k* 0 analysis in pb-pb collision at √s nn = 2.76 tev
DESCRIPTION
K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV. Subhash Singha NISER, Bhubaneswar. India-ALICE Collaboration Meeting 27-28 April 2013. Outline: --- Motivation --- Data Sets and analysis detail --- Mass/Width as a function of p T --- Systematic error extraction - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/1.jpg)
K*0 analysis in Pb-Pb collision at √sNN = 2.76 TeV
Subhash SinghaNISER, Bhubaneswar
27/04/13 1
India-ALICE Collaboration Meeting27-28 April 2013
![Page 2: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/2.jpg)
27/04/13 2
Outline:
--- Motivation
--- Data Sets and analysis detail
--- Mass/Width as a function of pT
--- Systematic error extraction
--- Corrected pT spectra
--- Particle ratio: K*0/K-
--- Summary
![Page 3: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/3.jpg)
Re-scattering
time
Re-generation
Kinetic freeze out
Lifetime of resonances are comparable to the lifetime of fireball sensitive to the properties of the medium.
Re-scattering and re-generation:
K*0/K
Centrality
Qualitative plot
(K*0/K)AA and (K*0/K)pp re-scattering / re-generation effects.
Lifetime(fm/c)
K*0 4
ϕ 45
Motivation
27/04/13 3
![Page 4: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/4.jpg)
27/04/13 4
Data Sets: Pb-Pb/AOD04990 Good Runs with No V-drift problems
Data Set
00 to 20 ===> 3.05627e+0620 to 40 ===> 3.04396e+0640 to 60 ===> 3.04714e+0660 to 80 ===> 3.06153e+0600 to 80 ===> 1.22089e+07
![Page 5: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/5.jpg)
27/04/13 5
Event, Track and PID selection
Track Selection: --- pT > 0.15 GeV/c.--- |η| < 0.8--- |(DCA)r (pT)| < 0.018 + 0.035pT -1.01
--- |(DCA)z|< 2 cm--- ITS and TPC refits.--- min cluster in TPC: 70--- max Chi-square in TPC: 4--- Kπ pair rapidity |y|< 0.5
PID Selection: |Nσ| < 2.0 (using TPC only)Decay Channel:
K*0 K+ π- , K- π+ (BR: 66%)
Event Selection: Physics Selections, |vZ| < 10 cm
Centrality Selection: using V0M
Standard 2010 track quality cuts with filterbit 32
![Page 6: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/6.jpg)
27/04/13 6
K*0 Signal extraction: Event Mixing (EM) and Like Sign (LS) distributions
Kπ invariant mass distribution
Background estimated using:
Event mixing techniqueLike Sign technique
Event mixing:
Number of mixed events = 510 bins in Z vertex (-10, 10)10 bins in centrality (0,100)12 bins in event plane angle (0,2π)
Like Sign:
€
NK*0 = NK1
+π 1− +N
K1−π 1
+ − R × NK1
+π i− +N
K1−π i
+ +NK i
+π 1−
i
∑ +NK i
−π 1+
⎛
⎝ ⎜
⎞
⎠ ⎟
€
NK*0 = NK1
+π 1− +N
K1−π 1
+ − 2 × NK1
+π 1+ × N
K1−π 1
−
R Normalization factor
![Page 7: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/7.jpg)
27/04/13 7
Example of K*0 Signal extraction
0.8 < pT < 1.2 GeV/c2 0.8 < pT < 1.2 GeV/c2
The combinatorial background is normalized in the invariant mass region (1.1, 1.3) GeV/c2
![Page 8: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/8.jpg)
27/04/13 8
0.8 < pT < 1.2 GeV/c2 0.8 < pT < 1.2 GeV/c2
Where
After combinatorial background subtraction, signal is fitted with a p-wave relativistic Breit Wigner function
Example of K*0 Signal extraction
Mass(M0) and width(Γ0) extractedfrom fit parameters
BW
![Page 9: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/9.jpg)
27/04/13 9
Mass of K*0 as a function of pT
Mass consistent with PDG value
![Page 10: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/10.jpg)
27/04/13 10
Width of K*0 as a function of pT
Width consistent to PDG value
![Page 11: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/11.jpg)
27/04/13 11
Mass and Width of K*0: comparison with MC
Mass and width consistent with MC HIJING simulations
K* signal in MC HIJING
0-20%
![Page 12: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/12.jpg)
27/04/13 12
List of Systematic checks:
Varying fitting ranges
Varying normalization regions
Varying residual backgrounds (poly2 vs. poly3)
Keeping free width vs. fixed PDG width
Varying Non Rel. BW and Rel. BW
Track Selections (10% constant as a function of pT)
PID : N sigma cuts
Material Budget. (1% constant as a function of pT)
Centrality Selection
Like Sign Method (consistency check)
Sources of systematic uncertainty
![Page 13: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/13.jpg)
27/04/13 13
Sources of systematic uncertainty in K*0 yield
![Page 14: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/14.jpg)
27/04/13 14
Sources of uncorrelated systematic uncertainty in K*0 yield
![Page 15: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/15.jpg)
27/04/13 15
pT Spectra of K*0: Tsallis Levy Fit
dN/dy and <pT> calculated usingdata in the measured region andfit in the extrapolation region.
