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《中国科学院近代物理研究所和兰州重离子研究装置年报:英文版》
>4.2-18.2 keV Ar2+ Subsequent Radiative Decay of Electron Capture from 50 - 200 MeV/u Bare Xe54+ Ions in Collisions with Krypton and Xenon Gaseous Targets
4.2-18.2 keV Ar2+ Subsequent Radiative Decay of Electron Capture from 50 - 200 MeV/u Bare Xe54+ Ions in Collisions with Krypton and Xenon Gaseous Targets
In collisions between energetic highly charged ions and atoms,the ions could remove the electrons of the target atoms,or be excited into high-level states.In the first case,the target electrons not only be captured into ground and excited states of the projectile ions,but also be ionized to free.Non-radiative capture(NRC)and radiative electron capture(REC)are two competing mechanisms in fast collisions[1].NRC means electron transfer from a bound state of the target to a bound states of the projectile without the emission of radiation;REC is produced with simultaneous the emission of photon for satisfying energy and momentum conservation laws.The physical essence is the competition between the“electron-nucleus”interaction and the“electron-vacuum”interaction.NRC is dominant in collisions of high-Z ions with heavy target atoms at moderate energies.REC entirely determine the electron capture channel for high collision velocities and light targets[1].Measuring the relative strength of the projectile x-ray emission associated with electron capture could determine state-selective population,angular distribution of single capture Ly 1 or double capture K 1 and K 2,would provide new detailed information on the dynamics of ion-atom collisions and atomic structure studies[1].
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