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Maki Kurosawa for the PHENIX Collaboration RIKEN Nishina Center 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 1 Recent Open Heavy Flavor Results from.

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Presentation on theme: "Maki Kurosawa for the PHENIX Collaboration RIKEN Nishina Center 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 1 Recent Open Heavy Flavor Results from."— Presentation transcript:

1 Maki Kurosawa for the PHENIX Collaboration RIKEN Nishina Center 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 1 Recent Open Heavy Flavor Results from PHENIX

2 Why Open Heavy Flavor  Heavy flavors are primarily produced via gluon fusion in initial stage of the collision  Travel through the created medium.  Almost no interaction with hadronic phase.  No breakup effects like quarkonium productions.  Mass-dependence of cold/hot nuclear matter (CNM/HNM) effects. Heavy ion collisions are mixed of both effects.  CNM effects  Cronin effects  Gluon shadowing/anti-shadowing effects  Initial state energy loss prior the formation of hot matter  Gluon saturation (CGC)  HNM effects  Radiative energy loss  Collisional energy loss  Recombination of quarks  Dissociation and fragmentation of heavy-flavor mesons 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 2 Good probe

3 Use Various System Size 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 3 Use various system size to study CNM/HNM effects p+p collisions Baseline for heavy ion collisions p+A collisions By reducing system size, no sizable volume of hot matter  CNM effects Heavy ion collisions (A+A) Formed hot matter  CNM + HNM effects d + Au (CNM) 3 < N coll < 15 Cu + Cu (transition region between dominance of CNM and HNM 5 < N coll < 180 Au + Au (HNM dominance) 15 < N coll < 1000

4 Use Various Rapidity Range  Variation of rapidity and energy probe different kinematic regions inside the nucleus  e.g.  Probe CNM effects (shadowing) in p + A collisions 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 4 forward midbackward Au d backward midforward

5 Open Heavy Flavor Results from PHENIX  d + Au collisions (200GeV)  Modification factor, R dAu, of heavy flavor   Forward/Backward rapidity  Cu + Cu collisions (200GeV)  Modification factor, R CuCu, of heavy flavor e  Mid-rapidity  Au + Au collisions (62.4GeV)  Elliptic flow of heavy flavor e and R AuAu  Mid-rapidity 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 5 Transition region between dominance of CNM and HNM effects CNM effects Energy dependence of CNM and HNM effects

6 Heavy Flavor   at forward and backward rapidity in d+Au (200GeV) 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 6 d Backward Forward Au d Negative muons are used. S/N is better than positive muons  - : 1 < p T < 6 GeV/c, 1.4 < |  | < 2.0 anti-shadowing shadowing Backward -2.0 < |  | < -1.4 Forward 1.4 < |  | < 2.0 CNM : shadowing anti-shadowing

7 Modification factor for   at forward and backward rapidity 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 7 Peripheral collisions : No significant modifications in forward and backward rapidity. Central collisions : Suppression at forward rapidity Enhancement at backward rapidity EPS09s nPDF based calculation doesn’t reproduce data at backward rapidity. Modification factor, R dA Peripheral Central collision Require other CNM effects parton recombination in final state Enhance Suppress

8 Comparison with R dA of J/ 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 8 Compared with R dA of J/  Should be sensitive to the same effect on heavy- flavor productions J/  production has additional effect of breakup in nuclear matter Modification factor, R dA Comparison shows the breakup of J/  into heavy-meson pairs has a significant effect in quarkonium productions.

