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Field dependence of the transverse spin glass phase transition: Quantitative agreement between Monte Carlo simulations and experiments
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10.1063/1.3671432
/content/aip/journal/jap/111/7/10.1063/1.3671432
http://aip.metastore.ingenta.com/content/aip/journal/jap/111/7/10.1063/1.3671432
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color online) x-T phase diagram of the ±J bond-frustrated Heisenberg model in three dimensions (where x is the fraction of antiferromagnetic bonds, i.e., J =  –1). The T C line separates paramagnetic (PM) and ferromagnetic phases. The line of spin glass transitions T sg separates the PM phase from the spin glass (SG) phase. Below the T xy line, SG order develops transverse to the magnetization. T C was identified using different numerical criteria (○, Δ, □; for details, see Ref. 4). The same topology is exhibited by the experimental phase diagram of a—FexZr100−x 3 (inset).

Image of FIG. 2.
FIG. 2.

Crossing of the ξ xy /L data for simulation system sizes of L =  4, 6, 8, 10, and 12 at a concentration x =  0.15, with magnetic fields B =  0, 0.01, 0.03, 0.1, 0.3, 0.6, and 1 (data have been shifted vertically for clarity). Solid lines through L > 6 data show clear crossings, while the dashed line through the L =  4 and L =  6 data cross at slightly higher T. Where error bars are not apparent, they are smaller than the symbol size.

Image of FIG. 3.
FIG. 3.

(Color online) A comparison of T xy (B) obtained from Monte Carlo simulations with T xy (B) obtained from experiments on a—FexZr100−x. The solid line is a fit to Eq. (1).

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/content/aip/journal/jap/111/7/10.1063/1.3671432
2012-02-14
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Field dependence of the transverse spin glass phase transition: Quantitative agreement between Monte Carlo simulations and experiments
http://aip.metastore.ingenta.com/content/aip/journal/jap/111/7/10.1063/1.3671432
10.1063/1.3671432
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