St. Petersburg Mathematical Journal, 4. cilt,4-6. sayılarAmerican Mathematical Society, 1993 |
Kitabın içinden
82 sonuçtan 1-3 arası sonuçlar
Sayfa 926
... gives us that B1 ( 1 – λ ) βι + λδι = B1 δι c ( λ ) = λ ( yı − 1 ) + 1 − 81 ( 1 − 2 ) , which together with ( 4 ) gives us that - - ¥ 1 + 81 = λ ( Y1 + 81 − 1 ) + 1 , i.e. , 71 + 81 = 1 . 1 81 The equalities ẞ1 = 0 and y1 + 81 = 1 ...
... gives us that B1 ( 1 – λ ) βι + λδι = B1 δι c ( λ ) = λ ( yı − 1 ) + 1 − 81 ( 1 − 2 ) , which together with ( 4 ) gives us that - - ¥ 1 + 81 = λ ( Y1 + 81 − 1 ) + 1 , i.e. , 71 + 81 = 1 . 1 81 The equalities ẞ1 = 0 and y1 + 81 = 1 ...
Sayfa 940
Since fЄ A , Lemma 1.1 gives us that n || H78 || q ≤ Ca |||| - || 8 || p . Since fo " e Aa , it follows that P_ ( fe " ) e Aa ( the operators P and P. map the space Aa into itself ) , and Lemma 1.2 gives us || T78 || q ≤ Ca || P_ ( ƒ ...
Since fЄ A , Lemma 1.1 gives us that n || H78 || q ≤ Ca |||| - || 8 || p . Since fo " e Aa , it follows that P_ ( fe " ) e Aa ( the operators P and P. map the space Aa into itself ) , and Lemma 1.2 gives us || T78 || q ≤ Ca || P_ ( ƒ ...
Sayfa 968
In the present article we give a new description of such models that does not make immediate use of the theory of extensions , and we give a direct construction of a semibounded three - particle Hamiltonian corresponding to pair ...
In the present article we give a new description of such models that does not make immediate use of the theory of extensions , and we give a direct construction of a semibounded three - particle Hamiltonian corresponding to pair ...
İçindekiler
MATHEMATICS | 665 |
150 | 832 |
ABSTRACT Let be an elliptic differential operator of order n2 with constant | 940 |
Telif Hakkı | |
4 diğer bölüm gösterilmiyor
Diğer baskılar - Tümünü görüntüle
Sık kullanılan terimler ve kelime öbekleri
a₁ analytic assertion assume asymptotic Blaschke product boundary bounded C₁ cone consider const constant construction convex corresponding covector cubes D₁ decomposition defined definition denote diffeomorphisms differential domain eigenvalues English transl equality equation equivalent estimate exists finite follows function f H₁ hence Hilbert space Hölder holds inequality inner function integral irreducible lattice Lemma Leningrad Lie algebra linear M₁ mapping Mathematical Mathematics Subject Classification maximum principle morphism multiplicity nonlinear norm obtained operator pair perturbation polynomial problem proof of Theorem properties Proposition proved representation Riemann-Roch theorem S₁ satisfying the conditions scattering matrix scattering theory selfadjoint singular smooth solution Soviet Math space spectral spectrum Steklov subspace sufficiently Suppose t₁ Theorem 1.1 theory trace formula trace-class unique unitary V₁ zero