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Operator isotropic exchange

The isotropic exchange discussed so far represents only a portion of the total exchange interaction operating in binuclear and oligonuclear systems. [Pg.642]

The scalar product in the isotropic exchange operator can be expressed by using the shift (step-up and step-down) operators... [Pg.702]

The isotropic exchange operator does not contain the extra electron so that it projects only to the subspace of genuine spin functions /0) = SaSbScSabSM) with the usual matrix elements as listed in Table 11.4. In the case of an isosceles triangle the eigenvalues reduce to a simple formula... [Pg.790]

The conventional interaction which is usually assumed to take place between RE-ions and conduction electrons is the isotropic exchange interaction of the form -IJnsSii. Here s, S t denote the conduction electron and RE-ion spin. In terms of electron creation and annihilation operators c, Cka the interaction hamiltonian is written as... [Pg.314]

The B% can be directly expressed in terms of /-operator products. Within the formalism just outlined the spherical Coulomb interaction is specified by (A, S) = (0, 0) with / = /. The isotropic exchange interaction with a q-independent /ex is characterized by A, S) = (0, 1) and / = / = 0. yl = 0 implies that it is not depending on the orbital moment and 2 = 1 states that the spin part transforms like a vector (tensor of rank equal to one). [Pg.315]

The physical meaning of and f L.., is obvious they govern the relaxation of rotational energy and angular momentum, respectively. The former is also an operator of the spectral exchange between the components of the isotropic Raman Q-branch. So, equality (7.94a) holds, as the probability conservation law. In contrast, the second one, Eq. (7.94b), is wrong, because, after substitution into the definition of the angular momentum correlation time... [Pg.254]

In noncubic materials, A must be replaced by the 3x3 exchange-stiffness tensor A v, and the energy is X J A v dM/dxy dM/dxv dV. Here the indices ju and v denote the spatial coordinates x, y, and z of the bonds. The energy is anisotropic with respect to the nabla operator = d/d (bond anisotropy) but isotropic with respect to the magnetization M. By contrast, the relativistic anisotropic exchange Xa i Ha(i VMa VMP dV is isotropic with respect to V but anisotropic with respect to M. [Pg.48]

The spin-spin interaction is not necessarily restricted to quadratic terms in the spin operators. Higher-order terms could be considered, among which the (isotropic) biquadratic exchange reads... [Pg.581]

The expressions assumed for the angular dependence of the free energy and the simple relations (eq. 6.42) between the coefficients k/" and Bf" are strictly valid only in the limit where the anisotropy is much smaller than the isotropic two-ion exchange interaction. Under these conditions the expectation values of the Stevens operators renormalize with temperature in the straight-forward manner calculated by Callen and Callen (1%5, 1966) ... [Pg.451]

Eu +, Gd +, Tb + ions have a half-filled 4f-shell with zero total orbital moment and spin 5 = I in the ground state. The pure spin magnetic moment of 5-ions is represented by an operator is =gfJ,BS with the g-value close to 2. The exchange interaction of 5-ions is supposed to be isotropic and is presented in the Heisenberg form ... [Pg.342]


See other pages where Operator isotropic exchange is mentioned: [Pg.184]    [Pg.279]    [Pg.277]    [Pg.611]    [Pg.79]    [Pg.555]    [Pg.633]    [Pg.643]    [Pg.692]    [Pg.831]    [Pg.5150]    [Pg.238]    [Pg.581]    [Pg.286]    [Pg.87]    [Pg.23]    [Pg.179]    [Pg.70]    [Pg.288]    [Pg.306]    [Pg.288]    [Pg.160]    [Pg.677]    [Pg.417]    [Pg.113]    [Pg.10]    [Pg.48]    [Pg.98]    [Pg.57]    [Pg.35]    [Pg.288]    [Pg.456]    [Pg.112]    [Pg.475]    [Pg.69]    [Pg.16]    [Pg.43]    [Pg.21]    [Pg.258]    [Pg.429]   
See also in sourсe #XX -- [ Pg.643 ]




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