Search results for "phase space"

showing 10 items of 176 documents

Remarks on quantum groups

1991

We give a Poisson-bracket realization of SL q (2) in the phase space ℝ2. We then discuss the physical meaning of such a realization in terms of a modified (regularized) toy model, the nonregularized version of which is due to Klauder. Some general remarks and suggestions are also presented in this Letter.

Poisson bracketTheoretical physicsToy modelQuantum groupPhase spaceComplex systemStatistical and Nonlinear PhysicsMeaning (non-linguistic)QuantumRealization (systems)Mathematical PhysicsMathematicsMathematical physicsLetters in Mathematical Physics
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Antiproton over proton and K$^-$ over K$^+$ multiplicity ratios at high $z$ in DIS

2020

The $\bar{\rm p} $ over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, $z>0.5$. The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar $^6$LiD target. The regime of deep-inelastic scattering is ensured by requiring $Q^2$ > 1 (GeV/$c$)$^2$ for the photon virtuality and $W > 5$ GeV/$c^2$ for the invariant mass of the produced hadronic system. The range in Bjorken-$x$ is restricted to $0.01 < x < 0.40$. Protons and antiprotons are identified in the momentum range $20 ��60$ GeV/$c$. In the whole studied $z$-region, the $\…

ProtonIsoscalarHadron0 [higher-order]Deep-inelastic scatteringtarget: isoscalar01 natural sciencesCOMPASSdeep inelastic scattering [muon+ nucleon]High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]anti-p: multiplicityInvariant massisoscalar [target]Nuclear Experiment (nucl-ex)Nuclear ExperimentHadron multiplicitiesNuclear ExperimentQuantum chromodynamicsPhysicsmultiplicity [K+]quark: fragmentation functionhigher-order: 0K+: multiplicityphotonperturbation theory: higher-orderhigher-order: 1multiplicity [anti-p]lcsh:QC1-999Bjorken [scaling]beam [muon]factorization [cross section]1 [higher-order]Particle Physics - Experimentperturbation theory [quantum chromodynamics]Nuclear and High Energy PhysicsFOS: Physical sciencesratio [multiplicity]530pQCDfragmentation function [quark]scaling: Bjorkenx-dependenceNuclear physicsQuantum chromodynamics; pQCD; Deep-inelastic scattering; Hadron multiplicities; COMPASSphase space0103 physical sciencesddc:530quantum chromodynamics: perturbation theory010306 general physicsmuon+ nucleon: deep inelastic scatteringp: multiplicityMuonmultiplicity [K-]multiplicity: ratio010308 nuclear & particles physicshep-exmuon: beamcross section: factorizationCERN SPSDeep inelastic scatteringmultiplicity: measured [charged particle]higher-order [perturbation theory]K-: multiplicityAntiprotonHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamicscharged particle: multiplicity: measuredhadronizationmultiplicity [p]experimental results
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Integrability via Reversibility

2017

Abstract A class of left-invariant second order reversible systems with functional parameter is introduced which exhibits the phenomenon of robust integrability: an open and dense subset of the phase space is filled with invariant tori carrying quasi-periodic motions, and this behavior persists under perturbations within the class. Real-analytic volume preserving systems are found in this class which have positive Lyapunov exponents on an open subset, and the complement filled with invariant tori.

Pure mathematicsClass (set theory)Dense setGeneral Physics and AstronomyLyapunov exponentDynamical Systems (math.DS)IntegrabilityCoexistence of integrability and chaotic behavior01 natural sciencessymbols.namesakeReversibility0103 physical sciencesFOS: MathematicsOrder (group theory)0101 mathematicsInvariant (mathematics)Mathematics - Dynamical SystemsMathematical PhysicsMathematicsComplement (set theory)010102 general mathematicsTorusPhase spacesymbols010307 mathematical physicsGeometry and Topology
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The 0-Parameter Case

1998

As an introduction to the theory of bifurcations, in this chapter we want to consider individual vector fields, i.e., families of vector fields with a 0-dimensional parameter space. We will present two fundamentals tools: the desingularization and the asymptotic expansion of the return map along a limit periodic set. In the particular case of an individual vector field these techniques give the desired final result: the desingularization theorem says that any algebraically isolated singular point may be reduced to a finite number of elementary singularities by a finite sequence of blow-ups. If X is an analytic vector field on S 2, then the return map of any elementary graphic has an isolate…

Pure mathematicsPhase spaceVector fieldLimit (mathematics)Singular point of a curveFixed pointParameter spaceAsymptotic expansionFinite setMathematics
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Generic Properties of Dynamical Systems

