21 sep 2006 kentaro miki for the phenix collaboration university of tsukuba the physical society of...

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21 Sep 2006 Kentaro MIKI for the PHENIX collaboration Kentaro MIKI for the PHENIX collaboration University of Tsukuba University of Tsukuba The Physical Society of Japan 62th Annual Meeting The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX RHIC-PHENIX 実実実実実実実実実実実実実実実 実実実実実実実実実実実実実実実 実実実実実実実実実実実実実実実実実 実実実実実実実実実実実実実実実実実 Azimuthal anisotropy measurement of high p Azimuthal anisotropy measurement of high p T direct photon direct photon in sqrt{s_NN}=200GeV Au+Au collisions at RHIC-PHENIX in sqrt{s_NN}=200GeV Au+Au collisions at RHIC-PHENIX

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Page 1: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21 Sep 2006

Kentaro MIKI for the PHENIX collaborationKentaro MIKI for the PHENIX collaborationUniversity of TsukubaUniversity of Tsukuba

The Physical Society of Japan 62th Annual Meeting The Physical Society of Japan 62th Annual Meeting

RHIC-PHENIXRHIC-PHENIX 実験における高横運動量領域での実験における高横運動量領域での直接光子の楕円的方位角異方性の測定直接光子の楕円的方位角異方性の測定

Azimuthal anisotropy measurement of high pAzimuthal anisotropy measurement of high pTT direct photon direct photon

in sqrt{s_NN}=200GeV Au+Au collisions at RHIC-PHENIXin sqrt{s_NN}=200GeV Au+Au collisions at RHIC-PHENIX

Page 2: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 2

1. Direct photon1. Direct photonDirect photon ( 直接光子 )  測定される全ての光子から、ハドロン崩壊を起源に持つ光子を除いたもの

0

prompt photon

thermal photon

jet fragment photon

hadron decay photon

direct photon hadron decay photon

Page 3: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 3

2. Azimuthal anisotropy2. Azimuthal anisotropy

x

z

: azimuthal angle of particles : azimuthal angle of reaction plane

Elliptic flow (v2) 発生粒子の、方位角方向における分布の偏りの強度

Page 4: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 4

3. direct photon v3. direct photon v22

annihilationcompton scattering

Bremsstrahlung (energy loss)

direct photon の v2 は 0 か?有限の値を持つか?

prompt photon v2 = 0 thermal photon v2 > 0

jet fragment photon

Page 5: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 5

4. How to measure ?4. How to measure ?

1

* _2

.2.

2

R

vvRv

photonBGphotonincphotondir

photonBG

photoninc

N

NR

_

.

1. 0 v2

2. inclusive photon v2

3. hadron decay photon v2

4. direct photon v2

PHENIX preliminary

Page 6: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 6

5. result 5. result ~ direct photon v~ direct photon v2 2 ~~

PHENIX preliminary PHENIX preliminary

PHENIX preliminary

PHENIX preliminary

Page 7: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 7

6. result 6. result ~ direct photon v~ direct photon v2 2 ~~

PHENIX preliminary

1. 5GeV/c 以上の領域で 0 (0 は有限の値を持つ ) 。 -> prompt photon が支配的。

2. 3 ~ 4 GeV/c 領域においても、 proton とは違う値を持つ。 -> 生成過程において、 proton とは違う構造の存在を示唆。

3. 3 ~ 4 GeV/c 領域において、 direct photon の v2 は 0 では無い。 -> ・・・ thermal photon ??

Page 8: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 8

7. summary and to do list7. summary and to do list

summary

to do

0, inclusive photon の v2 から、 direct photon の v2 を計算した。

5 GeV 以上の領域では、 direct photon の v2 は、 0 である。

3 GeV 付近の領域で、 direct photon の v2 が有限の値を持つ兆候が見えた。

direct photon の v2 についてより深く考察するために、計算法の工夫等により、結果の精度を向上させる。( ex. conversion method の活用等)

yield, RAA 等の解析と組み合わせた考察を行なう。

Page 9: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 9

Ex. Back upEx. Back up

Back up

Page 10: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 10

4-1. result 4-1. result ~ “subtracted” photon ~~ “subtracted” photon ~

…comment…

PHENIX preliminary PHENIX preliminary

PHENIX preliminary PHENIX preliminary

Page 11: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 11

5-1. Next step …5-1. Next step …

For the improvement of direct photon v2 …

  - Improvement of double ratio by more statistics or etc …    It is possible to expect to improvement in middle ~ high pT.

- To the improvement in low pT region, try to other methods. -> Ex. conversion method.

red : run 4blue : run 2

double ratio R direct photon v2

Page 12: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 12

5-2. Next step …5-2. Next step …

Thermal photon v2 will be measured by conversion method.

Page 13: 21 Sep 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 62th Annual Meeting RHIC-PHENIX 実験における高横運動量領域での

21/Sep/2006 Kentaro MIKI 13

Ex. result Ex. result ~ direct photon v~ direct photon v2 2 ~~

PHENIX preliminary PHENIX preliminary

PHENIX preliminary

PHENIX preliminary