Search results for "Transformation"

showing 10 items of 1634 documents

$$O_2(\mathbb {C})$$O2(C)-Vector Bundles and Equivariant Real Circle Actions

2020

The main goal of this article is to give an expository overview of some new results on real circle actions on affine four-space and their relation to previous results on \(O_2(\mathbb {C})\)-equivariant vector bundles. In Moser-Jauslin (Infinite families of inequivalent real circle actions on affine four-space, 2019, [13]), we described infinite families of equivariant real circle actions on affine four-space. In the present note, we will describe how these examples were constructed, and some consequences of these results.

Pure mathematics010102 general mathematics0103 physical sciencesAffine spaceVector bundleEquivariant map010307 mathematical physicsAffine transformation0101 mathematics01 natural sciencesMathematics
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q-Fock Space Representations of the q-Lorentz Algebra and Irreducible Tensors

1993

We present the q-deformation of the Lorentz algebra, with Hopf structure, in terms of four independent harmonic oscillators. The explicit realization of the q-Fock space is given and the irreducible finite-dimensional representations of so(1,3)q are described and characterized by its two q-Casimir operators. The concept of irreducible q-Lorentz tensor is also introduced. The analysis is made for a real deformation parameter.

Pure mathematics010308 nuclear & particles physicsLorentz transformation010102 general mathematics(gK)-moduleIrreducible elementSpace (mathematics)01 natural sciencesFock spaceAlgebrasymbols.namesakeSubdirectly irreducible algebra0103 physical sciencessymbolsTensor0101 mathematicsRealization (systems)Mathematics
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Some overdetermined problems related to the anisotropic capacity

2018

Abstract We characterize the Wulff shape of an anisotropic norm in terms of solutions to overdetermined problems for the Finsler p-capacity of a convex set Ω ⊂ R N , with 1 p N . In particular we show that if the Finsler p-capacitary potential u associated to Ω has two homothetic level sets then Ω is Wulff shape. Moreover, we show that the concavity exponent of u is q = − ( p − 1 ) / ( N − p ) if and only if Ω is Wulff shape.

Pure mathematics0211 other engineering and technologiesConvex set02 engineering and technology01 natural sciencesHomothetic transformationOverdetermined systemMathematics - Analysis of PDEs35N25 35B06 35R25FOS: MathematicsConcavity exponent0101 mathematicsAnisotropyMathematics021103 operations researchCapacityApplied Mathematics010102 general mathematicsAnalysiWulff shapeAnisotropic normExponentOverdetermined problemMathematics::Differential GeometryAnalysisAnalysis of PDEs (math.AP)
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Cyclic covers of affine T-varieties

2015

Abstract We consider normal affine T -varieties X endowed with an action of finite abelian group G commuting with the action of T . For such varieties we establish the existence of G-equivariant geometrico-combinatorial presentations in the sense of Altmann and Hausen. As an application, we determine explicit presentations of the Koras–Russell threefolds as bi-cyclic covers of A 3 equipped with a hyperbolic G m -action.

Pure mathematicsAlgebra and Number TheoryAffine transformationAbelian groupAction (physics)MathematicsJournal of Pure and Applied Algebra
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On exotic affine 3-spheres

2014

Every A 1 \mathbb {A}^{1} -bundle over A ∗ 2 , \mathbb {A}_{\ast }^{2}, the complex affine plane punctured at the origin, is trivial in the differentiable category, but there are infinitely many distinct isomorphy classes of algebraic bundles. Isomorphy types of total spaces of such algebraic bundles are considered; in particular, the complex affine 3 3 -sphere S C 3 , \mathbb {S}_{\mathbb {C}}^{3}, given by z 1 2 + z 2 2 + z 3 2 + z 4 2 = 1 , z_{1}^{2}+z_{2}^{2}+z_{3}^{2}+z_{4}^{2}=1, admits such a structure with an additional homogeneity property. Total spaces of nontrivial homogeneous A 1 \mathbb {A}^{1} -bundles over A ∗ 2 \mathbb {A}_{\ast }^{2} are classified up to G m \mathbb {G}_{m}…

Pure mathematicsAlgebra and Number TheoryHomogeneousSPHERESGeometry and TopologyIsomorphismAffine transformationDifferentiable functionAlgebraic numberInvariant (mathematics)Exotic sphereMathematicsJournal of Algebraic Geometry
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Noncancellation for contractible affine threefolds

2011

We construct two nonisomorphic contractible affine threefolds X X and Y Y with the property that their cylinders X × A 1 X\times \mathbb {A}^{1} and Y × A 1 Y\times \mathbb {A}^{1} are isomorphic, showing that the generalized Cancellation Problem has a negative answer in general for contractible affine threefolds. We also establish that X X and Y Y are actually biholomorphic as complex analytic varieties, providing the first example of a pair of biholomorphic but not isomorphic exotic A 3 \mathbb {A}^{3} ’s.

