Search results for "Theoretical physics"

showing 10 items of 751 documents

Relaxion fluctuations (self-stopping relaxion) and overview of relaxion stopping mechanisms

2020

Journal of high energy physics 2005(5), 80 (2020). doi:10.1007/JHEP05(2020)080

effect: quantumNuclear and High Energy Physicscosmological modelCosmology and Nongalactic Astrophysics (astro-ph.CO)production [gauge boson]Field (physics)FOS: Physical sciencesParameter spaceHiggs particle01 natural sciences530Theoretical physicsHigh Energy Physics - Phenomenology (hep-ph)gauge boson: productionfluctuation: quantum0103 physical sciencesddc:530lcsh:Nuclear and particle physics. Atomic energy. Radioactivityinflation010306 general physicsQuantum fluctuationInflation (cosmology)PhysicsGauge boson010308 nuclear & particles physicsElectroweak interactionscale: electroweak interactionquantum [fluctuation]electroweak interaction [scale]Cosmology of Theories beyond the SMHigh Energy Physics - PhenomenologyHomogeneousquantum [effect]Beyond Standard Modelaxion-like particleslcsh:QC770-798Electroweak scaleAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian

2018

The electroweak sector of the Standard Model can be formulated in a way similar to Chiral Perturbation Theory (ChPT), but extended by a singlet scalar. The resulting effective field theory (EFT) is called Higgs-Electroweak Chiral Lagrangian (EWCh$\mathcal{L}$) and is the most general approach to new physics in the Higgs sector. It solely assumes the pattern of symmetry breaking leading to the three electroweak Goldstone bosons (i.e. massive $W$ and $Z$) and the existence of a Higgs-like scalar particle. The power counting of the EWCh$\mathcal{L}$ is given by a generalization of the momentum expansion of ChPT. It is connected to a loop expansion, making the theory renormalizable order by ord…

effective Lagrangian: chiralNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectroweak interaction: symmetry breakingHigh Energy Physics::LatticeScalar (mathematics)standard modelFOS: Physical sciencesTechnicolorsinglet: scalarHiggs particleexpansion: higher-order01 natural sciencesHiggs sectorStandard ModelrenormalizationRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)effective field theoryfluctuation: scalar0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)010306 general physicsPhysicselectroweak interaction010308 nuclear & particles physicsnew physicsElectroweak interactionHigh Energy Physics::Phenomenologyhigher-order: 1perturbation theory: chiralGoldstone particleHiggs fieldHigh Energy Physics - Phenomenologyscalar particlebackground field[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Goldstone bosonHiggs bosonHiggs modellcsh:QC770-798expansion: heat kernelfield theory: renormalizableexpansion: momentum
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Quantum memories with zero-energy Majorana modes and experimental constraints

2016

In this work we address the problem of realizing a reliable quantum memory based on zero-energy Majorana modes in the presence of experimental constraints on the operations aimed at recovering the information. In particular, we characterize the best recovery operation acting only on the zero-energy Majorana modes and the memory fidelity that can be therewith achieved. In order to understand the effect of such restriction, we discuss two examples of noise models acting on the topological system and compare the amount of information that can be recovered by accessing either the whole system, or the zero-modes only, with particular attention to the scaling with the size of the system and the e…

media_common.quotation_subjectZero-point energyMarkov processFidelityFOS: Physical sciences02 engineering and technologyTopology01 natural sciencessymbols.namesakeTheoretical physics0103 physical sciencesThermal010306 general physicsScalingQuantummedia_commonPhysicsQuantum PhysicsTOPOLOGICAL INSULATORS; ONE 2ND; FERMIONS; SUPERCONDUCTOR; COMPUTATION; SUPERFLUIDS; ANYONS021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterMAJORANAsymbols0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)
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Spherical Top Theory and Molecular Spectra

2011

In this article, we present an overview of the present state of the art of the theory of high-resolution spherical-top spectra in the framework of the effective Hamiltonian approach. We describe the specific features of this class of molecules to explain the basic concepts of the theoretical methods used for the analysis (line positions and intensities) and the simulation of absorption (including pure rotation) and Raman spectra of such species. The non conventional formalism that we use is essentially based on irreducible tensor methods and is especially adapted to computational treatments and global analyses of complex interacting band systems. We give examples concerning mainly methane (…

sulfur hexafluoride010504 meteorology & atmospheric sciences[PHYS.PHYS.PHYS-GEN-PH] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]group theory01 natural sciencesSpectral linerovibronic spectrasymbols.namesakeTheoretical physicsSpherical-topsvibrational polyads0103 physical sciencesMolecule[ PHYS.PHYS.PHYS-GEN-PH ] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Physics::Chemical PhysicsSpectroscopy0105 earth and related environmental sciences010304 chemical physicsChemistrymethaneRotational–vibrational spectroscopy[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Homogeneous spacesymbolsextension to lower symmetriescollisional broadeningprograms and databasesAtomic physicsHamiltonian (quantum mechanics)Raman spectroscopyrovibrational spectroscopytensorial formalismGroup theory
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Computing the Trace

