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Southern Methodist University February 13-15, 2017 Introduction - PowerPoint PPT Presentation

Santa Fe Jets and Heavy Flavor Workshop Vector boson production in pPb and PbPb collisions at the LHC and its impact on nCTEQ15 PDFs arxiv: 1610.02925 Florian Lyonnet with A. Kusina, D.B. Clark, E. Godat, T. Jezo, K. Kovarik, F.I. Olness, I.


  1. Santa Fe Jets and Heavy Flavor Workshop Vector boson production in pPb and PbPb collisions at the LHC and its impact on nCTEQ15 PDFs arxiv: 1610.02925 Florian Lyonnet with A. Kusina, D.B. Clark, E. Godat, T. Jezo, K. Kovarik, F.I. Olness, I. Schienbein, J.Y. Yu Southern Methodist University February 13-15, 2017

  2. Introduction W/Z@LHC Reweighting Conclusion Methodology: Parametrization: ◮ e.g. xg p/A ( x, Q 2 ) = c 0 x c 1 (1 − x ) c 2 e c 3 x (1 + e c 4 x ) c 5 ◮ c k → c k, 0 + c k, 1 (1 − A − c k, 2 ) 3 10 NMC EMC Global fit to various SLAC BCDMS experimental data 2 10 Hermes FNAL E665 DY: FNAL ◮ DIS Q 2 [GeV 2 ] 1 10 ◮ DY ◮ Pion production 0 10 -1 10 -4 -3 -2 -1 0 10 10 10 10 10 x 10 − 2 ≤ x ≤ 0 . 7 Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 2 / 20

  3. Introduction W/Z@LHC Reweighting Conclusion Methodology: Parametrization: ◮ e.g. xg p/A ( x, Q 2 ) = c 0 x c 1 (1 − x ) c 2 e c 3 x (1 + e c 4 x ) c 5 ◮ c k → c k, 0 + c k, 1 (1 − A − c k, 2 ) 2.5 DIS DIS 8 π 0 DIS DIS DIS DY DIS DY DIS & & 2.0 DY DY 1.5 χ 2 / dof 1.0 47 28 28 12 2 9 7 32 14 26 33 3 111 14 11 28 27 21 3 0.5 3 14 3 2 14 32 7 0.0 Fe/D Fe/Be Fe/C He/D Li/D Be/D C/D N/D Al/D Ca/D Cu/D Kr/D Ag/D Sn/D Xe/D W/D Au/D Pb/D C/Li Ca/Li W/Be Be/C Al/C Ca/C Sn/C Pb/C DAu/pp Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 2 / 20

  4. Introduction W/Z@LHC Reweighting Conclusion Methodology: Parametrization: ◮ e.g. xg p/A ( x, Q 2 ) = c 0 x c 1 (1 − x ) c 2 e c 3 x (1 + e c 4 x ) c 5 ◮ c k → c k, 0 + c k, 1 (1 − A − c k, 2 ) nCTEQ15 A total of 740 points after kinematical cuts ◮ χ 2 = 587 . 4 ⇒ χ 2 /d.o.f = 0 . 81 Error analysis via the Hessian method ◮ 32 Eigenvalues Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 2 / 20

  5. Introduction W/Z@LHC Reweighting Conclusion 16 0.7 A=1 14 g s 0.6 A=4 A=9 12 A=12 0.5 A=27 10 A=40 0.4 xf p/A xf p/A A=56 8 A=84 0.3 A=119 6 A=131 0.2 A=197 4 A=208 0.1 2 0 0.0 -1 -1 10 -3 10 -2 10 1 10 -3 10 -2 10 1 x x 0.6 0.35 u v d v 0.30 0.5 0.25 0.4 0.20 xf p/A xf p/A 0.3 0.15 0.2 0.10 0.1 0.05 0.0 0.00 -3 -2 -1 -3 -2 -1 10 10 10 1 10 10 10 1 x x 0.9 0.9 0.8 u 0.8 d 0.7 0.7 0.6 0.6 xf p/A 0.5 xf p/A 0.5 0.4 0.4 0.3 0.3 0.2 0.2 0.1 0.1 0.0 0.0 -3 -2 10 -1 -3 -2 10 -1 10 10 1 10 10 1 x x 0.8 0.8 ¯ ¯ 0.7 u 0.7 d 0.6 0.6 0.5 0.5 xf p/A xf p/A 0.4 0.4 0.3 0.3 0.2 0.2 0.1 0.1 0.0 0.0 10 -3 10 -2 10 -1 1 10 -3 10 -2 10 -1 1 x x Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 3 / 20

