STAR Collaboration Meeting, MIT, July 2006 1 Interference in Coherent Vector Meson Production in UPC Au+Au Collisions at √s = 200GeV Brooke Haag UC Davis.

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Presentation transcript:

STAR Collaboration Meeting, MIT, July Interference in Coherent Vector Meson Production in UPC Au+Au Collisions at √s = 200GeV Brooke Haag UC Davis

STAR Collaboration Meeting, MIT, July Outline Ultra Peripheral Heavy Ion Collisions (UPCs) What is a UPC? Vector Meson Production / Interference STAR detectors / Triggers Analysis of UPC events Fitting Scheme Observation of interference effects in t spectrum Systematic Errors and Outlook

STAR Collaboration Meeting, MIT, July Ultra Peripheral Collisions What is a UPC? Photonuclear interaction Two nuclei “miss” each other (b > 2R A ), electromagnetic interaction dominates over strong interaction Photon flux ~ Z 2 Weizsacker-Williams Equivalent Photon Approximation No hadronic interactions.. Au

STAR Collaboration Meeting, MIT, July Exclusive  o Production Photon emitted by a nucleus fluctuates to virtual qq pair Virtual qq pair elastically scatters from other nucleus Real vector meson (i.e. J/ ,  o ) emerges Photon and pomeron are emitted coherently Coherence condition limits transverse momentum of produced  Courtesy of F. Meissner Au+Au  Au+Au+  o

STAR Collaboration Meeting, MIT, July  o Production With Coulomb Excitation Au+Au  Au*+Au*+  o Au  P Au* ( 2+  ) 00 Courtesy of S. Klein Coulomb Excitation Photons exchanged between ions give rise to excitation and subsequent neutron emission Process is independent of  o production

STAR Collaboration Meeting, MIT, July Courtesy of S. Klein Nucleus 1 emits photon which scatters from Nucleus 2 Nucleus 2 emits photon which scatters from Nucleus 1 -Or- Interference Amplitude for observing vector meson at a distant point is the convolution of two plane waves: Cross section comes from square of amplitude: We can simplify the expression if y  0:

STAR Collaboration Meeting, MIT, July Central Trigger Barrel Time Projection Chamber STAR Analysis Detectors Zero Degree Calorimeter Zero Degree Calorimeter

STAR Collaboration Meeting, MIT, July UPC Topology Central Trigger Barrel divided into four quadrants Verification of  decay candidate with hits in North/South quadrants Cosmic Ray Background vetoed in Top/Bottom quadrants Au+Au  Au+Au+  o Triggers UPC Minbias Minimum one neutron in each Zero Degree Calorimeter required Low Multiplicity Not Hadronic Minbias! Trigger Backgrounds Cosmic Rays Beam-Gas interactions Peripheral hadronic interactions Incoherent photonuclear interactions Au+Au  Au*+Au*+  o

STAR Collaboration Meeting, MIT, July Studying the Interference Determine   candidates by applying cuts to the data qTot0 nTot2 nPrim2 |zVertex|< 50 cm |rVertex|< 8 cm rapidity> 0.1 < 0.5 M Inv > 0.55 GeV < 0.92 GeV pTpT > 0 GeV < 0.1 GeV

STAR Collaboration Meeting, MIT, July Studying the Interference Generate similar MC histograms

STAR Collaboration Meeting, MIT, July Studying the Interference Generate MC ratio Fit MC ratio

STAR Collaboration Meeting, MIT, July Measuring the Interference Apply overall fit c = 1 expected degree of interference c = 0 no interference C = 1.034±0.131 A= overall normalization k = exponential slope c = degree of interference C = 0 C = 1.034±0.131

STAR Collaboration Meeting, MIT, July Results Topology C = ±  2 /DOF = 87.92/47 Minbias C = 1.009±0.081  2 /DOF = 50.77/47 Au+Au  Au*+Au*+  o Au+Au  Au+Au+  o

STAR Collaboration Meeting, MIT, July Results Summary c  2 /dof Minbias 0.1 < y < ± / < y <  /47 Topology 0.1 < y < ± / < y <  /47

STAR Collaboration Meeting, MIT, July Interference routine for minbias 0 > y > 0.5 flat ratio ~10% statistics

STAR Collaboration Meeting, MIT, July Systematic Error Study Standard CutVaried CutData Set EntriesUncertainty zVertex|zVertex| < < y < 0.5 zVertex > 0minbias topology |zVertex| < < y < 1.0 zVertex > 0minbias topology |zVertex| < < y < 0.5 zVertex < 0minbias topology |zVertex| < < y < 1.0 zVertex < 0minbias topology rapidity0.1 < y < 0.50 < y < 0.5minbias

STAR Collaboration Meeting, MIT, July Systematic Error Study FitData Set Uncertainty 6 parameterminbias % topology % The 5 parameter fit is sufficient -- adding another parameter doesn’t improve the analysis.

STAR Collaboration Meeting, MIT, July Paper Proposal