Critical behavior of two- and three-dimensional ferromagnetic and antiferromagnetic spin-ice systems using the effective-field renormalization group technique - art. no. 014418
Aj. Garcia-adeva et Dl. Huber, Critical behavior of two- and three-dimensional ferromagnetic and antiferromagnetic spin-ice systems using the effective-field renormalization group technique - art. no. 014418, PHYS REV B, 6401(1), 2001, pp. 4418
In this work we generalize and subsequently apply the effective-field renor
malization-group (EFRG) technique to the problem of ferro- and antiferromag
netically coupled Ising spins with local anisotropy axes in geometrically f
rustrated geometries (kagome and pyrochlore lattices). In this framework, w
e calculate the various ground states of these systems and the correspondin
g critical points. Excellent agreement is found with exact and Monte Carlo
results. The effects of frustration are discussed. As pointed out by other
authors, it turns out that the spin-ice model can be exactly mapped to the
standard Ising model, but with effective interactions of the opposite sign
to those in the original Hamiltonian. Therefore, the ferromagnetic spin ice
is frustrated and does not order. Antiferromagnetic spin ice (in both two
and three dimensions) is found to undergo a transition to a long-range-orde
red state. The thermal and magnetic critical exponents for this transition
are calculated. It is found that the thermal exponent is that of the Ising
universality class, whereas the magnetic critical exponent is different, as
expected from the fact that the Zeeman term has a different symmetry in th
ese systems. In addition, the recently introduced generalized constant coup
ling method is also applied to the calculation of the critical points and g
round-state configurations. Again, a very good agreement is found with exac
t, Monte Carlo, and renormalization-group calculations for the critical poi
nts. Incidentally, we show that the generalized constant coupling approach
can be regarded as the lowest-order limit of the EFRG technique, in which c
orrelations outside a frustrated unit are neglected, and scaling is substit
uted by strict equality of the thermodynamic quantities.