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Low Temperature Physics

Kinetics of low-temperature gas of hydrogen-like atoms in an external electromagnetic field

Anatolij G. Zagorodny, Yu. V. Slyusarenko, S.N. Shulga

Published Oct 1, 2018• 1 citation
Publisher

Abstract

A microscopic approach for the construction of the kinetic theory of low-temperature hydrogen-like gases in an external electromagnetic field was developed. The approach is based on the formulation of secondary quantization in the presence of bound states of particles. It is suggested that the bound state (for example, a hydrogen-like atom of alkali metal) is formed by two charged fermions of different sorts — the valence electron and the ion core. The reduced description of relaxation processes establishes the basis for the formulation of the kinetic equations. Within the developed theoretical framework, the system of kinetic equations for Wigner’s distribution functions of free fermions of both sorts and their bound states, hydrogen-like atoms, is developed accounting for an external and self-consistent (intermediate) fields acting on the system. The obtained equations of motion for Wigner’s distribution functions serve as a basis for analyzing non-equilibrium effects and phenomena related to the influence of an external electromagnetic field on low-temperature gases of alkali metals.

DOI
10.1063/1.5055846

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A microscopic approach for the construction of the kinetic theory of low-temperature hydrogen-like gases in an external electromagnetic field was developed. The approach is based on the formulation of secondary quantization in the presence of bound states of particles. It is suggested that the bound state (for example, a hydrogen-like atom of alkali metal) is formed by two charged fermions of different sorts — the valence electron and the ion core. The reduced description of relaxation processes establishes the basis for the formulation of the kinetic equations. Within the developed theoretical framework, the system of kinetic equations for Wigner’s distribution functions of free fermions of both sorts and their bound states, hydrogen-like atoms, is developed accounting for an external and self-consistent (intermediate) fields acting on the system. The obtained equations of motion for Wigner’s distribution functions serve as a basis for analyzing non-equilibrium effects and phenomena related to the influence of an external electromagnetic field on low-temperature gases of alkali metals.
The response of the system, consisting of two kinds of opposite-charged fermions and their bound states (hydrogen-like atoms), to the perturbation by the external electromagnetic field in low particle kinetic energies region is studied. Expressions for Green functions that describe the system response to the external electromagnetic field and take into account the presence of particle bound states (atoms) are found. Macroscopic parameters of the system, such as conductivity, permittivity and magnetic permeability in terms of these Green functions are introduced. As an example, the perturbation of the ideal hydrogen-like plasma by the external electromagnetic field in low temperature region is considered. Such approach also enables to study the propagation properties of the signal, tuned up to the transition between two hyperfine ground state levels of alkali atoms that are considered in Bose-Einstein condensation (BEC) state. It is shown that the signal can propagate in such system with rather small energy loss. Such fact allows to introduce the group velocity concept and to study the slowing down conditions for the microwave signal that propagates in BEC.
We propose a microscopic approach describing the interaction of an ideal gas of hydrogenlike atoms with a weak electromagnetic field. This approach is based on the Green-function formalism and an approximate formulation of the method of second quantization for quantum many-particle systems in the presence of bound states of particles. The dependencies of the propagation velocity and damping rate of electromagnetic pulses on the microscopic characteristics of the system are studied for a gas of hydrogenlike atoms. For a Bose-Einstein condensate of alkali-metal atoms we find the conditions when the electromagnetic waves of both the optical and microwave regions are slowed. In the framework of the proposed approach, the influence of an external homogeneous and static magnetic field on the slowing phenomenon is studied.
At low temperatures the De Broglie wavelength of the gas particles becomes on the order of their average separation, and the effects of their indistinguishability become important. In the absence of a phase transition in the gas, the quantum mechanical Wigner distribution function for a dilute gas of fermions or bosons satisfies the Uehling-Uhlenbeck equation. This equation satisfies an H- theorem with equilibrium solutions being ideal boson or ideal fermion distributions. Navier-Stokes equations can be derived by standard methods. A low temperature gas of weakly interacting bosons undergoes a Bose-Einstein condensation with a macroscopically occupied ground state. A different approach is required to describe the non-equilibrium processes in such a situation. A kinetic equation can be derived for the Bogoliubov excitations in the gas at very low temperatures. The associated hydrodynamic equations are the Landau-Khaltnikov, two fluid equations, and explicit expressions are obtained for the six associated transport coefficients.
We propose a microscopic approach for a description of interaction of the ideal gas of alkali atoms with a weak electromagnetic radiation. The description is constructed in the framework of the Green functions formalism that is based on a new formulation of the second quantization method in case of the bound states (atoms) presence. For a gas in the Bose-condensed (BEC) state we study the dependencies of the propagation velocity and damping rate on the microscopic characteristics of the system. For a condensed dilute gas of sodium atoms we find the conditions of the group velocity reducing for optical pulses tuned up close to the resonant transitions. We also show that the slowing phenomenon can strongly depend on the intensity of the external static magnetic field.
The external electromagnetic interactions of hydrogenic atoms, which exhibit global Galilean invariance but preserve the relativistic description of the electron, are investigated. The Hamiltonian for the free atom consists of the Breit Hamiltonian for a relativistic electron interacting with a nonrelativistic spinless proton. Approximate generators of the Galilean group are constructed in terms of individual-particle position, momentum, and spin operators in several unitarily equivalent representations. In one of these the Hamiltonian is separable in conventional relative and center-of-mass coordinates. This separability facilitates the treatment of a number of external-field problems. An effective Hamiltonian for the interaction of the atom with a constant external electric field is given and compared to that obtained by other authors. The low-energy theorem for Compton scattering from the composite system is explicitly verified including corrections due to atomic binding. This also gives an independent verification of recently obtained bound-state corrections to the atomic magnetic moment. Finally, an effective interaction of a charged Dirac particle with a hydrogenic atom is given in the representation in which the atomic Hamiltonian is separable.
We present the rigorous microscopic quantum theory of the interaction of ultracold Bose and Fermi gases with the electromagnetic field of vacuum and laser photons. The main attention has been paid to the consistent consideration of dynamical dipole-dipole interactions. The theory developed is shown to be consistent with the general principles of the canonical quantization of electromagnetic field in a medium. Starting from the first principles of QED we have derived the general system of Maxwell-Bloch equations for atomic creation and annihilation operators and the propagation equation for the laser field which can be used for the self-consistent analysis of various linear and nonlinear phenomena in atom optics at high densities of the atomic system. All known equations which are used for the description of the behaviour of an ultracold atomic ensemble in a radiation field can be obtained from our general system of equations in a low-density limit.