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Heavy ion physics at LHCb Jiayin Sun (Tsinghua University) On behalf of the LHCb collaboration The 21 st Particles & Nuclei International Conference 1-5 September 2017, IHEP, Beijing, China 9/2/2017 PANIC2017 1 Outline LHCb detector


  1. Heavy ion physics at LHCb Jiayin Sun (Tsinghua University) On behalf of the LHCb collaboration The 21 st Particles & Nuclei International Conference 1-5 September 2017, IHEP, Beijing, China 9/2/2017 PANIC2017 1

  2. Outline โ€ข LHCb detector โ€ข ๐‘ž Pb collisions: recent results โ€ข Open heavy flavor results โ€ข Hidden heavy flavor results โ€ข PbPb collisions: work in progress โ€ข Fixed target: first results โ€ข Heavy flavor in ๐‘ž Ar โ€ข Antiproton in ๐‘ž He 9/2/2017 PANIC2017 2

  3. LHCb detector โ€ข A single arm forward spectrometer designed for the study of particles containing c or b quark. โ€ข Acceptance: 2 < ๐œƒ < 5 โ€ข Vertex detector โ€ข IP resolution ~ 20 m m โ€ข Tracking system โˆ†๐‘ž โ€ข ๐‘ž = 0.5% โˆ’ 1% (5-200 GeV/ c ) โ€ข RICH โ€ข K/ p /p separation โ€ข Electromagnetic + hadronic Calorimeters โ€ข Muon systems JINST 3 (2008) S08005 9/2/2017 PANIC2017 3 IJMPA 30 (2015) 1530022

  4. ๐‘ž Pb datasets and recent results โ€ข Rapidity Coverage Forward โ€ข ๐‘ง โˆ— : rapidity in nucleon-nucleon cms โ€ข ๐‘ง ๐‘‘๐‘›๐‘ก = ยฑ0.465 ๐‘ž Pb โ€ข Forward: 1.5 < ๐‘ง โˆ— < 4.0 โ€ข Backward: โˆ’5.0 < ๐‘ง โˆ— < โˆ’2.5 p Pb โ€ข Common region: 2.5 < |๐‘ง โˆ— | < 4.0 โ€ข ๐‘ก ๐‘‚๐‘‚ = 5 TeV (2013) โ€ข ๐‘ž Pb ( 1.06 nb -1 ) + Pb ๐‘ž ( 0.52 nb -1 ) Backward โ€ข Open heavy flavor ๐ธ 0 and ฮ› ๐‘‘ + Pb ๐‘ž โ€ข Collectivity โ€ข ๐‘ก ๐‘‚๐‘‚ = 8 TeV (2016) p Pb โ€ข ๐‘ž Pb ( 13.6 nb -1 ) + Pb ๐‘ž ( 21.8 nb -1 ) โ€ข Hidden heavy flavor ฮค ๐พ ๐œ” 9/2/2017 PANIC2017 4

  5. Prompt ๐ธ 0 measurement in ๐‘ž Pb at 5TeV PV ๐ฟ โˆ’ ๐‰๐ Forward ๏‚ฏ Backward ๏‚ฏ ๐ธ 0 ๐œŒ + โ€ข Reconstructed through decay channel: ๐ธ 0 โ†’ ๐ฟ โˆ’ ๐œŒ + โ€ข Inclusive ๐ธ 0 mesons from fitting invariant mass dist.: โ€ข Signal: Crystal Ball โ€ข Background: linear โ€ข Prompt ๐ธ 0 fraction extracted from fitting impact parameter dist.: โ€ข Prompt: simulation โ€ข ๐ธ 0 -from- b : simulation โ€ข Background: sideband in data arXiv:1707.02750 9/2/2017 PANIC2017 5

