Search results for "Mathematical physics"

showing 10 items of 2687 documents

Metric-affine f(R,T) theories of gravity and their applications

2018

We study $f(R,T)$ theories of gravity, where $T$ is the trace of the energy-momentum tensor ${T}_{\ensuremath{\mu}\ensuremath{\nu}}$, with independent metric and affine connection (metric-affine theories). We find that the resulting field equations share a close resemblance with their metric-affine $f(R)$ relatives once an effective energy-momentum tensor is introduced. As a result, the metric field equations are second-order and no new propagating degrees of freedom arise as compared to GR, which contrasts with the metric formulation of these theories, where a dynamical scalar degree of freedom is present. Analogously to its metric counterpart, the field equations impose the nonconservatio…

Physics010308 nuclear & particles physics0103 physical sciencesScalar (mathematics)Degrees of freedom (statistics)Weak fieldAffine transformationAffine connectionPoisson's equation010306 general physicsField equation01 natural sciencesMathematical physicsPhysical Review D
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Theoretical analysis of the γγ→π0η process

2017

We present a theoretical study of the $\ensuremath{\gamma}\ensuremath{\gamma}\ensuremath{\rightarrow}\ensuremath{\pi}\ensuremath{\eta}$ process from the threshold up to 1.4 GeV in the $\ensuremath{\pi}\ensuremath{\eta}$ invariant mass. For the s-wave ${a}_{0}(980)$ resonance state we adopt a dispersive formalism using a coupled-channel Omn\`es representation, while the d-wave ${a}_{2}(1320)$ state is described as a Breit-Wigner resonance. An analytic continuation to the ${a}_{0}(980)$ pole position allows us to extract its two-photon decay width as ${\mathrm{\ensuremath{\Gamma}}}_{{a}_{0}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}}=0.27(4)\text{ }\text{ }\mathrm{keV}$.

Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaAnalytic continuation0103 physical sciencesResonanceHigh Energy Physics::ExperimentInvariant massState (functional analysis)010306 general physics01 natural sciencesMathematical physicsPhysical Review D
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Investigation of Gamma Rays from the36S(p,γ)37Cl Reaction

1973

The excitation curve of the 36S(p,γ)37Cl reaction has been measured in the proton energy range 1 000-1 900 keV. 109 resonances were observed. The decay schemes for 13 resonances and energies and branching ratios of 15 bound states have been obtained by means of Ge(Li) detectors. Seven of the bound states have not been reported earlier. Lifetimes or lifetime limits of 5 bound states have been measured by means of Doppler-shift attenuation method.

Physics010308 nuclear & particles physicsAttenuationGamma rayCondensed Matter PhysicsBranching (polymer chemistry)Proton energy01 natural sciencesAtomic and Molecular Physics and Optics0103 physical sciencesBound stateAtomic physics010306 general physicsMathematical PhysicsExcitationPhysica Scripta
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Evidence for Two-Nucleon Polarization in the π(h9/2i13/2)11- ν(j-2)0+ Level in 208Po

1974

From in-beam gamma-ray spectroscopy measurements on the 208Pb(α, 4n)208Po reaction using the Stockholm 225-cm cyclotron, we have concluded that there is an 11-, 8 ns isomeric state in 208Po, which lies 1 175 keV above the π(h 9/2 2)8+ state and that this isomeric state should have the configuration π(h 9/2 i 13/2)11- ν(j -2)0+. Calculations based on the use of empirical two-particle interactions give a position of the 11- level which deviates by about + 100 keV from the experimentally found position. It is suggested that this deviation is mainly due to the difference in the polarization of the 206Pb-and 208Pb-cores by the two aligned h 9/2 and i 13/2 protons.

Physics010308 nuclear & particles physicsCyclotronCondensed Matter PhysicsPolarization (waves)01 natural sciencesAtomic and Molecular Physics and Opticslaw.inventionlaw0103 physical sciencesAtomic physics010306 general physicsNucleonSpectroscopyMathematical PhysicsPhysica Scripta
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Scattering Amplitudes from Superconformal Ward Identities

2018

We consider finite superamplitudes of N=1 matter, and use superconformal symmetry to derive powerful first-order differential equations for them. Because of on-shell collinear singularities, the Ward identities have an anomaly, which is obtained from lower-loop information. We show that in the five-particle case, the solution to the equations is uniquely fixed by the expected analytic behavior. We apply the method to a nonplanar two-loop five-particle integral. We consider finite superamplitudes of N=1 matter, and use superconformal symmetry to derive powerful first-order differential equations for them. Due to on-shell collinear singularities, the Ward identities have an anomaly, which is …

Physics010308 nuclear & particles physicsDifferential equation[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]hep-thGeneral Physics and Astronomyanomalydifferential equationshep-phsingularity: collinear16. Peace & justice01 natural sciencesSymmetry (physics)Scattering amplitudesymmetry: conformal[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesGravitational singularityAnomaly (physics)010306 general physicsWard identity: conformalParticle Physics - TheoryMathematical physicsParticle Physics - Phenomenology
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Numerical evolutions of spherical Proca stars

