Correlations, Coherence, and Order by V. L. Aksenov, V. S. Shakhmatov (auth.), Diana V. Shopova,

By V. L. Aksenov, V. S. Shakhmatov (auth.), Diana V. Shopova, Dimo I. Uzunov (eds.)

This quantity includes a selection of evaluation articles which are prolonged types of invited lectures given on the First Pamporovo wintry weather Workshop on Cooperative Phe­ nomena in Condensed topic held in villa "Orlitza" (7th-15th March 1998, Pamporovo Ski inn, Bulgaria). chosen examine works stated on the Workshop were released within the magazine of actual reviews - a brand new overseas magazine for examine papers in experimental and theoretical physics (Lviv college, Lviv, Ukraine). those experiences are meant to be prestige studies and current new insights won from the swiftly constructing examine of remarkable difficulties in condensed subject physics similar to structural houses and part transitions in fullerene crystals, great­ conductivity ofstrongly interacting electrons in copper oxides, spin polarized Fermi liq­ uids, chaotic vortex filaments in superfluid turbulent Helium-II, desorption triggered through digital transitions in ionic compounds, fluctuation phenomena in superconductors, and quantum severe phenomena in low dimensional magnets and quantum beverages. we've got set the fabric in accordance with the alphabetic order of authors' names even supposing the hot temperature superconductivity seems the not easy kernel in condensed topic physics. The authors have taken care to provide the new advances of their examine in a kind that's readable and helpful not just to specialists within the respective box, but additionally to younger scientists. for this reason the lectures comprise a entire creation to the problem and in addition a longer dialogue of methodical details.

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The present work has been performed within the State Scientific and Technical Program Fullerenes and Atomic Clusters, N 97032, supported by the INTAS-RFFI grant 95-0639 and the INTAS grant 98 MO-45. 26 REFERENCES 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. 23. 24. 25. 26. 27. 28. 29. 30. 31. H. W. Kroto, J. R. Heath, S. C. O'Brien, R. F. Curl, and R. E. Smalley, Naturd18:162 (198;»). E. Osawa, Kogaku (Kyoto), Jap. 25:854 (1970). D. A. Bochvar, and E. D. Galpern, Doklady AN SSSR 209:610 (1973).

There is no real HLTC in the IBG because of the lack of fluctuation interactions, but we can consider the crossover from HT to ZT at constant dt,nsity p > 0 produced by the change of the dimensionality from d > a to d < a. This formal dependence describes the difference between the high-dimensional (d > a) critical phenomena at finite critical temperatures and those of ZT BEC at constant density p > () and low dimensionality (d < a). 42 4. , Kadanoff and Baym (1962), and Abrikosov et a1. (1963).

In contrast, there is no such similarity between the LT T - and X -transitions. For X -transitions, the criterion (1) yields It(X)1 > MXc )] 1/" r >"(T) L , (11 ) where all quantities are defined by the change of T with X in (3) and (4). Having in millcl Eq. (2) and the fact that the critical region (lines 1 and 2 in Fig. 1) along the Xaxis is c1efined by It(X)1 < 1, it becomes evident, that in the LT range (X '" Xo), where [~o(Xc)I>"(T) < 1]' the quantum subdomain gradually enlarges when the temperature is c1ecreasecl Of, equivalently, when Xc(T) approaches X o.

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Correlations, Coherence, and Order by V. L. Aksenov, V. S. Shakhmatov (auth.), Diana V. Shopova,
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