A phase-imaging technique for cyclotron-frequency measurements

被引:91
作者
Eliseev, S. [1 ]
Blaum, K. [1 ]
Block, M. [2 ]
Doerr, A. [1 ,3 ]
Droese, C. [4 ]
Eronen, T. [1 ]
Goncharov, M. [1 ,3 ]
Hoecker, M. [1 ]
Ketter, J. [1 ,3 ]
Ramirez, E. Minaya [2 ,5 ]
Nesterenko, D. A. [6 ,7 ]
Novikov, Yu N. [6 ,7 ]
Schweikhard, L. [4 ]
机构
[1] Max Planck Inst Kernphys, D-69117 Heidelberg, Germany
[2] GSI Helmholtzzentrum Schwerionenforsch GmbH, D-64291 Darmstadt, Germany
[3] Heidelberg Univ, Fak Phys & Astron, D-69120 Heidelberg, Germany
[4] Ernst Moritz Arndt Univ Greifswald, Inst Phys, D-17487 Greifswald, Germany
[5] Johannes Gutenberg Univ Mainz, Helmholtz Inst Mainz, D-55099 Mainz, Germany
[6] Petersburg Nucl Phys Inst, St Petersburg 188300, Russia
[7] St Petersburg State Univ, Dept Phys, St Petersburg 198504, Russia
来源
APPLIED PHYSICS B-LASERS AND OPTICS | 2014年 / 114卷 / 1-2期
关键词
PRECISION MASS-SPECTROMETRY; PENNING TRAP; ION MOTION; OCTUPOLAR EXCITATION; RAMSEY METHOD; ACCURACY; ELECTRON; PARTICLE; NUCLEI; LIMITS;
D O I
10.1007/s00340-013-5621-0
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
A novel approach to mass measurements at the 10(-9) level for short-lived nuclides with half-lives well below one second is presented. It is based on the projection of the radial ion motion in a Penning trap onto a position-sensitive detector. Compared with the presently employed time-of-flight ion-cyclotron-resonance technique, the novel approach is 25-times faster and provides a 40-fold gain in resolving power. Moreover, it offers a substantially higher sensitivity since just two ions are sufficient to determine the ion's cyclotron frequency. Systematic effects specific to the technique that can change the measured cyclotron frequency are considered in detail. It is shown that the main factors that limit the maximal accuracy and resolving power of the technique are collisions of the stored ions with residual gas in the trap, the temporal instability of the trapping voltage, the anharmonicities of the trapping potential and the uncertainty introduced by the conversion of the cyclotron to magnetron motion.
引用
收藏
页码:107 / 128
页数:22
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