Chemical Physics of Intercalation II by Guy Ouvrard (auth.), Patrick Bernier, John E. Fischer,

By Guy Ouvrard (auth.), Patrick Bernier, John E. Fischer, Siegmar Roth, Stuart A. Solin (eds.)

This quantity offers a checklist of the second one ASI at the topic "Chemical Physics of Intercalation", which used to be patterned after its hugely profitable July 1987 predecessor. A growing to be group of chemists, physicists and fabrics scientists has come to understand the application of extending the intercalation idea to everyday guest-host compounds and stable options. The unifying subject matters are the advanced section equilibria which outcome from the contest among repulsive and tasty interactions among and in the visitor and host substructures, the tunability of houses by means of keep watch over of visitor focus and superlattice periodicity, and the wide spectrum of power functions which those fabrics may supply. The luck of this initiative should be judged via noting the enlarged scope of fabrics coated during this quantity compared to its predecessor. the current quantity covers the spectrum from third-dimensional oxides, 2-dimensional classical layer intercalates,- dimensional doped polymers and zero-dimensional doped fullerene lattices. Hybrid platforms comparable to polymers in layer hosts and nonporous hosts also are handled. numerous chapters offer worldwide unifying viewpoints via focussing on offered kingdom chemical elements, delivery and optical homes, the prevalence of superconductivity, etc.

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Gopalakrishnan, J. Solid State Chem. 42:217 (1982) 14. M. G. Thomas, W. I. David, J. B. Goodenough and P. Groves, Mat. Res. Bull. 20:1137 (1985) 15. A. Maazaz and C. Delmas, C. R. Acad. Sci. 295:759 (1982) 16. L. Blandeau, G. Ouvrard, Y. Calage, R. Brec and J. Rouxel, J. Phys. C: Solid State Physics 20:4271 (1987) 17. R. Brec, A. Dugast and A. LeMehaute, Mat. Res. Bull. 15:619 (1980) 18. A. Dugast, R. Brec, G. Ouvrard and J. Rouxel, Solid State lonics 5:375 (1981) 19. P. Gard, C. Sourisseau, G.

It describes well experimental B c2 ( 0) data as is shown for some examples in Fig. 9. 54 K) e- 100 _ 300 o 40 8: 20 N ... '. '--:-';=---'-_-:-'. 4 100 O~~~ o __~~__~~__L-~ 30 60 8 (deg) 120 Figure 9. 73 K). The inset shows the determination ofT c from a transition curve [32], [32] (Fig. 10). This may be indicative for a partial type I behaviour depending on the orientation in the magnetic field (for 0 = 0° ± 50°). 54 K) [32]. 8 (K) Figure 11. Linear temperature dependence of upper critical field curves for CsKHg at different pressures [20].

Bull. 15:1797 (1980) 13. K. Vidyasagar and J. Gopalakrishnan, J. Solid State Chem. 42:217 (1982) 14. M. G. Thomas, W. I. David, J. B. Goodenough and P. Groves, Mat. Res. Bull. 20:1137 (1985) 15. A. Maazaz and C. Delmas, C. R. Acad. Sci. 295:759 (1982) 16. L. Blandeau, G. Ouvrard, Y. Calage, R. Brec and J. Rouxel, J. Phys. C: Solid State Physics 20:4271 (1987) 17. R. Brec, A. Dugast and A. LeMehaute, Mat. Res. Bull. 15:619 (1980) 18. A. Dugast, R. Brec, G. Ouvrard and J. Rouxel, Solid State lonics 5:375 (1981) 19.

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