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Volumn 79, Issue 21, 2009, Pages

1/f noise in the quasi-two-dimensional organic conductor κ- (BEDT-TTF) 2 Cu [N (CN) 2] Cl

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EID: 68949108097     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.214521     Document Type: Article
Times cited : (22)

References (44)
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  • 34
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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.).
    • 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.).
  • 35
    • 0004003420 scopus 로고    scopus 로고
    • edited by M. Ziese and M. J. Thornton (Springer, Berlin, Heidelberg
    • B. Raquet, in Spin Electronics, edited by, M. Ziese, and, M. J. Thornton, (Springer, Berlin, Heidelberg, 2001).
    • (2001) Spin Electronics
    • Raquet, B.1
  • 37
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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.).
    • 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.).
  • 40
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    • Ph.D. thesis TU Dresden
    • J. Müller, Ph.D. thesis, TU Dresden, 2002.
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    • Müller, J.1
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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).
    • 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).
  • 44
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    • The analysis of the noise amplitude at different frequencies reveals a shift in temperature of the maximum in D (E).
    • The analysis of the noise amplitude at different frequencies reveals a shift in temperature of the maximum in D (E).


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