Search results for "Mixing"

showing 10 items of 795 documents

Shape coexistence in neutron-deficient Hg isotopes studied via lifetime measurements inHg184,186and two-state mixing calculations

2014

The neutron-deficient mercury isotopes, $^{184,186}$Hg, were studied with the Recoil Distance Doppler Shift (RDDS) method using the Gammasphere array and the Koln Plunger device. The Differential Decay Curve Method (DDCM) was employed to determine the lifetimes of the yrast states in $^{184,186}$Hg. An improvement on previously measured values of yrast states up to $8^{+}$ is presented as well as first values for the $9_{3}$ state in $^{184}$Hg and $10^{+}$ state in $^{186}$Hg. $B(E2)$ values are calculated and compared to a two-state mixing model which utilizes the variable moment of inertia (VMI) model, allowing for extraction of spin-dependent mixing strengths and amplitudes.

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsYrastMoment of inertia7. Clean energy01 natural sciencesRecoilAmplitude0103 physical sciencesNeutronGammasphereAtomic physicsNuclear Experiment010306 general physicsMixing (physics)Physical Review C
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CP violation and limits on New Physics including recent B-s measurements

2007

We analyse present constraints on the SM parameter space and derive, in a model independent way, various bounds on New Physics contributions to $B_d^0$--$\bar B_d^0$ and $B_s^0$--$\bar B_s^0$ mixings. Our analyses include information on a large set of asymmetries, leading to the measurement of the CKM phases $\gamma$ and $\bar\beta$, as well as recent data from D0 and CDF related to the $B_s^0$--$\bar B_s^0$ system such as the measurement of $\Delta M_{B_s}$, $A_{SL}$ and $\Delta\Gamma_{s}^{CP}$. We examine in detail several observables such as the asymmetries $A_{sl}^d$, $A_{SL}$, the width differences $\Delta\Gamma_{d}$ and $\Delta\Gamma_{s}^{CP}$ and discuss the r\^ole they play in estab…

PhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciencesFísicaObservableParameter space01 natural sciencesAsymmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Large set (Ramsey theory)0103 physical sciencesCP violation010306 general physicsMixing (physics)media_common
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Sweeping the Space of Admissible Quark Mass Matrices

2002

We propose a new and efficient method of reconstructing quark mass matrices from their eigenvalues and a complete set of mixing observables. By a combination of the principle of NNI (nearest neighbour interaction) bases which are known to cover the general case, and of the polar decomposition theorem that allows to convert arbitrary nonsingular matrices to triangular form, we achieve a parameterization where the remaining freedom is reduced to one complex parameter. While this parameter runs through the domain bounded by a circle with radius R determined by the up-quark masses around the origin in the complex plane one sweeps the space of all mass matrices compatible with the given set of d…

PhysicsNuclear and High Energy PhysicsMathematical analysisPolar decompositionFOS: Physical sciencesSpace (mathematics)Domain (mathematical analysis)High Energy Physics - PhenomenologyClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Cover (topology)Mixing (mathematics)Bounded functionComplex planeEigenvalues and eigenvectors
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Fine structure in -decay and shape coexistence in

1999

Excited states in populated in the -decay of have been identified through -particle-conversion electron coincidences. The level scheme has been interpreted using a configuration mixing calculation, providing estimates of the mixing matrix elements, mixing amplitudes and the energies of unperturbed and unobserved levels.

PhysicsNuclear and High Energy PhysicsMatrix (mathematics)Amplitude010308 nuclear & particles physicsExcited state0103 physical sciencesStructure (category theory)ElectronAtomic physics010306 general physics01 natural sciencesMixing (physics)Journal of Physics G: Nuclear and Particle Physics
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a 0 (980)− f 0 (980) mixing in χ c1 → π 0 f 0 (980)→ π 0 π + π − and χ c1 → π 0 a 0 (980)→ π 0 π 0 η

2017

Abstract We study the isospin breaking in the reactions χ c 1 → π 0 π + π − and χ c 1 → π 0 π 0 η and its relation to the a 0 ( 980 ) − f 0 ( 980 ) mixing, which was measured by the BESIII Collaboration. We show that the same theoretical model previously developed to study the χ c 1 → η π + π − reaction (also measured by BESIII), and further explored in the predictions to the η c → η π + π − , can be successfully employed in the present study. We assume that the χ c 1 behaves as an S U ( 3 ) singlet to find the weight in which trios of pseudoscalars are created, followed by the final state interaction of pairs of mesons to describe how the a 0 ( 980 ) and f 0 ( 980 ) are dynamically generat…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsScatteringPropagator01 natural sciencesPseudoscalarAmplitudeIsospinQuantum mechanics0103 physical sciencesSinglet stateAtomic physics010306 general physicsMixing (physics)Physics Letters B
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Tri/Bi-maximal lepton mixing and leptogenesis

