COMPASS における高横方向運動量ハドロンを 用いたグルーオン偏極度解析 岩田高広,石元茂1 ,近藤薫,鈴木肇2 ,堂下典弘,糠塚元気,橋本亮, 堀川直顕2 ,松田達郎3 ,@松田洋樹,宮地義之, 他 COMPASS Collaboration 山形大理 1 KEK 2中部大工 3宮崎大工 28.Mar.2014 28.Mar.2014 日本物理学会 28aSD-9 1 / 15 . Outline Introduction COMPASS Recent published results @ COMPASS Data taking @ COMPASS Theory Theoretical estimations Results Asymmetry calculation Kinematic distributions Deuteron Proton Summary 28.Mar.2014 日本物理学会 28aSD-9 2 / 15 . Outline Introduction COMPASS Recent published results @ COMPASS Data taking @ COMPASS Theory Theoretical estimations Results Asymmetry calculation Kinematic distributions Deuteron Proton Summary 28.Mar.2014 日本物理学会 28aSD-9 3 / 15 COMPASS @ CERN . Setup ▶ ▶ Polarised µ+ beam with 160/200 GeV energy 1 × 108 muons per spill ▶ ▶ ▶ ▶ . ▶ µ filter spill: ∼ 10 sec. cycle time: ∼ 50 sec. Beam polarisation: ∼ 80 % acceptance: ∼ ±180 mrad two stages: ∼ 60 m Magnet Magnet RICH µ+ Polarised target 28.Mar.2014 日本物理学会 28aSD-9 Kinematic acceptance 4 / 15 ∆g/g results @ COMPASS . Recent published results LO @ high-pT hadron pair NLO @ open charm COMPASS, high p , Q2>1 (GeV/c) 2, prel., 02-06 T COMPASS, high p , Q2<1 (GeV/c) 2, prel., 02-04 0.8 Q2 = 13 (GeV/c)2 T HERMES, high p , all Q2 ∆g/g ∆g/g T COMPASS, open charm, prel., 02-07 SMC, high p , Q2>1 (GeV/c)2 0.6 T COMPASS Global fit with ∆ G>0, µ2=3(GeV/c)2 0.4 COMPASS Global fit with ∆ G<0, µ =3(GeV/c) 2 2 COMPASS open charm 0.6 COMPASS (∆g>0) COMPASS (∆g<0) DSSV 0.4 LSS (∆g>0) 0.2 LSS (∆g sign changing) 0.2 0 0 -0.2 −0.2 −0.4 -0.4 10−2 -0.6 -2 10 -1 10 10−1 x xg PRD 87 (2013) 052018 PLB 718 (2013) 922 ∆g/g @ COMPASS ▶ +0.02 ± 0.09 ± 0.06 @ xg = ⟨0.01⟩ LO, high-pT pair, Q2 < 1, PLB 633 (2006) 25 ▶ +0.13 ± 0.06 ± 0.06 @ xg = ⟨0.09⟩ LO, high-pT pair, Q2 > 1, PLB 718 (2013) 922 ▶ −0.47 ± 0.44 ± 0.15 @ xg = ⟨0.11⟩ LO, open charm, arXiv:0802.3023 ▶ −0.49 ± 0.27 ± 0.11 @ xg = ⟨0.11⟩ LO, open charm, PLB 676 (2009) 31 ▶ −0.06 ± 0.21 ± 0.08 @ xg = ⟨0.20⟩ LO, open charm, PRD 87 (2013) 052018 ▶ −0.13 ± 0.15 ± 0.15 @ xg = ⟨0.11⟩ NLO, open charm, PRD 87 (2013) 052018 28.Mar.2014 日本物理学会 28aSD-9 5 / 15 . Data taking 2002-2011 muon program Year 2002 2003 2004 2006 2007 2011 Target Beam Energy(GeV/c) Acceptance(mrad) 75 LiD 160 180 NH3 200 . high-pT Hadron yield in this analysis (cut: pT > 1, Q2 < 1) Year Hadron yield(×106 ) 28.Mar.2014 2002 16.3 2003 30.9 2004 53.3 日本物理学会 28aSD-9 2006 34.2 2007 65.7 2011 39.8 6 / 15 Theory . Purpose ▶ ∆g/g evaluation from double longitudinal