  6. + measurement in ๐‘ž Pb at 5TeV Prompt ฮ› ๐‘‘ PV ๐ฟ โˆ’ ๐‰๐ Forward ๏‚ฏ Backward ๏‚ฏ + ฮ› ๐‘‘ ๐œŒ + ๐‘ž โ€ข Reconstructed through decay channel + โ†’ ๐‘ž๐ฟ โˆ’ ๐œŒ + ฮ› ๐‘‘ + baryons from โ€ข Inclusive ฮ› ๐‘‘ fitting invariant mass dist.: โ€ข Signal: Gaussian โ€ข Background: linear + fraction โ€ข Prompt ฮ› ๐‘‘ extracted from fitting impact parameter dist.: โ€ข Prompt: simulation โ€ข ฮ› ๐‘‘ + -from- b : simulation โ€ข Background: sideband in data LHCb-CONF-2017-005 9/2/2017 PANIC2017 6

  7. Prompt ๐ธ 0 at 5TeV JHEP 10 (2003) 046 Eur. Phys. J. C77 (2017) 1, nuclear modification factor in ๐‘ž Pb Comput. Phys. Commun. 184 (2013) 2562 Comput. Phys. Commun. 198 (2016) 238 ๐œ ๐‘žPb (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) ๐‘† ๐‘žPb ๐‘ง โˆ— , ๐‘ž ๐‘ˆ = 1 ๐ต ร— ๐œ ๐‘ž๐‘ž (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) , A= 208 Updated since preliminary result: Directly measured with prompt ๐ธ 0 in ๐‘ž๐‘ž at ๐‘ก = 5 TeV arXiv:1610.02230 โ€ข Nuclear modification factor smaller at large rapidity โ€ข Measurements consistent with theoretical calculations arXiv:1707.02750 9/2/2017 PANIC2017 7

  8. Prompt ๐ธ 0 at 5TeV forward-backward production ratio ๐‘’๐œ(+ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ = ๐‘’๐œ(โˆ’ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ does not need results from ๐‘ž๐‘ž collisions. โ€ข Compared to next-to-leading order NLO calculations with different nPDFs โ€ข Consistent with theoretical calculations within uncertainty arXiv:1707.02750 Comput. Phys. Commun. 184 (2013) 2562 Eur. Phys. J. C77 (2017) 1, Comput. Phys. Commun. 198 (2016) 238 9/2/2017 PANIC2017 8

  9. + at 5TeV Prompt ฮ› ๐‘‘ LHCb-CONF-2017-005 forward-backward production ratio ๐‘’๐œ(+ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ = ๐‘’๐œ(โˆ’ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ does not need results from ๐‘ž๐‘ž collisions. โ€ข Compared to next-to-leading order NLO calculations with different nPDFs โ€ข Consistent with theoretical calculations within uncertainty Comput. Phys. Commun. 184 (2013) 2562 Eur. Phys. J. C77 (2017) 1, Comput. Phys. Commun. 198 (2016) 238 9/2/2017 PANIC2017 9

  10. Charmed baryon/meson production ratio ๐‘† + ๐ธ 0 at 5TeV ฮค ฮ› ๐‘‘ LHCb-CONF-2017-005 + (๐‘ง โˆ— ,๐‘ž ๐‘ˆ ) ๐œ ฮ› ๐‘‘ โ€ข ๐‘† + ๐ธ 0 = ฮ› ๐‘‘ ฮค ๐œ ๐ธ0 (๐‘ง โˆ— ,๐‘ž ๐‘ˆ ) โ€ข EPS09LO & EPS09NLO Forward gives similar predictions. โ€ข nCTEQ15 slightly lower. โ€ข Forward: โ€ข Consistent at lower ๐‘ž T โ€ข Below theory at higher ๐‘ž T โ€ข Backward: Eur. Phys. J. C77 (2017) 1, Comput. Phys. Commun. 184 Backward โ€ข Consistent for all ๐‘ž T (2013) 2562 Comput. Phys. Commun. 198 (2016) 238 9/2/2017 PANIC2017 10

