We analyze the momentum dependence of static susceptibilities of layered local-moment systems below Curie (Neel) temperature within the 1/S expansion, the renormalization-group (RG) approach, and the first order of the 1/N expansion. We argue that already at sufficiently low temperatures the previously known results of the spin-wave theory and RG approach for the transverse spin susceptibility acquire strong corrections, which appear due to the interaction of the incoming magnon having momentum q with virtual magnons having momenta k<q. Such corrections cannot be treated in the standard RG approach but can be described by both 1/S and 1/N expansions. The results of these expansions can be successfully extrapolated to T=TM, yielding the corr...
We consider a system of parallel layers of a metallic spin glass (such as CuMn) of width $w$ separat...
We develop a self-consistent relativistic disordered local moment (RDLM) scheme aimed at describing ...
The use of the classical Heisenberg model which incorporates only transverse spin degrees of freedom...
publisher[Abstract] Thermal expansion in quasi one-dimensional (1-D) weakly and nearly antiferromagn...
The basic issues of renormalization group (RG) theory, i.e. universality, crossover phenomena, relev...
We discuss the magnetic properties of the Hubbard model in honeycomb lattice layers. A ground state ...
A field theoretical description for the static crossover in dipolar ferromagnets is presented. New n...
We develop a finite-temperature perturbation theory for quasi-one-dimensional quantum spin systems, ...
The influence of the nonlinearity of the spin equations of motion on the dynamic structure factor of...
The response of a disordered interacting electron gas to a time and spatially varying magnetic field...
An explicit self-consistent calculation of the zero-point (ZP) and thermally excited (TE) contributi...
The temperature dependence of the longitudinal magnetization as well as the longitudinal susceptibil...
We employ a recently developed variant of the functional renormalization group method for spin syste...
SIGLEAvailable from British Library Document Supply Centre- DSC:8053.4153(RAL--90-029) / BLDSC - Bri...
We determine the magnetic susceptibility of thermal QCD matter by means of first principles lattice ...
We consider a system of parallel layers of a metallic spin glass (such as CuMn) of width $w$ separat...
We develop a self-consistent relativistic disordered local moment (RDLM) scheme aimed at describing ...
The use of the classical Heisenberg model which incorporates only transverse spin degrees of freedom...
publisher[Abstract] Thermal expansion in quasi one-dimensional (1-D) weakly and nearly antiferromagn...
The basic issues of renormalization group (RG) theory, i.e. universality, crossover phenomena, relev...
We discuss the magnetic properties of the Hubbard model in honeycomb lattice layers. A ground state ...
A field theoretical description for the static crossover in dipolar ferromagnets is presented. New n...
We develop a finite-temperature perturbation theory for quasi-one-dimensional quantum spin systems, ...
The influence of the nonlinearity of the spin equations of motion on the dynamic structure factor of...
The response of a disordered interacting electron gas to a time and spatially varying magnetic field...
An explicit self-consistent calculation of the zero-point (ZP) and thermally excited (TE) contributi...
The temperature dependence of the longitudinal magnetization as well as the longitudinal susceptibil...
We employ a recently developed variant of the functional renormalization group method for spin syste...
SIGLEAvailable from British Library Document Supply Centre- DSC:8053.4153(RAL--90-029) / BLDSC - Bri...
We determine the magnetic susceptibility of thermal QCD matter by means of first principles lattice ...
We consider a system of parallel layers of a metallic spin glass (such as CuMn) of width $w$ separat...
We develop a self-consistent relativistic disordered local moment (RDLM) scheme aimed at describing ...
The use of the classical Heisenberg model which incorporates only transverse spin degrees of freedom...