Search results for "Berg"

showing 10 items of 758 documents

Rydberg Series Excitation of a Single Trapped Ca+40 Ion for Precision Measurements and Principal Quantum Number Scalings

2021

A complete set of spectroscopic data is indispensable when using Rydberg states of trapped ions for quantum information processing. We carried out Rydberg series spectroscopy for $n{S}_{1/2}$ states with $38\ensuremath{\le}n\ensuremath{\le}65$ and for $n{D}_{5/2}$ states with $37\ensuremath{\le}n\ensuremath{\le}50$ on a single trapped $^{40}{\mathrm{Ca}}^{+}$ ion. We determined the ionization energy of 2 870 575.582(15) GHz, 60 times more accurately as compared to the accepted value and contradicting it by 7.5 standard deviations. We confirm quantum defect values of ${\ensuremath{\delta}}_{{S}_{1/2}}=1.802\text{ }995(5)$ and ${\ensuremath{\delta}}_{{D}_{5/2}}=0.626\text{ }888(9)$ for $n{S}_…

PhysicsGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmasIonsymbols.namesakeQuantum defectIonization0103 physical sciencesPrincipal quantum numberRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physicsIonization energy010306 general physicsSpectroscopyExcitationPhysical Review Letters
researchProduct

A semiconductor laser system for the production of antihydrogen

2012

Laser-controlled charge exchange is a promising method for producing cold antihydrogen. Caesium atoms in Rydberg states collide with positrons and create positronium. These positronium atoms then interact with antiprotons, forming antihydrogen. Las er excitation of the caesium atoms is essential to increase the cross section of the charge-exchange collisions. This method was demonstrated in 2004 by the ATRAP collaboration by using an available copper vapour laser. For a second generation of charge-e xchange experiments we have designed a new semiconductor laser system that features several improvements compared to the copper vapour laser. We describe this new laser system and show the resul…

PhysicsGeneral Physics and Astronomychemistry.chemical_elementLaserlaw.inventionSemiconductor laser theoryPositroniumsymbols.namesakechemistrylawAntimatterExcited stateCaesiumPhysics::Atomic and Molecular ClustersRydberg formulasymbolsddc:530Physics::Atomic PhysicsAtomic physicsAntihydrogenNew Journal of Physics
researchProduct

Entangling a Three High-Q Cavity System in a GHZ State

2001

PhysicsGreenberger–Horne–Zeilinger stateQuantum mechanicsGeneral Physics and AstronomyAtomic physicsFortschritte der Physik
researchProduct

Classical thermodynamics of the Heisenberg chain in a field by generalized Bethe ansatz method

1990

Abstract Using the classical action-angle variables for the continuous model, we study the thermodynamics of the classical Heisenberg chain in an applied field by a generalized Bethe ansatz approach. The crucial point consists in the derivation of a phase-shifted density of states for the excitations of the model, obtained by imposing periodic boundary conditions. In the thermodynamic limit, the free energy can be expressed in terms of the solution of a non-linear integral equation, showing the universal dependece of the variable x=(JH) 1 2 /T .

PhysicsHeisenberg modelGeneral Physics and AstronomyThermodynamicssine-Gordon equationIntegral equationBethe ansatzsymbols.namesakeThermodynamic limitsymbolsPeriodic boundary conditionsBoundary value problemHamiltonian (quantum mechanics)Mathematical physicsPhysics Letters A
researchProduct

Mass spectrum and thermodynamics of quasi-conformal gauge theories from gauge/gravity duality

2011

We use gauge/gravity duality to study simultaneously the mass spectrum and the thermodynamics of a generic quasi-conformal gauge theory, specified by its beta function. The beta function of a quasi-conformal theory almost vanishes, and the coupling is almost constant between two widely separated energy scales. Depending on whether the gravity dual has a black hole or not, the mass spectrum is either a spectrum of quasinormal oscillations or a normal T=0 mass spectrum. The mass spectrum is quantitatively correlated with the thermal properties of the system. As the theory approaches conformality, the masses have to vanish. We show that in this limit, the masses calculated via gauge/gravity du…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsGravity (chemistry)FOS: Physical sciencesDuality (optimization)GravitationBlack holeHigh Energy Physics::TheoryGeneral Relativity and Quantum CosmologyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsQuasinormal modeSeiberg dualityDilatonGauge theoryMathematical physics
researchProduct

