Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva...

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Vector meson photo- production at RHIC using \/s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA 10 th October 2014 1 For the STAR collaboration L. Chanaka De Silva, Creighton University Fourth Joint Meeting of the Nuclear Physics Divisions of the American Physical Society and The Physical Society of Japan Hawaii, USA, 7 -11 October 2014

Transcript of Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva...

Page 1: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

Vector meson photo-production at RHIC

using \/sNN = 200 GeV Au+Au collisions

L. Chanaka De Silva Hawaii 2014, Hawaii, USA 10th October 2014 1

For the STAR collaboration

L. Chanaka De Silva, Creighton University

Fourth Joint Meeting of the Nuclear Physics Divisions of the

American Physical Society and The Physical Society of JapanHawaii, USA, 7 -11 October 2014

Page 2: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

10th October 2014

• Ultra peripheral collisions

• STAR UPC trigger

• STAR Highlights

• Future directions

• Offline analyses cuts

• Data and comparison to theory

• Summary and outlook

2L. Chanaka De Silva Hawaii 2014, Hawaii, USA

Page 3: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

10th October 2014

• High energy photonuclear reaction

• Impact parameter (b) is larger than the sum of radii of participating nuclei

• Nuclei interact via strong electromagnetic fields– EM field can be viewed as a flux of quasi-real photons

– Photon flux is proportional to Z2

– Photon flux is well described in Fermi-Weizsäcker-Williams approximation

– Hadronic processes are strongly suppressed

– Maximum CM photon energy at RHIC ~ γh/RA ~ 3GeV

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Ultra Peripheral Collision (UPC)

Physics motivations• To study non linear effects at low-x in the gluon

distribution of the target

• To measure nuclear gluon shadowing and saturation (via vector meson photo-production)

• To study partonic form factors

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

Page 4: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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STAR - Solenoidal Tracker At RHIC• Large acceptance; TPC: -1 < η < 1 and –π < ϕ < π

• Excellent PID; ToF and TPC dE/dx

STAR UPC Trigger• 1≤ beam neutrons ≤ 6 in both ZDCs

• veto on small BBC tiles 3 < |η| < 5

• 2 ≤ TOF hits ≤ 6

• Low multiplicityL. Chanaka De Silva Hawaii 2014, Hawaii, USA

Alex Schmah Y. Gorbunov

Page 5: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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• ρ0 photo-production in AuAu collisions at \/sNN = 64 GeV with the STAR detector

- Phys. Rev. C 85 (2012) 14910

• Observation of π+π-π+π- photo-production in ultra peripheral heavy-ion collisions at \/sNN = 200 GeV at the STAR detector

- Phys. Rev. C 81 (2010) 44901

• Observation of two-Source Interference in the photo-production reaction AuAu -> AuAuρ0

- Phys. Rev. Lett. 102 (2009) 112301

• ρ0 photo-production in ultra-peripheral

relativistic heavy ion collisions at \/sNN = 200 GeV with STAR

- Phys. Rev. C 77 (2008) 34910

• Production of e+e− pairs accompanied by nuclear dissociation in ultra peripheral heavy-ion collisions

- Phys. Rev. C 70 (2004) 031902(R)

• Coherent ρ0 production in ultra peripheral heavy-Ion collisions

- Phys. Rev. Lett. 89 (2002) 272302

STAR publications

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

First π spectra from two different triggers, 2002 e+e- pair rapidity compared to theory, 2004

ρ0 production cross section, 2008 Resonant ρ0 production, 2008

ρ0 production differential cross section, 2008

π+π-π+π- photonuclear production, 2010 Energy dependence of total ρ0 cross section, 2012

Page 6: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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ρ0 photo-production with higher statistics 2010 AuAu 200 GeV data

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

J/ψ photo-production using 2010 AuAu 200 GeVdata• To study non linear effects at low-x in the gluon

distribution of the target

• To measure nuclear gluon shadowing and saturation (via vector meson photo-production)

• Cross section for mid rapidity J/ψ production can provide insight in to nuclear gluon distribution dσ/dy ~ [g(x,Q2)2]

• We focus on observing the diffractive pattern with higher statistics, and also repeat measurements we had in earlier publications• Study of Au partonic form factor via Fourier transform of d2σ/dtdy• Diffraction pattern detail helps constraining dipole cross section models

