By F. Pobell (auth.), Samuel B. Trickey, Wiley P. Kirk, James W. Dufty (eds.)
The current quantity represents the good majority of the papers awarded on Sanibel Island on the first Symposium on Quantum information and Many-Body difficulties (January 26-29, 1975). In his Introductory feedback, Professor Lawdin outlines the heritage of the unique Symposia, and the genesis of the convention whose papers contain this quantity. We subscribe to him in his expression of thank you, and observe, also, our gratitude to him and to Professors N. Y. Ohrn, J. R. Sabin, E. D. Adams, and John Daunt. The papers are grouped a little bit in a different way from their order of presentation. It appeared handy to start with the six papers which care for sound propagation in a single shape or one other, then have a two-paper diversion into sturdy Helium. The SHe superf1uid subject matter is picked up back with 4 papers on spin dynamics, orbit waves, etc., via a range of 5 papers on numerous experimental and theoretical features of the SHe superf1uid challenge. paintings within the parts of movies, mono1ayers, and combos is gifted subsequent, via papers on liquid ~He. We finish with a range of six papers on different quantum fluids and normal statistical mechanics. we're so much thankful to the members to this quantity for his or her persistence and cooperation; they've got had as editors 3 utter newbies! we've got discovered a lot, either scientifically and editorially. we are hoping that this quantity could be of a minimum of a few support to others as well.
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Extra resources for Quantum Statistics and the Many-Body Problem
W. Serene, P. G. de Gennes, P. Wolfle, and J. W. Wilkins for helpful discussions of the theory. We are grateful to H. A. Fairbank and E. K. Riedel for a critical reading of the manuscript. References (1) D. D. Osheroff, W. J. Gully, R. C. Richardson and D. M. Lee, Phys. Rev. Lett. 29, 920 (1972). (2) A. J. Leggett, Ann. Phys. (New York) 85, 11 (1974). (3) P. W. Anderson and P. Morel, Phys. Rev. 123, 1911 (1961). (4) P. W. Anderson and W. F. Brinkman, Phys. Rev. Lett. 30, 1108 (1973) • (5) P. G.
Ketterson, preprint; Pat R. Roach, B. M. Abraham, P. D. Roach, and J. B. Ketterson, preprint. (13) W. J. Gully, D. D. Osheroff, D. T. Lawson, R. C. Richardson and D. M. Lee, Phys. Rev. A~, 1633 (1973). (14) V. Ambegaokar and N. D. Mermin, Phys. Rev. Lett. 30, 81 (1973). SOUND PROPAGATION AND ANISOTROPY 33 (15) D. T. Lawson, W. J. Gully, S. Goldstein, R. C. Richardson and D. M. Lee, Phys. Rev. Lett. 30, 541 (1973), and J. Low Temp. Phys. 15, 169 (1974). (16) R. Balian and N. R. Werthamer, Phys. Rev.
None of these effects have been observed for 6 = O. 1 cm- l ) in the attenuation occurs. Fig. 4 shows these attenuation steps for 6 = 0 and 6 = 90°. The steps shown for 6 = 0 in Fig. 4 are highly reproducible and are of the same magnitude for both warming and cooling through the B transition. At 6 = 90° we find that the attenuation increase on warming through the B transition may differ by more than a factor of two from the previous transition on cooling at the same temperature. Cooling transition signatures, however, agree quite well with the immediately preceding transition on warming.
Quantum Statistics and the Many-Body Problem by F. Pobell (auth.), Samuel B. Trickey, Wiley P. Kirk, James W. Dufty (eds.)