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  • 1970-1974  (2)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 238 (1970), S. 121-129 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The “conserving and self-consistent” approximation scheme of Kadanoff and Baym is generalized to systems of particles of non-zero spin. The additional conservation law of the total spin of the system restricts the possible approximations for the self-energy part, and thus the approximations for the irreducible vertex part occuring in the equation for the correlation function. This guarantees, for instance, the correct behavior of the dynamical susceptibility in the long wave length limit. Two examples are discussed under these aspects: the Hartree-Fock and theT-matrix approximation for the self-energy part and the resulting susceptibility.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 4 (1971), S. 79-95 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The self-consistent and “conserving” (in particular the total spin is conserved) approximation scheme, developed in a previous paper for itinerant ferromagnetism, is extended to the region below the phase-transition point. The former general condition for the transformation properties of any approximate self-energy part with regard to infinitesimal transformations in spin space is applied to the case where the transformation is a finite rotation in spin space; these rotations correspond to rotations of the direction of the spontaneous magnetization which is fixed here by an infinitesimal auxiliary fieldH. This transformation property of the self-energy part ensures that the equations determining the corresponding Green's and correlation functions are covariant in form with respect to rotations ofH. Two examples are considered: the “Hartree-Fock” and the “particle-hole T-matrix” approximations for the contact interaction or Hubbard model. In the first example the resulting susceptibilities are shown to be causal response functions, provided the Stoner equation is fulfilled. In the second example the self-energy part and theT matrix are discussed for the two cases whereH is parallel and perpendicular to the axis of spin quantization. In fact, these expressions can be transformed into each other by means of the corresponding rotation matrix in spin space.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
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