Soliton excitation in a one-dimentional antiferromagnetic-chain with bond alternation
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Soliton excitation in a one-dimentional antiferromagnetic-chain with bond alternation
Acta Scientiarum Naturalium Universitatis SunYatseniVol. 55, Issue 3, Pages: 89-96(2016)
作者机构:
华南师范大学物理与电信工程学院,广东,广州,510006
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Published:2016,
Published Online:25 May 2016,
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WANG Sen. Soliton excitation in a one-dimentional antiferromagnetic-chain with bond alternation. [J]. Acta Scientiarum Naturalium Universitatis SunYatseni 55(3):89-96(2016)
DOI:
WANG Sen. Soliton excitation in a one-dimentional antiferromagnetic-chain with bond alternation. [J]. Acta Scientiarum Naturalium Universitatis SunYatseni 55(3):89-96(2016)DOI:
Soliton excitation in a one-dimentional antiferromagnetic-chain with bond alternation
The soliton excitation of a onedimensional Heisenberg antiferromagnetic chain with bond alternation was studied. In the Hamiltonian of this antiferromagnetic model
the interactions between the nearest neighbor lattice and next nearest neighbor lattice,Dzyaloshinskii-Moriya interaction and constant external magnetic field were considered. By using Holstain-Primakoff transformation and the multiscale method
spin wave frequency ω was obtained when nonlinear term in the system was neglect
and two bright soliton solutions of the two sets of sublattice were obtained when nonlinear term was considered. Finally
the effects of the wave vector k and bond alternation strength m ( the nearest exchange interaction parameter ratios J′
1
/J
1
)on ω,the soliton peak value,width and energy were discussed. The results show that ω can be divided into optical branch ω
+
and acoustic branch ω
-
. ω does not exist near kb=0
±2π(b is the distance between the two nearest neighbor cells). Acoustic branch ω
-
corresponds to bright soliton solution
optical does not. When J
1
is certain
the smaller the m is
the smaller the gap between ω
+
and ω
-
will be. The peak width,phase velocity,group velocity and energy quantum of the two bright soliton solutions are of the same values,but the envelop amplitude and phase are different with the same parameter. The energy quantum of the soliton solutions is smaller than the energy quantum of the spin wave solution when nonlinear term is not considered
so the two soliton solution is stable. The m affects not only the relative peak value
but also the relative phase of the two solitons.The peak value of two soliton solutions vary with the changes of m and k
but the change is not the same. The peak width does not increase monotonously with the crease of k
nor does it increase monotonously with that of m.