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For a 10-2 - 102 Hz frequency domain and a typical attempt time of τ0 ∼ 10-12 - 10-14 s the observable fluctuations necessarily involve transition energies between 7 meV and 0.8 eV for temperatures of 4-300 K (Ref.).
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For a 10-2 - 102 Hz frequency domain and a typical attempt time of τ0 ∼ 10-12 - 10-14 s the observable fluctuations necessarily involve transition energies between 7 meV and 0.8 eV for temperatures of 4-300 K (Ref.).
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For κ- (ET) 2 Cu [N (CN) 2] Br and its deuterated analog there is a kink in the dc resistance at the glasslike-transition temperature Tg. Also, the temperature dependence of the dc resistance below Tg and the actual ground-state properties are strongly affected by the conformational changes (e.g., induced by different cooling rates or annealing procedures) of the ET molecules' ethylene endgroups (Refs.).
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For κ- (ET) 2 Cu [N (CN) 2] Br and its deuterated analog there is a kink in the dc resistance at the glasslike-transition temperature Tg. Also, the temperature dependence of the dc resistance below Tg and the actual ground-state properties are strongly affected by the conformational changes (e.g., induced by different cooling rates or annealing procedures) of the ET molecules' ethylene endgroups (Refs.).
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In the ac specific-heat experiment τ is linked to the measurement frequency; in thermal expansion τ is estimated using a simple two-state model (see Ref. and references therein).
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In the ac specific-heat experiment τ is linked to the measurement frequency; in thermal expansion τ is estimated using a simple two-state model (see Ref. and references therein).
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The analysis of the noise amplitude at different frequencies reveals a shift in temperature of the maximum in D (E).
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The analysis of the noise amplitude at different frequencies reveals a shift in temperature of the maximum in D (E).
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