R为1.2m对称双聚焦高场强、高分辨率分析磁铁
R1.2 MEMER SYMMETRIC DOUBLE FOCUSING HIGH MAGNETIC INDUCTION, HIGH RESOLVING POWER ANALYZING MAGNET
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摘要: R=1.2m,90°偏转对称双聚焦高场强、高分辨率分析磁铁采用近似的Rogowski磁极边界来克服局部磁饱和现象,具有磁感应强度高于 1.8 T和质量分辨率 M/△M大于 208的特点。在磁感应强度小于1.08 T时,磁场非均匀度小于±4×10~(-4)。该分析磁铁的边缘场分布测试结果表明:在实际使用情况下,随着磁感应强度的改变(0.4—1.5T),边缘场等效边界S_0的变化小于0.006 g_0,g_0为磁极间隙(g_0=40 mm)。聚焦修正因子I_1的变化小于 0.028,I_2的变化小于0.006。对核磁铁进行一阶修正和考虑二阶的计算结果表明:离子束入射和出射角应为27.13°,若在将分析磁铁的出口曲率半径改为 1443 mm的凹曲面,则有可能将二阶象差减到最小。在铅离子能量为 630,530,430keV的条件下,质谱分析表明,在前、后缝各开 6 mm时,可将~(204)Pb~+,~(206)Pb~+,~(207)Pb~+,~(208)Pb~+完全分开,其中~(204)Pb~+的束流强度达10 μA,可用于重元素同位素离子注入。Abstract: R 1.2 meter, 90°deflecting, symmetric double focusing high magnetic induc-tion, high resolving power analyzing magnet was bui1t, using approximateRogowski pole contour to overcome the local magnetic saturation, the max.magnetic induction>1. 8 T. The mass resolving power≥208. The non--homogeneityof the magnetic field is less than±4×10~(-4) when the magnetic induction≤1.008 T.The measured results of the extended fringing fields of this magnet indicate:When the magnetic induction changes from 0.4 to 1.5 T, the variations of thevirtual field boundaries of the extended fringing field, So, are less than 0.006 g_0(g_0=40 mm, the gap of the magnetic pole), the integrals I_1 and I_2 are less than0.028 and 0.006 respectively. The first-order corrections and second-order aberration calculations werecarried out. in the case of entrance and exit angles are equal to 27.13°, thesymmetric double focusing can be realized and by using concave shape exit poleedge with radius of 1443 mm, the second-order aberrations can be furtherreduced. The lead isotope ions ~(204)Pb~+, ~(206)Pb~+, ~(207)Pb~+ and ~(208)Pb~+ can be separatedclearly, the beam current of ~(208)Pb~+ reaches 10 μA on the target, so heavy elementisotope ion implantation is practicable.