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This minimum corresponds to an antiphase boundary that has been observed experimentally in dissociated dislocation cores in various perovskites.
As a result, two bending moment limit values are obtained and their minimum corresponds to the real bearing capacity of the element.
Its minimum corresponds to both copper-containing systems and maximum relates to zinc- and nickel-containing systems.
This investigation provides us with the 2D function χ 2 ε,M), whose minimum corresponds to the maximum likelihood values for the mean magnetic thickness and the mean magnetization.
In [16], Koldobsky and Zymonopoulou studied the extremal sections of B p ( C n ), for 0 < p ≤ 2 and showed that the minimum corresponds to hyperplanes orthogonal to vectors ξ = ( ξ 1, …, ξ n ) ∈ C n with | ξ 1 | = ⋯ = | ξ n | and the maximum corresponds to hyperplanes orthogonal to vectors with only one non-zero coordinate.
Its minimum corresponds to the sub-strategy ratio optimizing overall response time in the complex/far condition.
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The afterslip depth-profile crossing the center of the seismic source area showed two peaks, and the local minimum corresponded to the large coseismic slip area (Fig. 2c, gray and black lines).
The minimum corresponded to the thickness measured in the plane orthogonal to the former.
The frequencies at which measured losses became minima corresponded to the calculation results by the plane-wave model.
These minima correspond to twisting of either the dimethylanilino group or the dimethylamino group (δ and μ torsion, respectively).
The protein energy landscape is represented by two harmonic wells of stiffness κ1 and κ2, whose minima correspond to conformations C1 and C2.
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