spin asymmetry ALL (pT ) ▶ ▶ High-pT (> 1.0 GeV/c) and low-Q2 (< 1 (GeV/c)2 ) All COMPASS data(2002 - 2011) Theoretical framework ▶ ▶ photoproduction of single inclusive hadrons: l + N → l′ + H + X based on JSV framework (Eur.Phys.J. C44, 533 (2005), hep-ph/0505157) Direct γ-contribution Resolved γ-contribution l l H Dc γ H b Δ fp (a) 28.Mar.2014 H Dc X ∆ fγ : Photon’s parton density ∆ f p : Nucleon p’s parton density ∆σ: ˆ spin-dependent partonic hard scattering cross section a, b, c = q, q, ¯ g H Dc : fragmentation function 日本物理学会 28aSD-9 H c a ´` Δσ p γ Δ fγ c ´` Δσ X b p Δ fp (b) 7 / 15 Theoretical estimations of ALL . ∑ ▶ ALL ∆σ ≡ = σ ∆ fal ⊗∆ fbN ⊗∆σ ˆ ab→cX ⊗Dhc ∑ a, b, c fal ⊗ fbN ⊗σ ˆ ab→cX ⊗Dhc a, b, c ▶ ALL @ COMPASS Kinematic range h, d ALL 0.3 0.2 h, p ALL 0.3 'Δg = -g' 'Δg = -g' 0.2 'max. γ ' 'min. γ ' 'Δg = 0' 0.1 'Δg = 0' 'std. Δg' 0.1 'Δg = g' input 'std. Δg' 0 'Δg = g' input L = 1 / fb -0.1 1 2 3 pT [GeV] 4 0 -0.1 L = 1 / fb ⇒ 4 /fb for all COMPASS data 1 2 3 pT [GeV] 4 Proton Deuteron ref: Eur.Phys.J. C44, 533 (2005), hep-ph/0505157 ▶ Different curves with different ∆g scenarios . 28.Mar.2014 日本物理学会 28aSD-9 8 / 15 . Outline Introduction COMPASS Recent published results @ COMPASS Data taking @ COMPASS Theory Theoretical estimations Results Asymmetry calculation Kinematic distributions Deuteron Proton Summary 28.Mar.2014 日本物理学会 28aSD-9 9 / 15 Asymmetry calculation . Double longitudinal asymmetry ( ⇄ ) ( ⇄ ) ∆σ 1 σ − σ⇔ 1 N − N⇔ ALL ≡ ≈ = σ f Pb Pt σ⇄ + σ⇔ f P b Pt N ⇄ + N ⇔ ▶ f : Dilution factor: 0.4(6 LiD), 0.16(NH3 ) ▶ Pb : Beam polarisation: ∼ 80 % Pt : Target polarisation: ∼ 50 %(6 LiD), ∼ 85 %(NH3 ) N: Hadron yield ▶ ▶ 28.Mar.2014 日本物理学会 28aSD-9 10 / 15 Kinematic distributions . pT , Q2 in 2004 and 2007 105 hadrons hadrons pT 105 2004 (1 week) deuteron 2007 (1 week) proton 104 102 el im 10 103 1 0 1 Pr 10 Pr 10 ry ry in a 2 in a Before cut After cut 103 el im 104 2 3 4 1 0 5 pT (GeV/c) 1 2 3 events 2004 (1 week) deuteron 2 5 pT (GeV/c) Proton ×103 events Deuteron Q2 4 ×103 2007 (1 week) proton 1.5 1.5 ar y im in im in ar y 1 1 0 10-4 10-3 10-2 el Pr el 0.5 Pr 0.5 10-1 Q2 1 (GeV2/c 2) 10 0 10-4 Deuteron 28.Mar.2014 10-3 10-2 10-1 Q2 1 (GeV2/c 2) 10 Proton 日本物理学会 28aSD-9 11 / 15 Asymmetry: deuteron . 2002-2006 COMPASS Deuteron y r ina 0 -0.02 0.6 0.8 1 0.2 m i l re 1.2 1.4 pT (GeV/c) 1.6 1.8 2 0.3 0.1 ALL ALL 0.02 P 0 -0.1 1 2 3 4 p (GeV/c) T . 28.Mar.2014 日本物理学会 28aSD-9 12 / 15 Asymmetry: deuteron . 