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
researchProduct

Spiral Inflation with Coleman-Weinberg Potential

2015

We apply the idea of spiral inflation to Coleman-Weinberg potential, and show that inflation matching well observations is allowed for a symmetry-breaking scale ranging from an intermediate scale to GUT scale even if the quartic coupling $\lambda$ is of $\mathcal{O}(0.1)$. The tensor-to-scalar ratio can be of $\mathcal{O}(0.01)$ in case of GUT scale symmetry-breaking.

PhysicsInflation (cosmology)Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Scale (ratio)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaCoupling (probability)01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsQuartic function0103 physical sciencesColeman–Weinberg potentialGrand Unified TheorySymmetry breaking010306 general physicsMathematical physicsAstrophysics - Cosmology and Nongalactic Astrophysics
researchProduct

Isotope shifts and hyperfine structure in calcium 4snp and 4snf F Rydberg states

2000

Isotope shifts and hyperfine structure have been measured in 4snp 1 P1 and Rydberg states for all stable calcium isotopes and the radioisotope 41Ca using high-resolution laser spectroscopy. Triple-resonance excitation via Rydberg state was followed by photoionization with a CO2 laser and mass selective ion detection. Isotope shifts for the even-mass isotopes have been analyzed to derive specific mass shift and field shift factors. The apparent isotope shifts for 41Ca and 43Ca exhibit anomalous values that are n-dependent. This is interpreted in terms of hyperfine-induced fine-structure mixing, which becomes very pronounced when singlet-triplet fine-structure splitting is comparable to the h…

PhysicsIsotopePhotoionizationAtomic and Molecular Physics and OpticsIsotopes of calciumsymbols.namesakeIsotopic shiftKinetic isotope effectRydberg formulasymbolsPhysics::Atomic PhysicsRydberg stateAtomic physicsHyperfine structureThe European Physical Journal D
researchProduct

Classical Heisenberg antiferromagnets with nearest and next-nearest neighbor interactions on the face-centered cubic lattice: a model for EuTe?

1989

Magnetic properties of the Heisenberg antiferromagnet with spin quantum numberS→∞ on the face-centered cubic lattice are studied as function of temperature and magnetic field, using molecular field approximation and Monte Carlo methods. In order to model Europiumtelluride, we use isotropic exchange interactions between nearest- and nextnearest neighbors; the values of these exchange constants are taken from experiments. In addition, a pseudo-dipolar anisotropy (truncated after the next-nearest neighbor distance) is included; the molecular field calculations also are performed with the full dipolar of real EuTe in two respects: the structure in zero magnetic field involves 8 sublattices in t…

PhysicsMagnetizationDipoleCondensed matter physicsHeisenberg modelExchange interactionAntiferromagnetismGeneral Materials ScienceCubic crystal systemCondensed Matter PhysicsElectronic Optical and Magnetic Materialsk-nearest neighbors algorithmMagnetic fieldZeitschrift f�r Physik B Condensed Matter
researchProduct

Ground-state properties of generalized Heisenberg chains with composite spin.

1988

We consider in detail the ground-state properties of recently introduced generalized Heisenberg models which can have several spin operators at each site and which interpolate smoothly between Heisenberg chains of different spin lengths. We show that the mappings to field-theoretical models used to describe the critical properties of the Heisenberg model remain valid in the composite-spin model. In models which interpolate between the spin-(1/2 and the spin-1 behavior, these mappings predict an extended singlet phase around the isotropic antiferromagnetic point whenever the models move away from the spin-(1/2 point. Numerical calculations on finite chains seem to confirm the existence of th…

PhysicsMathematical modelHeisenberg modelQuantum mechanicsIsotropyCondensed Matter::Strongly Correlated ElectronsSinglet stateAngular momentum operatorGround stateMathematical OperatorsSpin-½Physical review. B, Condensed matter
researchProduct