Abstract
The effective Hamiltonian and the negative eigenvalue theorem are used to obtain an analytic formula for the integrated density of electron states in a linear chain with an arbitrary number of impurities within the tight binding approximation. From this formula, the analytic conditions for the existence of localized electron states lying above or below the band of states of host atoms are obtained. The way of obtaining the energies of localized states and the form of eigenvectors are also discussed.
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Skála L., Czech. J. Phys.B 26 (1976), 199.
Goodwin E. T., Proc. Cambr. Phil. Soc.35 (1939), 221.
Puszkarski H., Surf. Sci.34 (1973), 125.
Löwdin P. O., J. Appl. Phys. Suppl.33 (1962), 251.
Micha D. A.,in Advances in Quantum Chemistry Vol. 8, Academic Press, New York and London 1974.
Levy H., Lessman F., Finite Difference Equations, Sir Isaac Pitman and Sons, Ltd., London 1959.
Marcus M., Minc H., A Survey of Matrix Theory and Matrix Inequalities, Allyn and Bacon Inc., Boston 1964.
Dean P., Rev. Mod. Phys.44 (1972), 127.
Jeffreys H., Jeffreys B. S., Methods of Mathematical Physics, At the University Press, Cambridge 1946, p. 127.
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Skála, L. Analytic conditions for the existence of localized electron states in a linear chain with an arbitrary number of impurities. Czech J Phys 27, 1152–1160 (1977). https://doi.org/10.1007/BF01589006
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DOI: https://doi.org/10.1007/BF01589006