Search results for "Mathematical physics"

showing 10 items of 2687 documents

Renormalization group flow of quantum gravity in the Einstein-Hilbert truncation

2002

The exact renormalization group equation for pure quantum gravity is used to derive the non-perturbative $\Fbeta$-functions for the dimensionless Newton constant and cosmological constant on the theory space spanned by the Einstein-Hilbert truncation. The resulting coupled differential equations are evaluated for a sharp cutoff function. The features of these flow equations are compared to those found when using a smooth cutoff. The system of equations with sharp cutoff is then solved numerically, deriving the complete renormalization group flow of the Einstein-Hilbert truncation in $d=4$. The resulting renormalization group trajectories are classified and their physical relevance is discus…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsDensity matrix renormalization groupAsymptotic safety in quantum gravityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Renormalization groupGeneral Relativity and Quantum CosmologyRenormalizationGeneral Relativity and Quantum CosmologyClassical mechanicsHigh Energy Physics - Theory (hep-th)Functional renormalization groupQuantum gravitySemiclassical gravityUltraviolet fixed pointMathematical physicsPhysical Review D
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Supersymmetry in non commutative superspaces

2003

Non commutative superspaces can be introduced as the Moyal-Weyl quantization of a Poisson bracket for classical superfields. Different deformations are studied corresponding to constant background fields in string theory. Supersymmetric and non supersymmetric deformations can be defined, depending on the differential operators used to define the Poisson bracket. Some examples of deformed, 4 dimensional lagrangians are given. For extended superspace (N>1), some new deformations can be defined, with no analogue in the N=1 case.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesFísicaSupersymmetrySuperspaceString theoryDifferential operatorNoncommutative geometryPoisson bracketQuantization (physics)High Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Commutative propertyComputer Science::DatabasesParticle Physics - TheoryMathematical physics
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Weyl Invariance and Black Hole Evaporation

1995

We consider the semiclassical dynamics of CGHS black holes with a Weyl-invariant effective action for conformal matter. The trace anomaly of Polyakov effective action is converted into the Virasoro anomaly thus leading to the same flux of Hawking radiation. The covariance of semiclassical equations can be restored through a non-local redefinition of the metric-dilaton fields. The resulting theory turns out to be equivalent to the RST model. This provides a mechanism to solve semiclassical equations of 2D dilaton gravity coupled to conformal matter for classically soluble models.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesSemiclassical physicsConformal mapRST modelBlack holeGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)AstronomiaDilatonAnomaly (physics)Effective actionMathematical physicsHawking radiation
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On selfdual spin-connections and asymptotic safety

2016

We explore Euclidean quantum gravity using the tetrad field together with a selfdual or anti-selfdual spin-connection as the basic field variables. Setting up a functional renormalization group (RG) equation of a new type which is particularly suitable for the corresponding theory space we determine the non-perturbative RG flow within a two-parameter truncation suggested by the Holst action. We find that the (anti-)selfdual theory is likely to be asymptotically safe. The existing evidence for its non-perturbative renormalizability is comparable to that of Einstein-Cartan gravity without the selfduality condition.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsField (physics)010308 nuclear & particles physicsMathematics::Analysis of PDEsAsymptotic safety in quantum gravityFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Euclidean quantum gravitySpace (mathematics)01 natural sciencesGeneral Relativity and Quantum Cosmologylcsh:QC1-999Action (physics)High Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Flow (mathematics)0103 physical sciencesFunctional renormalization groupMathematics::Differential Geometry010306 general physicsTetradlcsh:PhysicsMathematical physicsPhysics Letters B
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A note on Einstein gravity on AdS(3) and boundary conformal field theory

1998

We find a simple relation between the first subleading terms in the asymptotic expansion of the metric field in AdS$_3$, obeying the Brown-Henneaux boundary conditions, and the stress tensor of the underlying Liouville theory on the boundary. We can also provide an more explicit relation between the bulk metric and the boundary conformal field theory when it is described in terms of a free field with a background charge.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsField (physics)Cauchy stress tensorBoundary (topology)Boundary conformal field theoryFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Free fieldGeneral Relativity and Quantum Cosmologysymbols.namesakeHigh Energy Physics - Theory (hep-th)symbolsAstronomiaBoundary value problemCamps Teoria quàntica deEinsteinAsymptotic expansionMathematical physics
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One-loop effective action for a generic 2d dilaton gravity theory

