Search results for "ddc:510"

showing 6 items of 16 documents

A parts-per-billion measurement of the antiproton magnetic moment

2017

The magnetic moment of the antiproton is measured at the parts-per-billion level, improving on previous measurements by a factor of about 350. Comparing the fundamental properties of normal-matter particles with their antimatter counterparts tests charge–parity–time (CPT) invariance, which is an important part of the standard model of particle physics. Many properties have been measured to the parts-per-billion level of uncertainty, but the magnetic moment of the antiproton has not. Christian Smorra and colleagues have now done so, and report that it is −2.7928473441 ± 0.0000000042 in units of the nuclear magneton. This is consistent with the magnetic moment of the proton, 2.792847350 ± 0.0…

ProtonCPT symmetry01 natural sciencesddc:070Standard ModelNuclear physicsPhysics in Generalcharge–parity–time (CPT) invariance0103 physical sciencesddc:530atomic and molecular physicsddc:510010306 general physicsNuclear magnetonPhysicsMultidisciplinaryMagnetic moment010308 nuclear & particles physicsDewey Decimal Classification::500 | Naturwissenschaften::510 | MathematikSymmetry (physics)AntiprotonAntimatterHigh Energy Physics::ExperimentDewey Decimal Classification::500 | Naturwissenschaften::530 | PhysikPräzisionsexperimente - Abteilung BlaumAntiproton Decelerator facility
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An Itô Formula for rough partial differential equations and some applications

2020

AbstractWe investigate existence, uniqueness and regularity for solutions of rough parabolic equations of the form $\partial _{t}u-A_{t}u-f=(\dot X_{t}(x) \cdot \nabla + \dot Y_{t}(x))u$ ∂ t u − A t u − f = ( X ̇ t ( x ) ⋅ ∇ + Y ̇ t ( x ) ) u on $[0,T]\times \mathbb {R}^{d}.$ [ 0 , T ] × ℝ d . To do so, we introduce a concept of “differential rough driver”, which comes with a counterpart of the usual controlled paths spaces in rough paths theory, built on the Sobolev spaces Wk,p. We also define a natural notion of geometricity in this context, and show how it relates to a product formula for controlled paths. In the case of transport noise (i.e. when Y = 0), we use this framework to prove a…

Sobolev spacePure mathematicsPartial differential equationMaximum principleProduct (mathematics)UniquenessChain ruleddc:510Parabolic partial differential equationVDP::Matematikk og Naturvitenskap: 400::Matematikk: 410AnalysisDomain (mathematical analysis)Mathematics
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Automorphisms of $mathbb{A}^{1}$-fibered affine surfaces

2011

We develop technics of birational geometry to study automorphisms of affine surfaces admitting many distinct rational fibrations, with a particular focus on the interactions between automorphisms and these fibrations. In particular, we associate to each surface S of this type a graph encoding equivalence classes of rational fibrations from which it is possible to decide for instance if the automorphism group of S is generated by automorphisms preserving these fibrations.

Surface (mathematics)Graph encodingPure mathematicsApplied MathematicsGeneral MathematicsFibered knotBirational geometryType (model theory)AutomorphismMathematics::Algebraic TopologyMathematics::Group TheoryMathematics::Algebraic GeometryAffine transformationddc:510Focus (optics)Mathematics::Symplectic GeometryMathematics
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Projective metrics and mixing properties on towers

2001

Transfer operatorApplied MathematicsGeneral MathematicsGeometryddc:510Projective testTowerMixing (physics)MathematicsTransactions of the American Mathematical Society
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Algebraic (2, 2)-transformation groups

2009

This paper contains the more significant part of the article with the same title that will appear in the Volume 12 of Journal of Group Theory (2009). In this paper we determine all algebraic transformation groups $G$, defined over an algebraically closed field $\sf k$, which operate transitively, but not primitively, on a variety $\Omega$, provided the following conditions are fulfilled. We ask that the (non-effective) action of $G$ on the variety of blocks is sharply 2-transitive, as well as the action on a block $\Delta$ of the normalizer $G_\Delta$. Also we require sharp transitivity on pairs $(X,Y)$ of independent points of $\Omega$, i.e. points contained in different blocks.

Transitive relationAlgebra and Number TheoryNaturwissenschaftliche Fakultät -ohne weitere Spezifikation-14L30permutation groupsBlock (permutation group theory)-Group Theory (math.GR)Permutation groupCentralizer and normalizerAction (physics)CombinatoricsFOS: Mathematicsddc:510Variety (universal algebra)Algebraically closed fieldAlgebraic numberMathematics - Group TheoryMathematicsJournal of Group Theory
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Sub-Riemannian geometry: one-parameter deformation of the Martinet flat case

1998

[ MATH.MATH-OC ] Mathematics [math]/Optimization and Control [math.OC]sub-Riemannian geometrysub-Riemannian sphere and distanceabnormal geodesics[MATH.MATH-OC] Mathematics [math]/Optimization and Control [math.OC][MATH.MATH-OC]Mathematics [math]/Optimization and Control [math.OC]ddc:510
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