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It is notable that the square-root dependence on ρs is a typical behavior of the order parameter as expected from the Ginzburg-Landau theory[23].
Likewise, upon binding ligand (MLL, pKID, or both), the oscillatory behavior of the order parameters in helix α2 is lost, and helix α2 displays relatively uniform order parameters in ligand bound states.
An oscillatory behavior of the order parameters is observed for the segment of helix α2 between residues 625 637 with lowest order parameters found for residues M625, L628, V629, K632, K633, and E636 and higher order parameters for residues between these.
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The switching between the two regimes is accompanied by hysteresis and transient behavior on the order of 2 4 h in a small 1cm2 cell.
Xu et al. [30, 31] studied the thermal expansion behavior of the ordered silver nanowire arrays embedded in AAMs, and pointed out that the collective effects of the intrinsic expansion of silver nanowires together with surface pressure from the AAM and the vacancies incorporated into the silver lattice were responsible for the thermal expansion.
In addition, using fractional order stability analysis, the chaotic behavior of the fractional order NSG (FNSG) is studied.
This unusual behavior of the higher order peaks was explained by the lamellar insertion model of Hama and Tashiro.
Single component adsorption isotherms can be estimated from local derivatives of the adsorption isotherm at specified steady-state concentrations, which are obtained from the low frequency asymptotic behavior of the higher order frequency response functions (FRFs) of a chromatographic column.
In this paper, we are concerned with oscillation behavior of the second order quasilinear neutral delay dynamic equations.
Leviatan [3] has investigated the behavior of the higher order derivatives of approximation polynomials for the differentiable function f on ([-1,1]), as follows.
In 2010, Sun et al. [21] are concerned with oscillation behavior of the second order quasilinear neutral delay dynamic equations of the form (1.4).
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