Search results for "Casimir effect"

showing 10 items of 56 documents

Casimir-Lifshitz force out of thermal equilibrium between dielectric gratings

2014

We calculate the Casimir-Lifshitz pressure in a system consisting of two different 1D dielectric lamellar gratings having two different temperatures and immersed in an environment having a third temperature. The calculation of the pressure is based on the knowledge of the scattering operators, deduced using the Fourier Modal Method. The behavior of the pressure is characterized in detail as a function of the three temperatures of the system as well as the geometrical parameters of the two gratings. We show that the interplay between non-equilibrium effects and geometrical periodicity offers a rich scenario for the manipulation of the force. In particular, we find regimes where the force can…

ACS number(s): 12.20.−m42.79.Dj42.50.Ct42.50.Lc[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]Degrees of freedom (physics and chemistry)Non-equilibrium thermodynamicsFOS: Physical sciencesDielectricCasimir Force Out of Thermal equilibrium systems GratingsSettore FIS/03 - Fisica Della Materiasymbols.namesake[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Lamellar structure[PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech]PhysicsThermal equilibriumQuantum PhysicsCondensed matter physicsScatteringAtomic and Molecular Physics and OpticsCasimir effectFourier transformClassical mechanicssymbolsQuantum Physics (quant-ph)Physics - OpticsOptics (physics.optics)
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Application of the star-product method to the angular momentum quantization

1992

We define a *-product on ℝ3 and solve the polarization equation f*C=0 where C is the Casimir of the coadjoint representation of SO(3). We compute the action of SO(3) on the space of solutions. We then examine the case of non-zero eigenvalues of C, in order to find finite-dimensional representations of SO(3). Finally, we compute \(\sqrt C *\sqrt C \) as an asymptotic series of C. This gives an explanation of the use of the star square root of C in a paper by Bayen et al. instead of its natural square root.

Casimir effectAngular momentumQuantization (physics)Coadjoint representationSquare rootStar productStatistical and Nonlinear PhysicsGeometryAsymptotic expansionMathematical PhysicsEigenvalues and eigenvectorsMathematicsMathematical physicsLetters in Mathematical Physics
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Electrostatic interactions in critical solvents

2011

The subtle interplay between critical phenomena and electrostatics is investigated by considering the effective force acting on two parallel walls confining a near-critical binary liquid mixture with added salt. The ion-solvent coupling can turn a non-critical repulsive electrostatic force into an attractive one upon approaching the critical point. However, the effective force is eventually dominated by the critical Casimir effect, the universal properties of which are not altered by the presence of salt. This observation allows a consistent interpretation of recent experimental data.

Casimir effectMaterials scienceCritical point (thermodynamics)Chemical physicsEffective forceCritical phenomenaGeneral Physics and AstronomySoft Condensed Matter (cond-mat.soft)FOS: Physical sciencesCondensed Matter - Soft Condensed MatterElectrostatics
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A microscopic approach to Casimir forces between metal bodies

2014

We consider the Casimir interaction between macroscopic metallic objects in terms of the dispersion interactions (Casimir-Polder and van der Waals) between their constituents. Expressions for two- and three-body dispersion interactions between the microscopic parts of a metal are obtained, both in the retarded and non-retarded limits. They are then used to evaluate two- and three-body contributions of the Casimir force between two flat ideal metallic slabs. Our results show the non-applicability of the Hamaker approximation in this geometry. It is further seen that the three-body contributions give an overall repulsive contribution to the force, which is of the same order of magnitude as th…

Casimir effectVacuum fluctuationsCasimir-Polder force
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Il vuoto: da Galileo al XXI secolo

2009

Casimir effectvacuum fluctuationQuantum vacuum
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Causality, non-locality and three-body Casimir–Polder energy between three ground-state atoms

2006

The problem of relativistic causality in the time-dependent three-body Casimir–Polder interaction energy between three atoms, initially in their bare ground-state, is discussed. It is shown that the non-locality of the spatial correlations of the electromagnetic field emitted by the atoms during their dynamical self-dressing may become manifest in the dynamical three-body Casimir–Polder interaction energy between the three atoms.

