The PHENIX Hadron Blind Detector Craig Woody PHENIX Focus February 9, 2010.
Shengli Huang Vanderbilt University for the PHENIX Collaboration
-
Upload
eleanor-rowe -
Category
Documents
-
view
39 -
download
0
description
Transcript of Shengli Huang Vanderbilt University for the PHENIX Collaboration
![Page 1: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/1.jpg)
Measurements of long-range angular correlation and identified particle v2 in 200 GeV d+Au collisions
from PHENIX
Shengli HuangVanderbilt University
for the PHENIX Collaboration
![Page 2: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/2.jpg)
2
Outline
Motivations
Long-range angular correlations across Rapidity, Centrality and Trigger pT
Identified particles v2 using event-plane method
Summary
![Page 3: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/3.jpg)
3
“Ridge” and ”v2” in [email protected] TeV
A “ridge” is observed in the central p + [email protected] TeV The distribution shows a cos(2) structure The identified particle v2 shows a mass ordering
ALICE: Physics Letters B 726 (2013)ATLAS: Phys. Rev. Lett. 110(2013)CMS: Phys. Lett. B 7198(2013
![Page 4: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/4.jpg)
4
V2 in d+Au@ 200 GeV
The cos(2) structure is also seen in 0-5% d+Au. The cut of ||>0.48 is the limit of our central arm acceptance
The v2 in 0-5% d+Au is higher than that in 0-2% p+Pb collisions, which is consistent with hydro calculation
The measurement with large || is required!
PHENIX: Phys. Rev. Lett. 111, 212301 (2013)
![Page 5: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/5.jpg)
5
Initial or final state effect?
CGC Hydrodynamics
The study of long-range correlation and precise measurements of anisotropy in d + Au collisions will be helpful in investigating these models.
Is there “ridge” in dAu collisions?How about the difference between the v2 in dAu and pPb? Is there mass ordering for identified particle v2 in dAu?
![Page 6: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/6.jpg)
6
Extend the rapidity range
PHOBOS Phys. Rev. C72, 031901
MPC Au-going
MPC d-going
Muon Piston Calorimeter Forward/backward-rapidity 3<||<4 Extend the rapidity range by measuring the
correlation between Tracks (<||<0.35) and MPC towers: ||>2.75!
![Page 7: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/7.jpg)
7
Angular correlations between Track and Tower: C()
is the transverse energy of each tower is number of pair of track-tower in same event =
M() is track-tower correlation in mixed events
![Page 8: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/8.jpg)
8
C(,pT) of pp and 0-5% dAu In pp, the distribution is
dominated by the dipole term cos(), which may due to the momentum conservation
In dAu, the distribution shows a near side peak
Dijet contribution can’t be taken out by subtracting the conditional yield of pp from dAu
Dijet contributions to c2 in dAu can be estimated from c2 in ppd+Au 0-5% p+p
arXiv:1404.7461
pT
![Page 9: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/9.jpg)
9
Compare c2 from d+Au and p+p
The difference indicates that the contribution from di-jet, resonance decay … is less than 10% for
arXiv:1404.7461
![Page 10: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/10.jpg)
10
“Au-going” vs “d-going”
![Page 11: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/11.jpg)
11
mid-forward(d-going) correlation
The mid-forward rapidity correlation in central d+Au is different from that in peripheral, even though there is no near-side peak
![Page 12: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/12.jpg)
12
Mid-backward(Au-going) correlation
The near-side peak is visible until 10-20% centrality
In peripheral collisions, the Au-going correlation is similar to the d-going correlation
![Page 13: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/13.jpg)
13
A ridge is observed with| |>6.0
Correlation between Au-going and d-going MPC towers
![Page 14: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/14.jpg)
14
Event-plane method for v2Muon piston Calorimeter
MPC (3.1<||<3.9)
Central Arm tracking(||<0.35)2,CNT
Zero Degree Calorimeters(ZDC)Shower Max Detectors(SMD)ZDC-SMD (||>6.5)1,smd_s by Au-going spectator
x
y
beam
reaction plane
The difference between c2(dAu) and c2(pp) indicates that in EP methods, the contribution from dijet, resonance … is less than 10% for pT up to 4.5 GeV/c
The event-plane 2,MPC_S resolution is estimated from three-sub events which include the 2,CNT and 1,SMD_S
2,MPC_S Au-going
![Page 15: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/15.jpg)
QM2014 Shengli Huang 15
The charged hadron v2 measured by the event plane method in central dAu is similar to that in central pPb
V2(EP) of charged hadron in 0-5% d+Au
arXiv:1404.7461
![Page 16: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/16.jpg)
16
Mass ordering is observed in 0-5% d+Au This ordering can be reproduced in hydro calculation
from P. Romatschke et al.
Identified particles’ v2 from EP methods
arXiv:1404.7461
Hydro: P. Romatschke, private communication. J. Nagle et al., arXiv:1312.4565.
![Page 17: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/17.jpg)
17
Weaker radial flow in dAu?
The magnitude of mass ordering in p+Pb is larger than that in d+Au Weaker radial flow in d+Au?
Subtract method
![Page 18: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/18.jpg)
18
Summary Is there “ridge” in dAu collisions?
How about the difference between the v2 in dAu and pPb?
Is there mass ordering for identified particle v2 in dAu?
The input from CGC model calculation is expected for the further understanding the physics of “ridge” and “v2” in small collision system
There is “Ridge” in dAu even with ||>6.0
v2 in central dAu is similar to that in central pPb, while hydro calculation show a significant difference
The mass ordering is observed in central dAu , while it is smaller comparing with central pPb, it may be due to a weaker radial flow in dAu
![Page 19: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/19.jpg)
QM2014 Shengli Huang 19
BackUp
![Page 20: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/20.jpg)
20
Scalar Product Method: <Q>
STAR: PRL93,252301(2004) PRC72,014904(2005)
In heavy ion collision:<Q> <> M v2(pt) M 2(pt)The nonflow in AA(dA) is same as pp
For the tower of MPC Q = (icos(2tower,i), isin(2tower,i)) i is ET of each MPC tower of Au-going
<Q> = ET c2(pt)
The dijet, resonance et al contributions in d+Au collisions can be estimated in p+p collisions with the scale of
![Page 21: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/21.jpg)
21
c2 and c3 vs pT
The c3 is close to 0, comparing with the sizeable c2
![Page 22: Shengli Huang Vanderbilt University for the PHENIX Collaboration](https://reader034.fdocuments.us/reader034/viewer/2022051315/56812d0d550346895d91e3a1/html5/thumbnails/22.jpg)
QM2014 Shengli Huang 22