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12:QO QThF4 Mechanical effects of the resonant dipole-dipole interaction on two trapped atoms

U. Janicke, Martin Wilkens

Published Jan 1, 1995• 0 citations
OpenAlex

Abstract

We study the mechanical impact of the emission of a photon on the center-of-mass state of two atoms in a trap. In optical diagnostics of trapped atoms, this problem is of relevance for the understanding of the back-action of photon scattering on the distribution of the atoms over the trap states. For the envisioned laser-like source of atoms (‘boser”) based on optical pumping [l], an understanding of the mechanical effects of the emitted photon is crucial as they effect strongly the small signal gain and also the atom number statistics in the “bosing” mode. For trap sizes L >> A, the resonant dipole-dipole interaction can be understood in terms of an exchange of “ballistic” photons which generally leads to heating and in 3D prevents the boser from reaching threshold [2]. For L A, the ballistic model becomes inapplicable and a refined treatment of the interaction is compulsory. We study the case of two atoms when one atom is excited initially while the other atom is in the electronic ground state. We take into account the full tensor character of the induced dipole-dipole interaction and also treat the center-of-mass motion quantum mechanically utilizing Monte-Carlo wave packet simulations [see Fig. l(left)]. We compare our findings with simplified models based on classical center-of-mass dynamics [see Fig. l(right)]. We also discuss our results with respect to the problem of small signal gain of the boser.

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We study the mechanical impact of the emission of a photon on the center-of-mass state of two atoms in a trap. In optical diagnostics of trapped atoms, this problem is of relevance for the understanding of the back-action of photon scattering on the distribution of the atoms over the trap states. For the envisioned laser-like source of atoms (‘boser”) based on optical pumping [l], an understanding of the mechanical effects of the emitted photon is crucial as they effect strongly the small signal gain and also the atom number statistics in the “bosing” mode. For trap sizes L >> A, the resonant dipole-dipole interaction can be understood in terms of an exchange of “ballistic” photons which generally leads to heating and in 3D prevents the boser from reaching threshold [2]. For L A, the ballistic model becomes inapplicable and a refined treatment of the interaction is compulsory. We study the case of two atoms when one atom is excited initially while the other atom is in the electronic ground state. We take into account the full tensor character of the induced dipole-dipole interaction and also treat the center-of-mass motion quantum mechanically utilizing Monte-Carlo wave packet simulations [see Fig. l(left)]. We compare our findings with simplified models based on classical center-of-mass dynamics [see Fig. l(right)]. We also discuss our results with respect to the problem of small signal gain of the boser.
We solve the spontaneous-emission problem for an atom coupled to a standing-wave cavity mode. The interaction between the atom and the cavity mode is treated nonperturbatively with the quantized motion of the atom along the cavity axis included. Results are presented for the spontaneous-emission spectrum and the final momentum distribution of the atom. For equal atomic and cavity linewidths analytical results are obtained using a Bloch-state basis (eigenstates of the coupled atom and cavity mode); these are compared with results calculated in the Raman-Nath approximation. The case of unequal linewidths may be solved numerically using the eigenstates of the uncoupled atom and cavity mode as a basis, or analytically by making a secular approximation in the Bloch-state basis. The distribution of final atomic momentum shows that under strong-coupling conditions the atom is diffracted by its radiation reaction field. We compare the spontaneous emission spectra with spectra calculated by treating the motion of the atom classically. Generally there is good agreement when the classical results are averaged over the quantum-mechanical uncertainty in the initial position of the atom. The agreement is lost for sufficiently strong dipole coupling or sufficiently light atoms. Then, spectra that are symmetric in the classical treatment are asymmetric in the quantum treatment due to energy exchange between the internal degrees of freedom and center-of-mass degrees of freedom of the atom.
We compute the near-resonant dipole-dipole interaction between atoms in a three-dimensional optical lattice. After a general derivation, we concentrate specifically on the case of a J=1/2\ensuremath{\rightarrow}J=3/2 off-resonant transition, in which case the excited electronic states can be adiabatically eliminated. We present in detail the spatial dependence of the resulting effective dipole-dipole potential, and discuss the physical origin of its anisotropy. In addition to impacting the center-of-mass motion of the atoms, the effective dipole-dipole potential can induce electronic transitions within one or both atoms. The symmetries of the matrix elements corresponding to these various mechanisms are also commented upon. \textcopyright{} 1996 The American Physical Society.
We investigate theoretically the mechanical effects of light on atoms trapped by an external potential, whose dipole transition couples to the mode of an optical resonator and is driven by a laser. We derive an analytical expression for the quantum center-of-mass dynamics, which is valid in presence of a tight external potential. This equation has broad validity and allows for a transparent interpretation of the individual scattering processes leading to cooling. We show that the dynamics is a competition of the mechanical effects of the cavity and of the laser photons, which may mutually interfere. We focus on the good-cavity limit and identify novel cooling schemes, which are based on quantum interference effects and lead to efficient ground-state cooling in experimentally accessible parameter regimes.
We study the near-resonant dipole-dipole interaction between two atoms in a broadband squeezed vacuum. We show that this ``vacuum'' modifies the rate of spontaneous emission of the atoms so that it may depend not merely on their relative position, as is normally the case, but also on their center-of-mass position. The explicit form of this latter dependence is a function of the way squeezing is achieved. We also show that in contrast to the spontaneous decay rate, squeezed vacua do not modify the dipole-dipole potential between the atoms as compared to its usual form. Finally, we develop a Monte Carlo wave-function description of the interaction between atoms with an arbitrary internal structure and a squeezed vacuum and apply this formalism to the case of off-resonant excitation of the atoms. We find that in addition to the usual light shift, the squeezed vacuum results in an additional contribution to the effective potential governing the evolution of the atomic ground states. \textcopyright{} 1996 The American Physical Society.
We investigate theoretically the spectrum of resonance fluorescence of a harmonically trapped atom, whose internal transitions are $\ensuremath{\Lambda}$ shaped and driven at two-photon resonance by a pair of lasers, which cool the center-of-mass motion. For this configuration, photons are scattered only due to the mechanical effects of the quantum interaction between light and atom. We study the spectrum of emission in the final stage of laser cooling, when the atomic center-of-mass dynamics is quantum mechanical and the size of the wave packet is much smaller than the laser wavelength (Lamb-Dicke limit). We use the spectral decomposition of the Liouville operator of the master equation for the atomic density matrix and apply second-order perturbation theory. We find that the spectrum of resonance fluorescence is composed of two narrow sidebands---the Stokes and anti-Stokes components of the scattered light---while all other signals are in general orders of magnitude smaller. For very low temperatures, however, the Mollow-type inelastic component of the spectrum becomes visible. This exhibits novel features which allow further insight into the quantum dynamics of the system. We provide a physical model that interprets our results and discuss how one can recover temperature and cooling rate of the atom from the spectrum. The behavior of the considered system is compared with the resonance fluorescence of a trapped atom whose internal transition consists of two levels.
We study the effects of the resonant dipole interaction between identical atoms undergoing polarization-gradient laser cooling. A generalized master equation, which includes both the atom-field interaction and the dipole-dipole interaction between atoms, is derived. We then apply this equation to the particular case of two identical atoms cooled simultaneously by a one-dimensional cooling field. We show that, as the average center-of-mass separation between the two atoms is reduced to be less than an optical wavelength \ensuremath{\lambda}/2\ensuremath{\pi}, the population of the ground motional state of the atoms begins to decrease sharply, indicating a breakdown of the cooling mechanism due to the enhanced atom-atom interaction.