  11. Charmed baryon/meson production ratio ๐‘† + ๐ธ 0 at 5TeV LHCb-CONF-2017-005 ฮค ฮ› ๐‘‘ + (๐‘ง โˆ— ,๐‘ž ๐‘ˆ ) ๐œ ฮ› ๐‘‘ โ€ข ๐‘† + ๐ธ 0 = ฮ› ๐‘‘ ฮค ๐œ ๐ธ0 (๐‘ง โˆ— ,๐‘ž ๐‘ˆ ) โ€ข EPS09LO & EPS09NLO gives similar predictions. โ€ข nCTEQ15 slightly lower. โ€ข Forward: โ€ข Consistent for all |๐‘ง โˆ— | โ€ข Backward: โ€ข Consistent at lower |๐‘ง โˆ— | โ€ข Displays a rising trend Eur. Phys. J. C77 (2017) 1, with increasing |๐‘ง โˆ— | Comput. Phys. Commun. 184 (2013) 2562 Comput. Phys. Commun. 198 (2016) 238 9/2/2017 PANIC2017 11

  12. Prompt and nonprompt ฮค ๐พ ๐œ” in p Pb at 8TeV โ€ข Reconstructed through arXiv:1706.07122 ๐พ ๐œ” โ†’ ๐œˆ + ๐œˆ โˆ’ ฮค โ€ข Signal extraction with 2D simultaneous fit to mass and the pseudo proper decay time ๐‘ข ๐‘จ โ‰ก ๐‘จ ฮค ๐พ ๐œ” โˆ’ ๐‘จ ๐‘„๐‘Š ร— ๐‘ ฮค ๐พ ๐œ” ๐‘ž ๐‘จ โ€ข Prompt and nonprompt (from- b - hadrons) separated โ€ข Fraction from b hadrons: โ€ข Increasing trend โ€ข Low ๐‘ž T : cold nuclear matter effects different for the prompt and nonprompt 9/2/2017 PANIC2017 12

  13. Prompt ฮค ๐พ ๐œ” at 8TeV nuclear modification factor in ๐‘ž Pb ๐œ ๐‘žPb (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) ๐‘† ๐‘žPb ๐‘ง โˆ— , ๐‘ž ๐‘ˆ = 1 ๐ต ร— ๐œ ๐‘ž๐‘ž (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) , A= 208 โ€ข pp reference: interpolation of LHCb measurements at 7, 8 and 13TeV โ€ข Forward rapidity: suppression up to 50% at low ๐‘ž T , decreasing with increasing ๐‘ž T โ€ข Backward rapidity: closer to unity โ€ข Overall agreement with models with large uncertainties on the gluon PDFs at low x โ€ข Compatible with 5TeV results arXiv:1706.07122 9/2/2017 PANIC2017 13

  14. ฮค ๐พ ๐œ” -from- b -hadrons at 8TeV nuclear modification factor in ๐‘ž Pb ๐œ ๐‘žPb (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) ๐‘† ๐‘žPb ๐‘ง โˆ— , ๐‘ž ๐‘ˆ = 1 ๐ต ร— ๐œ ๐‘ž๐‘ž (๐‘ง โˆ— ,๐‘ž ๐‘ˆ , ๐‘ก ๐‘‚๐‘‚ ) , A= 208 โ€ข pp reference: interpolation of LHCb measurements at 7, 8 and 13TeV โ€ข Forward rapidity: smaller suppression up to 30% at low ๐‘ž T , reach unity at higher ๐‘ž T โ€ข Backward: compatible with unity โ€ข FONLL with EPS09NLO consistent with data JHEP 04 (2009) 065 arXiv:1706.07122 โ€ข Compatible with 5TeV results 9/2/2017 PANIC2017 14

