Critical thermodynamics of a three-dimensional chiral model for N>3
暂无分享,去创建一个
[1] M. Itakura. Monte Carlo Renormalization Group Study of the Heisenberg and the XY Antiferromagnet on the Stacked Triangular Lattice and the Chiral φ4 Model , 2003 .
[2] S. Sachdev. Order and quantum phase transitions in the cuprate superconductors , 2002, cond-mat/0211005.
[3] A. Caneschi,et al. Specific heat andμ+SRmeasurements inGd(hfac)3NITiPrmolecular magnetic chains: Indications for a chiral phase without long-range helical order , 2002, cond-mat/0210133.
[4] E. V. Orlov,et al. Chiral critical behavior of frustrated spin systems in two dimensions from five-loop renormalization-group expansions , 2002, cond-mat/0207187.
[5] M. Tissier,et al. XY frustrated systems: Continuous exponents in discontinuous phase transitions , 2001, cond-mat/0107183.
[6] S. Sachdev. Understanding correlated electron systems by a classification of Mott insulators , 2002, cond-mat/0211027.
[7] J. Gracey. Critical exponent ω at O(1/N) in O(N)×O(m) spin models , 2002, hep-th/0209053.
[8] J. Gracey. Chiral exponents in O ( N ) × O ( m ) spin models at O ( 1 / N 2 ) , 2002, cond-mat/0208309.
[9] P. Calabrese,et al. Chiral phase transitions: Focus driven critical behavior in systems with planar and vector ordering , 2002, cond-mat/0205046.
[10] M. Fiebig,et al. Interaction of frustrated magnetic sublattices in ErMnO3. , 2001, Physical review letters.
[11] A. Pelissetto,et al. Critical phenomena and renormalization-group theory , 2000, cond-mat/0012164.
[12] J. Kulda,et al. Chiral criticality in helimagnet Ho studied by polarized neutron scattering , 2001 .
[13] A. Pelissetto,et al. Chiral exponents in frustrated spin models with noncollinear order , 2001, cond-mat/0106525.
[14] P. Calabrese,et al. Critical behavior of two-dimensional frustrated spin models with noncollinear order , 2001, cond-mat/0105551.
[15] A. Pelissetto,et al. Large-n critical behavior of O(n)×O(m) spin models , 2001, hep-th/0104024.
[16] A. Peles,et al. Spin stiffness of stacked triangular antiferromagnets , 2001, cond-mat/0209056.
[17] M. Tissier,et al. AN EXACT RENORMALIZATION GROUP APPROACH TO FRUSTRATED MAGNETS , 2001, cond-mat/0101167.
[18] A. Pelissetto,et al. Critical behavior of frustrated spin models with noncollinear order , 2000, cond-mat/0007389.
[19] Visser,et al. Chiral critical exponents of the triangular-lattice antiferromagnet CsMnBr3 as determined by polarized neutron scattering , 2000, Physical review letters.
[20] Delamotte,et al. Frustrated heisenberg magnets: A nonperturbative approach , 2000, Physical review letters.
[21] A. Pelissetto,et al. Randomly dilute spin models: A six-loop field-theoretic study , 2000, cond-mat/0002402.
[22] H. Diep,et al. Critical behavior of frustrated systems: Monte Carlo simulations versus renormalization group , 2000, cond-mat/0001105.
[23] R. Folk,et al. Effective and Asymptotic Critical Exponents of Weakly Diluted Quenched Ising Model: 3d Approach Versus $ε^{1/2}$-Expansion , 1999, cond-mat/9909121.
[24] H. Kawamura. Universality of phase transitions of frustrated antiferromagnets , 1998, cond-mat/9805134.
[25] O. Petrenko,et al. Review/Synthèse: Triangular antiferromagnets , 1997 .
[26] H. Diep,et al. Phase diagram of XY antiferromagnetic stacked triangular lattices. , 1996, Physical review. B, Condensed matter.
[27] A. Sokolov,et al. Chiral transitions in three-dimensional magnets and higher order ϵ expansion , 1995, cond-mat/9803377.
[28] H. Janssen,et al. On the crossover to universal criticality in dilute Ising systems , 1995 .
[29] Antonenko,et al. Phase transitions in anisotropic superconducting and magnetic systems with vector order parameters: Three-loop renormalization-group analysis. , 1994, Physical review. B, Condensed matter.
[30] G. Zumbach. Phase transitions with O(n) symmetry broken down to O(n − p) , 1994 .
[31] T. Jolicoeur,et al. A renormalization-group study of helimagnets in D = 2 + ϵ dimensions , 1993, cond-mat/9304049.
[32] Kawamura. Erratum: Renormalization-group analysis of chiral transitions , 1990, Physical review. B, Condensed matter.
[33] H. Kawamura. Generalized Chiral Universality , 1990 .
[34] Delamotte,et al. Nonuniversality in helical and canted-spin systems. , 1990, Physical review letters.
[35] T. Mason,et al. Neutron scattering measurements of critical exponents in CsMnBr/sub 3/: A Z/sub 2/greater than or equal to/sub 1/ antiferromagnet , 1989 .
[36] Kawamura,et al. Renormalization-group analysis of chiral transitions. , 1988, Physical review. B, Condensed matter.
[37] H. Kadowaki,et al. New Critical Exponent β of the XY Antiferromagnet on Stacked Triangular Lattice, CsMnBr3 , 1988 .
[38] S. Shapiro,et al. New Universality Class of Antiferromagnetic Phase Transition in CsMnBr3 , 1988 .
[39] G. Shirane,et al. Experimental Study of New Type Phase Transition in Triangular Lattice Antiferromagnet VCl2 , 1987 .
[40] G. Parisi. Field-theoretic approach to second-order phase transitions in two- and three-dimensional systems , 1980 .
[41] Jean Zinn-Justin,et al. Critical exponents from field theory , 1980 .
[42] Jean Zinn-Justin,et al. Critical Exponents for the N Vector Model in Three-Dimensions from Field Theory , 1977 .