Search results for "Linear"

showing 10 items of 7165 documents

Bootstrapping pentagon functions

2018

In PRL 116 (2016) no.6, 062001, the space of planar pentagon functions that describes all two-loop on-shell five-particle scattering amplitudes was introduced. In the present paper we present a natural extension of this space to non-planar pentagon functions. This provides the basis for our pentagon bootstrap program. We classify the relevant functions up to weight four, which is relevant for two-loop scattering amplitudes. We constrain the first entry of the symbol of the functions using information on branch cuts. Drawing on an analogy from the planar case, we introduce a conjectural second-entry condition on the symbol. We then show that the information on the function space, when comple…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsBasis (linear algebra)010308 nuclear & particles physicsFunction spaceFOS: Physical sciencesClassification of discontinuitiesSpace (mathematics)01 natural sciencesSymbol (chemistry)AlgebraScattering amplitudePentagonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Simple (abstract algebra)0103 physical sciencesPerturbative QCDlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsScattering AmplitudesJournal of High Energy Physics
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Modular transformations of elliptic Feynman integrals

2021

We investigate the behaviour of elliptic Feynman integrals under modular transformations. This has a practical motivation: Through a suitable modular transformation we can achieve that the nome squared is a small quantity, leading to fast numerical evaluations. Contrary to the case of multiple polylogarithms, where it is sufficient to consider just variable transformations for the numerical evaluations of multiple polylogarithms, it is more natural in the elliptic case to consider a combination of a variable transformation (i.e. a modular transformation) together with a redefinition of the master integrals. Thus we combine a coordinate transformation on the base manifold with a basis transf…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsClass (set theory)Basis (linear algebra)010308 nuclear & particles physicsbusiness.industryCoordinate systemFOS: Physical sciencesModular designBase (topology)01 natural sciencesManifoldAlgebraHigh Energy Physics - PhenomenologyTransformation (function)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsbusinessVariable (mathematics)
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Nonsingular electrovacuum solutions with dynamically generated cosmological constant

2013

We consider static spherically symmetric configurations in a Palatini extension of General Relativity including R-2 and Ricci-squared terms, which is known to replace the central singularity by a wormhole in the electrovacuum case. We modify the matter sector of the theory by adding to the usual Maxwell term a nonlinear electromagnetic extension which is known to implement a confinement mechanism in flat space. One feature of the resulting theory is that the nonlinear electric field leads to a dynamically generated cosmological constant. We show that with this matter source the solutions of the model are asymptotically de Sitter and possess a wormhole topology. We discuss in some detail the…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsGeneral relativityBlack holesFOS: Physical sciencesCosmological constantSpace (mathematics)Einsten equantionsTheoretical physicsNonlinear systemGeneral Relativity and Quantum CosmologyClassical mechanicsSingularityHigh Energy Physics - Theory (hep-th)De Sitter universeGravitational singularityWormhole
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On Overlapping Divergences

1998

Using set-theoretic considerations, we show that the forest formula for overlapping divergences comes from the Hopf algebra of rooted trees.

PhysicsHigh Energy Physics - TheoryPure mathematicsHigh Energy Physics - Theory (hep-th)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)FOS: Physical sciencesStatistical and Nonlinear PhysicsHopf algebraMathematical Physics
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A star-product approach to noncompact Quantum Groups

1995

Using duality and topological theory of well behaved Hopf algebras (as defined in [2]) we construct star-product models of non compact quantum groups from Drinfeld and Reshetikhin standard deformations of enveloping Hopf algebras of simple Lie algebras. Our star-products act not only on coefficient functions of finite-dimensional representations, but actually on all $C^\infty$ functions, and they exist even for non linear (semi-simple) Lie groups.

PhysicsHigh Energy Physics - TheoryPure mathematics[MATH.MATH-RT]Mathematics [math]/Representation Theory [math.RT]010102 general mathematicsLie groupDuality (optimization)Statistical and Nonlinear Physics16. Peace & justiceHopf algebra01 natural sciences[ MATH.MATH-RT ] Mathematics [math]/Representation Theory [math.RT]Nonlinear systemSimple (abstract algebra)Product (mathematics)Mathematics::Quantum Algebra0103 physical sciencesLie algebraMathematics - Quantum Algebra010307 mathematical physics0101 mathematicsQuantumMathematical PhysicsComputingMilieux_MISCELLANEOUS
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Modular Schrödinger equation and dynamical duality.

