Search results for "Vector"

showing 10 items of 2660 documents

Actions de IR et courbure de ricci du Fibré unitaire tangent des surfaces

1986

Characterisation of 2-dimensional Riemannian manifolds (M, g) (in particular, of surfaces with constant gaussian curvatureK=1/c2, o,−1/c2, respectively) whose tangent circle bundle (TcM, gs) (gs=Sasaki metric) admit an «almost-regular» vector field belonging to an eigenspace of the Ricci operator.

Pure mathematicsGeneral MathematicsCircle bundleGaussianMathematical analysisTangentsymbols.namesakeUnit tangent bundlesymbolsVector fieldMathematics::Differential GeometryExponential map (Riemannian geometry)Ricci curvatureEigenvalues and eigenvectorsMathematicsRendiconti del Circolo Matematico di Palermo
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Expecting the unexpected: Quantifying the persistence of unexpected hypersurfaces

2021

If $X \subset \mathbb P^n$ is a reduced subscheme, we say that $X$ admits an unexpected hypersurface of degree $t$ for multiplicity $m$ if the imposition of having multiplicity $m$ at a general point $P$ fails to impose the expected number of conditions on the linear system of hypersurfaces of degree $t$ containing $X$. Conditions which either guarantee the occurrence of unexpected hypersurfaces, or which ensure that they cannot occur, are not well understand. We introduce new methods for studying unexpectedness, such as the use of generic initial ideals and partial elimination ideals to clarify when it can and when it cannot occur. We also exhibit algebraic and geometric properties of $X$ …

Pure mathematicsGeneral MathematicsComplete intersectionVector bundleAlgebraic geometrysymbols.namesakeMathematics - Algebraic GeometryAV-sequence; Complete intersection; Generic initial ideal; Hilbert function; Partial elimination ideal; Unexpected hypersurfaceUnexpected hypersurfaceFOS: MathematicsAlgebraic numberAV-sequenceAlgebraic Geometry (math.AG)Complete intersectionGeneric initial idealMathematicsHilbert series and Hilbert polynomialSequencePartial elimination idealSettore MAT/02 - AlgebraHypersurfaceHyperplanePrimary: 14C20 13D40 14Q10 14M10 Secondary: 14M05 14M07 13E10Hilbert functionsymbolsSettore MAT/03 - GeometriaAV-sequence Complete intersection Generic initial ideal Hilbert function Partial elimination ideal Unexpected hypersurface
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Volumes transverses aux feuilletages d'efinissables dans des structures o-minimales

2003

Let Fλ be a family of codimension p foliations defined on a family Mλ of manifolds and let Xλ be a family of compact subsets of Mλ. Suppose that Fλ, Mλ and Xλ are definable in an o-minimal structure and that all leaves of Fλ are closed. Given a definable family Ωλ of differential p-forms satisfaying iZ Ωλ = 0 forany vector field Z tangent to Fλ, we prove that there exists a constant A > 0 such that the integral of on any transversal of Fλ intersecting each leaf in at most one point is bounded by A. We apply this result to prove that p-volumes of transverse sections of Fλ are uniformly bounded.

Pure mathematicsGeneral MathematicsMathematical analysisStructure (category theory)Structures o-minimalesTangentCodimensionTransversal (combinatorics)Bounded functionUniform boundednessIntégration de formes différentiellesVector fieldConstant (mathematics)Feuilletages réelsMathematics
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Multidimensional Borg–Levinson theorems for unbounded potentials

2018

We prove that the Dirichlet eigenvalues and Neumann boundary data of the corresponding eigenfunctions of the operator $-\Delta + q$, determine the potential $q$, when $q \in L^{n/2}(\Omega,\mathbb{R})$ and $n \geq 3$. We also consider the case of incomplete spectral data, in the sense that the above spectral data is unknown for some finite number of eigenvalues. In this case we prove that the potential $q$ is uniquely determined for $q \in L^p(\Omega,\mathbb{R})$ with $p=n/2$, for $n\geq4$ and $p>n/2$, for $n=3$.

Pure mathematicsGeneral MathematicsOperator (physics)010102 general mathematicsMathematics::Spectral TheoryEigenfunction01 natural sciencesOmega010101 applied mathematicsDirichlet eigenvalueBoundary data0101 mathematicsSpectral dataFinite setEigenvalues and eigenvectorsMathematicsAsymptotic Analysis
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Nonlinear Eigenvalue Problems of Schrödinger Type Admitting Eigenfunctions with Given Spectral Characteristics

2002

The following work is an extension of our recent paper [10]. We still deal with nonlinear eigenvalue problems of the form in a real Hilbert space ℋ with a semi-bounded self-adjoint operator A0, while for every y from a dense subspace X of ℋ, B(y ) is a symmetric operator. The left-hand side is assumed to be related to a certain auxiliary functional ψ, and the associated linear problems are supposed to have non-empty discrete spectrum (y ∈ X). We reformulate and generalize the topological method presented by the authors in [10] to construct solutions of (∗) on a sphere SR ≔ {y ∈ X | ∥y∥ℋ = R} whose ψ-value is the n-th Ljusternik-Schnirelman level of ψ| and whose corresponding eigenvalue is t…