  15. Prompt ฮค ๐พ ๐œ” at 8TeV forward-backward production ratio arXiv:1706.07122 ๐‘’๐œ(+ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ = ๐‘’๐œ(โˆ’ ๐‘ง โˆ— ,๐‘ž ๐‘ˆ )/๐‘’๐‘ฆ โ€ข ๐‘† ๐บ๐ถ does not need results from ๐‘ž๐‘ž collisions. โ€ข Prompt ฮค ๐พ ๐œ” : โ€ข Clear forward-backward asymmetry โ€ข Increasing trend with increasing ๐‘ž T โ€ข Nonprompt ฮค ๐พ ๐œ” : โ€ข Closer to unity โ€ข Models for prompt ฮค ๐พ ๐œ” only โ€ข Consistent with 5TeV results 9/2/2017 PANIC2017 15

  16. PbPb collisions โ€ข December 2015: first LHCb PbPb data taken ๐‘ก ๐‘‚๐‘‚ = 5 TeV (3-5 m b -1 ) โ€ข โ€ข Event classification: total energy in the calorimeters (Ecal) โ€ข Analyses limited by saturation in Vertex Locator (VELO) โ€ข Track reconstruction: 50-100% event activity (~15k clusters) Activity 50-70% ๐พ ๐œ” โ†’ ๐œˆ + ๐œˆ โˆ’ ฮค ๐ธ 0 โ†’ ๐ฟ โˆ’ ๐œŒ + 9/2/2017 PANIC2017 16 https://twiki.cern.ch/twiki/bin/view/LHCb/LHCbPlots2015

  17. Fixed target physics โ€ข LHCb: only experiment at the LHC can operate in fixed-target mode โ€ข SMOG: The System for Measuring Overlap with Gas โ€ข Unique feature โ€ข noble gas (He, Ne, Ar โ€ฆ) injection inside the LHC beam close to the interaction point โ€ข Luminosity measurement โ€ข Internal gas target โ€ข Allows p -gas and ion-gas collisions โ€ข ๐‘ก ๐‘‚๐‘‚ region between 20 GeV (SPS) and 200 GeV (RHIC) โ€ข Access nPDF anti-shadowing region and intrinsic charm content in the nucleon 9/2/2017 PANIC2017 17

  18. Charm production in ๐‘žAr collisions LHCb-CONF-2017-001 โ€ข Dataset: JHEP (2013) 2013:122 JHEP (2013) 2013: 155 โ€ข ๐‘ก ๐‘‚๐‘‚ = 1 10 GeV (2015) โ€ข 6.5 TeV proton beam on Ar gas target โ€ข Protons on target: 4 ร— 10 22 ๐พ ๐œ” and ~6500 ๐ธ 0 โ€ข ~500 ฮค โ€ข Shapes consistent with PYTHIA and interpolation between HERA-B and PHENIX ฮค ๐พ ๐œ” ฮค ฮค ๐พ ๐œ” ๐พ ๐œ” ๐ธ 0 ๐ธ 0 ๐ธ 0 9/2/2017 PANIC2017 18

  19. Charm production in ๐‘žAr collisions LHCb-CONF-2017-001 โ€ข ๐พ ๐œ” ๐ธ 0 cross section ratio ฮค ฮค โ€ข Luminosity cancels โ€ข Increase with ๐‘ž T โ€ข Little dependence on rapidity โ€ข Demonstrate the feasibility of a heavyโˆ’flavorโˆ’fixedโˆ’target program at LHCb โ€ข Theoretical calculations are welcome 9/2/2017 PANIC2017 19

  20. าง ๐‘ž production in ๐‘žHe collisions Measurement of าง LHCb-CONF-2017-002 โ€ข AMS-2: possible anti-proton excess at high energies โ€ข ๐‘ž/๐‘ž ratio predictions limited by ๐‘ž production cross- uncertainties on าง sections, particularly for p -He โ€ข Prompt production at ๐‘ก ๐‘‚๐‘‚ = 1 10 GeV in ๐‘ž He collisions โ€ข EPOS LHC prediction: โ€ข Data/MC ~ 1.19 ยฑ 0.08 9/2/2017 PANIC2017 20

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