Pure mathematicsApplied MathematicsGeneral Mathematics010102 general mathematics0103 physical sciences010307 mathematical physicsAffine transformation0101 mathematics01 natural sciencesContractible spaceMathematicsProc. Amer. Math. Soc.
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Uniform estimates for the local restriction of the Fourier transform to curves

2013

We prove sharp estimates, with respect to the ane arclength measure, for the restriction of the Fourier transform to a class of curves in R^d that includes curves of nite type. This measure possesses certain invariance and mitigation properties which are important in establishing uniform results. Peer reviewed

Pure mathematicsClass (set theory)Applied MathematicsGeneral Mathematics010102 general mathematicsType (model theory)01 natural sciencesMeasure (mathematics)symbols.namesakeFourier transform0103 physical sciences111 MathematicssymbolsCalculus010307 mathematical physicsAffine transformation0101 mathematicsMathematicsTransactions of the American Mathematical Society
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Self-affine sets with fibered tangents

2016

We study tangent sets of strictly self-affine sets in the plane. If a set in this class satisfies the strong separation condition and projects to a line segment for sufficiently many directions, then for each generic point there exists a rotation $\mathcal O$ such that all tangent sets at that point are either of the form $\mathcal O((\mathbb R \times C) \cap B(0,1))$, where $C$ is a closed porous set, or of the form $\mathcal O((\ell \times \{ 0 \}) \cap B(0,1))$, where $\ell$ is an interval.

Pure mathematicsClass (set theory)General MathematicsDynamical Systems (math.DS)Interval (mathematics)iterated function system01 natural sciencesself-affine setGeneric pointLine segmentstrictly self-affine sets0103 physical sciencesClassical Analysis and ODEs (math.CA)FOS: MathematicsPoint (geometry)Porous set0101 mathematicsMathematics - Dynamical SystemsMathematicsApplied Mathematics010102 general mathematicsta111Tangenttangent setsTangent setMathematics - Classical Analysis and ODEs010307 mathematical physicsAffine transformation
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Devroye Inequality for a Class of Non-Uniformly Hyperbolic Dynamical Systems

2005

In this paper, we prove an inequality, which we call "Devroye inequality", for a large class of non-uniformly hyperbolic dynamical systems (M,f). This class, introduced by L.-S. Young, includes families of piece-wise hyperbolic maps (Lozi-like maps), scattering billiards (e.g., planar Lorentz gas), unimodal and H{\'e}non-like maps. Devroye inequality provides an upper bound for the variance of observables of the form K(x,f(x),...,f^{n-1}(x)), where K is any separately Holder continuous function of n variables. In particular, we can deal with observables which are not Birkhoff averages. We will show in \cite{CCS} some applications of Devroye inequality to statistical properties of this class…

Pure mathematicsClass (set theory)[MATH.MATH-PR] Mathematics [math]/Probability [math.PR]Dynamical systems theoryLorentz transformation[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]General Physics and AstronomyHölder condition[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Of the formDynamical Systems (math.DS)01 natural sciencesUpper and lower bounds010104 statistics & probabilitysymbols.namesakeFOS: Mathematics0101 mathematicsMathematics - Dynamical SystemsMathematical PhysicsMathematicsApplied Mathematics010102 general mathematicsProbability (math.PR)Statistical and Nonlinear PhysicsObservableFunction (mathematics)[MATH.MATH-PR]Mathematics [math]/Probability [math.PR]symbols[ MATH.MATH-PR ] Mathematics [math]/Probability [math.PR]Mathematics - Probability
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𝔸1-contractibility of affine modifications

2019

We introduce Koras–Russell fiber bundles over algebraically closed fields of characteristic zero. After a single suspension, this exhibits an infinite family of smooth affine [Formula: see text]-contractible [Formula: see text]-folds. Moreover, we give examples of stably [Formula: see text]-contractible smooth affine [Formula: see text]-folds containing a Brieskorn–Pham surface, and a family of smooth affine [Formula: see text]-folds with a higher-dimensional [Formula: see text]-contractible total space.

Pure mathematicsComputer Science::Information RetrievalGeneral Mathematics010102 general mathematicsAstrophysics::Instrumentation and Methods for AstrophysicsZero (complex analysis)Computer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)01 natural sciencesSuspension (topology)Motivic cohomology0103 physical sciencesComputer Science::General LiteratureFiber bundle010307 mathematical physicsAffine transformation0101 mathematicsAlgebraically closed fieldMathematicsInternational Journal of Mathematics
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