Pure mathematicsGeneral MathematicsOperator (physics)Mathematical analysisHilbert spaceEigenfunctionType (model theory)symbols.namesakeNonlinear systemElliptic partial differential equationsymbolsDivide-and-conquer eigenvalue algorithmEigenvalues and eigenvectorsMathematicsMathematische Nachrichten
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Weyl's Theorems and Extensions of Bounded Linear Operators

2012

A bounded operator $T\in L(X)$, $X$ a Banach space, is said to satisfy Weyl's theorem if the set of all spectral points that do not belong to the Weyl spectrum coincides with the set of all isolated points of the spectrum which are eigenvalues and having finite multiplicity. In this article we give sufficient conditions for which Weyl's theorem for an extension $\overline T$ of $T$ (respectively, for $T$) entails that Weyl's theorem holds for $T$ (respectively, for $\overline T$).

Pure mathematicsGeneral MathematicsSpectrum (functional analysis)Extension of bounded operators Weyl type theoremsBanach spaceMultiplicity (mathematics)Extension (predicate logic)Mathematics::Spectral TheoryBounded operatorSet (abstract data type)47A1047A1147A55Settore MAT/05 - Analisi MatematicaBounded function47A53Mathematics::Representation TheoryEigenvalues and eigenvectorsMathematics
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Sato's universal Grassmannian and group extensions

1991

An extension \(\widehat{GL}\) of the symmetry group GL of Sato's universal Grassmannian GM is constructed. The extension plays a similar role to that of the central extension \(\widehat{GL}_{{\text{res}}}\) in the approach of Segal and Wilson to τ functions and KP hierarchy. Our group G contains GLres as a subgroup and the associated τ function is a deformation of the usual τ function, leading to a deformed KP hierarchy. A relation to current algebra of Yang-Mills theory in 3+1 dimension is discussed.

Pure mathematicsGroup (mathematics)Current algebraStatistical and Nonlinear PhysicsExtension (predicate logic)Yang–Mills theoryFunction (mathematics)Symmetry groupAlgebraHigh Energy Physics::TheoryGrassmannianMathematical PhysicsVector spaceMathematicsLetters in Mathematical Physics
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Quantization on the Virasoro group

1990

The quantization of the Virasoro group is carried out by means of a previously established group approach to quantization. We explicitly work out the two-cocycles on the Virasoro group as a preliminary step. In our scheme the carrier space for all the Virasoro representations is made out of polarized functions on the group manifold. It is proved that this space does not contain null vector states, even forc≦1, although it is not irreducible. The full reduction is achieved in a striaghtforward way by just taking a well defined invariant subspace ℋ(c, h), the orbit of the enveloping algebra through the vacuum, which is irreducible for any value ofc andh. ℋ(c, h) is a proper subspace of the sp…

Pure mathematicsGroup (mathematics)Quantization (signal processing)Invariant subspaceStatistical and Nonlinear Physics81S10ManifoldGroup representation17B68Algebra58F06Null vector81R10Algebra representation22E65Mathematical PhysicsSymplectic geometryMathematics
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An invariant analytic orthonormalization procedure with an application to coherent states

2007

We discuss a general strategy which produces an orthonormal set of vectors, stable under the action of a given set of unitary operators Aj, j=1,2,n, starting from a fixed normalized vector in H and from a set of unitary operators. We discuss several examples of this procedure and, in particular, we show how a set of coherentlike vectors can be produced and in which condition over the lattice spacing this can be done. © 2007 American Institute of Physics.

Pure mathematicsHilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)coherent statesUnitary stateMathematical OperatorsSet (abstract data type)symbols.namesakeUnit vectorsymbolsSet theoryInvariant (mathematics)Settore MAT/07 - Fisica MatematicaOrthonormalityComputer Science::DatabasesMathematical PhysicsMathematics
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Generalized Bogoliubov transformations versus D-pseudo-bosons

2015

We demonstrate that not all generalized Bogoliubov transformations lead to D -pseudo-bosons and prove that a correspondence between the two can only be achieved with the imposition of specific constraints on the parameters defining the transformation. For certain values of the parameters, we find that the norms of the vectors in sets of eigenvectors of two related apparently non-selfadjoint number-like operators possess different types of asymptotic behavior. We use this result to deduce further that they constitute bases for a Hilbert space, albeit neither of them can form a Riesz base. When the constraints are relaxed, they cease to be Hilbert space bases but remain D -quasibases.

Pure mathematicsHilbert spaceStatistical and Nonlinear PhysicsBase (topology)Mathematical Operatorssymbols.namesakeTransformation (function)symbolsQASettore MAT/07 - Fisica MatematicaMathematical PhysicsEigenvalues and eigenvectorsQCStatistical and Nonlinear PhysicBosonMathematics
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