Search results for "PROPAGATOR"

showing 10 items of 173 documents

Indirect determination of the Kugo-Ojima function from lattice data

2009

We study the structure and non-perturbative properties of a special Green's function, u(q), whose infrared behavior has traditionally served as the standard criterion for the realization of the Kugo-Ojima confinement mechanism. It turns out that, in the Landau gauge, u(q) can be determined from a dynamical equation, whose main ingredients are the gluon propagator and the ghost dressing function, integrated over all physical momenta. Using as input for these two (infrared finite) quantities recent lattice data, we obtain an indirect determination of u(q). The results of this mixed procedure are in excellent agreement with those found previously on the lattice, through a direct simulation of …

PhysicsNuclear and High Energy PhysicsParticle physicsInfraredHigh Energy Physics::LatticeFísicaNonperturbative effectsFOS: Physical sciencesPropagatorQCDGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)ConfinementMathematical physics
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Probing Higgs-portal dark matter with vector-boson fusion

2020

We constrain the Higgs-portal model employing the vector-boson fusion channel at the LHC. In particular, we include the phenomenologically interesting parameter region near the Higgs resonance, where the Higgs-boson mass is close to the threshold for dark-matter production and a running-width prescription has to be employed for the Higgs-boson propagator. Limits for the Higgs-portal coupling as a function of the dark-matter mass are derived from the CMS search for invisible Higgs-boson decays in vector-boson fusion at 13 TeV. Furthermore, we perform projections for the 14 TeV HL-LHC and the 27 TeV HE-LHC taking into account a realistic estimate of the systematic uncertainties. The respectiv…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHiggs PhysicsBranching fractionDark matterHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciences530Resonance (particle physics)Vector bosonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonlcsh:QC770-798ddc:530High Energy Physics::Experimentlcsh:Nuclear and particle physics. Atomic energy. RadioactivityBosonJournal of High Energy Physics
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A new technique for computing the spectral density of sunset-type diagrams: integral transformation in configuration space

1998

We present a new method to investigate a class of diagrams which generalizes the sunset topology to any number of massive internal lines. Our attention is focused on the computation of the spectral density of these diagrams which is related to many-body phase space in $D$ dimensional space-time. The spectral density is determined by the inverse $K$-transform of the product of propagators in configuration space. The inverse $K$-transform reduces to the inverse Laplace transform in any odd number of space-time dimensions for which we present an explicit analytical result.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryComputationMathematical analysisSpectral densityPropagatorInverseFOS: Physical sciencesInverse Laplace transformNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTransformation (function)High Energy Physics - Phenomenology (hep-ph)Phase spaceConfiguration space
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On the evaluation of sunset-type Feynman diagrams

1999

We introduce an efficient configuration space technique which allows one to compute a class of Feynman diagrams which generalize the scalar sunset topology to any number of massive internal lines. General tensor vertex structures and modifications of the propagators due to particle emission with vanishing momenta can be included with only a little change of the basic technique described for the scalar case. We discuss applications to the computation of $n$-body phase space in $D$-dimensional space-time. Substantial simplifications occur for odd space-time dimensions where the final results can be expressed in closed form through rational functions. We present explicit analytical formulas fo…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryComputationScalar (mathematics)FOS: Physical sciencesPropagatorRational functionSunsetNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Phase spacesymbolsFeynman diagramConfiguration spaceNuclear Physics B
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Beyond the dark matter effective field theory and a simplified model approach at colliders

2016

Direct detection of and LHC search for the singlet fermion dark matter (SFDM) model with Higgs portal interaction are considered in a renormalizable model where the full Standard Model (SM) gauge symmetry is imposed by introducing a singlet scalar messenger. In this model, direct detection is described by an effective operator m_q \bar{q} q \bar{\chi} \chi as usual, but the full amplitude for monojet + \not E_T involves two intermediate scalar propagators, which cannot be seen within the effective field theory (EFT) or in the simplified model without the full SM gauge symmetry. We derive the collider bounds from the ATLAS monojet + \not E_T as well as the CMS t\bar{t} + \not E_T data, findi…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciences01 natural scienceslcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryHiggs bosonHigh Energy Physics::ExperimentGauge theory010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters B
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Fundamental Principles of Quantum Mechanics

2001

There are two alternative methods of quantizing a system: a) quantization via the Feynman Path Integral (equivalent to Schwinger’s Action Principle); b) canonical quantization.

