Search results for "Matrix"

showing 10 items of 3205 documents

Probing CP violation with non-unitary mixing in long-baseline neutrino oscillation experiments: DUNE as a case study

2016

When neutrino masses arise from the exchange of neutral heavy leptons, as in most seesaw schemes, the effective lepton mixing matrix $N$ describing neutrino propagation is non-unitary, hence neutrinos are not exactly orthonormal. New CP violation phases appear in $N$ that could be confused with the standard phase $\delta_{\text{CP}}$ characterizing the three neutrino paradigm. We study the potential of the long-baseline neutrino experiment DUNE in probing CP violation induced by the standard CP phase in the presence of non-unitarity. In order to accomplish this we develop our previous formalism, so as to take into account the neutrino interactions with the medium, important in long baseline…

PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryViolació CP (Física nuclear)0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationLepton
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On the corner elements of the CKM and PMNS matrices

2013

Recent experiments show that the top-right corner element (U-e3) of the PMNS matrix is small but nonzero, and suggest further via unitarity that it is smaller than the bottom-left corner element (U-tau 1). Here, it is shown that if to the assumption of a universal rank-one mass matrix, long favoured by phenomenologists, one adds that this matrix rotates with scale, then it follows that A) by inputting the mass ratios m(c)/m(t), m(s)/m(b), m(mu)/m(tau), and m(2)/m(3), i) the corner elements are small but nonzero, ii) V-ub < V-td, U-e3 < U-tau 1, iii) estimates result for the ratios V-ub/V-td and U-e3/U-tau 1, and B) by inputting further the experimental values of V-us, V-tb and U-e2, U-mu 3,…

PhysicsParticle physicsUnitarityCabibbo–Kobayashi–Maskawa matrixGeneral Physics and AstronomyMass matrixPartícules (Física nuclear)CombinatoricsStrong CP ProblemMatrix (mathematics)Rotating Mass MatrixStrong CP problemFísica nuclearHiggs Decay
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Statistical properties of the eigenvalue spectrum of the three-dimensional Anderson Hamiltonian

1993

A method to describe the metal-insulator transition (MIT) in disordered systems is presented. For this purpose the statistical properties of the eigenvalue spectrum of the Anderson Hamiltonian are considered. As the MIT corresponds to the transition between chaotic and nonchaotic behavior, it can be expected that the random matrix theory enables a qualitative description of the phase transition. We show that it is possible to determine the critical disorder in this way. In the thermodynamic limit the critical point behavior separates two different regimes: one for the metallic side and one for the insulating side.

PhysicsPhase transitionCritical phenomenaCondensed Matter::Disordered Systems and Neural Networkssymbols.namesakeCritical point (thermodynamics)Thermodynamic limitsymbolsCondensed Matter::Strongly Correlated ElectronsStatistical physicsHamiltonian (quantum mechanics)Random matrixAnderson impurity modelEigenvalues and eigenvectorsPhysical Review B
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Renormalization group flows for Wilson-Hubbard matter and the topological Hamiltonian

2019

Understanding the robustness of topological phases of matter in the presence of interactions poses a difficult challenge in modern condensed matter, showing interesting connections to high energy physics. In this work, we leverage these connections to present a complete analysis of the continuum long-wavelength description of a generic class of correlated topological insulators: Wilson-Hubbard topological matter. We show that a Wilsonian renormalization group (RG) approach, combined with the so-called topological Hamiltonian, provide a quantitative route to understand interaction-induced topological phase transitions that occur in Wilson-Hubbard matter. We benchmark two-loop RG predictions …

PhysicsPhase transitionQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciences02 engineering and technologyRenormalization group021001 nanoscience & nanotechnologyTopology01 natural sciencesMatrix multiplicationsymbols.namesakeCondensed Matter - Strongly Correlated ElectronsQuantum Gases (cond-mat.quant-gas)Topological insulator0103 physical sciencessymbolsddc:530Quantum Physics (quant-ph)010306 general physics0210 nano-technologyHamiltonian (quantum mechanics)Condensed Matter - Quantum Gases
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Quantum chemical study of electron‐phonon interaction in crystals

2013

Study of the interaction of the electromagnetic radiation with nonlocal potentials and the electron-phonon interaction is motivated by its key role in non-classical phenomena in dielectrics and semiconductors. Actual in second quantization is decoupling of the undesirable mixture of electronic and phonon birth/annihilation operators and obtaining the effect of radiation in presence of the nonlocal potentials. Here we transform an arbitrary effective electron- phonon Hamiltonian in two matrices – the matrix of a new interaction Hamiltonian and the matrix of the transformation. For a particular effective Hamiltonian formulated in second quantization these two matrices outline a starting point…

