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(b) Kuhn, C. Synth. Met. 1991, 41-43, 3681.
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(e) Aubry, S.; Quemerais, P. In Low-Dimensional Electronic Properties of Molybdenum Bronzes and Oxides; Schlenker, C., Ed.; Kluwer, Deventer, 1989.
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(g) Kanis, D. R.; Ratner, M. A.; Marks, T. J. Chem. Rev. 1994, 94, 195.
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(a) Li, Y. S.; van Daelen, M. A.; Wrinn, M.; King-Smith, D.; Newsam, J. M.; Delley, B.; Wimmer, E.; Klitsner, T.; Sears, M. P.; Carlson, G. A.; Nelson, J. S.; Allan, D. C.; Teter, M. P. J. Comput.-Aided Mater. Des. 1993, 1, 199.
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Klitsner, T.8
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Carlson, G.A.10
Nelson, J.S.11
Allan, D.C.12
Teter, M.P.13
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Some areas in which inverse design strategies are being pursued include: (a) Caudill, L. F.; Rabitz, H.; Askar, A. Inverse Problems 1994, 10, 1099.
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Askar, A.3
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(c) Dorren, H. J. S.; Muyzert, E. J.; Snieder, R. K. Inverse Problems 1994, 10, 865.
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Muyzert, E.J.2
Snieder, R.K.3
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(e) Godzik, A.; Kolinski, A.; Skolnick, J. J. Mol. Biol. 1992, 227, 227.
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Kolinski, A.2
Skolnick, J.3
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(g) Shen, L. Y.; Shi, S. H.; Rabitz, H. J. Phys. Chem. 1993, 97, 12114.
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Shi, S.H.2
Rabitz, H.3
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Vetterling, W.T.4
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0003455716
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McGraw Hill: New York
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For simplicity we discuss this design problem in the framework of an effective Hamiltonian theory, such as the tight-binding Hückel theory. Such semiempirical schemes write the diagonal and off-diagonal Hamiltonian elements as a function of atomic orbital properties and overlap integrals. As such, one can make a rough mapping from the "ideal" Hamiltonian onto "real" atoms and molecules. These schemes are described in: (a) Pople, J. A.; Beveredge, D. L. Approximate Molecular Orbital Theory; McGraw Hill: New York, 1970.
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Approximate Molecular Orbital Theory
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Beveredge, D.L.2
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Risser, S. M.; Beratan, D. N.; Marder, S. R. J. Am. Chem. Soc. 1993, 115, 7719.
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(a) Frauenfelder, H. In Structure and Dynamics of Nucleic Acids, Proteins and Membranes; Clementi, E., Chin, S., Eds.; Plenum Press: New York, 1986.
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(a) Kirkpatrick, S.; Gelatt, C. D.; Vecchi, M. P. Science 1983, 220, 671.
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Vecchi, M.P.3
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(b) Christofides, N., Mingozzi, A., Toth, P., Sandi, C., Eds. Combinatorial Optimization; Wiley-Interscience: London, 1979.
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Combinatorial Optimization
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26
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85033069728
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note
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Note that this factoring strategy is different from three-dimensional Euler angle strategies. Extension of the Euler strategy to higher dimensions is not directly performed.
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27
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84950296671
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Interscience Publishers: New York
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In example 2 below, this strategy is straightforward because of the problem's ID nature. If the problem is 2D or 3D, the correspondence between wave functions and eigenvalues is not trivial; see: Courant, R.; Hilbert, D. Methods of Mathematical Physics; Interscience Publishers: New York, 1953; Vol. 2. This difficulty is avoided in the hybrid method of section II(c).
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Courant, R.1
Hilbert, D.2
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29
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85033034547
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NAG subroutine, Numerical Algorithms Group (USA)
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(b) NAG subroutine, Numerical Algorithms Group (USA).
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(a) Piela, L.; Kostrowicki, J.; Scheraga, H. A. J. Phys. Chem. 1989, 93, 3339.
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(b) Scheraga, H. A. In Abstracts of Papers, 210th National Meeting of the American Chemical Society, Chicago, IL, Fall 1995; American Chemical Society: Washington, DC, 1985; PHYS 097.
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Risser, S.1
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