Search results for "RETRIEVAL"

showing 10 items of 1176 documents

Generalized Polarizabilities and the Chiral Structure of the Nucleon

1997

We are studying the electron scattering process e p to e' p' gamma in order to obtain information on the genuine virtual Compton scattering (VCS) process gamma^* N to gamma N. In addition to the two kinematical variables of real Compton scattering, e.g. the scattering angle theta and the energy omega' of the outgoing photon, the invariant amplitude for VCS depends on a third kinematical variable, which we choose as the absolute value of the three-momentum transfer to the nucleon. The structure-dependent coefficients in the VCS amplitude therefore acquire a momentum dependence and are termed ``generalized polarizabilities'' of the nucleon in analogy to real Compton scattering. Utilizing the …

Nuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryStructure (category theory)General Physics and AstronomyFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)PolarizabilityQuantum mechanics0103 physical sciencesPerturbation theoryNuclear Experiment010306 general physicsPhysicsChiral symmetry010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyCompton scatteringHigh Energy Physics - PhenomenologyNucleonElectron scattering
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Quantum algorithms for search with wildcards and combinatorial group testing

2012

We consider two combinatorial problems. The first we call "search with wildcards": given an unknown n-bit string x, and the ability to check whether any subset of the bits of x is equal to a provided query string, the goal is to output x. We give a nearly optimal O(sqrt(n) log n) quantum query algorithm for search with wildcards, beating the classical lower bound of Omega(n) queries. Rather than using amplitude amplification or a quantum walk, our algorithm is ultimately based on the solution to a state discrimination problem. The second problem we consider is combinatorial group testing, which is the task of identifying a subset of at most k special items out of a set of n items, given the…

Nuclear and High Energy PhysicsFOS: Physical sciencesGeneral Physics and Astronomy0102 computer and information sciences01 natural sciencesUpper and lower boundsTheoretical Computer ScienceCombinatoricsSet (abstract data type)Amplitude amplification0103 physical sciencesQuantum walk010306 general physicsMathematical PhysicsMathematicsQuantum PhysicsQuery stringComputer Science::Information RetrievalString (computer science)Statistical and Nonlinear PhysicsWildcard charactercomputer.file_formatComputational Theory and Mathematics010201 computation theory & mathematicsQuantum algorithmQuantum Physics (quant-ph)computerQuantum Information and Computation
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Vacuum correlators at short distances from lattice QCD

2021

Non-perturbatively computing the hadronic vacuum polarization at large photon virtualities and making contact with perturbation theory enables a precision determination of the electromagnetic coupling at the $Z$ pole, which enters global electroweak fits. In order to achieve this goal ab initio using lattice QCD, one faces the challenge that, at the short distances which dominate the observable, discretization errors are hard to control. Here we address challenges of this type with the help of static screening correlators in the high-temperature phase of QCD, yet without incurring any bias. The idea is motivated by the observations that (a) the cost of high-temperature simulations is typica…

Nuclear and High Energy PhysicsHigh Energy Physics::Latticepolecostshep-latFOS: Physical sciencesLattice QCDQC770-798nonperturbativeoperator product expansion53001 natural sciences7. Clean energythermal [correlation function]lattice [perturbation theory]High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityprecision measurement [electroweak interaction]quantum chromodynamics0103 physical sciencesPerturbative QCDhadronic [vacuum polarization]ddc:530010306 general physicsParticle Physics - Phenomenology010308 nuclear & particles physicsscreeningComputer Science::Information RetrievalphotonHigh Energy Physics - Lattice (hep-lat)lattice field theorytemperaturehep-phParticle Physics - LatticeHigh Energy Physics - Phenomenologyelectromagnetic [coupling]flavor [quark]Journal of High Energy Physics
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Effective field theory after a new-physics discovery

2018

When a new heavy particle is discovered at the LHC or at a future high-energy collider, it will be interesting to study its decays into Standard Model particles using an effective field-theory framework. We point out that the proper effective theory can not be constructed as an expansion in local, higher-dimensional operators; rather, it must be based on non-local operators defined in soft-collinear effective theory (SCET). For the interesting case where the new resonance is a gauge-singlet spin-0 boson, which is the first member of a new sector governed by a mass scale $M$, we show how a consistent scale separation between $M$ and the electroweak scale $v$ is achieved up to next-to-next-to…

Nuclear and High Energy PhysicsParticle physics530 PhysicsPhysics beyond the Standard ModelFOS: Physical sciences10192 Physics Institute01 natural sciencesResonance (particle physics)Standard ModelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsBosonPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologySoft-collinear effective theoryBeyond Standard Modellcsh:QC770-798ResummationElectroweak scaleJournal of High Energy Physics
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New method for calculating electromagnetic effects in semileptonic beta-decays of mesons

