Search results for " atom"

showing 10 items of 1526 documents

A$_{FB}$ in the SMEFT: precision Z physics at the LHC

2021

We study the forward-backward asymmetry $A_{FB}$ in $pp \to \ell^+\ell^-$ at the Z peak within the Standard Model Effective Field Theory (SMEFT). We find that this observable provides per mille level constraints on the vertex corrections of the Z boson to quarks,which close a flat direction in the electroweak precision SMEFT fit. Moreover, we show that current $A_{FB}$ data is precise enough so that its inclusion in the fit improves significantly LEP bounds even in simple New Physics setups. This demonstrates that the LHC can compete with and complement LEP when it comes to precision measurements of the Z boson properties

QuarkNuclear and High Energy PhysicsParticle physicsp p: scatteringangular distribution: asymmetryPhysics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciencesQC770-79801 natural sciencesAsymmetryStandard ModelquarkZ0: productionHigh Energy Physics - Phenomenology (hep-ph)effective field theoryflat directionNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesEffective field theory010306 general physicsmedia_commonPhysicsLarge Hadron Colliderelectroweak interaction010308 nuclear & particles physicsprecision measurementnew physicsElectroweak interactionHigh Energy Physics::PhenomenologyObservableCERN LEP StorEffective Field Theoriescorrection: vertexHigh Energy Physics - Phenomenologyp p --> lepton+ lepton-CERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelHigh Energy Physics::Experiment
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Light- and strange-quark mass dependence of the ρ(770) meson revisited

2020

Recent lattice data on $\pi\pi$-scattering phase shifts in the vector-isovector channel, pseudoscalar meson masses and decay constants for strange-quark masses smaller or equal to the physical value allow us to study the strangeness dependence of these observables for the first time. We perform a global analysis on two kind of lattice trajectories depending on whether the sum of quark masses or the strange-quark mass is kept fixed to the physical point. The quark mass dependence of these observables is extracted from unitarized coupled-channel one-loop Chiral Perturbation Theory. This analysis guides new predictions on the $\rho(770)$ meson properties over trajectories where the strange-qua…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsChiral perturbation theoryMeson530 PhysicsHigh Energy Physics::LatticeNuclear TheoryLattice QCDStrangeness01 natural sciencesPseudoscalar mesonHigh Energy Physics - Lattice0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsPhysicsTeoría de los quanta010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyObservableLattice QCDHigh Energy Physics - PhenomenologyChiral LagrangiansPartículaslcsh:QC770-798High Energy Physics::ExperimentJournal of High Energy Physics
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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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Time reversal invariance violation in neutron-nucleus scattering

2019

Planning and interpretation of the experiments searching for the time reversal (T) and parity (P) violation in neutron reactions require values of the matrix elements of the T,P-violating nuclear forces between nuclear compound states. We calculate the root mean square values and the ratio of the matrix elements of the T,P-violating and P-violating interactions using statistical theory based on the properties of chaotic compound states and present the results in terms of the fundamental parameters in four different forms: in terms of the constants of the contact nuclear interaction, meson exchange constants, QCD theta-term and quark chromo-EDMs. Using current limits on these parameters, we …

QuarkParticle physicsNuclear TheoryMesonAtomic Physics (physics.atom-ph)Nuclear TheoryFOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear forceNeutronNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyParity (physics)High Energy Physics - PhenomenologyDipoleHigh Energy Physics::Experiment
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Spectrum of fully-heavy tetraquarks from a diquark+antidiquark perspective

2019

Using a relativized diquark model Hamiltonian, we calculate the masses of $J^{PC}=0^{++}$ ground-state tetraquarks in the following systems: $b s \bar b \bar s$, $bb \bar n \bar n$ ($n=u, d$), $bb \bar s \bar s$, $cc\bar c \bar c$, $b b \bar b \bar b$, $b c\bar b \bar c$ and $b b \bar c \bar c$. We also compute extensive spectra for the fully-heavy quark flavour combinations. Finally, as a test of the diquark model approach, we compute the masses of fully-heavy baryons in the diquark model. Our results may be compared soon to the forthcoming experimental data for fully-heavy three-quark systems.

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceslcsh:AstrophysicshiukkasfysiikkaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)lcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Engineering (miscellaneous)Nuclear theoryNuclear ExperimentPhysicstheoretical physicskvarkitHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)DiquarkBaryonHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentHamiltonian (quantum mechanics)European Physical Journal
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Vacuum Induced CP Violation Generating a Complex CKM Matrix with Controlled Scalar FCNC

2018

We propose a viable minimal model with spontaneous CP violation in the framework of a two Higgs doublet model. The model is based on a generalised Branco–Grimus–Lavoura model with a flavoured Z2 symmetry, under which two of the quark families are even and the third one is odd. The lagrangian respects CP invariance, but the vacuum has a CP violating phase, which is able to generate a complex CKM matrix, with the rephasing invariant strength of CP violation compatible with experiment. The question of scalar mediated flavour changing neutral couplings is carefully studied. In particular we point out a deep connection between the generation of a complex CKM matrix from a vacuum phase and the ap…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelScalar (mathematics)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesComputer Science::Digital LibrariesHigh Energy Physics - ExperimentMinimal modelTwo-Higgs-doublet modelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHiggs bosonCP violationlcsh:QC770-798High Energy Physics::Experiment
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First global next-to-leading order determination of diffractive parton distribution functions and their uncertainties within the {\tt xFitter} framew…

