Study of Deep Inelastic Scattering of Polarized Electrons off Polarized Deuterons

M. Kuriki
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引用次数: 1

Abstract

This thesis describes a 29GeV electron - nucleon scattering experiment carried out at Stanford Linear Accelerator Center (SLAC). Highly polarized electrons are scattered off a polarized ND{sub 3} target. Scattered electrons are detected by two spectrometers located in End Station A (ESA) at angles of 4.5{degrees} and 7{degrees} with respect to the beam axis. We have measured the spin structure function g{sub 1} of deuteron over the range of 0.029 < x < 0.8 and 1. 0 < Q{sup 2} < 12.0(GeV/c){sup 2}. This integral indicates a discrepancy of more than three standard deviations from the prediction of the Ellis-Jaffe sum rule, 0.068{+-}0.005 at Q{sup 2} = 3.0(GeV/c){sup 2} while our result of g{sub 1}{sup d} in good agreement with SMC results. Combined with g{sub 1} of the proton, the measurement of {integral}{sub 0}{sup 1}(g{sub 1}{sup d}-g{sub 1}{sup n}) is 0.169{+-}0.008. We also obtained the strong coupling constant at Q{sup 2} = 3.0(GeV/c){sup 2} to be 0.417{sub -0.110}{sup +0.086}, using the power correction for the sum rule up to third order of {alpha}{sub s}. This result is in agreement with the strong coupling constant {alpha}{sub s}(Q{sup 2}) = 3.0(GeV/c{sup 2}) obtained from various experiments. Using our deuteron results and the axial vector couplings of hyperon decays, the total quark polarization along the nucleon spin is found to be 0.286{+-}.055, implying that quarks carry only 30% of the nucleon spin. The strange sea quark polarization is also determined to be -0.101 {+-} .023. These measurements are in agreement with other experiments and provide the world`s most precise measurement of these quark polarizations. 80 refs., 151 figs., 23 tabs.
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极化氘核对极化电子的深度非弹性散射研究
本文描述了在斯坦福直线加速器中心(SLAC)进行的29GeV电子-核子散射实验。高极化电子从极化ND{sub 3}目标上散射出去。位于终端站A (ESA)的两台光谱仪以相对于束流轴的4.5度和7度角探测散射电子。我们测量了氘核的自旋结构函数g{sub 1}在0.029 < x < 0.8和1的范围内。0 < Q{sup 2} < 12.0(GeV/c){sup 2}。该积分表明与Ellis-Jaffe和规则的预测有三个标准差以上的差异,在Q{sup 2} = 3.0(GeV/c){sup 2}时0.068{+-}0.005,而我们的g{sub 1}{sup d}的结果与SMC的结果很好地一致。结合质子的g{sub 1},{积分}{sub 0}{sup 1}(g{sub 1}{sup d}-g{sub 1}{sup n})的测量值为0.169{+-}0.008。我们还得到了Q{sup 2} = 3.0(GeV/c){sup 2}处的强耦合常数为0.417{sub -0.110}{sup +0.086},使用了对求和规则的功率校正,直到{alpha}{sub s}的三阶。这一结果与各种实验得到的强耦合常数{alpha}{sub s}(Q{sup 2}) = 3.0(GeV/c{sup 2})是一致的。利用我们的氘核结果和超子衰变的轴向矢量耦合,发现沿核子自旋的总夸克极化为0.286{+-}。055,这意味着夸克只携带30%的核子自旋。奇异海夸克极化也被确定为-0.101{+-}.023。这些测量结果与其他实验一致,并提供了世界上最精确的夸克极化测量。参80。, 151个无花果。, 23页。
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