Search results for "Collision"

showing 10 items of 908 documents

Recent results from PHENIX on the evolution of hot QCD

2014

The Relativistic Heavy Ion Collider’s (RHIC) energy scan program explores the phase transition between the hadron gas and the quark gluon plasma phases by varying center-of-mass energies from √sNN = 7.7 to 200 GeV and using various system sizes. The nuclear modification factor of π0 and the azimuthal anisotropy of charged hadrons were measured in Au+Au collisions at c.m. energies √sNN = 39, 62.4 and 200 GeV. In addition, we present recent results of direct photon yield and anisotropy measurements in Au+Au collisions at c.m. energy √sNN = 200 GeV.

Quantum chromodynamicsPhysicsParticle physicsPhase transitionta114PhysicsQC1-999HadronNUCLEUS-NUCLEUS COLLISIONSHigh Energy Physics::PhenomenologyNuclear TheoryModification factorCOLLABORATION7. Clean energyPhoton yield114 Physical sciencesNuclear physicsQuark–gluon plasmaHigh Energy Physics::ExperimentRelativistic Heavy Ion ColliderAnisotropyNuclear ExperimentMATTEREPJ Web of Conferences
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Objective features in quantum states

2023

One of the key features of quantum mechanics is that any superposition of quantum states is in itself a legitimate quantum state. This has far reaching consequences, and is behind the stark difference in behaviour between quantum and classical systems. In particular, quantum systems are not -unlike classical ones- intrinsically objective, that is, different observers are not always able to agree on the properties of the system. Understanding the conditions for objectivity in quantum states is therefore key to address the wider issue of the quantum-to-classical transition. Here, we discuss several aspects of quantum objectivity, and in particular subtleties that arise to the definitions of o…

Quantum objectivityOpen quantum systemQuantum DarwinismCollision modelsQuantum-to-classical transitionSettore FIS/03 - Fisica Della MateriaSpectrum broadcast structure
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Collision models in quantum optics

2017

AbstractQuantum collision models (CMs) provide advantageous case studies for investigating major issues in open quantum systems theory, and especially quantum non-Markovianity. After reviewing their general definition and distinctive features, we illustrate the emergence of a CM in a familiar quantum optics scenario. This task is carried out by highlighting the close connection between the well-known input-output formalism and CMs. Within this quantum optics framework, usual assumptions in the CMs’ literature - such as considering a bath of noninteracting yet initially correlated ancillas - have a clear physical origin.

Quantum opticsTechnologyQuantum PhysicsCollision models; quantum non-Markovian dynamics; input-output formalism.Formalism (philosophy)Computer scienceTFOS: Physical sciencesCollision modelCollision01 natural sciences010305 fluids & plasmasquantum non-Markovian dynamicTheoretical physicsquantum non-markovian dynamicsSystems theorycollision models0103 physical sciencesinput-output formalismConnection (algebraic framework)input-output formalism.010306 general physicsQuantum Physics (quant-ph)Quantum
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Quantum Lower Bound for Graph Collision Implies Lower Bound for Triangle Detection

2015

We show that an improvement to the best known quantum lower bound for GRAPH-COLLISION problem implies an improvement to the best known lower bound for TRIANGLE problem in the quantum query complexity model. In GRAPH-COLLISION we are given free access to a graph $(V,E)$ and access to a function $f:V\rightarrow \{0,1\}$ as a black box. We are asked to determine if there exist $(u,v) \in E$, such that $f(u)=f(v)=1$. In TRIANGLE we have a black box access to an adjacency matrix of a graph and we have to determine if the graph contains a triangle. For both of these problems the known lower bounds are trivial ($\Omega(\sqrt{n})$ and $\Omega(n)$, respectively) and there is no known matching upper …

Quantum queryQuantum PhysicsGeneral Computer ScienceFree accessTheoryofComputation_GENERALCollisionUpper and lower boundsOmegaGraphCombinatoricsComputer Science - Computational ComplexityAdjacency matrixQuantumMathematicsMathematicsofComputing_DISCRETEMATHEMATICS
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Diffractive dijet production and Wigner distributions from the color glass condensate