  6. Introduction W/Z@LHC Reweighting Conclusion Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 4 / 20

  7. Introduction W/Z@LHC Reweighting Conclusion To go further: Include LHC data on pP b (and possibly P b P b ) collisions ◮ LHCb: σ ( Z → ℓ + ℓ − ) ◮ ALICE: σ ( W +( − ) → ℓ +( − ) ν (¯ ν )) ◮ ATLAS: dσ ( Z → ℓ + ℓ − ) /dy , dσ ( W +( − ) → ℓ +( − ) ν (¯ ν )) /dy, A ℓ ◮ CMS: dσ ( Z → ℓ + ℓ − ) /dy , dσ ( W +( − ) → ℓ +( − ) ν (¯ ν )) /dy, A ℓ , A FB √ s pp = 7 TeV ⇒ � s P b P b = 2 . 76 TeV √ s pp = 8 TeV ⇒ � s pP b = 5 . 02 TeV Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 5 / 20

  8. Introduction W/Z@LHC Reweighting Conclusion To go further: Include LHC data on pP b (and possibly P b P b ) collisions ◮ LHCb: σ ( Z → ℓ + ℓ − ) ◮ ALICE: σ ( W +( − ) → ℓ +( − ) ν (¯ ν )) ◮ ATLAS: dσ ( Z → ℓ + ℓ − ) /dy , dσ ( W +( − ) → ℓ +( − ) ν (¯ ν )) /dy, A ℓ ◮ CMS: dσ ( Z → ℓ + ℓ − ) /dy , dσ ( W +( − ) → ℓ +( − ) ν (¯ ν )) /dy, A ℓ , A FB √ s pp = 7 TeV ⇒ � s P b P b = 2 . 76 TeV √ s pp = 8 TeV ⇒ � s pP b = 5 . 02 TeV ⇒ Vector boson production in pP b and P b P b collisions at the LHC Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 5 / 20

  9. Introduction W/Z@LHC Reweighting Conclusion I) Introduction II) LHC pP b and P b P b data III) Impact on the nCTEQ15 fit - Reweighting Analysis IV) Conclusion Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 6 / 20

  10. Introduction W/Z@LHC Reweighting Conclusion Kinematics x 2 is the momentum fraction in the Lead nucleus p S 5 2 = . . 0 7 8 2 6 T T T e e e V V V 1 4 − = y 3 − 10 − 1 = y 2 − = y 1 − = 10 − 2 y x 2 0 = y 1 = y 10 − 3 Z W ± 2 = y Z 3 = W ± y Z 10 − 4 4 W ± = y 10 − 4 10 − 3 10 − 2 10 − 1 1 x 1 Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 7 / 20

  11. Introduction W/Z@LHC Reweighting Conclusion Kinematics x 2 is the momentum fraction in the Lead nucleus 4 ATLAS CMS LHCb ALICE 3 2 1 0 y 1 2 3 W ± Z A W A Z 4 ℓ FB A W FB 5 10 -4 10 -3 10 -2 10 -1 10 0 x 2 Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 7 / 20

  12. Introduction W/Z@LHC Reweighting Conclusion Kinematics x 2 is the momentum fraction in the Lead nucleus 4 ATLAS CMS LHCb ALICE 3 2 1 0 y 1 2 3 W ± Z A W A Z 4 ℓ FB A W FB 5 10 -4 10 -3 10 -2 10 -1 10 0 x 2 All predictions @NLO using custom FEWZ Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 7 / 20

  13. Introduction W/Z@LHC Reweighting Conclusion P b P b 0.7 0.6 0.5 0.4 dσ dy Z σ tot 0.3 1 0.2 p s =2 . 76 TeV CMS Z → µµ PbPb , 0.1 nCTEQ15 CT10 0.0 0.0 0.5 1.0 1.5 2.0 1.4 1.2 R 1.0 0.8 0.6 0.0 0.5 1.0 1.5 2.0 y Z CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 8 / 20

