Ground state properties of spinless extended Falicov-Kimball model on a triangular lattice with finite magnetic field

2017 ◽  
Author(s):  
Umesh K. Yadav
Keyword(s):  
Magnetic Field ◽  
Triangular Lattice ◽  
Ground State ◽  
Ground State Properties

Ground-state properties of theS=1/2 Heisenberg antiferromagnet on a triangular lattice

1990 ◽  
Vol 42 (7) ◽  
pp. 4800-4803 ◽  
Author(s):  
Th. Jolicoeur ◽  
E. Dagotto ◽  
E. Gagliano ◽  
S. Bacci
Keyword(s):  
Triangular Lattice ◽  
Ground State ◽  
Heisenberg Antiferromagnet ◽  
Ground State Properties

STABILITY OF SKYRMIONS IN THE FRUSTRATED ANTIFERROMAGNETIC/FERROELECTRIC BILAYERS WITH THE TRIANGULAR LATTICE

2021 ◽  
Vol 0 (1) ◽  
pp. 17-22
Author(s):  
I.F. SHARAFULLIN ◽  
◽  
A.R. YULDASHEVA ◽  
N.M. NUGAEVA ◽  
H.T. DIEP ◽  
...  
Keyword(s):  
Magnetic Field ◽  
External Magnetic Field ◽  
Triangular Lattice ◽  
Ground State ◽  
Steepest Descent Method ◽  
Magnetic Phase Transitions ◽  
Magnetoelectric Interaction ◽  
Spin Configuration ◽  
Ferroelectric Layer ◽  
Antiferromagnetic Layer

The formation and conditions of stability of a skyrmions at the interface between a ferroelectric layer and antiferromagnetic layer with triangilar lattice and its phase transition are studied. All interactions between spins and polarizations are limited to nearest neighbors (NN). The antiferromagnetic exchange interaction among the spins inside antiferromagnetic layer will compete with the perpendicular interface interaction between adjacent layers. The ground state spin configuration at zero temperature is calculated by using the numerical high performance steepest descent method. The resulting configuration is non-collinear. Small values of external field yields small values of angles between spins in the plane so that the ground state configurations have antiferromagnetic and non collinear domains. We observe the creation of single spin vortices. We noted that for zero applied magnetic field the skyrmions in the antiferromagnetic/ferroelectric bilayers with triangular lattice can be created in the region of interface magnetoelectric interaction value between 0.85 and 1.95. The strong external magnetic field applied perpendicular to the interface with non-collinear Dzyaloshinskiy-Morya-like magnetoelectric interaction at the interface leads to remove the skyrmion phase and magnetic phase transitions. With increasing the interface magnetoelectric coupling, the skyrmion lattice disappear. We found the formation perfect skyrmion structure at non-zero external magnetic field and moderate values of magnetoelectric interaction. The skyrmions structure is stable in a large region of the interface magnetoelectric interaction between antiferromagnetic and ferroelectric films. The results of Monte Carlo simulations that we carried out confirm that observed skyrmions are stable up to a finite temperature.

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