GA (x,Q2)∝g(x,Q2)

x=MV

SNNe±y

dt∝Fg

2 (x, t)

Page 7: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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• 37 Million 200 GeV Au+Au UPC trigger events ( )• XnXn; Multiple neutron emissions from either nuclei • Z-vertex position; [-100, 100]cm• Fewer than 10 total tracks per event• An event vertex has two tracks associated to it (exclusive

production)• Mass cuts

• ρ: 0.4<Minv<1.1 GeV/c2

• J/ψ: 2.5<Minv<3.5 GeV/c2

• Background modeled with like-sign pairs, scaled to match data for pT > 0.2 GeV/c

• yDistribution– coherent cut; pT < 0.15 GeV/c

– 0.05 < |y| < 1.0 (Lower limit for cosmic rays/upper limit for STAR acceptance)

L=1.16 nb -1∫

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

Page 8: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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• Blue: unlike-sign pairs

• Red: background estimated with like-sign pairs

• The peaks at low transverse momenta is consistent with coherent production

• For analysis, only events with pT < 0.15 GeV/c are used

• Only statistical error bars are presented

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

2010 AuAu 200 GeV dataOnly acceptance corrected

ρ -> π+π- J/ψ -> e+e-

Page 9: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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• ρ mass is fit with a cocktail that includes a Söding term for interference with direct π pair production

• J/Ψ is fit with exponential for e+e- continuum, Gaussian for J/ψ signal and polynomial for background

• Approximately 0.65M ρ mesons are reconstructed

• Approximately 125 J/ψ mesons are reconstructed

• Only statistical error bars are presented

ρ J/ψ 2010 AuAu 200 GeV data

Pure ρ0

Direct ππ

Interference

Polynomial Background

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• After preliminary acceptance corrections

• Dip at y ~ 0 is from the cut to remove cosmic rays

• Trigger/Vertex and tracking efficiency studies are still in-progress

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

2010 AuAu 200 GeV dataρ -> π+π- J/ψ -> e+e-

Page 11: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

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• Blue: acceptance-corrected data

• Red: Klein-Nystrand model with mutual Coulomb dissociation

- S.R. Klein, J. Nystrand, Phys. Rev. C 60 (1999) 014903

• Black: Color dipole model, where the dipole nucleon cross section is from the IIM saturation model

- Gonçalves, Machado, Phys. Rev. C 84 (2011) 011902

2010 AuAu 200 GeV data

• Vector meson ratio gives an additional constraint on different photo-production mechanisms. E.g.: LO pQCD models, color dipole models and Glauber models

Color dipole model

STAR pre

limin

ary

Page 12: Vector meson photo-production at RHIC using \ /s NN = 200 GeV Au+Au collisions L. Chanaka De Silva Hawaii 2014, Hawaii, USA10 th October 2014 1 For the.

• Study of Au partonic form factor via Fourier transform of d2σ/dtdy- t-Distribution is predominantly due to the transverse spread of gluons in the nucleon /

nuclear density profile

• By applying a Fourier transformation on preliminary data, our result for Au radius is consistent with 6.38 fm

• Diffraction pattern detail helps constraining dipole cross section models

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ρ

dt∝Fg

2 (x, t)

*

*H. DeVries, C.W. De Jager, C. DeVries, ATOMIC DATA AND NUCLEAR DATA TABLES 36,495536 (1987)

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• STAR has pioneered in UPCs by carrying out broad range of measurements at different center of mass energies

• We have analyzed 37 million UPC trigger events from 2010 Au+Au 200 GeV data set ( )

• After applying offline analyses cuts, STAR observes ~0.65M ρ and 125 J/ψ vector mesons

• We measured and compared the Jψ/ρ vector meson ratio to theory predictions

• Preliminary ratio (~0.0028) is somewhat higher than predicted by both Klein-Nystrand and Gonçalves-Machado models

• STAR result on radius of Au nuclei is consistent with 6.38fm

• Final trigger/vertex efficiency and systematic studies are in progress

• Future: Preparing for the p+A run in 2015 with the inclusion of Roman pots

L. Chanaka De Silva Hawaii 2014, Hawaii, USA

L=1.16 nb -1∫