9 Heavy Flavor e at mid-rapidity in Cu+Cu (200GeV) 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 9 Cu + Cu system can be bridge between d + Au system and Au + Au system (CNM dominance region and HNM dominance region) R AA comparison between different systems Clear enhancement in d + Au Large suppression in Au + Au Cu + Cu system : intermediate R AA between that in d + Au and Au + Au

10 Comparison within different collision systems in similar 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 10 Similar enhancement and suppression are seen for the difference system at similar = 15 in d+Au = 15 in Cu+Cu = 7 in d+Au = 6 in Cu+Cu = 100 in Cu+Cu = 140 in Au+Au = 86 in Cu+Cu = 60 in Au+Au

11 vs in different Collision Systems 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 11 Cu + Cu system takes over from CNM dominant region to HNM dominant region

12 Comparison with R CuCu of  - for Forward Rapidity 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 12 No theoretical calculation to explain both data More suppression in  - yield Additional CNM effects like shadowing and initial state energy loss Theoretical calculation : partonic energy loss suppression due to fragmentation and dissociation of heavy-flavor hadrons shadowing effect Cronin effect

13 Modification Factor R AA of Heavy Flavor e at mid-rapidity in Au+Au (62.4GeV) 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 13 200 GeV d + Au and Au + Au Collisions 200 GeV 62.4 GeV in d + Au Collisions Minimum Bias Large suppression in 200 GeV Au + Au collisions In contrast to 200 GeV Au + Au data, show clear enhancement in 62.4 GeV Au + Au collisions Due to Less energy loss? Larger Cronin effects? or combination of those factors Used p + p data from ISR experiment R AA

14 Comparison with Theoretical Calculation 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 14 Theoretical calculation : partonic energy loss Dissociation of D and B mesons Model can describes 200 GeV suppression but it underpredicts 62.4 GeV data.

15 Elliptic Flow of Heavy Flavor e at mid- rapidity in Au+Au (62.4GeV) 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 15 Charm still has a positive v 2 in 62 GeV Au + Au. Collective motion of charm itself? Collective motion of charmed hadrons through recombination with flowing light partons? For further understanding, need more data in Au + Au and d + Au collisions at 62.4 GeV

16 c/b Separation with VTX/FVTX 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 16 FVTX VTX Cover wide rapidity range Nuclear modification : c/b separation with displaced vertex measurements Collective flow : Good resolution of reaction plane VTX/FVTX analysis is ongoing to publish

17 Run-14 200GeV Au + Au 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 17 Run14 ended. 2.6nb -1 were accumulated

18 Simulated Performance in Run-14 200GeV Au + Au 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 18 Run14 data will be the golden dataset for VTX/FVTX. Simulated performance of nuclear modification for VTX and FVTX

19 Improvement of Reaction Plane Resolution with VTX/FVTX 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 19 VTX and FVTX provides the highest reaction plane resolution Efficiency of VTX and FVTX are 85% and 95%, respectively.

20 Calibration of VTX in Run14 is ongoing 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 20 DCA (cm) counts Au primary vertex DCA D (B) e 1.0 < p T < 1.5 GeV/c  DCA = 82  m 2.0 < p T < 2.5 GeV/c  DCA = 74  m Alignment of VTX for Run14 is ongoing and almost done. DCA resolution with WEST barrel are 80  m at 1.0 < p T < 1.5 GeV/c 70  m at 2.0 < p T < 2.5 GeV/c Taebong Moon VTX DCA distribution in Run14

21 p T Dependence of DCA Resolution 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 21 Taebong Moon p T (GeV/c)  DCA (  m) ~ 70  m at 2 < p T

22 Summary  d + Au collisions (200GeV) Suppression at forward rapidity and enhancement at backward rapidity EPS09s nPDF based calculation doesn’t reproduce data at backward rapidity  Cu + Cu collisions (200GeV)  Cu + Cu system takes over from CNM dominant region to HNM dominant region  No theoretical calculation to explain both of mid and forward rapidity data.  Au + Au collisions (62.4GeV)  In contrast to 200 GeV Au + Au data, show clear enhancement in 62.4 GeV Au + Au collisions  Charm still has a positive v 2 in 62 GeV Au + Au  VTX/FVTX measure nuclear modification and collective flow of charm and bottom separately with displaced vertex (DCA) measurements.  Data analysis is ongoing  Run14 data will be the golden dataset for VTX/FVTX 5/11/2015RHIC/AGS User's Meeting Maki Kurosawa 22

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