Search results for "ASYM"

showing 10 items of 2151 documents

Pion–nucleus Drell–Yan data as a novel constraint for nuclear PDFs

2017

We have studied the prospects of using the Drell-Yan dilepton process in pion-nucleus collisions as a novel input in the global analysis of nuclear parton distribution functions (nPDFs). In a NLO QCD framework, we find the measured nuclear cross-section ratios from the NA3, NA10 and E615 experiments to be largely insensitive to the pion parton distributions and also compatible with the EPS09 and nCTEQ15 nPDFs. These data sets can thus be, and in EPPS16 have been, included in global nPDF analyses without introducing significant new theoretical uncertainties or tension with the other data. In particular, we explore the constraining power of these data sets on the possible flavour asymmetry in…

Quantum chromodynamicsPhysicsParticle physicsmedia_common.quotation_subjectHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyNuclear TheoryDrell–Yan processPartonInelastic scatteringDrell–Yan dilepton processAsymmetryDistribution functionPionnuclear PDFsHigh Energy Physics::ExperimentNuclear Experimentmedia_common
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Massive color-octet bosons and the charge asymmetries of top quarks at hadron colliders

2008

Several models predict the existence of heavy colored resonances decaying to top quarks in the TeV energy range that might be discovered at the LHC. In some of those models, moreover, a sizable charge asymmetry of top versus antitop quarks might be generated. The detection of these exotic resonances, however, requires selecting data samples where the top and the antitop quarks are highly boosted, which is experimentally very challenging. We asses that the measurement of the top quark charge asymmetry at the LHC is very sensitive to the existence of excited states of the gluon with axial-vector couplings to quarks. We use a toy model with general flavour independent couplings, and show that …

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsmedia_common.quotation_subjectHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaOmega baryonAsymmetrySigma baryonGluonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experimentmedia_common
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Method of analytic continuation by duality in QCD: Beyond QCD sum rules

1986

We present the method of analytic continuation by duality which allows the approximate continuation of QCD amplitudes to small values of the momentum variables where direct perturbative calculations are not possible. This allows a substantial extension of the domain of applications of hadronic QCD phenomenology. The method is illustrated by a simple example which shows its essential features.

Quantum chromodynamicsPhysicsTheoretical physicsQCD sum rulesParticle physicsContinuationAnalytic continuationSpace timeHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentElementary particleAsymptotic expansionPhenomenology (particle physics)Physical Review D
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Measurement of the forward-backward asymmetry in the distribution of leptons intt¯events in thelepton+jetschannel

2014

We present measurements of the forward-backward asymmetry in the angular distribution of leptons from decays of top quarks and antiquarks produced in proton-antiproton collisions. We consider the final state containing a lepton and at least three jets. The entire sample of data collected by the D0 experiment during Run II of the Fermilab Tevatron Collider, corresponding to 9.7 inverse fb of integrated luminosity, is used. The asymmetry measured for reconstructed leptons is $A_{FB}^l = \big(2.9 \pm 2.1(stat.) ^{+1.5}_{-1.7}(syst.) \big)$%. When corrected for efficiency and resolution effects within the lepton rapidity coverage of $|y_l|<1.5$, the asymmetry is found to be $A_{FB}^l = \big(4.2…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsGenerator (category theory)media_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronInverse7. Clean energyAsymmetryNuclear physicsHigh Energy Physics::ExperimentRapidityNuclear ExperimentLeptonmedia_commonPhysical Review D
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Violation of the Time-Reversal and Particle-Hole Symmetries in Strongly Correlated Fermi Systems: A Review

2020

In this review, we consider the time reversal T and particle-antiparticle C symmetries that, being most fundamental, can be violated at microscopic level by a weak interaction. The notable example here is from condensed matter, where strongly correlated Fermi systems like heavy-fermion metals and high Tc superconductors exhibit C and T symmetries violation due to so-called non-Fermi liquid (NFL) behavior. In these systems, tunneling differential conductivity (or resistivity) is a very sensitive tool to experimentally test the above symmetry break. When a strongly correlated Fermi system turns out to be near the topological fermion condensation quantum phase transition (FCQPT), it exhibits t…

Quantum phase transitionPhysics and Astronomy (miscellaneous)General Mathematicsmedia_common.quotation_subjectquantum phase transition; fermion condensation; tunneling conductivity; time-reversal symmetryWeak interaction01 natural sciencesAsymmetry010305 fluids & plasmastime-reversal symmetryBaryon asymmetry0103 physical sciencesComputer Science (miscellaneous)quantum phase transition010306 general physicstunneling conductivitymedia_commonPhysicsCondensed matter physicslcsh:MathematicsFermionlcsh:QA1-939Symmetry (physics)T-symmetryChemistry (miscellaneous)Computer Science::Programming LanguagesFermi liquid theoryfermion condensationSymmetry-Basel
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Baryon Asymmetry Resulting from FCQPT in the Early Universe

