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Phase diagram of the Ising antiferromagnet with nearest-neighbor and next-nearest-neighbor interactions on a square lattice
The phase diagram of the Ising model in the presence of nearest-neighbor ( J 1 ) and next-nearest-neighbor ( J 2 ) interactions on a square lattice is studied within the framework of the differential operator technique. The Hamiltonian is solved by effective-field theory in finite cluster (we have c...
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Published in: | Physics letters. A 2008-02, Vol.372 (8), p.1180-1184 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The phase diagram of the Ising model in the presence of nearest-neighbor (
J
1
) and next-nearest-neighbor (
J
2
) interactions on a square lattice is studied within the framework of the differential operator technique. The Hamiltonian is solved by effective-field theory in finite cluster (we have chosen
N
=
4
spins). We have proposed a functional for the free energy (similar to Landau expansion) to obtain the phase diagram in the (
T
,
α
) space (
α
=
J
2
/
J
1
), where the transition line from the superantiferromagnetic (SAF) to the paramagnetic (P) phase is of first-order in the range
1
/
2
<
α
<
0.95
in contrast to previous study of CVM (Cluster Variational Method) that predict first-order transition for
α
=
1.0
. Our results for
α
=
1.0
are in accordance with MC (Monte Carlo) simulations, that predict a second-order transition. |
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ISSN: | 0375-9601 1873-2429 |
DOI: | 10.1016/j.physleta.2007.09.059 |