High density polarized hydrogen gas target for storage rings

High density polarized hydrogen gas target for storage rings
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用于存储环的高密度极化氢气靶

DOI:
10.1063/1.1146388
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发表时间:
1995
影响因子:
1.6
通讯作者:
W. Haeberli
W. Haeberli
中科院分区:
工程技术4区
文献类型:
--
作者:
K. Zapfe;B. Braun;H.;M. Grieser;B. Povh;M. Rall;E. Steffens;F. Stock;J. Tonhäuser;C. Montag;F. Rathmann;D. Fick;W. Haeberli

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通过将极化氢原子(由Stern-Gerlach自旋分离产生)注入由两端打开的圆柱形管组成的存储单元中,形成气态极化氢靶。将靶材置于贮存环中,研究靶材的特性(核极化、靶材厚度、抗辐射性能)。采用弱横向引导场(5g)确定偏振方向。当选择处于单一超精细态的原子时,测得目标的核极化为0.80±0.02。在这些条件下,靶材的面密度为(5.5±0.2)×1013 H/cm2,而在两种自旋状态下(适用于高能环中可以对靶材施加强磁场的实验),靶材厚度为(8.2±0.3)×1013 H/cm2。当目标长时间暴露在高达1ma的光束下时,目标偏振不受影响。
A target of gaseous polarized hydrogen was formed by injecting polarized hydrogen atoms (produced by Stern–Gerlach spin separation) into a storage cell consisting of a cylindrical tube open at both ends. The target was placed in a storage ring to study the target characteristics (nuclear polarization, target thickness, radiation resistance). A weak transverse guide field (5 G) was applied to define the polarization direction. When atoms in a single hyperfine state were selected, the nuclear polarization of the target was measured to be 0.80±0.02. The areal density of the target under these conditions was (5.5±0.2)×1013 H/cm2, while for two spin states (applicable to experiments in high energy rings where a strong magnetic field can be applied to the target) the target thickness was found to be (8.2±0.3)×1013 H/cm2. The target polarization was unaffected by prolonged exposure of the target to beams up to 1 mA.