2009

In models with flavour symmetries added to the gauge group of the Standard Model the CP-violating asymmetry necessary for leptogenesis may be related with low-energy parameters. A particular case of interest is when the flavour symmetry produces exact Tri-Bimaximal lepton mixing leading to a vanishing CP-violating asymmetry. In this paper we present a model-independent discussion that confirms this always occurs for unflavoured leptogenesis in type I see-saw scenarios, noting however that Tri-Bimaximal mixing does not imply a vanishing asymmetry in general scenarios where there is interplay between type I and other see-saws. We also consider a specific model where the exact Tri-Bimaximal mi…

PhysicsNuclear and High Energy PhysicsParticle physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesAsymmetrySymmetry (physics)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)Gauge groupLeptogenesis0103 physical sciencesCP violationHigh Energy Physics::ExperimentSDG 7 - Affordable and Clean Energy010306 general physicsMixing (physics)media_commonParticle Physics - Phenomenology
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Predicting neutrino oscillations with “bi-large” lepton mixing matrices

2019

We propose two schemes for the lepton mixing matrix $U = U_l^\dagger U_\nu$, where $U = U_l$ refers to the charged sector, and $U_\nu$ denotes the neutrino diagonalization matrix. We assume $U_\nu$ to be CP conserving and its three angles to be connected with the Cabibbo angle in a simple manner. CP violation arises solely from the $U_l$, assumed to have the CKM form, $U_l\simeq V_{\rm CKM}$, suggested by unification. Oscillation parameters depend on a single parameter, leading to narrow ranges for the "solar" and "accelerator" angles $\theta_{12}$ and $\theta_{23}$, as well as for the CP phase, predicted as $\delta_{\rm CP}\sim 1.3\pi$.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciences01 natural scienceslcsh:QC1-999Matrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationMixing (physics)lcsh:PhysicsLeptonPhysics Letters B
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Bilarge neutrino mixing and the Cabibbo angle

2012

Recent measurements of the neutrino mixing angles cast doubt on the validity of the so-far popular tri-bimaximal mixing ansatz. We propose a parametrization for the neutrino mixing matrix where the reactor angle seeds the large solar and atmospheric mixing angles, equal to each other in first approximation. We suggest such bi-large mixing pattern as a model building standard, realized when the leading order value of the reactor angle equals the Cabibbo angle.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesFísica01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino010306 general physicsNeutrino oscillationParametrizationModel buildingMixing (physics)Ansatz
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Generation patterns, modified $\gamma-Z$ mixing, and hidden sector with dark matter candidates as framed standard model results

2018

A descriptive summary is given of the results to-date from the framed standard model (FSM) which: Assigns geometric meaning to the Higgs field and to fermion generations, hence offering an explanation for the observed mass and mixing patterns of quarks and leptons, reproducing near-quantitatively 17 of SM parameters with only 7. Predicts a new vector boson [Formula: see text] which mixes with [Formula: see text] and [Formula: see text], leading to deviations from the SM mixing scheme. For [Formula: see text] TeV, these deviations are within present experimental errors but should soon be detectable at LHC when experimental accuracy is further improved. Suggests the existence of a hidden sec…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterAstronomy and Astrophysics01 natural sciencesAtomic and Molecular Physics and OpticsStandard ModelHidden sectorHigh Energy Physics - Phenomenology0103 physical sciences010306 general physicsMixing (physics)
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Accidental stability of dark matter

2013

We propose that dark matter is stable as a consequence of an accidental Z(2) that results from a flavour symmetry group which is the double-cover group of the symmetry group of one of the regular geometric solids. Although model-dependent, the phenomenology resembles that of a generic >inert Higgs> dark matter scheme.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterHigh Energy Physics::Phenomenologyneutrino masses and mixingFOS: Physical sciencesFísicaSymmetry group01 natural sciencesdark matterHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Accidental0103 physical sciencesHiggs boson010306 general physicsPhenomenology (particle physics)flavour symmetry
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