Erratum: Frustrated classical Heisenberg model in one dimension with nearest-neighbor biquadratic exchange: Exact solution for the ground-state phase diagram [Phys. Rev. B80, 012407 (2009)]

2009 ◽  
Vol 80 (22) ◽  
Author(s):  
T. A. Kaplan
1999 ◽  
Vol 06 (05) ◽  
pp. 699-704 ◽  
Author(s):  
K. YASUTANI ◽  
M. KABURAGI ◽  
M. KANG

The structures of adsorbate-induced row-type alignments of the FCC(110) surface are analyzed using the two-dimensional Blume–Emmery–Griffiths (BEG) model with the nearest-neighbor (NN) and the next-nearest-neighbor (NNN) interactions. The ground state phase diagram in whole regimes of interactions is determined by the energy comparison method. Comparing the results of ground state analysis with experimentally observed structures of the O/Rh(110) and O/Pd(110), we determine the interaction regimes for these systems. From the thus determined interaction regime, we propose the model structure in the c(2 × 6) phase of the O/Pd(110).


2017 ◽  
Vol 3 (4) ◽  
Author(s):  
Ido Niesen ◽  
Philippe Corboz

Using infinite projected entangled pair states, we study the ground state phase diagram of the spin-1 bilinear-biquadratic Heisenberg model on the square lattice directly in the thermodynamic limit. We find an unexpected partially nematic partially magnetic phase in between the antiferroquadrupolar and ferromagnetic regions. Furthermore, we describe all observed phases and discuss the nature of the phase transitions involved.


2018 ◽  
Vol 98 (5) ◽  
Author(s):  
Masanori Kishimoto ◽  
Katsuhiro Morita ◽  
Yukihiro Matsubayashi ◽  
Shigetoshi Sota ◽  
Seiji Yunoki ◽  
...  

2011 ◽  
Vol 2011 ◽  
pp. 1-6
Author(s):  
M. R. Soltani ◽  
J. Vahedi ◽  
M. R. Abolhassani ◽  
A. A. Masoudi

We have considered the 1D spin-(1/2) Heisenberg model with added Dzyaloshinskii-Moriya interaction. The effect of a uniform magnetic field on the ground state phase diagram of the model is studied. We have mapped the model to an effective model which is known as the 1D XXZ in both uniform and staggered magnetic fields. By selecting a block of two or three spins, we have solved the Hamiltonian exactly. Our results show that the quantum phase transitions can be obtained from the block of pair or three spins.


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