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Huckel Hamiltonian

Finally, we should come back to Eq. (2) in the introduction. We learn that the scaling relations are a unique property of the Huckel Hamiltonian. Even the simplest extension, such as introduction of the variable P approximation, invalidates the scaling. This is certainly not a good news from the point of view of the practical applications. Still, the author believes that the appealing simplicity of the Huckel Hamiltonian makes it worthwhile to investigate, even if just for the pure fun of mathematical adventure. [Pg.98]

The results of a study of the Huckel Hamiltonian enabled the following classification of the shape of the total energy per unit cell, E, as function of the asyimetric distortion. A, of the chain (i) E 1 1 It yA (Peierls case) (ii)... [Pg.106]

We may immediately construct the Huckel Hamiltonian-matrix for butadiene it is going to be 4 x 4. The Coulomb integral, a, will occur along the diagonal since all atoms in the conjugated system are carbon and the only resonance integrals, p, which are non-zero are those between centres which are bonded. Thus the (1-2)-, (2-3)-, and (3-4)-elements are p, and so also, of course, are the (2-1)-, (3-2)-, and (4-3)-elements—the matrix must clearly be symmetrical since, if atom i is joined to atom j, then certainly atom j is joined to atom i Thus we have, with the vertex labelling adopted in Fig. 2-6,... [Pg.23]

The standard extended Huckel Hamiltonian (23) with a minimum basis set of Slater-type atomic orbitals were used in all calculations. The overlap and Hamiltonian matrices were computed for the RC fragment in the light conformation (12), which included Bph Qa Qb, the iron ion and the relevant protein environment Met , Met , His ,... [Pg.110]

Fig. 4. Eigenvalues of the Huckel Hamiltonian for linear polyacetylene with 10,000 atoms as a function of (a = 0, 8 = — 1, t = 0.2) PT 0 is the zeroth order energy, PT 1 is the energy to hrst order. Fig. 4. Eigenvalues of the Huckel Hamiltonian for linear polyacetylene with 10,000 atoms as a function of (a = 0, 8 = — 1, t = 0.2) PT 0 is the zeroth order energy, PT 1 is the energy to hrst order.
Note that if all the Yf,n are neglected, the standard Hubbard Hamiltonian results with its correlation parameter, U. (By the way, the U term, although a two electron term, is contained within the standard HF approximation, so a quantum chemist would not label it a correlation term, but a Coulomb term). Note further that if U is neglected in addition to Ynn general Huckel Hamiltonian results. [Pg.96]

The essence of this model is as follows. If the system lies in the xy plane, the underlying basis set consists of the 2p atomic orbitals of the atoms, that is, each atom contributes by a single orbital of symmetry n. The model remains strictly in the one-electron scheme, which means that it does not take into account any electron-electron interaction explicitly. Consequently, the Huckel Hamiltonian has the form of a one-electron Hamiltonian ... [Pg.66]

Let us specify the Huckel Hamiltonian for some important special cases. [Pg.68]

A system is called one-dimensional if its atoms form a chain, i.e., there is no branching in the molecular graph. As noted above, the Huckel Hamiltonian is insensitive to the geometrical arrangement, thus a geometrically bent or twisted system, in principle, can be considered as (quasi)one-dimensional. Under this condition, numbering the atoms in the chain consecutively from one end to... [Pg.68]

In the Htickel-Lewis family of methods, we use the fact that the Huckel Hamiltonian is versatile, so electrons can be localized by simply zeroing out some terms in a modified Hamiltonian matrix. This terms are those that correspond to single bonds in a Lewis stmcture. The new Hamiltonian leads to eigenvectors that correspond to local orbitals, and corresponding eigenvalues are also obtained. The wave function that describes the ith structure, is again a Slater determinant, obtained by distributing the electrons in the appropriate local orbitals. [Pg.343]

DOS and COOP plots for a single layer of MnP with the geometry given in 16.52. These are calculations using an extended Huckel Hamiltonian. The dotted line indicates the Fermi level for a nonmagnetic metallic state. [Pg.457]

In the Huckel tight-binding framework, the Hamiltonian is represented in matrix form for describing the electronic structure. The interactions are only accounted for between the / -orbitals, the basis functions of the p -orbitals are assumed orthonormal. The electronic interactions happen only between nearest neighbor sites. Thus, the Huckel Hamiltonian matrix is... [Pg.11]


See other pages where Huckel Hamiltonian is mentioned: [Pg.134]    [Pg.134]    [Pg.15]    [Pg.106]    [Pg.366]    [Pg.192]    [Pg.460]    [Pg.84]    [Pg.355]    [Pg.98]    [Pg.18]    [Pg.343]    [Pg.361]    [Pg.392]    [Pg.323]    [Pg.115]    [Pg.12]    [Pg.13]   
See also in sourсe #XX -- [ Pg.474 ]

See also in sourсe #XX -- [ Pg.17 , Pg.354 , Pg.362 , Pg.363 , Pg.371 , Pg.377 ]




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