TY - JOUR

T1 - Degeneracy and ordering of the noncoplanar phase of the classical bilinear-biquadratic Heisenberg model on the triangular lattice

AU - Korshunov, S. E.

AU - Mila, F.

AU - Penc, K.

PY - 2012/5/14

Y1 - 2012/5/14

N2 - We investigate the zero-temperature behavior of the classical Heisenberg model on the triangular lattice in which the competition between exchange interactions of different orders favors a relative angle between neighboring spins Φ (0,2π/3). In this situation, the ground states are noncoplanar and have an infinite discrete degeneracy. In the generic case, i.e., when Φπ/2,arccos(-1/3), the ground-state manifold is in one-to-one correspondence (up to a global rotation) with the set of noncrossing loop coverings of the three equivalent honeycomb sublattices into which the bonds of the triangular lattice can be partitioned. This allows one to identify the order parameter space as an infinite Cayley tree with coordination number 3. Building on the duality between a similar loop model and the ferromagnetic O(3) model on the honeycomb lattice, we argue that a typical ground state should have long-range order in terms of spin orientation. This conclusion is further supported by the comparison with the four-state antiferromagnetic Potts model [describing the Φ=arccos(-1/3) case], which at zero temperature is critical and in terms of the solid-on-solid representation is located exactly at the point of roughening transition. At Φarccos(-1/3), an additional constraint appears, whose presence drives the system into an ordered phase (unless Φ=π/2, when another constraint is removed and the model becomes trivially exactly solvable).

AB - We investigate the zero-temperature behavior of the classical Heisenberg model on the triangular lattice in which the competition between exchange interactions of different orders favors a relative angle between neighboring spins Φ (0,2π/3). In this situation, the ground states are noncoplanar and have an infinite discrete degeneracy. In the generic case, i.e., when Φπ/2,arccos(-1/3), the ground-state manifold is in one-to-one correspondence (up to a global rotation) with the set of noncrossing loop coverings of the three equivalent honeycomb sublattices into which the bonds of the triangular lattice can be partitioned. This allows one to identify the order parameter space as an infinite Cayley tree with coordination number 3. Building on the duality between a similar loop model and the ferromagnetic O(3) model on the honeycomb lattice, we argue that a typical ground state should have long-range order in terms of spin orientation. This conclusion is further supported by the comparison with the four-state antiferromagnetic Potts model [describing the Φ=arccos(-1/3) case], which at zero temperature is critical and in terms of the solid-on-solid representation is located exactly at the point of roughening transition. At Φarccos(-1/3), an additional constraint appears, whose presence drives the system into an ordered phase (unless Φ=π/2, when another constraint is removed and the model becomes trivially exactly solvable).

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U2 - 10.1103/PhysRevB.85.174420

DO - 10.1103/PhysRevB.85.174420

M3 - Article

AN - SCOPUS:84861674457

VL - 85

JO - Physical Review B-Condensed Matter

JF - Physical Review B-Condensed Matter

SN - 0163-1829

IS - 17

M1 - 174420

ER -