Non-photonic electron production in p+p collisions at √s=200 GeV Xiaozhi Bai for the STAR collaboration Central China Normal University University of Illinois.

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Presentation transcript:

Non-photonic electron production in p+p collisions at √s=200 GeV Xiaozhi Bai for the STAR collaboration Central China Normal University University of Illinois at Chicago APS April Meeting 2015,Baltimore,MD

4/11/15Xiaozhi (CCNU&UIC)2 Outline Motivation Data Analysis for Non-photonic electron (NPE) NPE spectrum Summary and outlook

4/11/15Xiaozhi (CCNU&UIC)3 Motivation Heavy flavor particles:  Large mass, produced dominantly by hard scatterings in the early stage  Excellent probe for the Quark-Gluon Plasma (QGP) Heavy flavor production in p+p collisions  Baseline for studies in heavy ion collisions, e.g. R AA  Test the validity and constrain the parameters of pQCD calculations of heavy quark production Non-photonic electrons  Produced from semi-leptonic decays of open heavy flavor hadrons  A good proxy to study open heavy flavor production

4/11/15Xiaozhi (CCNU&UIC)4 STAR Detector Time Projection Chamber (TPC) large acceptance: |η|<~1.3, 0<Φ<2π tracking, momentum electron ID through energy loss dE/dx Barrel Electromagnetic Calorimeter (BEMC) large acceptance: |η|<1, 0<Φ<2π electron ID through E/p and shower shape triggering on high p T (2.5 GeV/c<p T ) electron Time Of Flight (TOF) large acceptance: |η|<0.9, 0<Φ<2π electron ID through flight time at low p T (p T <2.5 GeV/c)

4/11/15Xiaozhi (CCNU&UIC)5 STAR Detector e,μ π k p d Time Projection Chamber (TPC) large acceptance: |η|<~1.3, 0<Φ<2π tracking, momentum electron ID through energy loss dE/dx Barrel Electromagnetic Calorimeter (BEMC) large acceptance: |η|<1, 0<Φ<2π electron ID through E/p and shower shape triggering on high p T (2.5 GeV/c<p T ) electron Time Of Flight (TOF) large acceptance: |η|<0.9, 0<Φ<2π electron ID through flight time at low p T (p T <2.5 GeV/c) Au+Au 200 GeV

4/11/15Xiaozhi (CCNU&UIC)6 STAR Detector Time Projection Chamber (TPC) large acceptance: |η|<~1.3, 0<Φ<2π tracking, momentum electron ID through energy loss dE/dx Barrel Electromagnetic Calorimeter (BEMC) large acceptance: |η|<1, 0<Φ<2π electron ID through E/p and shower shape triggering on high p T (2.5 GeV/c<p T ) electron Time Of Flight (TOF) large acceptance: |η|<0.9, 0<Φ<2π electron ID through flight time at low p T (p T <2.5 GeV/c)

4/11/15Xiaozhi (CCNU&UIC)7 STAR Detector e,μ π k p Time Projection Chamber (TPC) large acceptance: |η|<~1.3, 0<Φ<2π tracking, momentum electron ID through energy loss dE/dx Barrel Electromagnetic Calorimeter (BEMC) large acceptance: |η|<1, 0<Φ<2π electron ID through E/p and shower shape triggering on high p T (2.5 GeV/c<p T ) electron Time Of Flight (TOF) large acceptance: |η|<0.9, 0<Φ<2π electron ID through flight time at low p T (p T <2.5 GeV/c) Au+Au 200 GeV

4/11/15Xiaozhi (CCNU&UIC)8 Dataset and electron selection Fast detector BEMC select (or trigger on) interesting events High tower trigger event: an event with an energy deposition in a single tower of the BEMC above a certain threshold Data samples in p+p collisions at √s = 200 GeV from Run 2012

4/11/15Xiaozhi (CCNU&UIC)9 Analysis procedure Inclusive electron Non-photonic electron(from open heavy flavor decay ) bottom and charm hadrons via semi-leptonic decay. PHE  Gamma conversion (~54%)  π 0 Dalitz Decay (~36%)  η Dalitz Decay (~10%) After all the ePID cuts: Hadron contamination All ePID cuts and Invariant mass cuts Not 100% reconstructed The NPE invariant cross section: : electrons from open heavy flavor decay purity: purity of inclusive electron ε photonic : photonic electron reconstruction efficiency

4/11/15Xiaozhi (CCNU&UIC)10 Inclusive electron and photonic electron STAR 2012 p+p √s=200 GeV STAR Preliminary STAR 2012 p+p √s=200 GeV STAR Preliminary STAR 2012 p+p √s=200 GeV STAR Preliminary STAR 2012 p+p √s=200 GeV STAR Preliminary STAR 2012 p+p √s=200 GeV -1<nσ e <3

4/11/15Xiaozhi (CCNU&UIC)11 Raw spectra and detector efficiency STAR 2012 p+p √s=200 GeV ε dEdx TPC ePID cut efficiency from data ε EMC EMC ePID cut efficiency from data ε Trg High tower trigger efficiency from MC simulation ε Trk TPC tracking efficiency from MC simulation

4/11/15Xiaozhi (CCNU&UIC)12 NPE cross section Consistent with pQCD FONLL calculation and previous STAR results. This analysis has better precision and extended to a higher p T range STAR Preliminary [1] STAR collaboration, Phys. Rev. D 83 (2011) [2] R.E.Nelson, R.Vogt, and A.D.Frawley, Phys.Rev.C 87 (2013)

4/11/15Xiaozhi (CCNU&UIC)13 Summary and outlook A new and improved NPE cross section measurement in p+p collisions at √s=200 GeV at STAR. Results consistent with pQCD FONLL calculation and previous STAR results. The data analysis is ongoing to measure the NPE cross section for p T <2.5 GeV/c, using 700M MinBias events collected during year 2012 run. NPE invariant yield will be used as the baseline reference for the Nuclear modification factor R AA in Au+Au collisions.

4/11/15Xiaozhi (CCNU&UIC)14 Detector upgrade: Heavy Flavor Tracker High precision R AA and v 2 of Non- photonic electron from charm and bottom hadrons decay separately IST at 14cm PXL at 2.9 and 8cm SSD at 22 cm Simulation with HFT