2014

This Chapter does not follow the main line of the book that is the theory of HF compounds but illustrates how the ideas of FC may be applicable to describe a very dissimilar system. Namely, here we consider a novel mechanism for explaining the matter-antimatter asymmetry of the universe. We assume that the universe starts from completely symmetric state and then, as it cools down, it undergoes a quantum phase transition, which in turn causes an asymmetry between matter and anti-matter. As we shall see the quantum phase transition is represented by FCQPT. The mechanism does not require the baryon number violating interactions or \({\textit{CP}}\) violation at a microscopic level. The state F…

Quantum phase transitionPhysicsParticle physicsBaryon asymmetrymedia_common.quotation_subjectAntimatterQuantum critical pointSupersymmetryBaryon numberAsymmetryUniversemedia_common
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Metals with a Strongly Correlated Electron Liquid

2014

In this chapter, we consider the main properties of strongly correlated Fermi systems, which are formed by the fermion condensate leading to the emergence of flat bands. Namely, we consider the residual entropy \(S_0\) related to the flat bands that leads to the violation of the quasiparticle—hole symmetry. The presence of \(S_0\) has a profound impact on the universality of second order phase transitions. In that case under the application of magnetic field the curve of the second order AF phase transitions passes into a curve of the first order ones at the tricritical point, thus leading to a violation of the critical universality of the fluctuation theory. We demonstrate that a jump in t…

Quantum phase transitionPhysicsPhase transitionResidual resistivityTricritical pointCondensed matter physicsmedia_common.quotation_subjectElectron liquidFermionResidual entropyAsymmetrymedia_common
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Applicability of pion-nucleus Drell-Yan data in global analysis of nuclear parton distribution functions

2017

Despite the success of modern nuclear parton distribution functions (nPDFs) in describing nuclear hard-process data, they still suffer from large uncertainties. One of the poorly constrained features is the possible asymmetry in nuclear modifications of valence $u$ and $d$ quarks. We study the possibility of using pion-nucleus Drell-Yan dilepton data as a new constraint in the global analysis of nPDFs. We find that the nuclear cross-section ratios from the NA3, NA10 and E615 experiments can be used without imposing significant new theoretical uncertainties and, in particular, that these datasets may have some constraining power on the $u$/$d$ -asymmetry in nuclei.

QuarkDrell-Yan processParticle physicsNuclear and High Energy PhysicsNuclear Theorymedia_common.quotation_subjectNuclear TheoryDrell–Yan processFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciencesAsymmetry114 Physical sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)PionRATIO0103 physical sciencesmedicinePion–nucleus scatteringNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryNuclear Experimentmedia_commonPhysicsta114010308 nuclear & particles physicskvarkitHigh Energy Physics::PhenomenologyDrell–Yan processNuclear parton distribution functionsPion-nucleus scatteringlcsh:QC1-999pion–nucleus scatteringnuclear parton distribution functionsHigh Energy Physics - PhenomenologyDistribution functionmedicine.anatomical_structureDIMUON PRODUCTIONHigh Energy Physics::ExperimentNucleusPDFSlcsh:Physics
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Two-parton contribution to the heavy-quark forward–backward asymmetry in NNLO QCD

2006

Forward-backward asymmetries, $A_{FB}^Q$, are important observables for the determination of the neutral-current couplings of heavy quarks in inclusive heavy quark production, $e^+ e^- \to \gamma^*, Z^* \to Q +X$. In view of the measurement perspectives on $A_{FB}^Q$ at a future linear collider, precise predictions of $A_{FB}^Q$ are required for massive quarks. We compute the contribution of the $Q \bar Q$ final state to $A_{FB}^Q$ to order $\as^2$ in the QCD coupling. We provide general formulae, and we show that this contribution to $A_{FB}^Q$ is infrared-finite. We evaluate these two-parton contributions for $b$ and $c$ quarks on and near the $Z$ resonance, and for $t$ quarks above thres…

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticemedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesParton01 natural sciencesAsymmetrylaw.inventionNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesPERTURBATIVE QCDNuclear Experiment010306 general physicsCollidermedia_commonCondensed Matter::Quantum GasesPhysicsQuantum chromodynamicsCouplingASYMMETRY IN NNLO QCD010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceObservableHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentHEAVY QUARKSRADIATIVE CORRECTIONSNuclear Physics B
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Measurement of the Collins and Sivers asymmetries on transversely polarised protons

2010

The Collins and Sivers asymmetries for charged hadrons produced in deeply inelastic scattering on transversely polarised protons have been extracted from the data collected in 2007 with the CERN SPS muon beam tuned at 160 GeV/c. At large values of the Bjorken x variable non-zero Collins asymmetries are observed both for positive and negative hadrons while the Sivers asymmetry for positive hadrons is slightly positive over almost all the measured x range. These results nicely support the present theoretical interpretation of these asymmetries, in terms of leading-twist quark distribution and fragmentation functions.

QuarkNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectSivers asymmetryNuclear TheoryHadronFOS: Physical sciencesInelastic scattering01 natural sciencesAsymmetryCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesTransverse spin effectNuclear Experiment010306 general physicsmedia_commonPhysicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTransverse spin effectsCollins asymmetryPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentTransverse spin effects; Proton; Collins asymmetry; Sivers asymmetry; COMPASSProtonParticle Physics - Experiment
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