2006

The state of a concrete system (from physics, chemistry, ecology, or other sciences) is described using (finitely many, say n) observable quantities (e.g., positions and velocities for mechanical systems, population densities for echological systems, etc.). Hence, the state of a system may be represented as a point $x$ in a geometrical space $\mathbb R^n$. In many cases, the quantities describing the state are related, so that the phase space (space of all possible states) is a submanifold $M\subset \mathbb R^n$. The time evolution of the system is represented by a curve $x_t$, $t \in\mathbb R$ drawn on the phase space $M$, or by a sequence $x_n \in M$, $n \in\mathbb Z$, if we consider disc…

Pure mathematicsSequenceDynamical systems theoryGeneric property010102 general mathematicsObservableState (functional analysis)Space (mathematics)Submanifold01 natural sciencesPhase space0103 physical sciences010307 mathematical physics0101 mathematics
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From where do quantum groups come?

1993

The phase space realizations of quantum groups are discussed using *-products. We show that on phase space, quantum groups appear necessarily as two-parameter deformation structures, one parameter (v) being concerned with the quantization in phase space, the other (η) expressing the quantum groups as “deformation” of their Lie counterparts. Introducing a strong invariance condition, we show the uniqueness of the η-deformation. This suggests that the strong invariance condition is a possible origin of the quantum groups.

Quantization (physics)POVMCanonical quantizationQuantum processPhase spaceQuantum mechanicsQuantum operationGeneral Physics and AstronomyQuantum phasesGroup theoryMathematicsFoundations of Physics
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Multiple polylogarithms with algebraic arguments and the two-loop EW-QCD Drell-Yan master integrals

2020

We consider Feynman integrals with algebraic leading singularities and total differentials in $\epsilon\,\mathrm{d}\ln$ form. We show for the first time that it is possible to evaluate integrals with singularities involving unrationalizable roots in terms of conventional multiple polylogarithms, by either parametric integration or matching the symbol. As our main application, we evaluate the two-loop master integrals relevant to the $\alpha \alpha_s$ corrections to Drell-Yan lepton pair production at hadron colliders. We optimize our functional basis to allow for fast and stable numerical evaluations in the physical region of phase space.

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryBasis (linear algebra)010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLoop (topology)High Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Phase space0103 physical sciencesGravitational singularityHigh Energy Physics::ExperimentAlgebraic number010306 general physicsMathematical physics
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Wγproduction in vector boson fusion at NLO in QCD

2014

The next-to-leading order QCD corrections to ${W}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\gamma}$ production in association with two jets via vector boson fusion are calculated, including the leptonic decay of the $W$ with full off-shell effects and spin correlations. The process lends itself to a test of quartic gauge couplings. The next-to-leading order corrections reduce the scale uncertainty significantly and show a nontrivial phase space dependence.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsPhotonHigh Energy Physics::PhenomenologyOrder (ring theory)Scalar boson7. Clean energyVector bosonPhase spaceHigh Energy Physics::ExperimentProduction (computer science)Spin-½Physical Review D
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WZ Production in Association with Two Jets at Next-to-Leading Order in QCD

2013

We report on the calculation of W-+/- Zjj production with leptonic decays at hadron-hadron colliders at next-to-leading order in QCD. These processes are important both to test the quartic gauge couplings of the standard model and because they constitute relevant backgrounds to beyond standard model physics searches. Our results show that the next-to-leading order corrections reduce significantly the scale uncertainties and have a nontrivial phase space dependence.

Quantum chromodynamicsPhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyOrder (ring theory)Gauge (firearms)NLO QCD01 natural sciencesStandard ModelPhase spaceQuartic function0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsHadron colliders
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Phase transition of light on complex quantum networks

2012

Recent advances in quantum optics and atomic physics allow for an unprecedented level of control over light-matter interactions, which can be exploited to investigate new physical phenomena. In this work we are interested in the role played by the topology of quantum networks describing coupled optical cavities and local atomic degrees of freedom. In particular, using a mean-field approximation, we study the phase diagram of the Jaynes-Cummings-Hubbard model on complex networks topologies, and we characterize the transition between a Mott-like phase of localized polaritons and a superfluid phase. We found that, for complex topologies, the phase diagram is non-trivial and well defined in the…

Quantum opticsPhysicsQuantum phase transitionQuantum PhysicsQuantum networkModels StatisticalStatistical Mechanics (cond-mat.stat-mech)LightFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Quantum phasesCondensed Matter - Disordered Systems and Neural NetworksPhase TransitionOpen quantum systemOptical phase spaceQuantum critical pointQuantum mechanicsQuantum TheoryScattering RadiationComputer SimulationQuantum algorithmQuantum Physics (quant-ph)Condensed Matter - Statistical Mechanics
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