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Physical Review B - Condensed Matter and Materials Physics

Volumn 83, Issue 17, 2011, Pages

Single-ion anisotropy, Dzyaloshinskii-Moriya interaction, and negative magnetoresistance of the spin-12 pyrochlore R2V2O 7

(6) Xiang, H J a Kan, E J b Whangbo, M H b Lee, C b Wei, Su Huai c Gong, X G a

a FUDAN UNIVERSITY (China)

b NORTH CAROLINA STATE UNIVERSITY (United States)

c NATIONAL RENEWABLE ENERGY LABORATORY (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 79961075768 PISSN: 10980121 EISSN: 1550235X Source Type: Journal
DOI: 10.1103/PhysRevB.83.174402 Document Type: Article

Times cited : (48)

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- In our standard Metropolis MC simulations, we consider a conventional cubic cell with 16 spin sites. For one MC simulation, we first generate a random spin configuration. Then we decrease the system temperature from 100 to 0.1 K gradually. We repeat several MC simulations to confirm the spin ground state obtained from our MC simulations. If we do not include the single-ion anisotropy and the effect of the DM interaction, the ground state is a perfect isotropic ferromagnetic state. If we include only the DM interaction, the ground state is the same because of the collinearity of the state.
- In our standard Metropolis MC simulations, we consider a conventional cubic cell with 16 spin sites. For one MC simulation, we first generate a random spin configuration. Then we decrease the system temperature from 100 to 0.1 K gradually. We repeat several MC simulations to confirm the spin ground state obtained from our MC simulations. If we do not include the single-ion anisotropy and the effect of the DM interaction, the ground state is a perfect isotropic ferromagnetic state. If we include only the DM interaction, the ground state is the same because of the collinearity of the state.

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