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Low-mass dielectron measurement at RHIC-PHENIX
Yoshihide Nakamiya (for the PHENIX collaboration)Hiroshima University, Japan
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Outline Physics goals for low-mass dielectron measurement
Difficulties and Challenges for di-electron analysis in Au+Au collisions
Low-mass vector mesons () at low pT Mass shape Yield comparison among several decay modes.
Low-mass continuum at low pT. Continuum yield
Summary
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Physics of low-mass dielectronR. Rapp J. Phys G31 (2005) S217
M.Harada et. al. Phys.Rev.D74:114006,2006.
In hadronic phase
In partonic phase
RHIC
High energy heavy-ion collisions produced extremely high-temperature medium.
Several kinds of model calculations predict significant change of spectral function (but tendency of the change is different between them)
My motivation is what behavior is experimentally observed ?
KEK-PS/E325
Low-mass vector mesons as a probe Mass spectrum shape
Careful investigation of mass shape of light vector mesons are essential to discuss chiral symmetry restoration.
It is important to measure transparent probes like e+e- decay modes because electrons can pass through the medium with few interactions and therefore carry original information on the meson production.
Yield difference between e+e- and K+K-
Branching ratio between e+e- and K+K- may be sensitive to mass modification, since Mphi is approximately 2 MK.
Need to compare yield of e+e- and K+K-
T.Hatsuda and S.Lee Phys.Rev.C46-1 1992
mKK
m
4
CERES/NA45 (past experiment)
Enhancement of di-electron continuum had been discovered at CERES/NA45.
Some theoretical comparisons had been done. ex) dropping, collision broadening …
PHENIX experiments
Detailed analysis become possible at PHENIX since continuum distribution can be separated from mass peak of light vector mesons.
Low-mass dielectron continuum as a probe
Rapp-Wambach, 2000
--- dropping--- collision broadening
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Systematic studies give much information about properties of hot medium.
several collision species - p+p (as baseline) - d+Au (examine cold nuclear effects) - Au+Au (examine effects in partonic matter)
several decay channels
All data shown in this presentation are taken in 200 GeV (were taken in run3 - run5)
Fundamental strategy for low-mass dielectron measurement at PHENIX
mesons
-> e+e- BR = 10-4 -> K+K- BR = 50%
mesons -> e+e- BR = 10-5
-> 0 BR = 9% -> 0+- BR = 90%
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Particle detection at PHENIX
e+
e
Acceptance -0.35 < η < 0.35 2 x 90°in azimuthal
angle for two arms Electron detection
precision tracking : DC/PC
electron id : RICH, EMCal etc
e separation is 1/10-4
at pT < 4.7 GeV/c
The PHENIX spectrometers are excellent devices to measure electrons. (can also measure hadron/photon at the same time, it make systematic measurement possible) 7
Uncorrelated combinatorial pair
Difficulty(1) High multiplicity dNch/d ~ 650 ( in most central Au+Au collision at mid-rapidity)
Difficulty(2) Huge combinatorial background Dalitz decay (e+e-) photon conversion
Difficulty(3) Small fraction to dielectron decay mode from
Branching Ratio (BR) -> e+e- BR = 10-4 -> K+K- BR = 50%
-> e+e- BR = 10-5
-> 0 BR = 9%-> 0+- BR = 90%
0
PRL 91 052303(2003) 5
-5
0e+e-
e+e-
Difficulties in di-electron analysis in Au+Au 200GeV
ex)
It is a key to overcome their difficulties by analysis efforts. 8
Key challenges for di-electron analysis in Au+Au 200GeV
Difficulty(1) High multiplicity
accidental charged hadron contamination unphysical correlated background
Difficulty(2) Huge combinatorial background
background by uncorrelated pairs
Difficulty(3) Small fraction to dielectron decay mode
not avoidable (decided by physics)
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Challenge against each item are shown from the next slide.
Number of PMT distribution in RICH is different between real data and simulation due to random association tracks.
electron ID by RICH Charged hadron tracks are detected as electrons by random associations under high multiplicity environment.
Black : electron identified tracks (real data)Red : electrons (simulation)
Electron identification in high multiplicity environment (Au+Au 200GeV)
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Black : electron identified tracks (real data)Blue : random associated tracks (real data)
Detector response under high multiplicity environment is reasonably understood and evaluated.
