Elliptic flow of electrons from heavy flavor decays

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Presentation transcript:

Elliptic flow of electrons from heavy flavor decays Elliptic flow of electrons from heavy flavor decays in sqrt {s_{NN}} = 200 GeV Au+Au collisions at PHENIX Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba JSPS)

Elliptic flow (v2) y x py px dN/dφ ∝ N0(1+2v2cos(2φ)) Elliptic flow A powerful probe of the initial state of the high energy heavy ion collision transfer initial spatial anisotropy to momentum space anisotropy macroscopic ; hydro model => pressure gradient microscopic => scattering in the medium dN/dφ ∝ N0(1+2v2cos(2φ)) Initial spatial anisotropy px py Spatial anisotropy Thermal equilibrium The azimuthal anisotropy of particle emission is sensitive to the early stages of system evolution Probe of jet quenching Hydro model Measurement of identified particle v2 give up much more Information of the collision dynamics Momentum space anisotropy of particle emission 2006/6/4

v2 already developed in partonic phase ? identified hadrons v2 after scaling pT and v2 number of quarks v2 after scaling fall on same curve v2 already formed in the partonic phase for hadrons made of light quarks (u,d,s) => partonic level v2 charm quark also flow @ RHIC ? 2006/6/4

Charm quark Charm is believed to be produced in initial collisions via gluon fusion => total cross-section ; binary scaling (Ncoll) Charm propagates through medium created in the collisions => good probe of medium initial charm v2 might be 0 => charm quark v2 due to scattering in medium => non-zero charm v2 indicate very high dense medium created in the collision and quark level thermalization Phys.Rev.Lett.94:082301,2005 (PHENIX) 2006/6/4

Charm quark study @ PHENIX Electron sources charm decay beauty decay Dalitz decays Di-electron decays Photon conversions Kaon decays Thermal dileptons  Subtract photonic electrons following methods “Cocktail subtraction” – calculation of “photonic” electron background from all known sources “Converter subtraction”– extraction of “photonic” electron background by special run with additional converter  (brass, X = 1.7%) non-photonic photonic 2006/6/4

Charm quarks interact with medium ? non-photonic electron RAA clear suppression @ high pT in more central collisoion (RAA < 1.0) => one of the evidence charm quarks interact with the medium low pT and peripheral collision (centrality > 40 %) is consistent with binary scale v2 measurement (pT,cent) gives us additional info. of the interaction between charm and the medium 2006/6/4

Electron v2 measurement @ PHENIX Electron v2 is measured by R.P. method R.P. --- determined with BBC Tracking (pT,φ) --- DC + PC electron ID --- RICH & EMCal dN/d(-) = N (1 + 2v2obscos(2(-))) eID @ RICH After subtract B.G. Energy (EMcal) & momentum matching B.G. Fig : Energy (EMcal) & momentum matching of electrons identified by RICH. Clear electron signals around E/p-1 = 0 2006/6/4 (E-p/p/sigma) distribution

Non-photonic electron v2 measurement Non photonic electron v2 is given as; dNe/d = dNpho.e /d + dNnon-pho.e /d => v2enon-γ = {(1+RNP) v2 - v2eγ} } / RNP v2 --- inclusive electron v2 RNP --- e (non-γ)/ e(γ) v2eγ --- photonic electron v2 photonic electron v2 determination converter method (experiment) Measure inclusive electron v2 with/without converter. Then separate non-photonic & photonic e v2 cocktail method (simulation) Determined photonic electron v2 with simulation e (non-γ) / e (γ) Run04: X=0.4% Run02: X=1.3% (QM05 F. Kajihara) 2006/6/4

Inclusive electron v2 (in/out converter) difference between converter in / out => photonic & non-photonic e v2 is different 2006/6/4

Inclusive electron & photonic electron v2 ○ photonic electron v2 (converter method) photonic electron v2 (simulation ; pi0 -> e)   inclusive electron v2 (converter out) ○ --- photonic electron v2 (converter method) - Photonic electron v2 (simulation) compare with inclusive & photonic electron v2 photonic e v2 ; pT < 1.0 (conv.) & pT > 1.0 (cock.) inclusive electron v2 is smaller than photonic electron v2 2006/6/4

Non-photonic electron v2 PHENIX preliminary Non-photonic electron v2 : pT < 1.0 (conv.) & pT>1.0 (cock.) Non-photonic electron v2 has non-zero v2 2006/6/4

Non-photonic electron v2 (centrality dep.) non-photonic electron v2 seems like getting larger with centrality 2006/6/4

