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Atomic Physics Methods in Modern Research: Selection of by Klaus Jungmann, Joachim Kowalski, Irene Reinhard, Frank

By Klaus Jungmann, Joachim Kowalski, Irene Reinhard, Frank Traeger

Atomic physics has performed a relevant function within the improvement of recent physics. development used to be in accordance with newly invented clinical equipment and experimental instruments and at the present time those recommendations are effectively hired in a wide selection of hugely lively components in smooth study, extending from investigations of such a lot basic interactions in physics to experiments concerning subject matters in technologies and technical features. With progressively expanding value they're present in parts good outdoors of classical atomic physics in fields comparable to nuclear and particle physics, metrology, physics of condensed subject and surfaces, actual chemistry, chemistry, drugs and environmental study. This ebook offers an intensive survey of the tools and methods in key experiments of interdisciplinary learn.

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75, 4728. Kinoshita T. (1996): Rep. Prog. Phys. 59, 1459. Kinoshita T. and Nio M. (1996): Phys. Hey. D 53, 4909. Kponou A. , (1981): Phys. Rev. A24, 264. , Nistler W. and Weirauch W. (1995): Metrologia 32, 117. A. , (1970): Phys. Rev. A2, 86. , (1994): Phys. Lett. A 187, 247. G. , (1982): Phys. Rev. Lett. 49,993. , Nahum M. D. (1994): Phys. Rev. Lett. 72,904. O. , (1975): Phys. Rev. A l l , 1175. J. , (1984): Phys. Rev. Lett. 52, 910. Pachucki K. (1996): Phys. Rev. A53, 2092. Palmer R. 1996: (private communciation) "Review of Particle Properties" 1994:, Phys.

The distribution of time intervals between a stop of a muon and the detected decay of a m u o n i u m a t o m in vacu u m includes full information on the a t o m ' s production rate (Fig. 5). Using an effective diffusion equation for the movement of atoms inside the target parallel to an axis (y) orthogonal to the target surface the time distribution is derived for a diffusion length l = ~ which is small compared to the target thickness a 2-v~. DM • exp ( • /0 t dr' fo ~ dy S(y)x/~Tg (a -- y) (a - - y)2 4T~MM :7, ) , (4) with DM the diffusion constant, fM the fraction of muons stopped with a density S(y) inside of the target and forming muonium.

Baracci L. and Zavattini E. (1990): Phys. Rev. A 41 2352. A. G. (1995): Phys. Rev. Lett. 75, 2470. Bertin A. , (1975a): Phys. Lett. 55B, 411. Bertin A. , (1975b): Atomic Physics 4, ed. W. Weber and A. Winnacker (Plenum, New York) p. 141. , (1996): Phys. Rev. Lett. 76, 384. G. , (1995): Phys. Rev. A 52, 1948. , zu Putlitz G. (1996a): Comments Atomic and Molecular Physics 33, 17. G. , (1996b): Abstracts ZICAP, Amsterdam, The Netherlands, ThK3. E. , (1989): IEEE Trans. Instrum. Meas. 38, 284. Carboni G.

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