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Volumn 134, Issue 19, 2011, Pages

Third harmonics nonlinear susceptibility in supercooled liquids: A comparison to the box model

Author keywords

[No Author keywords available]

Indexed keywords

A-THERMAL; BOX MODELS; DYNAMICAL HETEROGENEITIES; ELECTRICAL POWER; FINITE FREQUENCIES; GLASS TRANSITION TEMPERATURE; HOLE BURNING; INTRINSIC CONTRIBUTION; NONLINEAR FEATURES; NONLINEAR SUSCEPTIBILITIES; NONRESONANT; PHONON BATHS; POLARISATION; STATIONARY REGIME; STRONG ELECTRIC FIELDS; SUPERCOOLED LIQUIDS; TEMPERATURE INCREASE; THIRD HARMONIC;

EID: 79957594174     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3591375     Document Type: Article
Times cited : (29)

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    • 0, dh because of the interferences effects depicted in Sec..
    • 0, dh because of the interferences effects depicted in Sec..
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    • 1, the latter quantity is taken as a constant when solving Eq.. The same approximation was made independently in, e.g., the Appendix of Ref..
    • 1, the latter quantity is taken as a constant when solving Eq.. The same approximation was made independently in, e.g., the Appendix of Ref..
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    • 2, klin, k, see Eq., we are led to the conclusion that our estimate should, again, be slightly overestimated.
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    • 0, tot, k, is exactly the same, in modulus and phase, as the one found by using Eqs..
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    • 3(, T) better than 1.
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    • note
    • The values of the temperatures in the calculations were tuned to yield the same values of the relaxation frequencies f as those found in the experiments of Ref.. Hence, the small differences (less than 1K) between the two sets of temperatures for Figs..
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    • 0 following Eq. (18) of Ref..
    • 0 following Eq. (18) of Ref..
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    • 3 and the measured one is even larger than in Fig., since the calculated phase never coincides with the experimental one, whatever the frequency.
    • 3 and the measured one is even larger than in Fig., since the calculated phase never coincides with the experimental one, whatever the frequency.


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