Search results for "Formula"

showing 10 items of 755 documents

Disentangling the Mn moments on different sublattices in the half-metallic ferrimagnet Mn3−xCoxGa

2011

Ferrimagnetic Mn3−xCoxGa compounds have been investigated by magnetic circular dichroism in x-ray absorption (XMCD). Compounds with x>0.5 crystallize in the CuHg2Ti structure. A tetragonal distortion of the cubic structure occurs for x≤0.5. For the cubic phase, magnetometry reveals a linearly increasing magnetization of 2x Bohr magnetons per formula unit obeying the generalized Slater–Pauling rule. XMCD confirms the ferrimagnetic character with Mn atoms occupying two different sublattices with antiparallel spin orientation and different degrees of spin localization and identifies the region 0.6<x≤0.8 as most promising for a high spin polarization at the Fermi level. Individual Mn moments on…

Physics and Astronomy (miscellaneous)Magnetic momentSpin polarizationCondensed matter physicsChemistryMagnetic circular dichroismFermi levelCondensed Matter::Materials ScienceMagnetizationTetragonal crystal systemsymbols.namesakeFerrimagnetismFormula unitsymbolsCondensed Matter::Strongly Correlated ElectronsApplied Physics Letters
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Dark matter stability and Dirac neutrinos using only Standard Model symmetries

2020

We provide a generic framework to obtain stable dark matter along with naturally small Dirac neutrino masses generated at the loop level. This is achieved through the spontaneous breaking of the global $U(1)_{B-L}$ symmetry already present in Standard Model. The $U(1)_{B-L}$ symmetry is broken down to a residual even $\mathcal{Z}_n$; $n \geq 4$ subgroup. The residual $\mathcal{Z}_n$ symmetry simultaneously guarantees dark matter stability and protects the Dirac nature of neutrinos. The $U(1)_{B-L}$ symmetry in our setup is anomaly free and can also be gauged in a straightforward way. Finally, we present an explicit example using our framework to show the idea in action.

Physics010308 nuclear & particles physicsDark matterDirac (software)FOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesAction (physics)Symmetry (physics)ddc:Standard Model (mathematical formulation)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceAnomaly (physics)Neutrino010306 general physics
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SO(3) family symmetry and axions

2018

Motivated by the idea of comprehensive unification, we study a gauged SO(3) flavor extension of the extended Standard Model, including right-handed neutrinos and a Peccei-Quinn symmetry with simple charge assignments. The model accommodates the observed fermion masses and mixings and yields a characteristic, successful relation among them. The Peccei-Quinn symmetry is an essential ingredient.

Physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesCharge (physics)FermionComputer Science::Digital Libraries01 natural sciencesSymmetry (physics)High Energy Physics - PhenomenologyTheoretical physicsStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Simple (abstract algebra)0103 physical sciencesNeutrino010306 general physicsAxionRotation group SOPhysical Review D
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Resonant ionization spectroscopy of autoionizing Rydberg states in cobalt and redetermination of its ionization potential

2017

Multi-step resonance ionization spectroscopy of cobalt has been performed using a hot-cavity laser ion source and three Ti:Sapphire lasers. The photoionization spectra revealed members of five new autoionizing Rydberg series that originate from three different lower levels of 3d74s5s h4F9/2, 3d74s4d f4G11/2, and 3d74s4d f4H13/2 and converge to the first four excited states of singly ionized Co. The analyses of the Rydberg series yield 63564.689 �� 0.036 cm-1 as the first ionization potential of Co, which is an order of magnitude more accurate than the previous estimation. Using a three-step resonance ionization scheme that employs an autoinizing Rydberg state in the last transition, we obta…

Physics010308 nuclear & particles physicsPhotoionizationMolar ionization energies of the elementsCondensed Matter Physics01 natural sciencesAtomic and Molecular Physics and OpticsIon sourcesymbols.namesakeAutoionizationExcited stateIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physicsRydberg state010306 general physicsJournal of Physics B: Atomic, Molecular and Optical Physics
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Low-lying level structure of Cu56 and its implications for the rp process

2017

The low-lying energy levels of proton-rich Cu56 have been extracted using in-beam γ-ray spectroscopy with the state-of-the-art γ-ray tracking array GRETINA in conjunction with the S800 spectrograph at the National Superconducting Cyclotron Laboratory at Michigan State University. Excited states in Cu56 serve as resonances in the Ni55(p,γ)Cu56 reaction, which is a part of the rp process in type-I x-ray bursts. To resolve existing ambiguities in the reaction Q value, a more localized isobaric multiplet mass equation (IMME) fit is used, resulting in Q=639±82 keV. We derive the first experimentally constrained thermonuclear reaction rate for Ni55(p,γ)Cu56. We find that, with this new rate, the …

Physics010308 nuclear & particles physicsQ valuerp-process01 natural sciencesNuclear physicsMass formulaExcited state0103 physical sciencesLevel structureIsobaric processAtomic physics010306 general physicsSpectroscopyMultipletPhysical Review C
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Chapter 1 The Resolution Challenge in 3D Optical Microscopy