2019

Experimental processes that are sensitive to parton Wigner distributions provide a powerful tool to advance our understanding of proton structure. In this work, we compute gluon Wigner and Husimi distributions of protons within the Color Glass Condensate framework, which includes a spatially dependent McLerran-Venugopalan initial configuration and the explicit numerical solution of the JIMWLK equations. We determine the leading anisotropy of the Wigner and Husimi distributions as a function of the angle between impact parameter and transverse momentum. We study experimental signatures of these angular correlations at a proposed Electron Ion Collider by computing coherent diffractive dijet p…

QuarkCOLLISIONSprotonitNuclear TheoryHIGH-ENERGY FACTORIZATIONFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciences114 Physical sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsDEEP-INELASTIC SCATTERINGUNITARITYHigh Energy Physics - Phenomenology (hep-ph)Recoil0103 physical sciences010306 general physicsNuclear Experimentproton structureQuantum chromodynamicsPhysicsta114010308 nuclear & particles physicsQUARKNONLINEAR GLUON EVOLUTIONQCDGluonHigh Energy Physics - Phenomenologyparton Wigner distributionsEP SCATTERINGSATURATIONPHOTOPRODUCTIONcolor glass condensateImpact parameterNucleonPhysical Review D
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Exclusive heavy vector meson production at next-to-leading order in the dipole picture

2021

We calculate exclusive production of a longitudinally polarized heavy vector meson at next-to-leading order in the dipole picture. The large quark mass allows us to separately include both the first QCD correction proportional to the coupling constant $\alpha_s$, and the first relativistic correction suppressed by the quark velocity $v^2$. Both of these corrections are found to be numerically important in $\mathrm{J}/\psi$ production. The results obtained are directly suitable for phenomenological calculations. We also demonstrate how vector meson production provides complementary information to structure function analyses when one extracts the initial condition for the energy evolution of …

QuarkNuclear and High Energy PhysicsParticle physicsCOLLISIONSProtonJ/PSI MESONSQC1-999High Energy Physics::LatticeNuclear TheoryStructure (category theory)FOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInitial value problemVector meson010306 general physicsNUCLEUSPhysicsCoupling constantQuantum chromodynamicskvarkit010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyELECTROPRODUCTIONEVOLUTIONDipoleHigh Energy Physics - PhenomenologyPHOTOPRODUCTIONHigh Energy Physics::Experiment
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Measurement of trilinear gauge boson couplings WWV, (V Z,gamma) in e(+)e(-) collisions at 189 GeV

2001

Measurements of the trilinear gauge boson couplings WWgamma and WWZ are presented using the data taken by DELPHI in 1998 at a centre-of-mass energy of 189 GeV and combined with DELPHI data at 183 GeV. Values are determined for Delta(g_1^Z) and Delta(kappa_gamma), the differences of the WWZ charge coupling and of the WWgamma dipole coupling from their Standard Model values, and for lambda_gamma, the WWgamma quadrupole coupling. A measurement of the magnetic dipole and electric quadrupole moment of the W is extracted from the results for Delta(kappa_gamma) and lambda_gamma. The study uses data from the final states jjlv, jjjj, lX, jjX and gammaX, where j represents a quark jet, l an identifie…

QuarkNuclear and High Energy PhysicsParticle physicsENERGIESAstrophysics::High Energy Astrophysical Phenomenastandard modelLEP-IIFOS: Physical sciencesLambda7. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentStandard ModelEVENTSHigh Energy Physics - Experiment (hep-ex)BHABHA SCATTERINGMONTE-CARLO0103 physical sciencesOPTIMAL OBSERVABLES[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]W-MASSgauge couplings010306 general physicsDETECTORQCDELPHIPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCharge (physics)LARGE ELECTRON POSITRON COLLIDERFIS/01 - FISICA SPERIMENTALECol·lisions (Física nuclear)QuadrupolePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIOPTIMAL OBSERVABLES; BHABHA SCATTERING; MONTE-CARLO; W-MASS; LEP-II; EVENTS; DETECTOR; DELPHI; E+E-->W+W; ENERGIESelectron-positron collisionPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentE+E-->W+WMagnetic dipoleLepton
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D mesic nuclei

