+Pb @ 2.76 . TeV.A. => E(. kin_total. )= 574 GeV . 0-5% central: . 25000 . particles. Relativistic. AA . and. . eA. . Collisions. 2. “versus” AdS/CFT. Perils, Pitfalls, Progress, Prospects. W.A. . Zajc. Physics Department. Columbia University, New York, NY. . ( . this talk available . at . http://. www.phenix.bnl.gov/phenix/WWW/publish/zajc/sp/presentations/Durham. with heavy-ions. Hou. . Keong. (Tim) Lou,. Simon . Knapen. , . Tongyan. Lin and Tom Melia. PhysRevLett.118.171801. a. Pb. Light Dark Matter 2017. *Disclaimer: Not Dark Matter! Sorry!. “Light”? “Dark”? . Bedanga. Mohanty. NISER. (For STAR Collaboration). Based on STAR: . arXiv. : 1701.07065 . 01/20. Goals of Heavy-Ion Collision. Find out the phase structure of QCD phase . d. iagram . e. xperimentally. . Ralf Rapp. . Cyclotron Institute + . Dept of Phys & Astro. Texas A&M University. College Station, TX, USA. rapp@comp.tamu.edu. Physics Opportunities with . Quarkonia. at the EIC.

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