Spin dynamics of triangular spin tubes
暂无分享,去创建一个
[1] H. Koo. On the cause for the no spin-gap behavior of the triangular spin tube system CsCrF4 , 2012 .
[2] T. Sakai,et al. Spin-chirality separation and S 3 symmetry breaking in the magnetization plateau of the quantum spin tube , 2011, 1109.0063.
[3] Y. Narumi,et al. Effects of Geometrical Spin Frustration on Triangular Spin Tubes Formed in CsCrF4 and α-KCrF4 , 2011 .
[4] S. Nishimoto,et al. Spin gap of the three-leg S = 3 2 Heisenberg tube , 2011, 1102.4559.
[5] Graham N. Newton,et al. Heat capacity reveals the physics of a frustrated spin tube. , 2010, Physical Review Letters.
[6] Y. Hirai,et al. Spin-Liquid State Study of Equilateral Triangle $S=3/2$ Spin Tubes Formed in CsCrF4 , 2009 .
[7] T. Sakai,et al. Field-induced quantum phase transitions of the asymmetric three-leg spin tube , 2008, 0807.4769.
[8] S. Nishimoto,et al. Low-lying excitations of the three-leg spin tube: A density-matrix renormalization group study , 2008, 0806.2474.
[9] T. Sakai,et al. Vector chirality and inhomogeneous magnetization in frustrated spin tubes in high magnetic fields , 2006, cond-mat/0611549.
[10] F. Mila,et al. Frustrated three-leg spin tubes: from spin 1/2 with chirality to spin 3/2 , 2005, cond-mat/0509217.
[11] L. Cronin,et al. Magnetic characterization of the frustrated three-leg ladder compound [(CuCl2tachH)3Cl]Cl2 , 2004, cond-mat/0403548.
[12] H. Manaka,et al. Crossover from S=1/2 to S=1 Haldane state in the ferromagnetic and antiferromagnetic alternating Heisenberg chain system (CH 3 ) 2 CHNH 3 CuCl 3 observed with EPR at 24 GHz , 2000 .
[13] Minoru Takahashi,et al. Three-Leg Antiferromagnetic Heisenberg Ladder with Frustrated Boundary Condition; Ground State Properties , 1997, cond-mat/9709271.
[14] J. Pannetier,et al. Ordered magnetic frustration: X. Magnetic structure of α-KCrF4 at 1.5 K , 1987 .
[15] S. Fujiki,et al. Nonlinear Susceptibility in the Spin Glass , 1981 .
[16] Philip W. Anderson,et al. Resonating valence bonds: A new kind of insulator? , 1973 .