By James S. Cohen (auth.), Leopold M. Simons, Dezsö Horváth, Gabriele Torelli (eds.)

This Workshop was once prepared to carry once again tagether the scientists of the fairly heterogeneaus box of unique atoms. at this time the most subject of the sector looks the learn of the atomic cascade. There are a few who learn it deliberately -Iet us name them cascadeurs -and others who imagine they examine different positive factors of the unique atoms (like Coulomb catch, particle move, muon catalyzed fusion, chemical results, primary houses, etc.) -users-while actually they research a few specific results of a similar atomic cascade. We made up our minds to get cascadeurs and clients talk about the issues of unique atoms at fabulous Erice, on the fifth process the foreign tuition of Physics of unique Atoms. Our Workshop was once really profitable, we have now heard very good talks from contributors from a dozen countfies and so much of them have ready written contributions for this quantity. The Organizers convey their gratitude to all individuals for his or her contributions, in particular to David Measday for bis concluding feedback (not published right here) and to James Cohen for leaping in for Leonid Ponomarev who needed to go away all at once in the midst of the assembly. We tremendously get pleasure from the enthusiastic support of Marianne Signer in each degree of the association paintings. Am!, in fact, the Workshop couldn't occur in any respect with out the particularly effective association through the Ettore Majorana Centre of medical tradition. Leopold M. Simons Dezsö Horvath Gabriele Torelli V CONTENTS commencing handle . . . . . . . . . . . . . . . . . . . . . . . . . . xi . . . . . . .

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Extra resources for Electromagnetic Cascade and Chemistry of Exotic Atoms

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Knowing all energies a could be determined. In fig. 1b the multiple scattering correction factors n/I, where I is the measured intensity per unit energy and time, for the MgF 2 and Au moderators are drawn vs T. Fig. 1c shows the spectral flux densities n for the MgF 2 and Au moderators, as deduced from the TOF spectra (fig. 1a), corrected for multiple scattering, vs T. Both distributions rise towards smaller energies, go through a maximum at about 3 keV for MgF 2 and 5 keV for Au and decrease slowly.

Garcia, N. H. Kwong, and J. S. Cohen, Phys. Rev. A 35, 4068 (1987). 7 N. H. Kwong, J. D. Garcia, and J. S. Cohen, in Muon Catalyzed Fusion {Sanibel Island, FL 1988}, American Institute of Physics Conference Proceedings 181, edited by S. E. Jones, J. Rafelski, and H. J. Monkhorst (AIP,New York, 1989), p. 236. s M. Leon, Phys. Rev. A 17, 2112 (1978). 9 U. Gastaldi and R. Klapisch, in From Nuclei to Particles, proceedings of the International School of Physics "Enrico Fermi," Course LXXIX, edited by A.

1 shows these differences as a function of velocity. The stopping power for positive particles becomes up to 30 % larger at low velocities. The solid curve is a prediction from theory [8]. It was pointed out by Lindhard [12] that this estimate could be too low by a factor of two as only distant collisions were taken into account. The dashed line is drawn according to this revised prediction. More details of a recent measurement performed with antiprotons at LEAR [11] are presented in a talk given at this school.

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