Titlebook: Recombination of Atomic Ions; W. G. Graham,W. Fritsch,J. A. Tanis Book 1992 Springer Science+Business Media New York 1992 Electron Beam Io

樹上結(jié)蜜糖

清澈

Interference Effects Affecting RTE nucleus, coupled with an excitation of a projectile electron by another target electron, 2 -electron Transfer and Excitation, 2eTE (also referred to as UTE and CTE)(16–19). Since in every case, it is possible to have initial and (semi-)final states that are identical it is intriguing to search for interference effects between these processes.

MEN

Early Measurements of Dielectronic Recombination: Multiply Charged Ionshich techniques to apply to obtain the required data? Multicharged ion sources were not highly developed. Moreover, since a signature of recombination is stabilized charged capture, and since capture cross sections from background gas are enormous at low velocities, we chose not to use low-energy multicharged ions.

fledged

Introductionchallenge for atomic collision physics. Apart from their intrinsic interest, a knowledge of the magnitude of recombination cross sections was required by those seeking to understand the processes which sustain high-temperature plasmas such as astrophysical and controlled nuclear fusion plasmas. The

Conjuction

Electron-Ion Recombination Processes — A General Overviewreview will therefore concentrate mostly on the development of the past ten years. The foundation of the recent work was laid by many earlier works, and we only emphasize the key milestones: In the 1920’s by Kramers. on the first quantum mechanical derivation of the radiative recombination (RR) cros

venous-leak

characteristic