Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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النتائج 1-3 من 8
الصفحة 203
Then for j = a ) the functional E has a minimizer ø1⁄2 in Cž , b ) there exist E , Є R ( in fact , E2 = E3 = 0 ) , such that the pair ( Ej , 45 ) solves ( 19.3 ) , c ) the minimizers 1.5 are unique up to a constant phase . div = ∞ The ...
Then for j = a ) the functional E has a minimizer ø1⁄2 in Cž , b ) there exist E , Є R ( in fact , E2 = E3 = 0 ) , such that the pair ( Ej , 45 ) solves ( 19.3 ) , c ) the minimizers 1.5 are unique up to a constant phase . div = ∞ The ...
الصفحة 208
The existence of a minimizer of E in Ce can be shown in a straightforward manner by employing the weak H1 - lower semicontinuity of Eελ . The difficult part is to recover ( 20.6 ) ( the function t logt is not differentiable at t = 0 ) ...
The existence of a minimizer of E in Ce can be shown in a straightforward manner by employing the weak H1 - lower semicontinuity of Eελ . The difficult part is to recover ( 20.6 ) ( the function t logt is not differentiable at t = 0 ) ...
الصفحة 210
Then for all λ > 0 the functional Eo1 has a unique minimizer ( no , po ) in Co . This minimizer solves ( 20.8 ) . Furthermore , for all 0 € ( 0,1 ) , no , po , Vo € L ~ ( N ) ~ H1 ( N ) ~ Cle ( N ) and there exists a loc constant Mε > 1 ...
Then for all λ > 0 the functional Eo1 has a unique minimizer ( no , po ) in Co . This minimizer solves ( 20.8 ) . Furthermore , for all 0 € ( 0,1 ) , no , po , Vo € L ~ ( N ) ~ H1 ( N ) ~ Cle ( N ) and there exists a loc constant Mε > 1 ...
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