PhysicsOpen quantum systemmedicine.medical_specialtyCanonical quantizationQuantization (signal processing)Quantum dynamicsStochastic interpretationPath integral formulationQuantum nanosciencemedicinePropagatorMathematical physics
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Comparison of two non-primitive methods for path integral simulations: Higher-order corrections vs. an effective propagator approach

2002

Two methods are compared that are used in path integral simulations. Both methods aim to achieve faster convergence to the quantum limit than the so-called primitive algorithm (PA). One method, originally proposed by Takahashi and Imada, is based on a higher-order approximation (HOA) of the quantum mechanical density operator. The other method is based upon an effective propagator (EPr). This propagator is constructed such that it produces correctly one and two-particle imaginary time correlation functions in the limit of small densities even for finite Trotter numbers P. We discuss the conceptual differences between both methods and compare the convergence rate of both approaches. While th…

PhysicsOperator (physics)Mathematical analysisCondensed Matter (cond-mat)Order (ring theory)PropagatorEstimatorFOS: Physical sciencesCondensed MatterRate of convergenceQuantum mechanicsPath integral formulationVirial expansionLimit (mathematics)
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Higgs decay into two photons in a warped extra dimension

2014

A detailed five-dimensional calculation of the Higgs-boson decay into two photons is performed in both the minimal and the custodially protected Randall–Sundrum (RS) model, where the Standard Model (SM) fields propagate in the bulk and the scalar sector lives on or near the IR brane. It is explicitly shown that the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$R_\xi $$\end{document}Rξ gauge invariance of the sum of diagrams involving bosonic fields in the SM also applies to the case of these RS scenarios. An e…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Scalar (mathematics)High Energy Physics::PhenomenologyPropagatorFermionStandard ModelAmplitudeHiggs bosonGauge theoryRegular Article - Theoretical PhysicsBraneEngineering (miscellaneous)The European Physical Journal C
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Mass dimension one fermions and their gravitational interaction

2019

We investigate in detail the interaction between the spin-${1/2}$ fields endowed with mass dimension one and the graviton. We obtain an interaction vertex that combines the characteristics of scalar-graviton and Dirac's fermion-graviton vertices, due to the scalar-dynamic attribute and the fermionic structure of this field. It is shown that the vertex obtained obeys the Ward-Takahashi identity, ensuring the gauge invariance for this interaction. In the contribution of the mass dimension one fermion to the graviton propagator at one-loop, we found the conditions for the cancellation of the tadpole term by a cosmological counter-term. We calculate the scattering process for arbitrary momentum…

PhysicsPhysics::General PhysicsNewtonian potentialField (physics)High Energy Physics::LatticeScalar (mathematics)GravitonGeneral Physics and AstronomyPropagatorFOS: Physical sciencesTadpole (physics)01 natural sciences010305 fluids & plasmasGravitational potentialTheoretical physicsHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGauge theory010306 general physics
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Non-locality and causal evolution in QFT

2006

Non locality appearing in QFT during the free evolution of localized field states and in the Feynman propagator function is analyzed. It is shown to be connected to the initial non local properties present at the level of quantum states and then it does not imply a violation of Einstein's causality. Then it is investigated a simple QFT system with interaction, consisting of a classical source coupled linearly to a quantum scalar field, that is exactly solved. The expression for the time evolution of the state describing the system is given. The expectation value of any arbitrary ``good'' local observable, expressed as a function of the field operator and its space and time derivatives, is o…

PhysicsQuantum PhysicsOperator (physics)photon| operatorsFOS: Physical sciencesPropagatorObservableExpectation valueCondensed Matter PhysicsAtomic and Molecular Physics and OpticsCausality (physics)Quantum nonlocalityQuantum statequantum electrodynamicsQuantum Physics (quant-ph)Scalar fieldMathematical physicsJournal of Physics B: Atomic, Molecular and Optical Physics
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