Black : electron identified tracks after subtracting random associated tracks Red : electrons (simulation)
electron ID by RICH Charged hadron tracks are detected as electrons by random associations under high multiplicity environment.
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Electron identification in high multiplicity environment (Au+Au 200GeV)
Blue : opening angle between two tracks on RICH plane(same event) Red : opening angle between two tracks on RICH plane(event mixing)
Effect from unphysical correlated tracks are understood and evaluated .
RICH plane
Unphysical correlated background in high multiplicity environment (Au+Au 200GeV) unphysical correlated background in RICH
When a points to the same ring as an electron, it is associated to the same ring. This happens for a typical values of opening angle which folded with the average momentum of the electron corresponded to a particular invariant mass.
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Multiplicity effects to E/p are reasonably evaluated and calibrated.
hadron rejection by Energy-momentum matching Energy-Momentum matching (E/P) is distributed about 1.
• small electron mass compared to measured momentum scale• hadrons deposit only MIP energy in EMCal.
Black : electron identified tracks (real data)Red : random associated tracks (real data)
Black : electron identified tracks after subtracting random associated tracks
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Electron identification in high multiplicity environment (Au+Au 200GeV)
Combinatorial background (Au+Au 200GeV)
--- same event N+-
--- mixed event N+-
shape from mixed event
Good agreement for uncorrelated distribution in same event
normalization between same event and mixed event
Normalize B++ and B to N++ and N .
Normalize mixed +- pairs to 2N N N
→ee
→ee
J
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Combinatorial background from uncorrelated pairs are evaluated.
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Result of mass shape analysis for e+e- in Au+Au 200 GeV
It is successful to extract signals in Au+Au 200 GeV … so far we cannot discussed mass shape due to lack of
statistics and signal to background ratio. need more statistics (3 times as many statistics as run4 has
already taken at run7 ) need to improve S/N (upgrade devices )
Future improvement of dielectron measurement by Hadron Blind detecor (HBD ) Remaining problems
We made analysis effort and extract the signal in Au+Au 200 GeV. But the following cases cannot be improved by analysis. case1) Counter part of electron pair go out from the PHENIX acceptance case2) Very low pT electrons cannot escape the magnetic field
Solutions HBD detector has capability to identify Dalitz decaying electrons via their opening angle. S/B will be expected to improve a factor 10 to 100.
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e+
e-0e+e-
Case 1
e+
e-
Case 2
0e+e-
HBD
Extended K+K- analysis
The three independent kaon analyses (double kaon id, no kaon ID and single kaon ID methods) are consistent with each other. Spectra between K+K- and e+e- are reasonable agreementin p+p.
d+Au0-20%
p+p
No ID Single ID Double ID
M.B.
Consistency check for mesons in p+p/d+Au 200 GeV
d+Au0-20%
p+p
No ID Single ID Double ID e+e-
M.B.
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Consistency check for mesons in p+p/d+Au 200GeV
spectra also show good agreement among several decay channels.
p+pd+Au
0 dAu MB (PRC75 151902)0+- dAu MB(PRC75 151902)e+e- pp MB (PHENIX preliminary)0 pp MB (PRC75 151902)0+- pp MB(PRC75 151902)0 pp ERT (PHENIX preliminary)0+- pp ERT (PHENIX preliminary)
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e+e- AuAu MB e+e- 20-40% x 10-3 e+e- 40-92% x 10-1 K+K- AuAu MB (no PID)K+K- AuAu MB (double PID) K+K- AuAu MB (PRC72 014903) K+K- 20-40% x 10-3 (double PID)K+K- 40-92% x 10-1 (double PID) K+K- 40-92% x 10-1 (PRC72 014903)
It’s successful to measure pT spectra of e+e- in Au+Au.
… so far we cannot make any clear statement about the comparison between spectra for e+e- and
More statistics and improvements of S/N are needed.
40-92%20-40%
Au+Au
pT spectra comparison for mesons in Au+Au 200 GeV
M.B.
K+K-
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pT spectra for mesons in Au+Au 200GeV
measurement are done up to 10 GeV/c.
Long awaited ee, along with ee
0-20%
20-60%60-92%
M.B.
