Search results for "UniFi"

showing 10 items of 302 documents

Classical Field Theory of Gravitation

2012

The classical field theories developed in the preceding chapters all have in common that they are formulated on a flat spacetime, i.e. on a four-manifold which is a Euclidean space and which locally is decomposable into a direct product M 4 = ℝR3 ℝR of a physical space ℝR3 x of motions, and a time axis ℝRt. The first factor is the threedimensional space as it is perceived by an observer at rest while the time axis displays the (coordinate) time that he/she measures on his/her clocks. This spacetime is endowed with the Poincare group as the invariance group of physical laws and inherits the corresponding specific causality structure.

PhysicsClassical unified field theoriesSpacetimeEuclidean spacePoincaré groupMinkowski spaceScalar theories of gravitationClassical field theoryNordström's theory of gravitationMathematical physics
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Unified model of fractal conductance fluctuations for diffusive and ballistic semiconductor devices

2006

We present an experimental comparison of magnetoconductance fluctuations measured in the ballistic, quasiballistic, and diffusive scattering regimes of semiconductor devices. In contradiction to expectations, we show that the spectral content of the magnetoconductance fluctuations exhibits an identical fractal behavior for these scattering regimes and that this behavior is remarkably insensitive to device boundary properties. We propose a unified model of fractal conductance fluctuations in the ballistic, quasiballistic, and diffusive transport regimes, in which the generic fractal behavior is generated by a subtle interplay between boundary and material-induced chaotic scattering events.

PhysicsCondensed matter physicsScatteringConductanceBoundary (topology)Semiconductor deviceUnified ModelCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic Materials[SPI]Engineering Sciences [physics]FractalQuantum dotChaotic scatteringStatistical physicsPhysical Review B
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On the unification of electroweak interactions with gravity

1982

It is shown that the electroweak interactions in the Salam-Weinberg model can be described by a space-time connection form which preserves the space-time metric multiplied by a conformal factor. In addition, one needs an extraSO(2)-connection form. The Dirac field in this formalism is described (after making a certain regularity assumption) by a vierbein field for the space-time metric and a complex scalar field.

PhysicsFormalism (philosophy of mathematics)Theoretical physicsClassical mechanicsUnificationHigh Energy Physics::PhenomenologyElectroweak interactionCartan formalismGeneral Physics and AstronomyConnection formConformal mapScalar fieldCzechoslovak Journal of Physics
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Weak Interactions and the Standard Model of Strong and Electroweak Interactions

2011

This chapter gives an introduction to the phenomenology and the theory of weak interaction processes involving leptons and hadrons. In Sects. 3.1, 3.2 we collect the most prominent and characteristic properties of weak interactions as they follow from the analysis of a set of key experiments, old and recent. The following sections 3.3–3.5 deal with the elements of non-Abelian local gauge theories in general, and with the unified theory of electroweak and strong interactions of Glashow, Salam and Weinberg (GSW), in particular.

PhysicsGauge bosonTheoretical physicsWeak isospinHigh Energy Physics::PhenomenologyElectroweak interactionHigh Energy Physics::ExperimentGauge theoryWeak interactionUnified field theoryPhenomenology (particle physics)Lepton
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Search for Supersymmetry Using Final States with One Lepton, Jets, and Missing Transverse Momentum with the ATLAS Detector ins=7  TeVppCollisions

2011

This Letter presents the first search for supersymmetry in final states containing one isolated electron or muon, jets, and missing transverse momentum from sqrt{s} = 7 TeV proton-proton collisions at the LHC. The data were recorded by the ATLAS experiment during 2010 and correspond to a total integrated luminosity of 35 pb-1. No excess above the standard model background expectation is observed. Limits are set on the parameters of the minimal supergravity framework, extending previous limits. For A_0 = 0 GeV, tan beta = 3, mu > 0 and for equal squark and gluino masses, gluino masses below 700 GeV are excluded at 95% confidence level.

PhysicsGluinoParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsSupergravityHigh Energy Physics::PhenomenologyATLAS experimentGeneral Physics and AstronomySupersymmetry01 natural sciencesNuclear physics0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsLeptonPhysical Review Letters
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A Model of Comprehensive Unification

2017

Comprehensive – that is, gauge and family – unification using spinors has many attractive features, but it has been challenged to explain chirality. Here, by combining an orbifold construction with more traditional ideas, we address that difficulty. Our candidate model features three chiral families and leads to an acceptable result for quantitative unification of couplings. A potential target for accelerator and astronomical searches emerges.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsSpinorUnification010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGauge (firearms)01 natural scienceslcsh:QC1-999Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciences010306 general physicsChirality (chemistry)lcsh:PhysicsOrbifold
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Seesaw scale, unification, and proton decay

2018

We investigate a simple realistic grand unified theory based on the $SU(5)$ gauge symmetry which predicts an upper bound on the proton decay lifetime for the channels $p \to K^+ \bar{\nu}$ and $p \to \pi^+ \bar{\nu}$, i.e. $\tau (p \to K^+ \bar{\nu}) \lesssim 3.4 \times 10^{35}$ and $\tau (p \to \pi^+ \bar{\nu}) \lesssim 1.7 \times 10^{34}$ years, respectively. In this context, the neutrino masses are generated through the type I and type III seesaw mechanisms, and one predicts that the field responsible for type III seesaw must be light with a mass below 500 TeV. We discuss the testability of this theory at current and future proton decay experiments.

PhysicsHigh Energy Physics - TheoryParticle physics010308 nuclear & particles physicsProton decayHigh Energy Physics::PhenomenologyFOS: Physical sciencesField (mathematics)Context (language use)Type (model theory)01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics - Theory (hep-th)0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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On the chirality of the SM and the fermion content of GUTs

2015

The Standard Model (SM) is a chiral theory, where right- and left-handed fermion fields transform differently under the gauge group. Extra fermions, if they do exist, need to be heavy otherwise they would have already been observed. With no complex mechanisms at work, such as confining interactions or extra-dimensions, this can only be achieved if every extra right-handed fermion comes paired with a left-handed one transforming in the same way under the Standard Model gauge group, otherwise the new states would only get a mass after electroweak symmetry breaking, which would necessarily be small (similar to 100 GeV). Such a simple requirement severely constrains the fermion content of Grand…

PhysicsHigh Energy Physics - TheoryParticle physicsNuclear and High Energy PhysicsGauge theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSymmetry breaking01 natural sciences3-generation superstring modelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Grand unification0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsHumanitiesNuclear Physics B
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Rigour and Rigidity: Systematics on particle physics D6-brane models on Z(2)xZ(6)

2014

We launch a systematic search for phenomenologically appealing string vacua with intersecting D-branes on the promising T6/Z(2)xZ(6)xOR orientifold with discrete torsion. The number of independent background lattices is reduced from six to two by new symmetries. The occurrence of USp(2N) and SO(2N) versus U(N) gauge groups is classified as well as D-branes without matter in the adjoint and/or symmetric representation. Supersymmetric fractional D6-branes allowing for RR tadpole cancellation are fully classified in terms of all possible values of the one complex structure modulus inherited from the underlying six-torus. We then systematically investigate the conditions for three particle gene…

PhysicsHigh Energy Physics - TheoryPati–Salam modelVacuum stateExotic matterFOS: Physical sciencesGeneral Physics and AstronomyTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Rigidity (electromagnetism)High Energy Physics - Theory (hep-th)OrientifoldHomogeneous spaceGrand Unified TheoryBrane
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Group-Theoretic analysis of the mixing angle in the electroweak gauge group

1996

In this paper the authors provide strong mathematical support for the idea that the experimentally measured magnitude 1 - M{sub W}{sup 2}/M{sub Z}{sup 2} associated with sin{sup 2}{theta}{sub w} in the standard model of electroweak interactions cannot be simultaneously identified with the squared quotient of the electric charge by the SU(2) charge, e{sup 2}/g{sup 2}. In fact, the natural, mathematical requirement that the Weinberg rotation between the gauge fields associated with the third component of the {open_quotes}weak isospin{close_quotes} (T{sub 3}) and the hypercharge (Y) proceeds from a global Lie-group homomorphism of the SU(2) {circle_times} U(1){sub y} gauge group in some locall…

PhysicsHyperchargeParticle physicsPhysics and Astronomy (miscellaneous)Gauge groupGeneral MathematicsLie algebraElectroweak interactionLie groupGrand Unified TheoryCharge (physics)Weinberg angleMathematical physicsInternational Journal of Theoretical Physics
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