Quantum critical point in the spin glass-antiferromagnetism competition for fermionic Ising Models
arXiv:cond-mat/0505072 · doi:10.1016/j.physa.2005.05.080
Abstract
The competition between spin glass () and antiferromagnetic order () is analyzed in two sublattice fermionic Ising models in the presence of a transverse and a parallel magnetic fields. The exchange interaction follows a Gaussian probability distribution with mean and standard deviation , but only spins in different sublattices can interact. The problem is formulated in a path integral formalism, where the spin operators have been expressed as bilinear combinations of Grassmann fields. The results of two fermionic models are compared. In the first one, the diagonal operator has four states, where two eigenvalues vanish (4S model), which are suppressed by a restriction in the two states 2S model. The replica symmetry ansatz and the static approximation have been used to obtain the free energy. The results are showing in phase diagrams ( is the temperature) {\it versus} , , and . When is increased, (transition temperature to a nonergodic phase) reduces and the Neel temperature decreases towards a quantum critical point. The field always destroys ; however, within a certain range, it favors the frustration. Therefore, the presence of both fields, and , produces effects that are in competition. The critical temperatures are lower for the 4S model and it is less sensitive to the magnetic couplings than the 2S model.
15 pages, 6 figures, accepted in Physica A
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Cited by in corpus (7)
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- Inverse freezing in the Hopfield Fermionic Ising Spin Glass
- A theoretical study of the cluster glass-Kondo-magnetic disordered alloys
- Antiferromagnetic Ising spin glass competing with BCS pairing interaction in a transverse field
- One-step replica symmetry breaking solution for a highly asymmetric two-sublattice fermionic Ising spin glass model in a transverse field
- Stability conditions for fermionic Ising spin-glass models in the presence of a transverse field
- The spin glass-antiferromagnetism competition in Kondo-lattice systems in the presence of a transverse applied magnetic field