ATI as a source for multiply charged ion production in a laser fieldA theory for the many-electron multi-photon process is presented. It is shown that after single-electron excitation into some level in the continuum (ATI) an inelastic collision of the excited…M. Yu. Kuchiev·Jan 17, 1996SaveLearn
Adiabatic mechanism of the multiply charged ion production by a laser field through ATI states of an atomATI can be followed by an inelastic collision of the ionized electron with the parent atomic particle resulting in an excitation of the ion. It may be a continuum state excitation producing the…M. Yu. Kuchiev·Jan 17, 1996SaveLearn
Motion Tomography of a single trapped ionA method for the experimental reconstruction of the quantum state of motion for a single trapped ion is proposed. It is based on the measurement of the ground state population of the trap after a…J. F. Poyatos, R. Walser, J. I. Cirac et al.·Jan 8, 1996SaveLearn
Conditional Hamiltonian and Reset Operator in the Quantum Jump ApproachFor the time development of a single system in the quantum jump approach or for quantum trajectories one requires the conditional (reduced) Hamiltonian between jumps and the reset operator after a…Gerhard C. Hegerfeldt, Dirk G. Sondermann·Dec 11, 1995SaveLearn
Coulomb Energy Averaged over the nN-Atomic States with a Definite SpinA purely group-theoretical approach (for which the symmetric group plays a central rôle), based upon the use of properties of fractional-parentage coefficients and isoscalar factors, is developed for…M. Kibler, Yu. F. Smirnov·Dec 4, 1995SaveLearn
The Periodic Table in FlatlandThe D-dimensional Coulomb system serves as a starting point for generating generalized atomic shells. These shells are ordered according to a generalized Madelung rule in D dimensions. This rule…T. Negadi, M. Kibler·Dec 2, 1995SaveLearn
Two-Photon Spectroscopy Between States of Opposite ParitiesMagnetic- and electric-dipole two-photon absorption (MED-TPA), recently introduced as a new spectroscopic technique for studying transitions between states of opposite parities, is investigated from…M. Daoud, M. Kibler·Nov 29, 1995SaveLearn
On the Use of Quantum Algebras in Rotation-Vibration SpectroscopyA two-parameter deformation of the Lie algebra u2 is used, in conjunction with the rotor system and the oscillator system, to generate a model for rotation-vibration spectroscopy of molecules and…R. Barbier, M. Kibler·Nov 13, 1995SaveLearn
Introduction to light forces, atom cooling, and atom trappingThis paper introduces and reviews light forces, atom cooling and atom trapping. The emphasis is on the physics of the basic processes. In discussing conservative forces the semi-classical dressed…Craig Savage·Oct 18, 1995SaveLearn
Band Gaps for Atoms in Light based WaveguidesThe energy spectrum for a system of atoms in a periodic potential can exhibit a gap in the band structure. We describe a system in which a laser is used to produce a mechanical potential for the…J. J. Hope, C. M. Savage·Oct 10, 1995SaveLearn
Quantum uncertainties in coupled harmonic oscillatorIn this paper we analyze the quantum uncertainties and the photon statistics in the interaction between the two modes of radiation by treating them as coupled harmonic oscillator with the motivation…Abir Bandyopadhyay, