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The COMBAS Fragment Separator

机译:COMBAS片段分离器

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摘要

The basic ion-optical characteristics of the COMBAS fragment separator are analyzed. The momentum distributions of radioactive ~6He, ~8He, and ~9Li nuclei obtained in the reaction (11)~B (33 A MeV, where A is the mass number of a particle) + ~9Be (332.6 mg/cm~2) have been investigated in forward-angle measurements on the COMBAS fragment separator. The momentum and angular (horizontal) acceptances of the COMBAS separator have been measured using the ~6He, ~8He, and ~9Li beams. It has been ascertained that the images of the ~6He, ~8He, and ~9Li nuclear beams in final achromatic focus of the separator F_a approximately twofold exceed the size of the beam on a producing target (input focus F_0), at which the primary beam has a diameter of 6 mm. The intensities of ~6He, ~8He, and ~9Li beams obtained at a 5-μA intensity of the primary (11)~B beam are 6.9 × 10~5, 2 × 10~4, and 4.7 × 10~5 particles/s, respectively. These values are sufficient for use in spectroscopic measurements. It is proposed that time-of-flight analysis of nuclear reaction products at the exit from the COMBAS separator will be used not only to measure the energy of transported particles over the whole operating range of the momentum acceptance, but also to identify them by mass A and charge Z without loss of these particles. The problem of reducing the count rates of detectors and further improvement of their energy resolution for detected particles can be solved by placing a high-resolution magnetic spectrometer past the second target accepting the secondary radioactive nuclear beams.
机译:分析了COMBAS碎片分离器的基本离子光学特性。反应(11)〜B(33 A MeV,其中A为粒子的质量数)中获得的放射性〜6He,〜8He和〜9Li核的动量分布+〜9Be(332.6 mg / cm〜2)已经在COMBAS碎片分离器的前角测量中进行了研究。使用〜6He,〜8He和〜9Li光束测量了COMBAS分离器的动量和角(水平)接受度。可以确定的是,分离器F_a的最终消色差焦点中〜6He,〜8He和〜9Li核束的图像大约是产生目标(输入焦点F_0)上的光束大小的两倍,光束的直径为6毫米。在一次(11)〜B光束的5μA强度下获得的〜6He,〜8He和〜9Li光束的强度为6.9×10〜5、2×10〜4和4.7×10〜5粒子/分别。这些值足以用于光谱测量。建议在COMBAS分离器出口处对核反应产物进行飞行时间分析,不仅用于测量在动量接受的整个工作范围内传输的粒子的能量,而且还用于按质量识别它们A并给Z充电而不会损失这些粒子。降低探测器计数率并进一步提高其对被探测粒子的能量分辨率的问题可以通过将高分辨率磁谱仪放置在接受次级放射性核束的第二目标上方来解决。

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