2002-2006 0 h, d ALL 0.3 0.2 -0.02 0.6 0.3 COMPASS Deuteron 'Δg = -g' y r ina 'max. γ ' 'min. γ ' 0.8 1 0.1 m i l re 1.2 1.4 pT (GeV/c) 1.6 1.8 2 P 0 'Δg = 0' 0.1 'std. Δg' 0 'Δg = g' input L = 1 / fb -0.1 0.2 ALL ALL 0.02 -0.1 1 2 3 1 2 3 pT [GeV] 4 4 p (GeV/c) T . 28.Mar.2014 日本物理学会 28aSD-9 12 / 15 Asymmetry: proton . 2007-2011 COMPASS Proton y r ina 0 -0.02 0.6 0.8 1 0.2 m i l re 1.2 1.4 pT (GeV/c) 1.6 1.8 2 0.3 0.1 ALL ALL 0.02 P 0 -0.1 1 2 3 4 p (GeV/c) T . 28.Mar.2014 日本物理学会 28aSD-9 13 / 15 Asymmetry: proton . 2007-2011 0 h, p ALL 0.3 0.3 'Δg = -g' COMPASS Proton y r ina 0.2 -0.02 0.6 0.8 1 0.1 m i l re 1.2 1.4 pT (GeV/c) 1.6 1.8 2 P 0 0.2 'Δg = 0' 'std. Δg' 0.1 'Δg = g' input ALL ALL 0.02 0 L = 1 / fb -0.1 -0.1 1 2 3 1 2 3 pT [GeV] 4 4 p (GeV/c) T . 28.Mar.2014 日本物理学会 28aSD-9 13 / 15 . Outline Introduction COMPASS Recent published results @ COMPASS Data taking @ COMPASS Theory Theoretical estimations Results Asymmetry calculation Kinematic distributions Deuteron Proton Summary 28.Mar.2014 日本物理学会 28aSD-9 14 / 15 Summary & Outlook . Summary ▶ ∆g/g evaluation from double longitudinal asymmetry ALL from high-pT hadrons with low-Q2 ▶ ▶ All COMPASS data with longitudinal beam/target used Asymmetries: compatible with zero except high-pT bin ▶ Systematic error: of the order of statistical error Outlook ▶ ▶ ▶ further quantification of systematic errors comparisons between data and theoretical calculation evaluation of ∆g/g 28.Mar.2014 日本物理学会 28aSD-9 15 / 15 Backup 28.Mar.2014 日本物理学会 28aSD-9 16 / 15 Comparison unpolarised cross section . COMPASS data v.s. theoretical calculation COMPASS data in 2004 ▶ ▶ C. Adolph, et. al., PRD 88 (2013) 091101 µ + d → µ′ + h± + X cross section at Q2 < 0.1 (GeV/c)2 µ+ + d → µ+ + h± + X 103 102 Theoretical calculations ▶ D. Florian, et. al., arXiv:1305.6468 Higher-order QCD corrections to the cross section Large logarithmic “threshold” corrections → improved the agreement between data and theory pb c2 G eV 2 ▶ 1 dσ 2π pT dpT ▶ 10 1 10− 1 10− 2 η ∈ [−0.10 : 2.38] 10− 3 ⇒ Valid within theoretical uncertainty 28.Mar.2014 L O µ = pT / 2, 2pT NL O µ = pT / 2, 2pT resum µ = pT / 2, 2pT LO NL O resum 日本物理学会 28aSD-9 2 2.5 pT (GeV / c) 3 3.5 17 / 15 Contributions to total cross section . From each process 1.5 dΔσres / dΔσ 1 0.5 0 dΔσdir / dΔσ (a) -0.5 dΔσab / dΔσ 2 0 -2 qg gq qq gg (b) 1 2 ▶ Resolved photon contribution dominates over the direct contribution ▶ Large cancellation between γg and γq → Numerically smaler resolved subprocesses become important γg γq 3 pT [GeV] 4 F ig. 5. (a) Direct and resolved NLO(MS) contributions and (b) NLO(MS) contributions of different partonic channels a+ b → c + X to the full NLO polarized photoproduction cross section shown in Fig. 2. 