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• W2071760839 abstract "The proportionality between the field-induced shifts ensuremath{Delta}${mathit{T}}_{mathit{c}}$(H) and ensuremath{Delta}${mathit{T}}_{mathrm{eq}}$(H) of the transition and equilibrium temperatures ${mathit{T}}_{mathit{c}}$(H) and ${mathit{T}}_{mathrm{eq}}$(H) and the root-mean-square random field ${mathit{h}}_{mathrm{RF}}$ was studied over a wide range of concentration (0.31ensuremath{le}xensuremath{le}0.84) in the ideal random-field Ising model (RFIM) system ${mathrm{Fe}}_{mathit{x}}$${mathrm{Zn}}_{1mathrm{ensuremath{-}}mathit{x}}$${mathrm{F}}_{2}$. $T sub c (H)--- and ${mathit{T}}_{mathrm{eq}}$(H) were determined experimentally from the optical birefringence ensuremath{Delta}n, for which d(ensuremath{Delta}n)/dT exhibits a peak at ${mathit{T}}_{mathit{c}}$(H) proportional to the magnetic specific heat. ${mathit{T}}_{mathrm{eq}}$(H) was determined from the point above which zero-field-cooled and field-cooled measurements gave identical results. For all x studied, ${mathit{T}}_{mathit{c}}$(H) and ${mathit{T}}_{mathrm{eq}}$(H) were found to shift from the H=0 transition at ${mathit{T}}_{mathit{N}}$ as [ensuremath{Delta}${mathit{T}}_{mathit{c}}$(H),ensuremath{Delta}${mathit{T}}_{mathrm{eq}}$(H)]=[c,${mathit{c}}_{mathrm{eq}}$] ${mathit{T}}_{mathit{N}}$${mathit{h}}_{mathrm{RF}}^{2/mathrm{ensuremath{varphi}}}$ as predicted, with ensuremath{varphi}=1.42ifmmodepmelsetextpmfi{}0.03, the universal random exchange to RFIM crossover exponent, after a mean-field correction ${mathit{bH}}^{2}$. The nonuniversal quantities c and ${mathit{c}}_{mathrm{eq}}$ were found to be of order unity as expected, but slightly x dependent. An empirical x dependence for c and ${mathit{c}}_{mathrm{eq}}$ is suggested. This analysis is applied to existing data on ${mathrm{Mn}}_{mathit{x}}$${mathrm{Zn}}_{1mathrm{ensuremath{-}}mathit{x}}$${mathrm{F}}_{2}$, and leads to very similar behavior for c, with essentially equal numerical values." @default.
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• W2071760839 date "1991-05-01" @default.
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• W2071760839 title "Concentration dependence of the random-field-crossover scaling in<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>Fe</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant=italic>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>Zn</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><…" @default.
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• W2071760839 doi "https://doi.org/10.1103/physrevb.43.10797" @default.
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