2008

We discuss quite surprising properties of the one-parameter family of modular (Auberson and Sabatier (1994)) nonlinear Schr\"{o}dinger equations. We develop a unified theoretical framework for this family. Special attention is paid to the emergent \it dual \rm time evolution scenarios which, albeit running in the \it real time \rm parameter of the pertinent nonlinear equation, in each considered case, may be mapped among each other by means of an "imaginary time" transformation (more seriously, an analytic continuation in time procedure).

PhysicsHigh Energy Physics - TheoryQuantum PhysicsNonlinear Sciences - Exactly Solvable and Integrable SystemsStochastic processTime evolutionDuality (optimization)Schrödinger equationsymbols.namesakeNonlinear systemClassical mechanicssymbolsDissipative systemQuantumBrownian motionCondensed Matter - Statistical MechanicsMathematical PhysicsPhysical review. E, Statistical, nonlinear, and soft matter physics
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Levy flights and nonlocal quantum dynamics

2013

We develop a fully fledged theory of quantum dynamical patterns of behavior that are nonlocally induced. To this end we generalize the standard Laplacian-based framework of the Schr\"{o}dinger picture quantum evolution to that employing nonlocal (pseudodifferential) operators. Special attention is paid to the Salpeter (here, $m\geq 0$) quasirelativistic equation and the evolution of various wave packets, in particular to their radial expansion in 3D. Foldy's synthesis of "covariant particle equations" is extended to encompass free Maxwell theory, which however is devoid of any "particle" content. Links with the photon wave mechanics are explored.

PhysicsHigh Energy Physics - TheoryQuantum PhysicsPhotonStatistical Mechanics (cond-mat.stat-mech)Wave packetQuantum dynamicsFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Schrödinger equationsymbols.namesakeMaxwell's equationsHigh Energy Physics - Theory (hep-th)symbolsSchrödinger pictureMatter waveQuantum Physics (quant-ph)QuantumCondensed Matter - Statistical MechanicsMathematical PhysicsMathematical physics
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RG flows of Quantum Einstein Gravity in the linear-geometric approximation

2014

We construct a novel Wetterich-type functional renormalization group equation for gravity which encodes the gravitational degrees of freedom in terms of gauge-invariant fluctuation fields. Applying a linear-geometric approximation the structure of the new flow equation is considerably simpler than the standard Quantum Einstein Gravity construction since only transverse-traceless and trace part of the metric fluctuations propagate in loops. The geometric flow reproduces the phase-diagram of the Einstein-Hilbert truncation including the non-Gaussian fixed point essential for Asymptotic Safety. Extending the analysis to the polynomial $f(R)$-approximation establishes that this fixed point come…

PhysicsHigh Energy Physics - Theory; High Energy Physics - Theory; General Relativity and Quantum CosmologyHigh Energy Physics - TheoryEntropic gravityGeneral relativityAsymptotic safety in quantum gravityGeneral Physics and AstronomyFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Euclidean quantum gravityGeneral Relativity and Quantum CosmologyGeneral Relativity and Quantum CosmologyClassical mechanicsHigh Energy Physics - Theory (hep-th)Linearized gravityTheoretical High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGQuantum gravitySemiclassical gravityf(R) gravityAnnals of Physics
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Superfield commutators for D = 4 chiral multiplets and their apppications

1987

The superfield commutators and their corresponding equal-time limits are derived in a covariant way for the D=4 free massive chiral multiplet. For interesting chiral multiplets, the general KAllen-Lehmann representation is also introduced. As applications of the free superfield commutators, the general solution of the Cauchy problem for chiral superfields is given, and an analysis of the closure of the bilinear products of superfields which desrcibe the extension of the internal currents for free supersymmetric chiral matter is performed.

PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyClosure (topology)General Physics and AstronomyBilinear interpolationSuperfieldHigh Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsChiral superfieldQuantum electrodynamicsInitial value problemCovariant transformationRepresentation (mathematics)MultipletMathematical physicsCzechoslovak Journal of Physics B
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The Poisson Bracket Structure of the SL(2, R)/U(1) Gauged WZNW Model with Periodic Boundary Conditions

2000

The gauged SL(2, R)/U(1) Wess-Zumino-Novikov-Witten (WZNW) model is classically an integrable conformal field theory. A second-order differential equation of the Gelfand-Dikii type defines the Poisson bracket structure of the theory. For periodic boundary conditions zero modes imply non-local Poisson brackets which, nevertheless, can be represented by canonical free fields.

PhysicsHigh Energy Physics::TheoryPoisson bracketNonlinear Sciences::Exactly Solvable and Integrable SystemsIntegrable systemUniqueness theorem for Poisson's equationConformal field theoryDifferential equationPoisson manifoldGeneral Physics and AstronomyPeriodic boundary conditionsPoisson algebraMathematical physicsFortschritte der Physik
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