28.Mar.2014 日本物理学会 28aSD-9 18 / 15 Difference between previous analyses . Fit method(This analysis) ▶ ▶ pQCD collinear NLO All hadrons with high-pT Compare data with theoretical curve ▶ quark distributions: from global fit ▶ Direct methods(COMPASS’s main stream method) high-pT hadron pair ▶ open charm LO 2 hadrons pair with high-pT ▶ ▶ ▶ (Neural Network tuned) Mote Carlo simulation High statistics ▶ (Neural Network tuned) Mote Carlo simulation Low statistics ▶ Large background ▶ Small background ▶ ▶ 28.Mar.2014 ▶ LO or NLO D meson from PGF 日本物理学会 28aSD-9 19 / 15 . PGF contribution PYTHIA simulation Contributions from each process @ Q2 < 1 PGF R 0.3 0.2 0.1 0 * QCDC γ g→qq * γ q→qg * γ q→q qq’→qq’ qg→qg gg→gg low pT Leading Ref: PLB 633 (2006) 25–32 28.Mar.2014 日本物理学会 28aSD-9 20 / 15 COMPASS data taking . Year Target Ebeam Detail 2002 2003 2004 2005 2006 2007 2008 2009 2010 2011 2012 2013 Deuteron Deuteron Deuteron 160 160 160 Deuteron Proton 160 160 Proton Proton Hydrogen 160 200 Longitudinal mode(∼20 % transverse mode) Longitudinal mode(∼20 % transverse mode) Longitudinal mode(∼20 % transverse mode) Shutdown & upgrade New setup, longitudinal mode 1/2 longitudinal, 1/2 transverse Phase-I Hadron physiscs Hadron physiscs Transverse Longitudinal Hadron physics(Primakoff) + DVCS test run and SIDIS Shutdown & upgrade 2014 2015 2016 2017 Proton Proton Hydrogen Hydrogen Drell-Yan Drell-Yan DVCS DVCS Phase-II . 28.Mar.2014 日本物理学会 28aSD-9 21 / 15 Asymmetry: year by year . 2002-2011 COMPASS 2003(Deuteron) 1 y nar i m i p (GeV/c) T 1 1 COMPASS 2006(Deuteron) 0 lim Pre COMPASS 2007(Proton) 0 -0.02 -0.02 1 y nar i m i 2 3 28.Mar.2014 T 2 mi li Pre 4 p (GeV/c) -0.2 0.02 COMPASS 2011(Proton) 0.4 0.2 -0.02 2 l Pre 1 0 0 -0.02 1 2 T 0.02 T A LL (p ) T A LL (p ) Pre 0.2 ry ina -0.02 2 li l Pre 0.02 ary min -0.02 2 0.02 0.4 0 A LL 0 -0.02 A LL COMPASS 2004(Deuteron) 1 1 y nar 2 3 T y nar i lim Pre 4 p (GeV/c) 日本物理学会 28aSD-9 2 A LL 0 -0.02 0 0.02 T A LL (p ) COMPASS 2002(Deuteron) A LL (p ) A LL 0 0.02 T A LL (p ) 0.02 T A LL (p ) 0.02 1 0 2 3 4 -0.2 p (GeV/c) T 22 / 15
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