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Exchange interaction, model

AEI Atomic exchange interaction (model) LMTO Linear muffin-tin orbital (method)... [Pg.515]

Our treatment so far has dealt with non-interacting electrons, yet we know for sure that electrons do interact with each other. Dirac (1930b) studied the effects of exchange interactions on the Thomas-Fermi model, and he soon discovered that this effect could be modelled by adding an extra term... [Pg.214]

The Lines approximation is expected to be quite accurate for the description of the exchange interaction between a strongly axial doublet and an arbitrary isotropic spin. For all other cases, the Lines model [84] is a reasonable approximation. Efficient implementation of the Lines model was done in the program POLY ANISO. [Pg.170]

Anisotropic exchange interaction within the Lines model described above. Dipole-dipole magnetic interaction between centres is calculated fully ah initio and is added to the exchange matrix. [Pg.172]

Ferromagnetic ordering of two-dimensional systems with dipole-dipole and exchange interactions in the approximation of a spherical model was examined in Ref. 73. The main simplifying assumption of the spherical model is the replacement of the condition er = 1 on the orientation vectors with the weaker condition... [Pg.24]

Let us now consider interpretation ii). Its pertinence was essentially discussed on the basis of a relation between the value of the rate k j and that of an exchange parameter J. This parameter characterizes the exchange interactions that take place between the P and H radicals when electron transfer is blocked beyond H. J was estimated to be about 10 cm from different experiments performed in R. sphaeroides [177, 178]. In Sect. 2.2.1, we have described a simplified model leading to relation (16) between the exchange parameter J and the electronic factor Tab, but we shall see that this relation cannot be applied to the primary electron transfer, due to the existence of numerous low-energy charge-transfer states. [Pg.36]

The Xa multiple scattering method generates approximate singledeterminant wavefunctions, in which the non-local exchange interaction of the Hartree-Fock method has been replaced by a local term, as in the Thomas-Fermi-Dirac model. The orbitals are solutions of the one-electron differential equation (in atomic units)... [Pg.60]


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