Leading-order determination of the gluon polarisation from semi-inclusive deep inelastic scattering data
Creators
- Adolph, C.1
- Braun, C.1
- Eyrich, W.1
- Lehmann, A.1
- Zink, A.1
- Aghasyan, M.2
- Birsa, R.2
- Dalla Torre, S.2
- Levorato, S.2
- Santos, C.2
- Sozzi, F.2
- Tessaro, S.2
- Tessarotto, F.2
- Akhunzyanov, R.3
- Alexeev, G.D.3
- Anfimov, N.V.3
- Anosov, V.3
- Efremov, A.3
- Gavrichtchouk, O.P.3
- Guskov, A.3
- Ivanshin, Yu.3
- Kisselev, Yu.3
- Kouznetsov, O.M.3
- Kroumchtein, Z.V.3
- Meshcheryakov, G.V.3
- Nagaytsev, A.3
- Olshevsky, A.G.3
- Orlov, I.3
- Peshekhonov, D.V.3
- Rossiyskaya, N.S.3
- Rybnikov, A.3
- Savin, I.A.3
- Selyunin, A.3
- Shevchenko, O.Yu.3
- Slunecka, M.3
- Smolik, J.3
- Tasevsky, M.3
- Zavada, P.3
- Zemlyanichkina, E.3
- Alexeev, M.G.4
- Amoroso, A.5, 4
- Balestra, F.5, 4
- Chiosso, M.5, 4
- Gnesi, I.5, 4
- Grasso, A.5, 4
- Ivanov, A.5, 4
- Kotzinian, A.M.5, 4
- Longo, R.5, 4
- Parsamyan, B.5, 4
- Takekawa, S.5, 4
- Andrieux, V.6
- Boer, M.6
- Curiel, Q.6
- Ferrero, A.6
- Fuchey, E.6
- Hose, N. d'6
- Kunne, F.6
- Levillain, M.6
- Magnon, A.6
- Marchand, C.6
- Neyret, D.6
- Platchkov, S.6
- Seder, E.6
- Thibaud, F.6
- Augustyniak, W.7
- Klimaszewski, K.7
- Kurek, K.7
- Marianski, B.7
- Sandacz, A.7
- Szabelski, A.7
- Sznajder, P.7
- Austregesilo, A.8
- Chung, S.U.8
- Friedrich, J.M.8
- Grabmueller, S.8
- Grube, B.8
- Haas, F.8
- Huber, S.8
- Kraemer, M.8
- Krinner, F.8
- Paul, S.8
- Uhl, S.8
- Azevedo, C.D.R.9
- Pereira, F.9
- Veloso, J.9
- Badelek, B.10
- Barth, J.11
- Hahne, D.11
- Klein, F.11
- Pretz, J.11
- Schmieden, H.11
- Beck, R.12
- Bisplinghoff, J.12
- Eversheim, P.D.12
- Hinterberger, F.12
- Jahn, R.12
- Joosten, R.12
- Ketzer, B.12
- Mikhasenko, M.12
- Bedfer, Y.6, 13
- Bernhard, J.14, 13
- Bicker, K.8, 13
- Bielert, E.R.13
- Mallot, G.K.13
- Schoenning, K.13
- Bodlak, M.15
- Finger, M.15
- Finger, M. Jr.15
- Matousek, J.15
- Pesek, M.15
- Roskot, M.15
- Bordalo, P.16
- Franco, C.16
- Nunes, A.S.16
- Quaresma, M.16
- Quintans, C.16
- Ramos, S.16
- Silva, L.16
- Stolarski, M.16
- Bradamante, F.2, 17
- Bressan, A.2, 17
- Dasgupta, S.2, 17
- Makke, N.2, 17
- Martin, A.2, 17
- Sbrizzai, G.2, 17
- Schiavon, P.2, 17
- Buechele, M.18
- Fischer, H.18
- Gorzellik, M.18
- Grussenmeyer, T.18
- Heinsius, F.H.18
- Herrmann, F.18
- Joerg, P.18
- Koenigsmann, K.18
- Kremser, P.18
- Nowak, W.D.18
- Regali, C.18
- Schmidt, K.18
- Schopferer, S.18
- Sirtl, S.18
- Szameitat, T.18
- Wolbeek, J. ter18
- Chang, W.C.19
- Hsieh, C.Y.19
- Sawada, T.19
- Choi, I.20
- Giordano, F.20
- Grosse Perdekamp, M.20
- Heitz, R.20
- Kulinich, Y.20
- Makins, N.20
- Montuenga, P.20
- Peng, J.C.20
- Riedl, C.20
- Cicuttin, A.21, 2
- Crespo, M.L.21, 2
- Dasgupta, S.S.22
- Dhara, L.22
- Sarkar, S.22
- Sinha, L.22
- Denisov, O.Yu.5
- Maggiora, A.5
- Panzieri, D.5
- Tosello, F.5
- Donskov, S.V.23
- Khaustov, G.V.23
- Khokhlov, Yu.A.23
- Kolosov, V.N.23
- Konstantinov, V.F.23
- Lednev, A.A.23
- Mikhailov, Yu.V.23
- Nikolaenko, V.I.23
- Polyakov, V.A.23
- Ryabchikov, D.I.23
- Samoylenko, V.D.23
- Doshita, N.24
- Hashimoto, R.24
- Ishimoto, S.24
- Iwata, T.24
- Kondo, K.24
- Matsuda, H.24
- Michigami, T.24
- Miyachi, Y.24
- Nukazuka, G.24
- Suzuki, H.24
- Duic, V.17
- Dziewiecki, M.25
- Kurjata, R.P.25
- Marzec, J.25
- Rychter, A.25
- Zaremba, K.25
- Ziembicki, M.25
- Fresne von Hohenesche, N. du14
- Harrach, D. von14
- Kabuss, E.14
- Nerling, F.14
- Ostrick, M.14
- Pochodzalla, J.14
- Weisrock, T.14
- Wilfert, M.14
- and others
- COMPASS Collaboration
- 1. Universitaet Erlangen-Nuernberg, Physikalisches Institut, Erlangen (Germany)
- 2. INFN, Trieste (Italy)
- 3. Joint Institute for Nuclear Research, Dubna, Moscow region (Russian Federation)
- 4. University of Turin, Department of Physics, Turin (Italy)
- 5. INFN, Turin (Italy)
- 6. CEA IRFU/SPhN Saclay, Gif-sur-Yvette (France)
- 7. National Centre for Nuclear Research, Warsaw (Poland)
- 8. Technische Universitaet Muenchen, Physik Department, Garching (Germany)