€
1
Nevt
d2N
dpTdy=
A
T(m +T)× pT × exp(
− pT2 +m2 −m
T)
![Page 16: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/16.jpg)
27/04/13 16
pT Spectra of K*0: Boltzmann Gibbs Blast Wave Fit
![Page 17: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/17.jpg)
27/04/13 17
<pT> of K*0
![Page 18: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/18.jpg)
27/04/13 18
<pT> of ϕ, K*0 with π, K, p-bar
Increasing mass
<pT>ϕ ~ <pT>K*0 ~ <pT>pbar
![Page 19: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/19.jpg)
27/04/13 19
Particle ratio: K*0/K- vs Npart
K*0/K- ratio vs Npart hadronic rescattering for central collisions(?)
Log scale on Y-axis
![Page 20: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/20.jpg)
27/04/13 20
Particle ratio: K*0/K- vs √sNN
(K*0/K-)AA < (K*/K-)pp hadronic recattering (?)
![Page 21: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/21.jpg)
27/04/13 21
Particle ratio: K*0/K- vs (dN/dη) 1/3
K*0/K- vs (dN/dη)1/3 effect of size of the fireball (?)
![Page 22: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/22.jpg)
27/04/13 22
Summary:
-- Mass and width of K*0 consistent with PDG value.
-- <pT>ϕ ~ <pT>K*0 ~ <pT>pbar
-- K*0/K- ratio vs Npart hadronic rescattering for
central collisions(?)
-- (K*0/K-)AA < (K*/K-)pp hadronic recattering in AA
collision.
-- K*0/K- vs (dN/dη)1/3 effect of size of the fireball(?).
![Page 23: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/23.jpg)
27/04/13 23
Back Up Slides
![Page 24: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/24.jpg)
27/04/13 24
Correlated and uncorrelated errors
Eratio= Echeck/YdefEratio= √(E2check- E2
def)/Ydef
![Page 25: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/25.jpg)
27/04/13 25
Sources of uncorrelated systematic uncertainty in K*0 yield
![Page 26: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/26.jpg)
04/18/13 26
pT Spectra of K*0: Blast Wave predictions (0-20%)
Integral of BW function = 19.88Integral of K* = 15.22
Blast wave parameters:=========================================================beta_max = 0.878514<beta> = 0.644618 +- 0.002296 (e+ = 0.002262, e- = -0.002292)T = 0.096984 +- 0.002141 (e+ = 0.002103, e- = -0.002047)n = 0.725690 +- 0.011371 (e+ = 0.011362, e- = -0.011364)chi2 = 57.718817ndf = 124.000000=========================================================
27/04/13 26
![Page 27: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/27.jpg)
27/04/13 27
![Page 28: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/28.jpg)
K*0 /K as a function of pT
Kaon
2827/04/13
![Page 29: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/29.jpg)
K*0 and K spectra
Since the pT binning of Kaon and K*0 spectra are different, I have takenthe Kaon yields using the fit function Boltzmann Gibbs Blast Wave.
2927/04/13
![Page 30: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/30.jpg)
K*0 (pT)/K(pT)
Linear scale Log scale
3027/04/13
![Page 31: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/31.jpg)
K*0 (p*T)/K(pT)
p*T = pT (MK/MK*)
Linear scale Log scale
31
After mass correction for radial flow
27/04/13
![Page 32: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/32.jpg)
27/04/13 32
K*0 BGBW model with parameters taking from Kaon
K*0 and K spectra: With BGBW model
![Page 33: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/33.jpg)
27/04/13 33
Comparison with preliminary analysis
![Page 34: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/34.jpg)
27/04/13 34
Comparison: K*0 Spectra
![Page 35: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/35.jpg)
27/04/13 35
K*0 : Mass/Width : Material Budget productions
Mat. Budg. Productions:LHC10h9 Pb-Pb Hijing (137366), 25 K events, +7% material
LHC10h10 Pb-Pb Hijing (137366), 25 K events, -7% material
![Page 36: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/36.jpg)
27/04/13 36
K*0 Signals
![Page 37: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/37.jpg)
27/04/13 37
K*0 signals : BW Fits (TPC analysis) 0-20%
![Page 38: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/38.jpg)
27/04/13 38
K*0 signals : BW Fits (TPC analysis) 20-40%
![Page 39: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/39.jpg)
27/04/13 39
K*0 signals : BW Fits (TPC analysis) 40-60%
![Page 40: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/40.jpg)
27/04/13 40
K*0 signals : BW Fits (TPC analysis) 60-80%
![Page 41: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/41.jpg)
27/04/13 41
Efficiency x Acceptance
![Page 42: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/42.jpg)
27/04/13 42
Efficiency x Acceptance
Production: LHC10a11a_bis/ESDs
![Page 43: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/43.jpg)
27/04/13 43
Efficiency of K* with different event and track selections
![Page 44: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/44.jpg)
(0.3-5.0) in 0.5 GeV step
27/04/13 44
(0.3-5.0) in 0.4 GeV step
Efficiency of K* with different pT combinations
![Page 45: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/45.jpg)
Efficiency of K* and anti-K*
27/04/13 45
![Page 46: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/46.jpg)
27/04/13 46
![Page 47: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/47.jpg)
27/04/13 47
Looking at K* and anti-K* separately
0-20%0-20%
0-20%An example:Comparison K+ π- and K- π+ distributions
Difference ~ 2%
![Page 48: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/48.jpg)
K*/anti-K* signals : 0-80%
27/04/13 48
K* Anti-K*
![Page 49: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/49.jpg)
27/04/13 49
![Page 50: K* 0 analysis in Pb-Pb collision at √s NN = 2.76 TeV](https://reader036.vdocuments.net/reader036/viewer/2022062500/568151a6550346895dbfd4a5/html5/thumbnails/50.jpg)
27/04/13 50
Other plots