By Barus C.
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Additional info for Adiabatic Expansion in Case of Vanishing Increments II
Gopalakrishnan, and A. Sleight, Phys. Rev. Lett. 61 (1988) 2608.  A. W. Hewat, E. A. Hewat, P. Bordet, J. Capponi, C. Chaillout, J. -L. Hodeau, and M. Marezio, Proc. Int. Sem. HTSC Dubna 89, World Scientific, Singapore 1990, p. 24, and quotations therein.  A. R. Moodenbaugh, Y. Xu, M. Suenaga, T. J. Folkerts, andR. N. Shelton, Phys. Rev. B38 (1989)4596.  L. Mattheiss, Phys. Rev. Lett. 58 (1987)1028; A. J. Freeman and J. Yu, Helvetica phys. acta 61 (1988)401.  P. W. Anderson, Science 235 (1987)1196.
Here, Uml and VI'I are the unit vectors directing from the m- and [' -sites to the [site, respectively. The electric field of light is in the x direction. A CU 4 013 cluster is given by Fig. 9. When, 3, 4 and 5 holes are introduced into the cluster, we have 25% electron-doped system, insulator, and 25% hole-doped system, respectively. In the numerical calculation, the ground state I 0) is obtained by using the modified Lanczos method. Then, u(w) is evaluated by using the Lanczos algorithm, where the continued fraction is truncated at 200 iterations.
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Adiabatic Expansion in Case of Vanishing Increments II by Barus C.