the phenix/rhic and totem/lhc experiments status and hungarian activities

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THE PHENIX/RHIC AND TOTEM/LHC EXPERIMENTS Status and Hungarian activities M. Csanád for PHENIX/Hu & TOTEM/Hu +

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+. The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities. M. Csanád for PHENIX/Hu & TOTEM/Hu. Heavy Ion Physics. Recreate conditions similar to those at the Big Bang Explore quark matter. The Relativistic Heavy Ion Collider. - PowerPoint PPT Presentation

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Page 1: The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities

THE PHENIX/RHIC AND TOTEM/LHC EXPERIMENTSStatus and Hungarian activitiesM. Csanád for PHENIX/Hu & TOTEM/Hu

+

Page 2: The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities

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Heavy Ion Physics Recreate conditions similar to those at

the Big Bang Explore quark matter

Page 3: The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities

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The Relativistic Heavy Ion Collider

RHIC: Brookhaven Nat’l Lab: Au+Au, Cu+Cu, d+Au, p+p 4 experimental collab’s: STAR, PHENIX, BRAHMS,

PHOBOS Institutional membership in PHENIX

RMKI, Eötvös University, Debrecen University

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Collision modes, recorded data Two independent rings

Separate magnetic field Proton polarization

Many different modes 9.2 GeV/n (Au) 22 GeV/n (Au, Cu, p) 56 GeV/n (Au) 62 GeV/n (Au, Cu, p) 130 GeV/n (Au) 200 GeV/n (Au, Cu, p) 410 GeV/n (p) 500 GeV/n (p) Energy scan program: QCD phase diagram

Science >1000 refereed papers, >24000 independent citations Discoveries

The future: e-RHIC & RHIC II Identified key scientific questions, started upgrades

Recorded events in millions

Page 5: The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities

The RHIC complex5

1.Tandem2.a: Tandem to

Booster2.b: Linac3.Booster4.Alternating Gradient

Synchrotron5.AGS to RHIC6.RHIC

Page 6: The PHENIX/RHIC and TOTEM/LHC Experiments Status and Hungarian activities

PHENIX setup Tracking, calorimetry,

identification Charged hadrons ( π±, K±, etc.) Photons, direct or decay (→ η , π0) Light mesons φ, ω and η Single leptons → heavy flavor Di-leptons → heavy flavor, J/Ψ

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Centrality determination7

Overlapping region: participants

Evaporated neutrons: toward ZDC (charged wiped out)

Participants: new particles toward BBC Centrality: EZDC versus QBBC

Spectators

Participants

Toward ZDCToward BBC

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Collisions of different centrality

Peripheral Central

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A PHENIX Event

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The first milestone: nuclear modification

Proton+protonNucleus+nucleus

Simply just more?A+A = many p+p?

Particle yield in A+A

Particle yield in p+p ×RAA= Number of p+p

collisions

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Suppression of high energy particles Peripheral Au+Au and d+Au: no suppression Central Au+Au: large suppression

Phys.Rev.C76, 034904 (2007)

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Strongly interacting medium Hadrons suppressed, photons not! Strong interaction in the medium

Central

Peripheral

Phys.Rev.Lett.94, 232301 (2005)

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Perfect fluid of quarks Elliptic flow measures azimuthal

asymmetry, v2 Hydro picture: collective evolution, v2>0

Even heavy flavour flow: perfect hydro confirmed

Scaling of elliptic flow with constituent quark number Flow versus kinectic energy for several

hadronsφ

Phys.Rev.Lett.98, 162301 (2007)

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Temperature from direct photons Photons fly out of the medium:

penetrating probe Information on the temperature Tinitial at least 2-300 MeV Quark-hadron trans. at ~170 MeV

Thermalization, expansion, cooling …… Freeze-outPhys. Rev. Lett. 104, 132301

(2010)

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The TOTEM experiment at LHC Measure p+p stot ± 1 mb, luminosity-independently

Elastic scattering at t 10-3 GeV2 Inelastic rates as well

Measure dstot/dt 10-3 – 101 GeV2

Measure LHC luminosity precisely

Measure diffractive dissociation single, double diffraction, multiple Pomeron exchange

02

/161

el ttot

el inel

dN dtN N

s

tot el inelN Ns L

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TOTEM Setup At the CMS interaction point Three detectors: Roman Pot, Telescope 1, Telescope 2

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Proton-proton scattering at the LHC Different proc. in

p+p Elastic, diffractive,

inelastic Trigger: large

rapidity

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Roman Pot detectors of TOTEM Special „edgeless” design to move close

to beam Distance ~ 10 s Reconstruct from there

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Differential cross-section at b*=3.5 m Measured over a large |t| range, will be extended Dip-hump structure first seen at ISR, also present

here Compared to models

Exponent: 7.8 ± 0.3 Slope: 23.5 ± 0.5 GeV˗2

Dip: 0.53 ± 0.5 GeV2

EPL, 95 (2011) 41001

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Total cross-section results at b*= 90 m Special LHC optics, agreement w/ previous

measurement Result from t=0 extrapolation:

stot = (98.3 ±0.2stat +2.82.7) mb sinel = (73.5 ±0.6stat +1.81.3) mb sel = (24.8 ±0.2stat ±1.2) mb

CERN-PH-EP-2011-158

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THANK YOUfor your attention

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The PHENIX/Hu group >20 PHENIX talks >50 internal working

group talks ~15 analysis notes 11 papers with direct

participation (paper group)

http://phenix.elte.hu http://phenix.kfki.hu

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The TOTEM/Hu group Tasks during setup: DAQ, data monitoring,

Roman Pot Phyics projects on the way, e.g. dsel/dt Working closely to theory groups

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Elastic scattering slope at low t Theoretical predictions differ in many

aspects

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Single diffraction low = p/p

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Single diffraction large

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Double POMERON exchange

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Double POMERON exchange