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利用CLAS测量质子自旋结构函数g1(x,Q2)在Q2从0.15到1.6 GeV2范围内的值。

Measurement of the proton spin structure function g1(x,Q2) for Q2 from 0.15 to 1.6 GeV2 with CLAS.

作者信息

Fatemi R, Skabelin A V, Burkert V D, Crabb D, De Vita R, Kuhn S E, Minehart R, Adams G, Anciant E, Anghinolfi M, Asavapibhop B, Audit G, Auger T, Avakian H, Bagdasaryan H, Ball J P, Barrow S, Battaglieri M, Beard K, Bektasoglu M, Bellis M, Bertozzi W, Bianchi N, Biselli A S, Boiarinov S, Bonner B E, Bosted P E, Bouchigny S, Bradford R, Branford D, Brooks W K, Butuceanu C, Calarco J R, Carman D S, Carnahan B, Cetina C, Ciciani L, Clark R, Cole P L, Coleman A, Connelly J, Cords D, Corvisiero P, Crannell H, Cummings J P, De Sanctis E, Degtyarenko P V, Denizli H, Dennis L, Dharmawardane K V, Dhuga K S, Djalali C, Dodge G E, Doughty D, Dragovitsch P, Dugger M, Dytman S, Eckhause M, Egiyan H, Egiyan K S, Elouadrhiri L, Empl A, Eugenio P, Farhi L, Feuerbach R J, Freyberger A, Ficenec J, Forest T A, Frolov V, Funsten H, Gaff S J, Garçon M, Gavalian G, Gilad S, Gilfoyle G P, Giovanetti K L, Girard P, Gordon C I O, Griffioen K A, Guidal M, Guillo M, Guo L, Gyurjyan V, Hadjidakis C, Hancock D, Hardie J, Heddle D, Heimberg P, Hersman F W, Hicks K, Hicks R S, Holtrop M, Hu J, Hyde-Wright C E, Ilieva Y, Ito M M, Jenkins D, Joo K, Keith C, Kelley J H, Kellie J D, Khandaker M, Kim K Y, Kim K, Kim W, Klein A, Klein F J, Klimenko A V, Klusman M, Kossov M, Koubarovski V, Kramer L H, Kuang Y, Kuhn J, Lachniet J, Laget J M, Lawrence D, Li Ji, Livingston K, Longhi A, Lukashin K, Major W, Manak J J, Marchand C, McAleer S, McNabb J W C, Mecking B A, Mehrabyan S, Mestayer M D, Meyer C A, Mikhailov K, Mirazita M, Miskimen R, Morand L, Morrow S A, Muccifora V, Mueller J, Mutchler G S, Napolitano J, Nasseripour R, Nelson S O, Niccolai S, Niculescu G, Niculescu I, Niczyporuk B B, Niyazov R A, Nozar M, O'Brien J T, O'Rielly G V, Osipenko M, Park K, Pasyuk E, Peterson G, Pivnyuk N, Pocanic D, Pogorelko O, Polli E, Pozdniakov S, Preedom B M, Price J W, Prok Y, Protopopescu D, Qin L M, Raue B A, Riccardi G, Ricco G, Ripani M, Ritchie B G, Rock S E, Ronchetti F, Rossi P, Rowntree D, Rubin P D, Sabatié F, Sabourov K, Salgado C, Santoro J P, Sapunenko V, Sargsyan M, Schumacher R A, Seely M, Serov V S, Sharabian Y G, Shaw J, Simionatto S, Smith E S, Smith T, Smith L C, Sober D I, Sorrel L, Spraker M, Stavinsky A, Stepanyan S, Stoler P, Strauch S, Taiuti M, Taylor S, Tedeschi D J, Thoma U, Thompson R, Todor L, Tur C, Ungaro M, Vineyard M F, Vlassov A V, Wang K, Weinstein L B, Weller H, Weygand D P, Whisnant C S, Wolin E, Wood M H, Yegneswaran A, Yun J, Zhang B, Zhao J, Zhou Z

机构信息

University of Virginia, Charlottesville, VA 22901, USA.

出版信息

Phys Rev Lett. 2003 Nov 28;91(22):222002. doi: 10.1103/PhysRevLett.91.222002. Epub 2003 Nov 25.

DOI:10.1103/PhysRevLett.91.222002
PMID:14683231
Abstract

Double-polarization asymmetries for inclusive ep scattering were measured at Jefferson Lab using 2.6 and 4.3 GeV longitudinally polarized electrons incident on a longitudinally polarized NH3 target in the CLAS detector. The polarized structure function g(1)(x,Q2) was extracted throughout the nucleon resonance region and into the deep inelastic regime, for Q(2)=0.15-1.64 GeV2. The contributions to the first moment Gamma(1)(Q2)= integral g(1)(x,Q2) dx were determined up to Q(2)=1.2 GeV2. Using a parametrization for g(1) in the unmeasured low x regions, the complete first moment was estimated over this Q2 region. A rapid change in Gamma(1) is observed for Q2<1 GeV2, with a sign change near Q(2)=0.3 GeV2, indicating dominant contributions from the resonance region. At Q(2)=1.2 GeV2 our data are below the perturbative QCD evolved scaling value.

摘要

在杰斐逊实验室,利用能量为2.6 GeV和4.3 GeV的纵向极化电子入射到CLAS探测器中纵向极化的NH₃靶上,测量了包含性电子-质子散射的双极化不对称性。在整个核子共振区并进入深度非弹性区,提取了极化结构函数g(1)(x,Q²),其中Q² = 0.15 - 1.64 GeV²。确定了直至Q² = 1.2 GeV²时对第一矩Gamma(1)(Q²)=∫g(1)(x,Q²)dx的贡献。利用未测量的低x区域中g(1)的参数化,估计了该Q²区域上的完整第一矩。观察到对于Q² < 1 GeV²,Gamma(1)有快速变化,在Q² = 0.3 GeV²附近有符号变化,表明共振区的贡献占主导。在Q² = 1.2 GeV²时,我们的数据低于微扰量子色动力学演化的标度值。

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