Atomic Physics with Heavy Ions by Andreas Wolf (auth.), Dr. Heinrich F. Beyer, Dr. Viatcheslav

By Andreas Wolf (auth.), Dr. Heinrich F. Beyer, Dr. Viatcheslav P. Shevelko (eds.)

The e-book courses the reader to the study frontiers in atomic physics with heavy ions, giving a concise picture of the complicated experimental and theoretical tools exemplified by means of the latest effects. It levels from accelerator and ion catch expertise, over the $64000 and primary info within the knowing of strongly certain far-electron structures, to radiative and collisional phenomena of those gadgets. The subfields were rigorously chosen; every one is roofed by means of top specialists who draw a full of life photograph in their research.

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Wagner: Nucl. Instrum. Methods. B 70, 427 (1992) 50. A. Lampert, A. Wolf, D. Habs, J. Kenntner, G. Kilgus, D. Schwalm, M. S. Pindzola, N. R. Badnell: Phys. Rev. A 53, 1413 (1996) 51. M. Bell, J. S. Bell: Part. Accel. 12, 49 (1982) 52. W. Zong, R. Schuch, E. Lindroth, H. Gao, D. R. DeWitt, S. Asp, H. Danared: Phys. Rev. A 56, 386 (1997) 53. C. Brandau, F. Bosch, G. Dunn, B. Franzke, A. Hoffknecht, C. Kozhuharov, P. H. Mokler, A. Miiller, F. Nolden, S. Schippers, Z. Stachura, M. Steck, T. Stohlker, T.

The top drift tube voltage is lowered to allow the ions to enter the trap. The drift tube voltage is adjusted to minimize the velocity of the ions in the trap. As the ions are reflected off the bottom drift tube potential, the voltage of the top drift tube is quickly raised, trapping the ions. The ions are then allowed to ionize for a time until the ionization balance comes to equilibrium. The electron energy is then changed to the "probe energy", which may either be constant or a function of time.

Even after including the shift from QED, there is still a difference of 62 A between the measurement and the calculated wavelength. Shabaev's [30] calculation uses a value for the nuclear magnetic moment of 16fiJIo of 4173(27) JLN tabulated by Lederer and Shirley [33] and based on a measurement by the atomic beam resonance method of 4094(44) JLN [34] (without diamagnetic correction), later recalculated in [35) to 4128(27) JLN (without diamagnetic correction). This value is cited in the literature as 4160(27) JLN, or 4173(27) JLN, depending on the size of the diamagnetic correction employed.

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