PhysicsPhononElectronCondensed Matter PhysicsElectromagnetic radiationSecond quantizationMatrix (mathematics)symbols.namesakeAtomic orbitalQuantum electrodynamicsQuantum mechanicssymbolsHamiltonian (quantum mechanics)Wave functionphysica status solidi c
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MuPix10: First Results from the Final Design

2021

Many years of research and development of High Voltage Monolithic Active Pixel Sensors (HVMAPS) have culminated in the final design for the Mu3e pixel sensor. MuPix10 is a fully monolithic sensor with an active pixel matrix size of $20\times20\,\mathrm{mm}^2$ produced in the $180\,\mathrm{nm}$ HV-CMOS process at TSI Semiconductors. The pixel size is $80\times80\,\mathrm{\mu m}^2$. Hits are read out using a column-drain architecture and sent over up to four serial links with up to $1.6\,\left.\mathrm{Gbit}\middle/\mathrm{s}\right.$ each. By means of DC/DC converters and exclusive usage of on-chip biasing, MuPix10 is fully operable with a minimal set of electrical connections. This is an inte…

PhysicsPhysics - Instrumentation and DetectorsPixelFOS: Physical sciencesBiasingPixel matrixHigh voltageInstrumentation and Detectors (physics.ins-det)ConvertersTopologyRadiation lengthProceedings of the 29th International Workshop on Vertex Detectors (VERTEX2020)
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Bloch analysis of finite periodic microring chains

2005

We apply Bloch analysis to the study of finite periodic cascading of microring resonators. Diagonalization of the standard transfer matrix approach not only allows to find an exact analytic expression for transmission and reflection, but also to derive a closed form solution for the field in every point of the structure. To give more physical insight we analyze the main features of the transmission resonances in a finite chain and we give some hints for their experimental verification

PhysicsPhysics and Astronomy (miscellaneous)Field (physics)Mathematical analysisGeneral EngineeringFOS: Physical sciencesGeneral Physics and AstronomyTransfer matrixResonatorReflection (mathematics)Chain (algebraic topology)Transmission (telecommunications)Point (geometry)Closed-form expressionOptics (physics.optics)Physics - OpticsApplied Physics B
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Improved search for heavy neutrinos in the decay π→eν

2018

A search for massive neutrinos has been made in the decay π+→e+ν. No evidence was found for extra peaks in the positron energy spectrum indicative of pion decays involving massive neutrinos (π→e+νh). Upper limits (90% C.L.) on the neutrino mixing matrix element |Uei|2 in the neutrino mass region 60–135 MeV/c2 were set and are an order of magnitude improvement over previous results.

PhysicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologySpectrum (functional analysis)Pontecorvo–Maki–Nakagawa–Sakata matrix01 natural sciencesSpectral linePositron energyNuclear physicsPion0103 physical sciencesHigh Energy Physics::ExperimentInvariant massNeutrino010306 general physicsOrder of magnitudePhysical Review D
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High selective H-plane TE dual mode cavity filter design by using nonresonating nodes

2013

The design of H-plane TE dual mode cavity filters using models containing nonresonating nodes is presented. From the models a coupling matrix is derived and decomposed into submatrices, each representing a subcircuit. The optimization and cascading of subcircuits represents a good starting point for the global optimization. © 2014 Wiley Periodicals, Inc. Microwave Opt Technol Lett 56:161–166, 2014

PhysicsPlane (geometry)NRNsDual modeBlock matrixCoupling matrixCondensed Matter PhysicsTopologyDual-mode filterAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsFilter designSynthesisControl theoryTEORIA DE LA SEÑAL Y COMUNICACIONESPoint (geometry)Elliptic filterElliptic filterElectrical and Electronic EngineeringH-plane filterGlobal optimizationMicrowave
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Classical and Quantum Nonultralocal Systems on the Lattice

1997

We classify nonultralocal Poisson brackets for 1-dimensional lattice systems and describe the corresponding regularizations of the Poisson bracket relations for the monodromy matrix. A nonultralocal quantum algebras on the lattices for these systems are constructed. For some class of such algebras an ultralocalization procedure is proposed. The technique of the modified Bethe-Anzatz for these algebras is developed and is applied to the nonlinear sigma model problem.

PhysicsPoisson bracketNonlinear systemPure mathematicsNonlinear Sciences::Exactly Solvable and Integrable SystemsSigma modelPoisson manifoldLattice (order)Quantum mechanicsMonodromy matrixQuantumPoisson algebra
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