2009

Publisher Summary This chapter discusses the theoretical principles of 3D microscopy with the widespread realizations of 3D microscopy.Based on the paraxial diffraction equations, it has been shown that conventional microscopes, when dealing with 3D fluorescent samples, provide sets of 2D images. These images of the different transverse sections of the 3D object contain, in addition to the sharp image of the in focus section, the blurred images of the rest of the specimen. The paraxial formalism has been generalized in a very simple way to a non-paraxial context, showing that the equations that govern non-paraxial imaging are similar to those that govern paraxial imaging. The only differenc…

Physics2d imagesFormalism (philosophy of mathematics)OpticsMicroscopeOptical microscopebusiness.industrylawParaxial approximationbusiness3d microscopyKirchhoff's diffraction formulalaw.invention
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Clustering effects inCr48composite nuclei produced via theMg24+Mg24reaction

2016

The nuclear properties of $^{48}\mathrm{Cr}$ composite $\ensuremath{\alpha}$-like nuclei produced at 60 MeV of excitation energy via the $^{24}\mathrm{Mg}+^{24}\mathrm{Mg}$ reaction were investigated. This excitation energy corresponds to a resonance with a narrow width (170 keV) observed in the elastic and inelastic channels, which was interpreted as a highly deformed state. To gain insight on the deformation of this state exclusive measurements of light charged particles were carried out with $8\ensuremath{\pi}\mathrm{LP}$ apparatus at Laboratori Nazionali di Legnaro and compared to statistical model predictions. The measured of $\ensuremath{\alpha}$-particle energy spectra, $\ensuremath{…

PhysicsAngular momentum010308 nuclear & particles physicsResonance01 natural sciencesCharged particleSpectral lineSemi-empirical mass formula0103 physical sciencesCluster (physics)Atomic physics010306 general physicsEnergy (signal processing)ExcitationPhysical Review C
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ATRAP antihydrogen experiments

2007

Antihydrogen (Hbar) was first produced at CERN in 1996. Over the past decade our ATRAP collaboration has made massive progress toward our goal of producing large numbers of cold Hbar atoms that will be captured in a magnetic gradient trap for precise comparison between the atomic spectra of matter and antimatter. The AD at CERN provides bunches of 3 × 107 low energy Pbars every 100 seconds. We capture and cool to 4 K, 0.1% of these in a cryogenic Penning trap. By stacking many bunches we are able to do experiments with 3 × 105 Pbars. ∼100 e+/sec from a 22Na radioactive source are captured and cooled in the trap, with 5 × 106 available experiments.We have developed 2 ways to make Hbar from t…

PhysicsAntiparticleCondensed Matter PhysicsPenning trapNuclear physicssymbols.namesakeAntiprotonLaser coolingAntimatterRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physicsNeutral particleAntihydrogenphysica status solidi c
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Analytical Solutions for the Self- and Mutual Inductances of Concentric Coplanar Disk Coils

2013

In this paper, closed-form solutions are presented for the self- and mutual inductances of disk coils which lie concentrically in a plane. The solutions are given as generalized hypergeometric functions which are closely related to elliptic integrals. The method used is a Legendre polynomial expansion of the inductance integral, which renders all integrations straightforward. Excellent numerical agreement with previous studies is obtained. An asymptotic formula for the approach to the ring coil limit is also derived and numerically validated. The methods presented here can be applied to noncoaxial and noncoplanar cases.

PhysicsAssociated Legendre polynomialsPlane (geometry)Electromagnetic coilMathematical analysisElliptic integralAsymptotic formulaElectrical and Electronic EngineeringHypergeometric functionDerivation of self inductanceLegendre polynomialsElectronic Optical and Magnetic MaterialsIEEE Transactions on Magnetics
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Anomalies in radiation-collisional kinetics of Rydberg atoms induced by the effects of dynamical chaos and the double Stark resonance

2013

Radiative and collisional constants of excited atoms contain the matrix elements of the dipole transitions and when they are blocked one can expect occurring a number of interesting phenomena in radiation-collisional kinetics. In recent astrophysical studies of IR emission spectra it was revealed a gap in the radiation emitted by Rydberg atoms ($RA$) with values of the principal quantum number of $n\approx10$. Under the presence of external electric fields a rearrangement of $RA$ emission spectra is possible to associate with manifestations of the Stark effect. The threshold for electric field ionization of $RA$ is $E\approx3\cdot10^{4}$ V/cm for states with $n>10$. This means that the emis…

PhysicsAtmospheric ScienceAtomic Physics (physics.atom-ph)FOS: Physical sciencesAerospace EngineeringResonanceAstronomy and AstrophysicsPhysics - Atomic Physicssymbols.namesakeGeophysicsAstrophysics - Solar and Stellar AstrophysicsStark effectSpace and Planetary ScienceExcited statePrincipal quantum numberRydberg atomRydberg formulasymbolsGeneral Earth and Planetary SciencesEmission spectrumAtomic physicsSolar and Stellar Astrophysics (astro-ph.SR)ExcitationAdvances in Space Research
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