St. Petersburg Mathematical Journal, 16. ciltAmerican Mathematical Society, 2005 |
Kitabın içinden
78 sonuçtan 1-3 arası sonuçlar
Sayfa 136
... Moreover , F ( X , x ) is holomorphically invertible in w x Ds " ( xo ) , because so are P2 ( A , x ) and H ( X ) . Finally , we see that F = 1 ST2BT1 if λ € No , ΦΗ if AE No. Therefore , the only possible poles of F are 0 and ∞ . Moreover ...
... Moreover , F ( X , x ) is holomorphically invertible in w x Ds " ( xo ) , because so are P2 ( A , x ) and H ( X ) . Finally , we see that F = 1 ST2BT1 if λ € No , ΦΗ if AE No. Therefore , the only possible poles of F are 0 and ∞ . Moreover ...
Sayfa 139
... Moreover , α0 , ∞ : = sup ( the order of the pole at 0 , ∞ ) < ∞ . xЄDs ( xo ) 2. The positions of the zeros of det M ( X , x ) in No \ w do not depend on x . If , moreover , M ( A , x ) is holomorphically invertible in ( No \ { 0 } ...
... Moreover , α0 , ∞ : = sup ( the order of the pole at 0 , ∞ ) < ∞ . xЄDs ( xo ) 2. The positions of the zeros of det M ( X , x ) in No \ w do not depend on x . If , moreover , M ( A , x ) is holomorphically invertible in ( No \ { 0 } ...
Sayfa 136
... Moreover , F ( X , x ) is holomorphically invertible in w × Ds " ( xo ) , because so are Þ2 ( λ , x ) and H ( X ) . Finally , we see that F = 1 ST2 BT1 if λ € Nx , | ΦΗ if XE No. Therefore , the only possible poles of F are 0 and ...
... Moreover , F ( X , x ) is holomorphically invertible in w × Ds " ( xo ) , because so are Þ2 ( λ , x ) and H ( X ) . Finally , we see that F = 1 ST2 BT1 if λ € Nx , | ΦΗ if XE No. Therefore , the only possible poles of F are 0 and ...
İçindekiler
ISOMETRIC EMBEDDINGS OF FINITEDIMENSIONAL pSPACES | 11 |
OVER THE QUATERNIONS | 104 |
1 Introduction | 117 |
Telif Hakkı | |
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analytic approximation assume asymptotic Birman BKN-equation bounded C(zIm coefficients cohomology classes compatible components constant corresponding defined denote diffeomorphism Dirac operator domain edge eigenvalues embedding English transl estimate Euler characteristic exists finite formula geodesic graph graph-manifold harmonic Hilbert space holomorphic implies inequality integral invertible isometric K₁ kernel Lemma length function linear Math matrix matrix-valued function maximal blocks meromorphic monodromy nonzero norm NPC-solution obtain oriented Painlevé equations pair paper polynomial positive potential problem proof of Theorem properties Proposition prove rational refinable function relation representation respect result Riemann-Hilbert Riemann-Hilbert problem Riemannian manifold S₁ satisfies Schrödinger operator Seifert fibered space self-affine selfadjoint selfadjoint operators singular Sobolev Sobolev spaces solution spectrum Subsection subspace supp Suppose symmetric Theorem Theorem 3.1 theory torus vector vertex vertices zero