Compare with RAA RAA ~ 1.0 @ peripheral collision but v2 still non-zero indicate charm quarks interact with medium not only central but also peripheral 2006/6/4

D meson flow ? electron v2 from D meson decay well reflect parent v2 simulation Phys.Lett.B597:328-332,2004 electron v2 from D meson decay well reflect parent v2 non-zero non-photonic electron v2 suggest D meson also flow @ RHIC 2006/6/4

expected D v2 from non-photonic e v2 expected D v2 from non-γ v2 process (1) D v2 = a*f(pT) a ; free parameter f(pT) ; pi,K,p (2) D -> e v2 (3) Calculate χ2 (4) Find χ2 minimum for “a” π, deuteron v2 --- PHENIX preliminary Π, deuteron v2 --- PHENIX preliminary  expected D meson v2 from non-photonic electron v2 smaller than pi v2 larger than Deuteron v2 “if D v2 shape same as pi, k, p” Mass D meson~ Mass Deuteron 2006/6/4

Charm quark flow ? Compared with quark coalescence model prediction. with/without charm quark flow (Greco, Ko, Rapp: PLB 595 (2004) 202) - No Bottom contribution - c v2 small u v2 @ low pT - quark v2 flat @ high pT Below 2.0 GeV/c ; consistent with charm quark flow model. => favor charm quark flow model assume c v2 < u v2 @ low pT => mass effect in partonic level ? pT[GeV/c] GeV/c 1 2 3 4 pT[GeV/c] 2006/6/4

B meson contribution ? B meson contribution is model dependent now v2 D & B v2 - assume D & B v2 same Hendrik, Greco, Rapp nucl-th/0508055 w.o. B meson (c flow) D -> e w. B meson (c,b flow) based on quark coalescence model c, b reso ; c,b get v2 by elastic scat. in QGP B -> e pT B meson contribution is model dependent now but the contribution is getting larger at high pT. electron v2 from B meson is smeared due to large mass difference => high pT single electron v2 is getting smaller ? 2006/6/4

[Silicon vertex detector] [Reaction plane detector] Near future single μ v2 new reaction plane detector good resolution => reduce error from R.P. J/ψ v2 & high pT non-photonic electron v2 silicon vertex detector direct measurement D meson v2 PHENIX muon arm beam [Silicon vertex detector] [Reaction plane detector] 2006/6/4

Summary Non-photonic electron v2 from heavy flavor decays has been measured with RHIC-PHENIX Non-photonic electron v2 has non-zero v2 => indicate non-zero D meson v2 Clear centrality dependence of non-photonic e v2 Compare with model calculation with charm flow (c v2 < u v2) => consistent with charm flow model below 2.0 GeV/c => mass effect in partonic level ? Estimate D meson v2 from non-photonic electron v2 assuming D meson v2 shape same as pion, Kaon, proton. 2006/6/4

Backup slides 2006/6/4

“experimentally” determined ! Converter method Separate non-photonic & photonic e v2 by using Non-converter run & converter run Non-converter ; Nnc = Nγ+Nnon-γ Converter ; Nc = R *Nγ+Nnon-γ (1+RNP)v2nc = v2γ + RNPv2non-γ (R +RNP) v2c = R v2γ + RNPv2non-γ v2non-γ(non-photonic) & v2γ(photonic) is “experimentally” determined ! R --- ratio of electrons with & without converter (measured) RNP --- non-photonic/photonic ratio (measured) v2nc --- inclusive e v2 measured with non-converter run (measured)  v2c --- inclusive e v2 measured with converter run (measured) 2006/6/4

Cocktail method Determined photonic electron v2 with simulation Then subtract it from electron v2 measured with non-converter run dNe/d = dNpho.e /d + dNnon-pho.e /d v2non-γ = {(1+RNP) v2 - v2γ} } / RNP measured measured calculate RNP --- non-photonic/photonic ratio experimentally determined v2 --- inclusive electron v2 (without converter) v2γ --- photonic electron v2 calculated from pi0 (pion) v2 From F. Kajihara 2006/6/4

D-> e v2 D meson v2 electron v2 Decay 2006/6/4

D v2 estimate from non-γ e v2 (2) Minimum ; 70 % Minimum ; 75 % Minimum ; 70 % Minimum ; 65 % χ2/ndf v.s. scale factor (a) current result can’t decide what shape is better. 2006/6/4

New reaction plane detector A new reaction plane detector position ; 1~|h|~2.5, resolution ; <cos2DF> ~ 0.7 (BBC ; <cos2ΔΦ> ~ 0.3) materials ; Pb converter + scintillator PHENIX muon arm 2006/6/4