TY - JOUR
T1 - Spiral antiferromagnets beyond the spin-wave approximation
T2 - Frustrated X y and Heisenberg models on the honeycomb lattice
AU - Di Ciolo, Andrea
AU - Carrasquilla, Juan
AU - Becca, Federico
AU - Rigol, Marcos
AU - Galitski, Victor
PY - 2014/3/19
Y1 - 2014/3/19
N2 - We examine the stability of classical states with a generic incommensurate spiral order against quantum fluctuations. Specifically, we focus on the frustrated spin-1/2 XY and Heisenberg models on the honeycomb lattice with nearest-neighbor J1 and next-nearest-neighbor J2 antiferromagnetic couplings. Our variational approach is based on the Jastrow wave functions, which include quantum correlations on top of classical spin waves. We perform a systematic optimization of wave vectors and Jastrow pseudopotentials within this class of variational states and find that quantum fluctuations favor collinear states over generic coplanar spirals. The Néel state with Q=(0,0) extends its stability well beyond the classical value J2/J1=1/6. Most importantly, the collinear states with Q=(0,2π/3) (and the two symmetry-related states) are found to be stable in a large regime with intermediate frustration, while at the classical level they are limited to the point J2/J1=0.5. For large frustration, the 120â̂̃ state is stabilized for finite values of J2/J1 in both models.
AB - We examine the stability of classical states with a generic incommensurate spiral order against quantum fluctuations. Specifically, we focus on the frustrated spin-1/2 XY and Heisenberg models on the honeycomb lattice with nearest-neighbor J1 and next-nearest-neighbor J2 antiferromagnetic couplings. Our variational approach is based on the Jastrow wave functions, which include quantum correlations on top of classical spin waves. We perform a systematic optimization of wave vectors and Jastrow pseudopotentials within this class of variational states and find that quantum fluctuations favor collinear states over generic coplanar spirals. The Néel state with Q=(0,0) extends its stability well beyond the classical value J2/J1=1/6. Most importantly, the collinear states with Q=(0,2π/3) (and the two symmetry-related states) are found to be stable in a large regime with intermediate frustration, while at the classical level they are limited to the point J2/J1=0.5. For large frustration, the 120â̂̃ state is stabilized for finite values of J2/J1 in both models.
UR - http://www.scopus.com/inward/record.url?scp=84897898702&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84897898702&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.89.094413
DO - 10.1103/PhysRevB.89.094413
M3 - Article
AN - SCOPUS:84897898702
SN - 1098-0121
VL - 89
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 9
M1 - 094413
ER -