Condensed Matter::Quantum GasesElectromagnetic fieldPhysicsQuantum opticsThree-body dispersion forces.Interaction energyCondensed Matter PhysicsThree-body problemAtomic and Molecular Physics and OpticsMany-body problemCausality (physics)Casimir effectQuantum electrodynamicQuantum mechanicsCausality and non-localityPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsGround stateJournal of Physics B: Atomic, Molecular and Optical Physics
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Effects of a uniform acceleration on atom–field interactions

2014

We review some quantum electrodynamical effects related to the uniform acceleration of atoms in vacuum. After discussing the energy level shifts of a uniformly accelerated atom in vacuum, we investigate the atom-wall Casimir-Polder force for accelerated atoms, and the van der Waals/Casimir-Polder interaction between two accelerated atoms. The possibility of detecting the Unruh effect through these phenomena is also discussed in detail.

Condensed Matter::Quantum GasesPhysicsQuantum PhysicsField (physics)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Condensed Matter PhysicsGeneral Relativity and Quantum CosmologyAtomic and Molecular Physics and OpticsCasimir effectGeneral Relativity and Quantum Cosmologysymbols.namesakeAccelerationUnruh effectUnruh effect Casimir–Polder forces vacuum fluctuationsAtomPhysics::Atomic and Molecular ClusterssymbolsPhysics::Accelerator PhysicsPhysics::Atomic Physicsvan der Waals forceAtomic physicsQuantum Physics (quant-ph)QuantumMathematical PhysicsPhysica Scripta
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Optomechanical Rydberg-atom excitation via dynamic Casimir-Polder coupling

2014

We study the optomechanical coupling of a oscillating effective mirror with a Rydberg atomic gas, mediated by the dynamical atom-mirror Casimir-Polder force. This coupling may produce a near-field resonant atomic excitation whose probability scales as $\propto (d^2\;a\;n^4\;t)^2/z_0^8$, where $z_0$ is the average atom-surface distance, $d$ the atomic dipole moment, $a$ the mirror's effective oscillation amplitude, $n$ the initial principal quantum number, and $t$ the time. We propose an experimental configuration to realize this system with a cold atom gas trapped at a distance $\sim 2\cdot10 \, \mu$m from a semiconductor substrate, whose dielectric constant is periodically driven by an ext…

CouplingPhysicsCondensed Matter::Quantum GasesQuantum PhysicsRydberg Atoms[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Dynamical Casimir and Casimir-Polder effectGeneral Physics and AstronomyFOS: Physical sciences7. Clean energyQuantum OptomechanicCasimir effectDipolesymbols.namesakeUltracold atomRydberg atomPrincipal quantum numberRydberg formulasymbolsPhysics::Atomic PhysicsAtomic physics[PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech]Quantum Physics (quant-ph)Excitation
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Dynamical Casimir-Polder forces

2011

We consider the dynamical Casimir-Polder force on an atom placed near an infinite conducting wall. The system is initially in a non equilibrium configuration such as a bare or a partially dressed state, and its time evolution is considered as well as the time dependence of the atom-wall Casimir-Polder interaction. A possible scheme to generate experimentally the initial partially dressed state and to detect the dynamical Casimir-Polder force is discussed.

Dynamical Casimir effectDynamical Casimir-Polder forceSettore FIS/03 - Fisica Della Materia
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Fluctuations of the Casimir-Polder force between an atom and a conducting wall

2007

We consider the quantum fluctuations of the Casimir-Polder force between a neutral atom and a perfectly conducting wall in the ground state of the system. In order to obtain the atom-wall force fluctuation we first define an operator directly associated to the force experienced by the atom considered as a polarizable body in an electromagnetic field, and we use a time-averaged force operator in order to avoid ultraviolet divergences appearing in the fluctuation of the force. This time-averaged force operator takes into account that any measurement involves a finite time. We also calculate the Casimir-Polder force fluctuation for an atom between two conducting walls. Experimental observabili…

Electromagnetic fieldAbraham–Lorentz forcePhysicsQuantum PhysicsForce field (physics)Exchange interactionAtom-surface interactionFOS: Physical sciencesAtomic and Molecular Physics and OpticsCasimir effectCentral forceQuantum electrodynamicsPhysics::Atomic and Molecular ClustersCasimir-Polder forcesPhysics::Atomic PhysicsForce fluctuationQuantum Physics (quant-ph)Conservative forceQuantum fluctuation
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