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JOURNAL OF MATHEMATICAL STUDYJ. Math. Study, Vol. x, No. x (201x), pp. 1-74. Astrophysical Dynamics and Cosmology. Tian Ma1, Shouhong Wang2,. 1 Department of Mathematics, Sichuan University, Chengdu, P. R. China.2 Department of Mathematics, Indiana

dV (t) =. ((ıH 1. 2aKKa. )dt dB(t)Ka. aKSdB(t) Tr((S I)>dΛ(t)))V (t),. ... dY (t) = Ka(t)dt SdB(t). C Controllability and Observability. Consider a complex linear (time invariant state-space) system described by the differentialequation.

In the second half of this text we study bounded linear op-erators on the generalised sequence space p(ZN , U ), where p [1, ] and U issome complex Banach space. ... Collective Compactness. In the mid 1960’s Anselone and co-workers (see[3] and the

The geometri representation theory of these algebras has been studied in [Lu1, Lu2, Lu3 and fundamental re-sults have appeared in [HO, Op. ... The following proposition provides a graded He ke analogue of the results in [Ka,Proposition 1.20 and [Ka,

1.4). 1.3. The analytic branches of eigenvalues and eigenvectors of A(t).According to the general analytic perturbation theory (see [Ka]), for |t| 6 t0there exist real-analytic functions

it induces an algebra homomorphism. Φ : Hp,qd EndG(V(λp,q) Vd)op. (3.5). ... p,qd ). op thanks to Theorem 3.9. The laststatement follows from Corollary 3.8.

Inother words, it is conjectured that for a ‘generic’ selfadjoint second-order elliptic op-erator with periodic coefficients on Rd each of the spectral gap’s endpoints is a unique(modulo