2010

The energies and widths of several D-0 meson bound states for different nuclei are obtained using a D-meson selfenergy in the nuclear medium, which is evaluated in a selfconsistent manner using techniques of unitarized coupled-channel theory. The kernel of the meson-baryon interaction is based on a model that treats heavy pseudoscalar and heavy vector mesons on equal footing, as required by heavy quark symmetry. We find D-0 bound states in all studied nuclei, from C-12 up to Pb-208. The inclusion of vector mesons is the keystone for obtaining an attractive D-nucleus interaction that leads to the existence of D-0-nucleus bound states, as compared to previous studies based on SU(4) flavor sym…

QuarkNuclear reactionNuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesHEAVY-ION COLLISIONS01 natural sciences7. Clean energyBOUND-STATESHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsENERGYHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)ANTIPROTON ANNIHILATION0103 physical sciencesBound stateHeavy quark effective theorySCATTERINGNuclear Experiment (nucl-ex)Basso continuoNuclear Experiment010306 general physicsNuclear ExperimentSUPPRESSIONPhysicsPIONIC ATOMS010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCHIRAL DYNAMICSHeavy quark symmetryETAPseudoscalarHigh Energy Physics - PhenomenologyMesic nucleiPhysics Letters B
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A search for new physics in dijet mass and angular distributions in pp collisions at [subscript √s=7] TeV measured with the ATLAS detector

2011

A search for new interactions and resonances produced in LHC proton–proton (pp) collisions at a centre-of-mass energy ps = 7 TeV was performed with the ATLAS detector. Using a dataset with an integrated luminosity of 36 pb−1, dijet mass and angular distributions were measured up to dijet masses of 3.5 TeV and were found to be in good agreement with Standard Model predictions. This analysis sets limits at 95% CL on various models for new physics: an excited quark is excluded for mass between 0.60 and 2.64 TeV, an axigluon hypothesis is excluded for axigluon masses between 0.60 and 2.10 TeV and quantum black holes are excluded in models with six extra space–time dimensions for quantum gravity…

QuarkParticle physicsChiral ColorCiências Naturais::Ciências FísicasPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]General Physics and AstronomyFOS: Physical sciencesddc:500.2dijet; mass; pp collisionts; ATLAS detector5307. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)Chiral color0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]String resonance010306 general physicsPhysicsQuantum chromodynamicsLarge Hadron ColliderScience & Technology010308 nuclear & particles physicsParton DistributionsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaHadron CollidersQCDmedicine.anatomical_structureExperimental High Energy Physicsddc:540ComputingMethodologies_DOCUMENTANDTEXTPROCESSINGQuarkFísica nuclearHigh Energy Physics::ExperimentParticle Physics - Experiment
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Tevatron constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quark pairs.

2015

et al.

QuarkParticle physicsHiggs bosonSTANDARD MODELTevatronFOS: Physical sciencesGeneral Physics and AstronomyATLAS DETECTORD0 EXPERIMENT01 natural sciences7. Clean energy530CDF collaborationHigh Energy Physics - ExperimentVector bosonNuclear physicsproton-antiproton collisionsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)SEARCH0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fysik010306 general physicsPhysics and Astronomy (all). B-JET IDENTIFICATIONCDF collaboration; Higgs boson; proton-antiproton collisionsDETECTORBosonPhysicsB-JET IDENTIFICATIONLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyATLASD0 experimentPARTON DISTRIBUTIONSExperimental High Energy PhysicsPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonATLAS; Higgs; Hadron-Hadron ScatteringHigh Energy Physics::ExperimentLHCB-JET IDENTIFICATION; STANDARD MODEL; PARTON DISTRIBUTIONS; ATLAS; DETECTOR; D0 EXPERIMENT; LHC; SEARCH
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