  14. Introduction W/Z@LHC Reweighting Conclusion P b P b 0.30 0.25 0.20 dy Z dσ σ tot 1 0.15 p s = 2 . 76 TeV 0.10 ATLAS Z PbPb nCTEQ15 CT10 0.05 3 2 1 0 1 2 3 1.4 1.2 R 1.0 0.8 0.6 3 2 1 0 1 2 3 y Z CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 8 / 20

  15. Introduction W/Z@LHC Reweighting Conclusion P b P b 0.4 0.3 0.2 0.1 A l 0.0 0.1 0.2 p s = 2 . 76 TeV ATLAS PbPb , W char . asym . 0.3 nCTEQ15 CT10 0.4 0.0 0.5 1.0 1.5 2.0 2.5 3 2 1 R 0 1 2 0.0 0.5 1.0 1.5 2.0 2.5 | y l | CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 8 / 20

  16. Introduction W/Z@LHC Reweighting Conclusion P b P b 0.4 0.3 0.2 0.1 A l 0.0 0.1 0.2 p s = 2 . 76 TeV CMS PbPb , W char . asym . 0.3 nCTEQ15 CT10 0.4 0.0 0.5 1.0 1.5 2.0 6 4 2 R 0 2 4 6 0.0 0.5 1.0 1.5 2.0 | y l | CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 8 / 20

  17. Introduction W/Z@LHC Reweighting Conclusion P b P b Comments Not really sensitive to nuclear corrections Uncertainties too large to bring constraints on nPDFs Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 8 / 20

  18. Introduction W/Z@LHC Reweighting Conclusion pP b : Z 35 30 dσ ( Z → ll ) /dy Z [nb] 25 20 15 10 p s = 5 . 02 TeV ATLAS pPb nCTEQ15 Data 5 CT10 0 3 2 1 0 1 2 3 1.50 1.25 R 1.00 0.75 0.50 3 2 1 0 1 2 3 y Z CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 9 / 20

  19. Introduction W/Z@LHC Reweighting Conclusion pP b : Z 25 dσ ( Z → ll ) /dy Z [nb] 20 15 10 p s = 5 . 02 TeV CMS pPb 5 nCTEQ15 Data CT10 0 2 1 0 1 2 1.4 1.2 R 1.0 0.8 0.6 2 1 0 1 2 y Z CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 9 / 20

  20. Introduction W/Z@LHC Reweighting Conclusion pP b : W + 100 dσ ( W + → l + ν ) /dy l + [nb] 80 60 40 p s = 5 . 02 TeV ATLAS pPb 20 nCTEQ15 Data CT10 0 2 1 0 1 2 1.4 1.2 R 1.0 0.8 0.6 2 1 0 1 2 y l + CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 10 / 20

  21. Introduction W/Z@LHC Reweighting Conclusion pP b : W + 120 dσ ( W + → l + ν ) /dy l + [nb] 100 80 60 40 p s = 5 . 02 TeV CMS pPb 20 nCTEQ15 Data CT10 0 2 1 0 1 2 1.4 1.2 R 1.0 0.8 0.6 2 1 0 1 2 y l + CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 10 / 20

  22. Introduction W/Z@LHC Reweighting Conclusion pP b : W − 120 ν ) /dy l − [nb] 100 80 dσ ( W − → l − ¯ 60 40 p s = 5 . 02 TeV CMS pPb 20 nCTEQ15 Data CT10 0 2 1 0 1 2 1.4 1.2 R 1.0 0.8 0.6 2 1 0 1 2 y l − CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 10 / 20

  23. Introduction W/Z@LHC Reweighting Conclusion pP b : W − 100 ν ) /dy l − [nb] 80 60 dσ ( W − → l − ¯ 40 p s = 5 . 02 TeV ATLAS pPb 20 nCTEQ15 Data CT10 0 2 1 0 1 2 1.4 1.2 R 1.0 0.8 0.6 2 1 0 1 2 y l − CT10: Lead nucleus made of CT10 protons Florian LYONNET Santa Fe Jets and Heavy Flavor Workshop February 13-15, 2017 10 / 20

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