2020

We construct several classes of hadronic matrix elements and relate them to the low-energy constants in Chiral Perturbation Theory that describe the electromagnetic effects in the semileptonic beta decay of the pion and the kaon. We propose to calculate them using lattice QCD, and argue that such a calculation will make an immediate impact to a number of interesting topics at the precision frontier, including the outstanding anomalies in $|V_{us}|$ and the top-row Cabibbo-Kobayashi-Maskawa matrix unitarity.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectromagnetic [effect]MesonNuclear TheoryHigh Energy Physics::LatticeHadronFOS: Physical scienceschiral [perturbation theory]anomalyLattice QCD01 natural sciences530High Energy Physics - ExperimentNuclear Theory (nucl-th)Matrix (mathematics)High Energy Physics - Experiment (hep-ex)Kaon PhysicsPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBeta (velocity)lcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530Precision QEDNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologysemileptonic decay [meson]lattice field theorysemileptonic decay [pi]Lattice QCDHigh Energy Physics - PhenomenologyChiral Lagrangianslcsh:QC770-798High Energy Physics::Experimentunitarity [CKM matrix]
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Adding pseudo-observables to the four-lepton experimentalist’s toolbox

2018

The "golden" channel, in which the newly-discovered Higgs boson decays to four leptons by means of intermediate vector bosons, is important for determining the properties of the Higgs boson and for searching for subtle new physics effects. Different approaches exist for parametrizing the relevant Higgs couplings in this channel; here we relate the use of pseudo-observables to methods based on specifying the most general amplitude or Lagrangian terms for the $HVV$ interactions. We also provide projections for sensitivity in this channel in several novel scenarios, illustrating the use of pseudo-observables, and analyze the role of kinematic distributions and (ratios of) rates in such $H\to4\…

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsPhysics beyond the Standard ModelFOS: Physical sciencesKinematicsQC770-79801 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivitySensitivity (control systems)010306 general physicsHiggs Physics ; Beyond Standard ModelParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyObservablehep-ph3. Good healthHigh Energy Physics - PhenomenologyAmplitudeBeyond Standard ModelHiggs bosonlcsh:QC770-798LeptonCommunication channelJournal of High Energy Physics
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Neutral baryonic systems with strangeness

2020

We review the status as regards the existence of three- and four-body bound states made of neutrons and $\Lambda$ hyperons. For interesting cases, the coupling to neutral baryonic systems made of charged particles of different strangeness has been addressed. There are strong arguments showing that the $\Lambda nn$ system has no bound states. $\Lambda\Lambda nn$ strong stable states are not favored by our current knowledge of the strangeness $-1$ and $-2$ baryon-baryon interactions. However, a possible $\Xi^- t$ quasibound state decaying to $\Lambda\Lambda nn$ might exist in nature. Similarly, there is a broad agreement about the nonexistence of $\Lambda\Lambda n$ bound states. However, the …

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyStrangenessFew-body systems01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateComputer Science::General LiteratureNeutronNuclear Experiment010306 general physicsPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalAstrophysics::Instrumentation and Methods for AstrophysicsHyperonComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)Charge (physics)BaryonHigh Energy Physics - PhenomenologyCoupling (physics)International Journal of Modern Physics E
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Fragment Flow and the Multifragmentation Phase Space

1995

Fragment distributions have been measured for Au+Au collisions at [ital E]/[ital A]=100 and 1000 MeV. A high detection efficiency for fragments was obtained by combining the ALADIN spectrometer and the MSU-Miniball/WU-Miniwall array. At both energies the maximum multiplicity of intermediate mass fragments (IMF) normalized to the size of the decaying system is about one IMF per 30 nucleons but the element distributions show significant differences. Within a coalescence picture the suppression of heavy fragments in central collisions at [ital E]/[ital A]=100 MeV may be related to a reduction of the density in momentum space which is caused by the collective expansion.

Nuclear reactionCoalescence (physics)PhysicsSpectrometer[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Computer Science::Information RetrievalGeneral Physics and AstronomyPosition and momentum space[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Space (mathematics)Nuclear physicsPhase spaceMultiplicity (chemistry)Atomic physicsNuclear ExperimentNucleonPhysical Review Letters
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Pion interaction with the trinucleon up to the eta production threshold

1993

Pion elastic, charge exchange scattering and induced eta production on the trinucleon systems are investigated in a coupled-channels approach in momentum space with Fadeev wave functions. The channel $\pi N \rightarrow \eta N$ is included using an isobar model with S-, P-, and D-wave resonances. While the coherent reactions like $^3$He($\pi,\pi)^3$He can be reasonably well reproduced up to $T_{\pi}$=500 MeV, large discrepancies appear for the incoherent processes, $^3$He($\pi^-,\pi^0)^3$H and $^3$He($\pi^-,\eta)^3$H at backward angles and energies above $\Delta$-resonance. In the forward direction the $(\pi,\eta)$ calculations underestimate the experimental measurements very close to thresh…

Nuclear reactionPhysicsElastic scatteringNuclear and High Energy PhysicsFaddeev equationsMesonNuclear Theory010308 nuclear & particles physicsComputer Science::Information RetrievalHadronNuclear TheoryFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsNuclear Theory (nucl-th)PionQuantum mechanics0103 physical sciences010306 general physicsWave functionNuclear Experiment
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Measurement of the p(γ,π^{0}) cross section at threshold

1990

Differential and absolute cross sections for the reaction {ital p}({gamma},{pi}{sup 0}) have been measured with energy-defined photons in the threshold region ({ital E}{sub {gamma}}=131.4--157.2 MeV). The {ital E}{sub 0+} amplitude has been extracted out of the data. The values found are in disagreement with predictions of low-energy theorems.

Nuclear reactionPhysicsPhotonAmplitudePionMesonComputer Science::Information RetrievalHadronGeneral Physics and AstronomyElementary particleAtomic physicsBosonPhysical Review Letters
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