2017

Vector boson stars, or $\textit{Proca stars}$, have been recently obtained as fully non-linear numerical solutions of the Einstein-(complex)-Proca system. These are self-gravitating, everywhere non-singular, horizonless Bose-Einstein condensates of a massive vector field, which resemble in many ways, but not all, their scalar cousins, the well-known (scalar) $\textit{boson stars}$. In this paper we report fully-non linear numerical evolutions of Proca stars, focusing on the spherically symmetric case, with the goal of assessing their stability and the end-point of the evolution of the unstable stars. Previous results from linear perturbation theory indicate the separation between stable and…

Physics010308 nuclear & particles physicsFOS: Physical sciencesPerturbation (astronomy)General Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyVector bosonGeneral Relativity and Quantum CosmologyNeutron starStarsClassical mechanics0103 physical sciencesSchwarzschild metricVector field010306 general physicsScalar fieldMathematical physicsBosonPhysical Review D
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$$\mathscr {D}{-}$$ D - Deformed and SUSY-Deformed Graphene: First Results

2016

We discuss some mathematical aspects of two particular deformed versions of the Dirac Hamiltonian for graphene close to the Dirac points, one involving \(\mathscr {D}\)-pseudo bosons and the other supersymmetric quantum mechanics. In particular, in connection with \(\mathscr {D}\)-pseudo bosons, we show how biorthogonal sets arise, and we discuss when these sets are bases for the Hilbert space where the model is defined, and when they are not. For the SUSY extension of the model we show how this can be achieved and which results can be obtained.

Physics010308 nuclear & particles physicsGrapheneHigh Energy Physics::PhenomenologyHilbert spaceDirac pointSupersymmetry01 natural scienceslaw.inventionsymbols.namesakelawBiorthogonal system0103 physical sciencessymbolsSupersymmetric quantum mechanics010306 general physicsHamiltonian (quantum mechanics)Mathematical physicsBoson
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Anomalous enhancement of the isospin-violating Λ(1405) production by a triangle singularity in Λc→π+π0π0Σ0

2018

The decay of ${\mathrm{\ensuremath{\Lambda}}}_{c}^{+}$ into ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{0}\mathrm{\ensuremath{\Lambda}}(1405)$ with the $\mathrm{\ensuremath{\Lambda}}(1405)$ decay into ${\ensuremath{\pi}}^{0}{\mathrm{\ensuremath{\Sigma}}}^{0}$ through a triangle diagram is studied. This process is initiated by ${\mathrm{\ensuremath{\Lambda}}}_{c}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\overline{K}}^{*}N$, and then the ${\overline{K}}^{*}$ decays into $\overline{K}\ensuremath{\pi}$ and $\overline{K}N$ produce the $\mathrm{\ensuremath{\Lambda}}(1405)$ through a triangle loop containing ${\overline{K}}^{*}N\overline{K}$ which develops a singularity around 1890 MeV. Th…

Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronLambda01 natural sciencesLoop (topology)SingularityIsospin0103 physical sciencesMass spectrumProduction (computer science)Invariant mass010306 general physicsMathematical physicsPhysical Review D
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Dynamical symmetry breaking and fermion mass hierarchy in the scale-invariant 3-3-1 model

2020

We propose an extension of the Standard Model (SM) based on the $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ (3-3-1) gauge symmetry and scale invariance. Maintaining the main features of the so-called 3-3-1 models, such as the cancellation of gauge anomalies related to the number of chiral fermion generations, this model exhibits a very compact scalar sector. Only two scalar triplets and one singlet are necessary and sufficient to break the symmetries dynamically via the Coleman-Weinberg mechanism. With the introduction of an Abelian discrete symmetry and assuming a natural hierarchy among the vacuum expectation values of the neutral scalar fields, we show that all particles in the model can get …

Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesFermionComputer Science::Digital Libraries01 natural sciencesSymmetry (physics)Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanism0103 physical sciences010306 general physicsMathematical physicsBosonGauge symmetryDiscrete symmetryPhysical Review D
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Discussion on triangle singularities in the Λb→J/ψK−p reaction

2016

We have analyzed the singularities of a triangle loop integral in detail and derived a formula for an easy evaluation of the triangle singularity on the physical boundary. It is applied to the ${\mathrm{\ensuremath{\Lambda}}}_{b}\ensuremath{\rightarrow}J/\ensuremath{\psi}{K}^{\ensuremath{-}}p$ process via ${\mathrm{\ensuremath{\Lambda}}}^{*}$-charmonium-proton intermediate states. Although the evaluation of absolute rates is not possible, we identify the ${\ensuremath{\chi}}_{c1}$ and the $\ensuremath{\psi}(2S)$ as the relatively most relevant states among all possible charmonia up to the $\ensuremath{\psi}(2S)$. The $\mathrm{\ensuremath{\Lambda}}(1890){\ensuremath{\chi}}_{c1}p$ loop is ver…

Physics010308 nuclear & particles physicsLattice field theoryHyperonLattice QCDQuantum numberLambda01 natural sciencesLoop integralLoop (topology)Quantum mechanics0103 physical sciencesIntermediate state010306 general physicsMathematical physicsPhysical Review D
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