2001

So far we have been interested in the general expression for the WKB-propagation function. Now we turn our attention to the trace of that propagator, since we want to exhibit the energy eigenvalues of a given potential. From earlier discussions we know that the energy levels of a given Hamiltonian are provided by the poles of the Green’s function:

symbols.namesakeTheoretical physicsComputer sciencesymbolsPropagatorStationary phase approximationGeneral expressionHamiltonian (quantum mechanics)Eigenvalues and eigenvectors
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ChemInform Abstract: Magnetic Exchange Between Metal Ions with Unquenched Orbital Angular Momenta: Basic Concepts and Relevance to Molecular Magnetism

2010

This review article is a first attempt to give a systematic and comprehensive description (in the framework of the unified theoretical approach) of the exchange interactions in polynuclear systems based on orbitally degenerate metal ions in the context of their relevance to the modern molecular magnetism. Interest in these systems is related to the fundamental problems of magnetism and at the same time steered by a number of impressive potential applications of molecular magnets, like high-density memory storage units, nanoscale qubits, spintronics and photoswitchable devices. In the presence of orbital degeneracy, the conventional spin Hamiltonian (Heisenberg–Dirac–van Vleck model) becomes…

symbols.namesakeTheoretical physicsSpintronicsMagnetismChemistryQubitExchange interactionDegenerate energy levelssymbolsContext (language use)General MedicineHamiltonian (quantum mechanics)Degeneracy (mathematics)ChemInform
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JIMWLK and beyond: From concepts to observables

2016

Volume: 112 Host publication title: 6th International Conference on Physics Opportunities at an Electron-Ion Collider The Color Glass Condensate and its associated evolution equation, the JIMWLK equation have applications to many observables far beyond totally inclusive observables. The phenomenology is so rich that little has been done to explore beyond scaling behavior of correlators. We show first examples that exemplify the considerations necessary to access additional information both experimentally and theoretically and demonstrate that the Wilson line correlators appearing throughout make it imperative to consistently take into account that one is dealing with correlators of group el…

ta114Operations research010308 nuclear & particles physicsComputer sciencePhysicsQC1-999scalingCOLOR GLASS CONDENSATEObservable114 Physical sciences01 natural sciencesSTATESMALL X EVOLUTIONColor-glass condensateWilson loopTheoretical physicsODDERONevolution equation0103 physical sciencesEvolution equationcolor glass condensate010306 general physicsScalingN-CEPJ Web of Conferences
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Quark structure of the χc(3P) and X(4274) resonances and their strong and radiative decays

2020

We calculate the masses of χc(3P) states with threshold corrections in a coupled-channel model. The model was recently applied to the description of the properties of χc(2P) and χb(3P) multiplets (Ferretti and Santopinto in Phys Lett B 789:550, 2019]. We also compute the open-charm strong decay widths of the χc(3P) states and their radiative transitions. According to our predictions, the χc(3P) states should be dominated by the charmonium core, but they may also show small meson-meson components. The X(4274) is interpreted as a cc¯ χc1(3P) state. More information on the other members of the χc(3P) multiplet, as well as a more rigorous analysis of the X(4274)’s decay modes, are needed to pro…

theoretical physicsHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimenthiukkasfysiikkaydinfysiikka
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Theoretical predictions of wimp-nucleus and neutrino-nucleus scattering in context of dark matter direct detection

2018

The nature of dark matter is at present an open question. Assuming the main component of dark matter consists of weakly interacting massive particles (WIMPs), directly detecting such particle via a scattering process with an atomic nucleus would be a strong probe into properties of dark matter. So far direct detection experiments have not provided a conclusive signal of dark matter. Traditionally the experiments aim to detect a coherent, spin- independent, elastic scattering signal which is enhanced by the square of the nuclear mass number. If the coherent channel is for some reason suppressed for WIMP-nucleus interactions, then spin-dependent interactions become important. In this thesis w…

theoretical physicsNuclear Theoryscatteringneutriinotksenonhiukkasfysiikkadark matterxenonpimeä aineneutrinotelluurinuclear physicstelluriumHigh Energy Physics::Experimentsirontaydinfysiikkakrypton
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Few-body insights of multiquark exotic hadrons

2018

In this contribution we discuss the adequate treatment of the $4-$ and $5-$body dynamics within a constituent quark framework. We stress that the variational and Born-Oppenheimer approximations give energies rather close to the exact ones, while the diquark approximation might be rather misleading. Hall-Post inequalities provide very useful lower bounds that exclude possible stable states for some mass ratios and color wave functions.

wave functionhadron: exoticBorn–Oppenheimer approximationConstituent quarkFOS: Physical sciences01 natural sciencesStability (probability)symbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)multiquarkquark: constituent0103 physical sciences010306 general physicsWave functionBorn-Oppenheimer approximationStable statePhysics010308 nuclear & particles physicsExotic hadronMass ratiostabilityDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]symbolsapproximation: diquarkmass ratio
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