- 9. University of Aveiro, Department of Physics, Aveiro (Portugal)
- 10. University of Warsaw, Faculty of Physics, Warsaw (Poland)
- 11. Universitaet Bonn, Physikalisches Institut, Bonn (Germany)
- 12. Universitaet Bonn, Helmholtz-Institut fuer Strahlen- und Kernphysik, Bonn (Germany)
- 13. CERN, Geneva 23 (Switzerland)
- 14. Universitaet Mainz, Institut fuer Kernphysik, Mainz (Germany)
- 15. Charles University in Prague, Faculty of Mathematics and Physics, Prague (Czech Republic)
- 16. LIP, Lisbon (Portugal)
- 17. University of Trieste, Department of Physics, Trieste (Italy)
- 18. Universitaet Freiburg, Physikalisches Institut, Freiburg (Germany)
- 19. Academia Sinica, Institute of Physics, Taipei (China)
- 20. University of Illinois at Urbana-Champaign, Department of Physics, Urbana, IL (United States)
- 21. Abdus Salam ICTP, Trieste (Italy)
- 22. Matrivani Institute of Experimental Research and Education, Calcutta (India)
- 23. State Scientific Center Institute for High Energy Physics of National Research Center 'Kurchatov Institute', Protvino (Russian Federation)
- 24. Yamagata University, Yamagata (Japan)
- 25. Warsaw University of Technology, Institute of Radioelectronics, Warsaw (Poland)
Description
Using a novel analysis technique, the gluon polarisation in the nucleon is re-evaluated using the longitudinal double-spin asymmetry measured in the cross section of semi-inclusive single-hadron muoproduction with photon virtuality Q2 > 1 (GeV/c)2. The data were obtained by the COMPASS experiment at CERN using a 160 GeV/c polarised muon beam impinging on a polarised 6LiD target. By analysing the full range in hadron transverse momentum pT, the different pT-dependences of the underlying processes are separated using a neural-network approach. In the absence of pQCD calculations at next-to-leading order in the selected kinematic domain, the gluon polarisation Δg/g is evaluated at leading order in pQCD at a hard scale of μ2 = left angle Q2 right angle = 3 (GeV/c)2. It is determined in three intervals of the nucleon momentum fraction carried by gluons, xg, covering the range 0.04 < xg < 0.28 and does not exhibit a significant dependence on xg. The average over the three intervals, left angle Δg/g right angle = 0.113 ± 0.038(stat.) ± 0.036(syst.) at left angle xg right angle ∼ 0.10, suggests that the gluon polarisation is positive in the measured xg range. (orig.)
Availability note (English)
Available from: http://dx.doi.org/10.1140/epjc/s10052-017-4716-xAdditional details
Identifiers
Publishing Information
- Journal Title
- European Physical Journal. C, Particles and Fields (Online)
- Journal Volume
- 77
- Journal Issue
- 4
- Journal Page Range
- p. 1-12
- ISSN
- 1434-6052
INIS
- Country of Publication
- Germany
- Country of Input or Organization
- Germany
- INIS RN
- 48053361
- Subject category
- S72: PHYSICS OF ELEMENTARY PARTICLES AND FIELDS;
- Resource subtype / Literary indicator
- Numerical Data
- Descriptors DEI
- COMPUTERIZED SIMULATION; DATA ANALYSIS; DEEP INELASTIC SCATTERING; DEUTERIUM TARGET; GEV RANGE 100-1000; GLUON MODEL; LITHIUM 6 TARGET; MONTE CARLO METHOD; MUON REACTIONS; MUON-NUCLEON INTERACTIONS; NEURAL NETWORKS; NUCLEONS; PARTICLE STRUCTURE; POLARIZATION-ASYMMETRY RATIO; POLARIZED TARGETS; RELATIVISTIC RANGE; SEMI-INCLUSIVE INTERACTIONS; SPIN ORIENTATION; THEORETICAL DATA; TRANSVERSE MOMENTUM
- Descriptors DEC
- BARYONS; CALCULATION METHODS; CHARGED-PARTICLE REACTIONS; DATA; DATA PROCESSING; DIMENSIONLESS NUMBERS; ELEMENTARY PARTICLES; ENERGY RANGE; FERMIONS; GEV RANGE; HADRONS; INCLUSIVE INTERACTIONS; INELASTIC SCATTERING; INFORMATION; INTERACTIONS; LEPTON REACTIONS; LEPTON-BARYON INTERACTIONS; LEPTON-HADRON INTERACTIONS; LEPTON-NUCLEON INTERACTIONS; LINEAR MOMENTUM; MATHEMATICAL MODELS; NUCLEAR REACTIONS; NUMERICAL DATA; ORIENTATION; PARTICLE INTERACTIONS; PARTICLE MODELS; PROCESSING; SCATTERING; SIMULATION; TARGETS
Optional Information
- Collaborations
- COMPASS Collaboration