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Hadronic source of ee “Cocktail” of ee from hadron decays
Dalitz decays
0ee, 0ee
Direct decays
eeJee
Semileptonic decays of heavy flavor
Drell Yan process
Estimate contribution from hadron decay Fit 0and± data
For ,J/ mesons, measured yields are used(in Au+Au/p+p)
For ther hadrons, we use normalization A under assumption they follows “mT scaling”
Charm production c= Ncoll x 567±57±193b from single electron measurement.
Binary scaling (Ncoll) to Au+Au.
n0T2TT
3
3
pp)bpapexp(
A
pd
σdE
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Continuum Extraction in p+p 200 GeV
Signal/Background ~ 1. Peaks have well separated due to high resolution. The main components of backgrounds are taken into account.
Uncorrelated background by event mixing Contamination from “jet pair” and “cross pair” is taken
into account.
π0π0
e+
e-
e+
e-
γ
γ
π0
e-γ
e+
“Jet pairs”
“Cross pairs”0
e e
e e
X
Correlated Signal = Data-Mix
Mixed events
“Jet pairs”
“Cross pair”
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Low-mass dielectron continuum in p+p 200 GeV
Excellent agreement has seen between data and hadron decay contribution from “cocktail” analysis. Charm cross section ( integration after cocktail subtraction)
c=544 ± 39 (stat) ± 142 (sys) ± 200 (model) b25
Continuum Extraction in Au+Au 200 GeV
Signal/Background ~ 1/200.
Peaks have well separated due to high resolution
Signal is also extracted in Au+Au 200 GeV.
Mixed events
Correlated Signal = Data-Mix
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Low-mass dielectron continuum in Au+Au 200 GeV
Charm from PYTHIAfiltered by acceptancec= Ncoll x 567±57±193b
Charm “thermalized” filtered by acceptancec= Ncoll x 567±57±193b
Continuum enhancement is observed in 150 < mee<750 MeV. Intermediate-mass dielectron continuum are consistent with PYTHIA if charm production from thermal radiation is taken into account.
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0<pT<0.7 GeV/c
0.7<pT<1.5 GeV/c 1.5<pT<8 GeV/c
0<pT<8.0 GeV/c
p+pAu+Au
arXiv: 0802.0050arXiv: 0706.3034
Low mass excess in Au+Au is concentrated in low pT. (Medium dependent effects)
pT dependence of continuum enhancement
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0 < pT < 8.0 GeV/c 0 < pT < 0.7 GeV/c
0.7 < pT < 1.5 GeV/c 1.5 < pT < 8.0 GeV/c
Centrality dependence of continuum enhancement
Mass window
(a) 150 < mee< 750 MeV (b) 0 < mee< 100 MeV
0 region (mee<100 MeV)
production scales approximately with Npart
Excess region (150<mee<750 MeV)
production from hot matter.scattering processes likeor qq annihilation) a yield rising faster than proportional to Npart
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Mass dependent dielectron pT spectra
p+p Au+Au
p+p data are consistent with “cocktail” up tp 3 GeV/c Au+Au data enhanced for all pT at the range above m
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Comparison to theoretical model (in Au+Au)
Both dropping and collision broadening models had beenwell reproduced in CEREC/NA45. Any models are not described continuum enhancement in PHENIX !?
Theoretical models
vacuum spectral function dropping collision broadening
Rapp-Wambach, 2000CERES/NA45
--- dropping--- collision broadening
PHENIX
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Di-electron analysis Difficulties of dielectron analysis in Au+Au 200 GeV are identified, attacked and
overcome.
Low-mass vector meson Make sure that pT spectra between several decay channels are consistent in p+p.
It is successful to extract signals in Au+Au 200 GeV.
(but statistical and systematic errors are large so far) 3 times as many statistics as at run4 has already taken at run7 signal/background will be improved by HBD.
Low-mass dilelectron continuum Dielectron mass spectra are well reproduced by “cocktail” analysis in p+p 200GeV.
Enhancement of continuum yields is observed in 150 < M ee < 750 MeV/c2 in Au+Au 200GeV.
Effective theoretical models to explain the enhancement are needed.
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Summary
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• After several experimental checking, we found integrated information is not enough to determine the difference between e+e- and K+K-.•Need a careful check of mT spectra.
Yield and temperature for mesons
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The invariant mass spectra for φ mesons e+e- p+p e+e- d+Au e+e- Au+Au
φφ
K+K- (double PID) d+Au K+K- (double PID) Au+Au
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