1997

We study the one-loop effective action for a generic two-dimensional dilaton gravity theory conformally coupled to $N$ matter fields. We obtain an explicit expression for the effective action in the weak-coupling limit under a suitable restriction of the dilaton potential asymptotics. Our result applies to the CGHS model as well as to the spherically symmetric general relativity. The effective action is obtained by using the background-field method, and we take into account the loop contributions from all the fields in the classical action and from the ghosts. In the large-$N$ limit, and after an appropriate field redefinition, the one-loop correction takes the form of the Polyakov-Liouvill…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsField (physics)General relativityCGHS modelFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyAction (physics)Loop (topology)General Relativity and Quantum CosmologyHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Dilatonlcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)Effective actionMathematical physicsNuclear Physics B
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Connections and geodesics in the space of metrics

2015

We argue that the exponential relation $g_{\mu\nu} = \bar{g}_{\mu\rho}\big(\mathrm{e}^h\big)^\rho{}_\nu$ is the most natural metric parametrization since it describes geodesics that follow from the basic structure of the space of metrics. The corresponding connection is derived, and its relation to the Levi-Civita connection and the Vilkovisky-DeWitt connection is discussed. We address the impact of this geometric formalism on quantum gravity applications. In particular, the exponential parametrization is appropriate for constructing covariant quantities like a reparametrization invariant effective action in a straightforward way. Furthermore, we reveal an important difference between Eucli…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsGeodesicFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)General Relativity and Quantum CosmologyExponential functionCombinatoricsGeneral Relativity and Quantum CosmologyFormalism (philosophy of mathematics)High Energy Physics - Theory (hep-th)Quantum mechanicsEuclidean geometryQuantum gravityCovariant transformationEffective actionMathematical PhysicsPhysical Review D
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Towards N=1 Super-Yang-Mills on the Lattice

1997

We consider the lattice regularization of N=1 supersymmetric Yang--Mills theory with Wilson fermions. This formulation breaks supersymmetry at any finite lattice spacing; we discuss how Ward identities can be used to define a supersymmetric continuum limit, which coincides with the point where the gluino becomes massless. As a first step towards the understanding of the zero gluino-mass limit, we present results on the quenched low-lying spectrum of SU(2) N=1 Super-Yang--Mills, at $\beta=2.6$ on a $V=16^3 \times 32$ lattice, in the OZI approximation. Our results, in spite of the quenched and OZI approximations, are in remarkable agreement with theoretical predictions in the supersymmetric t…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsGluinoHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesYang–Mills existence and mass gapParticle Physics - LatticeFermionSupersymmetryMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - LatticeLattice constantHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Regularization (physics)Lattice (order)Mathematical physics
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All-order equation of the effective gluon mass

2012

We present the general derivation of the full non-perturbative equation that governs the momentum evolution of the dynamically generated gluon mass, in the Landau gauge. The entire construction hinges crucially on the inclusion of longitudinally coupled vertices containing massless poles of non-perturbative origin, which preserve the form of the fundamental Slavnov-Taylor identities of the theory. The mass equation is obtained from a previously unexplored version of the Schwinger-Dyson equation for the gluon propagator, particular to the PT-BFM formalism, which involves a reduced number of "two-loop dressed" diagrams, thus simplifying the calculational task considerably. The two-loop contri…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPropagatorFísicaMonotonic functionIntegral equationGluonMassless particleMass formulaHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)HomogeneousLattice (order)Quantum electrodynamicsMathematical physics
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Cohomological analysis of gauged-fixed gauge theories

1999

The relation between the gauge-invariant local BRST cohomology involving the antifields and the gauge-fixed BRST cohomology is clarified. It is shown in particular that the cocycle conditions become equivalent once it is imposed, on the gauge-fixed side, that the BRST cocycles should yield deformations that preserve the nilpotency of the (gauge-fixed) BRST differential. This shows that the restrictions imposed on local counterterms by the Quantum Noether condition in the Epstein--Glaser construction of gauge theories are equivalent to the restrictions imposed by BRST invariance on local counterterms in the standard Lagrangian approach.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesCohomologyBRST quantizationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)symbolsGauge theoryNoether's theoremQuantumDifferential (mathematics)LagrangianParticle Physics - TheoryMathematical physics
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