Search results for "Dimension"

showing 10 items of 2766 documents

Duality relation between radiation thermodynamics and cosmic string loop thermodynamics

2011

We discuss thermodynamics of electromagnetic radiation, with p=(1/3){rho} and S{proportional_to}T{sup 3}V, and of cosmic string loops, with p=-(1/3){rho} and S{proportional_to}T{sup -3}V, where p stands for pressure, T temperature, {rho} energy density, S entropy, and V volume. We write the thermodynamic formalisms under a common framework that illustrates their formal relationship and allows us to go from one to the other through a smooth transformation. From a microscopic perspective, these relations arise from the energy relations u({lambda})=hc/{lambda} for the photons of electromagnetic radiation, and u(l)=(c{sup 4}/a{sup 2}G)l for cosmic string loops, a being a numerical (dimensionles…

PhysicsNuclear and High Energy PhysicsThermodynamicsElementary particleLambdaPlanck constantElectromagnetic radiationGravitational constantCosmic stringEntropy (classical thermodynamics)symbols.namesakeQuantum mechanicssymbolscosmic stringelectromagnetic radiation thermodynamics T-duality thermal duality.Settore MAT/07 - Fisica MatematicaDimensionless quantityPhysical Review D
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Measurement oftt¯production in theτ+jetstopology usingpp¯collisions ats=1.96  TeV

2010

We present a measurement of the t (t) over bar production cross section multiplied by the branching ratio to tau lepton decaying semihadronically (tau(h)) plus jets, sigma(p (p) over bar -> t (t) over bar + X) center dot BR(t (t) over bar -> tau(h) + jets), at a center of mass energy root s = 1.96 TeV using 1 fb(-1) of integrated luminosity collected with the D0 detector. Assuming a top quark mass of 170 GeV, we measure sigma(t (t) over bar) center dot BR tau h (+ j) = 0.60(-0.22)(+0.23)(stat)(-0.14)(+0.15)(syst) +/- 0.04(lumi) pb. In addition, we extract the t (t) over bar production cross section using the t (t) over bar -> tau(h) + jets topology, with the result sigma(t (t) over bar) = 6…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyElementary particleTopology01 natural sciencesNuclear physicsParticle decay0103 physical sciencesHigh Energy Physics::ExperimentCenter of mass010306 general physicsLeptonDimensionless quantityBar (unit)Physical Review D
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Limits on Anomalous Top Couplings from Z Pole Physics

1997

We obtain constraints on possible anomalous interactions of the top quark with the electroweak vector bosons arising from the precision measurements at the Z pole. In the framework of $SU(2)_L \otimes U(1)_Y$ chiral Lagrangians, we examine all effective CP-conserving operators of dimension five which induce fermionic currents involving the top quark. We constrain the magnitudes of these anomalous interactions by evaluating their one-loop contributions to the Z pole physics. Our analysis shows that the operators that contribute to the LEP observables get bounds close to the theoretical expectation for their anomalous couplings. We also show that those which break the $SU(2)_C$ custodial symm…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableCustodial symmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Bounded functionBoson
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Can power corrections be reliably computed in models with extra dimensions?

2003

We critically revisit the issue of power-law running in models with extra dimensions. The analysis is carried out in the context of a higher-dimensional extension of QED, with the extra dimensions compactified on a torus. It is shown that a naive $\beta$ function, which simply counts the number of modes, depends crucially on the way the thresholds of the Kaluza-Klein modes are crossed. To solve these ambiguities we turn to the vacuum polarization, which, due to its special unitarity properties, guarantees the physical decoupling of the heavy modes. This latter quantity, calculated in the context of dimensional regularization, is used for connecting the low energy gauge coupling with the cou…

PhysicsNuclear and High Energy PhysicsToy modelFOS: Physical sciencesFísicaContext (language use)Universal extra dimensionTheoretical physicsExtra dimensionsDimensional regularizationHigh Energy Physics - PhenomenologyClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Effective field theoryBeta function (physics)Vacuum polarization
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Pinch technique at two loops: The case of massless Yang-Mills theories

2000

The generalization of the pinch technique beyond one loop is presented. It is shown that the crucial physical principles of gauge-invariance, unitarity, and gauge-fixing-parameter independence single out at two loops exactly the same algorithm which has been used to define the pinch technique at one loop, without any additional assumptions. The two-loop construction of the pinch technique gluon self-energy, and quark-gluon vertex are carried out in detail for the case of mass-less Yang-Mills theories, such as perturbative QCD. We present two different but complementary derivations. First we carry out the construction by directly rearranging two-loop diagrams. The analysis reveals that, quit…

PhysicsNuclear and High Energy PhysicsUnitarityBackground field methodFOS: Physical sciencesFísicaYang–Mills existence and mass gapSymmetry (physics)RenormalizationHigh Energy Physics - PhenomenologyDimensional regularizationsymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicssymbolsFeynman diagramGauge theoryPhysical Review D
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EXTRACTION OF INFRARED DIVERGENCES IN THE DIMENSIONAL REGULARIZED TWO-LOOP LADDER GRAPH

1994

We consider the evaluation of the fundamental scalar integral in the on-shell two-loop ladder graph with different external masses and arbitrary transfer momentum. A method for cleanly extracting the infrared divergences in the Feynman parameter integrals using dimensional regularization is presented, and we analyze one of the finite part contributions to this integral.