2018

We present {\tt GKG18-DPDFs}, a next-to-leading order (NLO) QCD analysis of diffractive parton distribution functions (diffractive PDFs) and their uncertainties. This is the first global set of diffractive PDFs determined within the {\tt xFitter} framework. This analysis is motivated by all available and most up-to-date data on inclusive diffractive deep inelastic scattering (diffractive DIS). Heavy quark contributions are considered within the framework of the Thorne-Roberts (TR) general mass variable flavor number scheme (GM-VFNS). We form a mutually consistent set of diffractive PDFs due to the inclusion of high-precision data from H1/ZEUS combined inclusive diffractive cross sections me…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)parton distribution functionsHERAPREDICTIONSFOS: Physical scienceslcsh:AstrophysicsPartonhiukkasfysiikkaPROTON114 Physical sciences01 natural sciencesZeus (malware)CROSS-SECTIONSHigh Energy Physics - ExperimentDEEP-INELASTIC SCATTERINGHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)deep inelastic scatteringlcsh:QB460-4660103 physical sciencesquantum chromodynamicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQCD ANALYSIS010306 general physicsEngineering (miscellaneous)PhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicsHERADeep inelastic scatteringHigh Energy Physics - PhenomenologyDistribution functionTESTSPHOTOPRODUCTIONlcsh:QC770-798LHC
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Hall–Post inequalities: Review and application to molecules and tetraquarks

2019

A review is presented of the Hall–Post inequalities that give lower-bounds to the ground-state energy of quantum systems in terms of energies of smaller systems. New applications are given for systems experiencing both a static source and inner interactions, as well as for hydrogen-like molecules and for tetraquarks in some quark models. In the latter case, the Hall–Post inequalities constrain the possibility of deeply-bound exotic mesons below the threshold for dissociation into two quark–antiquark mesons. We also emphasize the usefulness of the Hall–Post bounds in terms of 3-body energies when some 2-body subsystems are ill defined or do not support any bound state.

QuarkParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryMesonenergy: ground stateHigh Energy Physics::LatticeFOS: Physical sciencesGeneral Physics and Astronomyquark antiquarkHall-Post inequalitiesdissociation01 natural sciencesDissociation (chemistry)Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Tetraquark0103 physical sciencesBound stateMoleculemoleculesPhysics - Atomic and Molecular Clusters010306 general physicsQuantumPhysicsquark modeltetraquarksHall–Post inequality010308 nuclear & particles physicsHigh Energy Physics::Phenomenologymeson: exoticMolecule[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]bound stateHigh Energy Physics - PhenomenologyQuantum Gases (cond-mat.quant-gas)few-body systems[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Atomic and Molecular Clusters (physics.atm-clus)Condensed Matter - Quantum GasesFew BodybaryonsAnnals of Physics
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Nucleon matrix elements from lattice QCD with all-mode-averaging and a domain-decomposed solver: An exploratory study

2017

We study the performance of all-mode-averaging (AMA) when used in conjunction with a locally deflated SAP-preconditioned solver, determining how to optimize the local block sizes and number of deflation fields in order to minimize the computational cost for a given level of overall statistical accuracy. We find that AMA enables a reduction of the statistical error on nucleon charges by a factor of around two at the same cost when compared to the standard method. As a demonstration, we compute the axial, scalar and tensor charges of the nucleon in $N_f=2$ lattice QCD with non-perturbatively O(a)-improved Wilson quarks, using O(10,000) measurements to pursue the signal out to source-sink sepa…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Scalar (physics)FOS: Physical sciencesCharge (physics)Lattice QCDComputational Physics (physics.comp-ph)Solver01 natural sciencesMatrix (mathematics)High Energy Physics - Lattice13. Climate actionQuantum electrodynamics0103 physical scienceslcsh:QC770-798ddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityTensor010306 general physicsNucleonPhysics - Computational PhysicsNuclear Physics B
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Dijets at Tevatron Cannot Constrain SMEFT Four-Quark Operators

2019

We explore the sensitivity of Tevatron data to heavy new physics effects in differential dijet production rates using the SMEFT in light of the fact that consistent and conservative constraints from the LHC cannot cover relatively low cutoff scales in the EFT. In contrast to the results quoted by the experimental collaborations and other groups, we find that, once consistency of the perturbation expansion is enforced and reasonable estimates of theoretical errors induced by the SMEFT series in $\frac{E}{\Lambda}$ are included, there is no potential to constrain four-quark contact interactions using Tevatron data. This shows the general difficulty of constraining physics model-independently …

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderLuminosity (scattering theory)Physics beyond the Standard ModelHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesEffective Field TheoriesLambdaComputer Science::Digital LibrariesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelComputer Science::Mathematical SoftwareCutofflcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentSensitivity (control systems)
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