首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >The Stern-Gerlach polarized ion source for the Munich MP-tandem laboratory, a bright source for unpolarized hydrogen and helium ion beams as well
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The Stern-Gerlach polarized ion source for the Munich MP-tandem laboratory, a bright source for unpolarized hydrogen and helium ion beams as well

机译:慕尼黑MP串联实验室的Stern-Gerlach极化离子源,也是非极化氢和氦离子束的亮源

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摘要

The design of our source of negatively charged, intense and brilliant DC beams of polarized hydrogen and deuterium ions was motivated by the excellent performance of the HERMES atomic beam source and the successful operation of a polarized ion source at TUNL. Deviating from their 30 K atomic beam technology we combine an 80 K atomic beam source (ABS) with subsequent ionization in an electron cyclotron resonance (ECR) plasma. In a separate unit, negative ions are obtained by successive two electron pickup from cesium in a vapour jet target. Our ABS provides a flux of 6.4 x 10~(15)atoms/s for hydrogen and of about 5 x 10~(16)atoms/s for deuterium into a compression tube of 10mm diameter and 100mm length. Polarized negative D~-/H~- ion beams of about 9 μA/15μA with an emittance of 20 πmm rad (eV)~(1/2) have been observed. After tandem acceleration we have polarized beam intensity of 2 μA on target of the Q3D spectrograph. The measured vector polarizations of the D and H ion beams are 72% and 67%, respectively, in accordance with expectations from source operation data. Using an external gas inlet for the ECR region, intense beams of unpolarized ~1H~-, ~2D~-, ~3He~-, and ~4He~- ions are obtained.
机译:HERMES原子束源的出色性能和TUNL上极化离子源的成功运行,促使我们设计了带负电,强烈且明亮的极化氢和氘离子DC束源。与他们的30 K原子束技术不同,我们将80 K原子束源(ABS)与随后的电子回旋共振(ECR)等离子体中的电离结合在一起。在单独的单元中,通过从蒸汽喷射靶中的铯中连续两次吸收电子来获得负离子。我们的ABS向直径为10mm,长度为100mm的压缩管中的氢通量为6.4 x 10〜(15)atoms / s,氘为5 x 10〜(16)atoms / s。观察到极化负D〜-/ H〜-离子束约为9μA/15μA,发射率为20πmmrad(eV)〜(1/2)。串联加速后,我们在Q3D光谱仪的目标上具有2μA的偏振光束强度。根据源操作数据的预期,测得的D和H离子束的矢量极化分别为72%和67%。使用外部气体入口进入ECR区域,可获得非极化〜1H〜-,〜2D〜-,〜3He〜-和〜4He〜-离子的强束。

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