PhysicsNuclear and High Energy Physicssymbols.namesakeDimensional regularizationInfraredMathematical analysisScalar (mathematics)symbolsFeynman diagramAstronomy and AstrophysicsLadder graphAtomic and Molecular Physics and OpticsInternational Journal of Modern Physics A
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New measurement of the K±→π±μ+μ− decay

2011

Abstract A sample of 3120 K ± → π ± μ + μ − decay candidates with ( 3.3 ± 0.7 ) % background contamination has been collected by the NA48/2 experiment at the CERN SPS, allowing a detailed study of the decay properties. The branching ratio was measured to be BR = ( 9.62 ± 0.25 ) × 10 − 8 . The form factor W ( z ) , where z = ( M μ μ / M K ) 2 , was parameterized according to several models. In particular, the slope of the linear form factor W ( z ) = W 0 ( 1 + δ z ) was measured to be δ = 3.11 ± 0.57 . Upper limits of 2.9 × 10 − 2 and 2.3 × 10 − 2 on possible charge asymmetry and forward–backward asymmetry were established at 90% CL. An upper limit BR ( K ± → π ∓ μ ± μ ± ) 1.1 × 10 − 9 was e…

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle decayAntiparticleMuonPionMesonBranching fractionAnalytical chemistryLeptonDimensionless quantityPhysics Letters B
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Measurement of the 151Sm n,gamma 152Sm cross section at n_TOF

2005

The 151 Sm(n, γ ) 152 Sm cross section, which is important for the interpretation of the 151 Sm branching as an s -process thermometer, was measured from 1 eV up to 1 MeV at the innovative n_TOF facility at CERN. Based on these data, the Maxwellian-averaged cross section at k T = 30  keV is found to be 3100±160 mb. This value can be used to constrain the thermodynamical conditions in Asymptotic Giant Branch (AGB) stars during He-shell burning.

PhysicsNuclear reactionNeutronsNuclear and High Energy Physics:Física [Àrees temàtiques de la UPC]Branching fraction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Giant star01 natural sciencesNeutrons--CaptureNuclear physicsStarsNucleosynthesis0103 physical sciencesAsymptotic giant branchAstrophysics::Solar and Stellar Astrophysics010306 general physicss-processNuclear Experiment010303 astronomy & astrophysicsDimensionless quantity
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Structure of theN=27isotones derived from theAr44(d,p)Ar45reaction

2008

The $^{44}\mathrm{Ar}$($d,p$)$^{45}\mathrm{Ar}$ neutron transfer reaction was performed at $10A$ MeV. Measured excitation energies, deduced angular momenta, and spectroscopic factors of the states populated in $^{45}\mathrm{Ar}$ are reported. A satisfactory description of these properties is achieved in the shell model framework using a new $\mathit{sdpf}$ interaction. The model analysis is extended to more exotic even-$Z$ nuclei down to ${}_{14}^{41}{\mathrm{Si}}_{27}$ to study how collectivity impacts the low-lying structure of $N=27$ neutron-rich nuclei.

PhysicsNuclear reactionNuclear and High Energy PhysicsAngular momentum010308 nuclear & particles physicsNuclear TheoryStructure (category theory)01 natural sciences0103 physical sciencesAstrophysics::Solar and Stellar AstrophysicsNeutronIsotopes of siliconAtomic physicsNuclear Experiment010306 general physicsRadioactive decayExcitationDimensionless quantityPhysical Review C
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Deep sub-threshold K*(892)0 production in collisions of Ar + KCl at 1.76A GeV

2013

Results on the deep sub-threshold production of the short-lived hadronic resonance K*(892)0 are reported for collisions of Ar + KCl at 1.76A GeV beam energy, studied with the High Acceptance Di-Electron Spectrometer (HADES) at SIS18/GSI. The K*(892)0 production probability per central collision of \( P_{K^{*0}}=(4.4\pm 1.1 \pm 0.5)\times 10^{-4}\) and the K*(892)0/K0 ratio of \( P_{K^{*0}}/P_{K^0}=(1.9\pm 0.5\pm 0.3)\times 10^{-2}\) are determined at the lowest energy so far (i.e. deep below the threshold for the corresponding production in nucleon-nucleon collisions, \( \sqrt{s_{NN}}-\sqrt{s_{thr}}=-340\) MeV). The K*0/K0 ratio is compared with results of other experiments and with the pre…

PhysicsNuclear reactionNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsBranching fractionHadron7. Clean energy01 natural sciencesHadronizationNuclear physics0103 physical sciencesProduction (computer science)Atomic physics010306 general physicsNuclear ExperimentEnergy (signal processing)Dimensionless quantity
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