SHELXT SHELXT (2) 直接法 F ϕ 3 ( ) ( ) + ( ) 6 ϕ h ϕ k ϕ h k exp{ iϕ( h) } exp iϕ( k ) exp iϕ h k { } { ( )} 7 h k h k F exp{ iϕ( h) } =

Neumann started investigation of the quantity k T K k 0 (which he called the configuration constant of K) in order to get a proof for the existence of the solution of the

Having established the existence of regular solutions to a small perturbation of the linearized equation for (1.5), we intend to apply a Nash-Moser type iteration procedure in

Since weak convergence is preserved by continuous mappings, the weak convergence in H α provides weak convergence results for H 0 α -continuous functionals of paths and for some

Hence, in the Dirichlet-type and Neumann-type cases respectively, the sets P k used here are analogous to the sets (0, ∞) × T k+1 and (0, ∞) × S k , and we see that using the sets P

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Taking care of all above mentioned dates we want to create a discrete model of the evolution in time of the forest.. We denote by x 0 1 , x 0 2 and x 0 3 the initial number of

F rom the point of view of analysis of turbulent kineti energy models the result.. presented in this paper an be onsidered as a natural ontinuation of

『国民経済計算年報』から「国内家計最終消費支出」と「家計国民可処分 所得」の 1970 年〜 1996 年の年次データ (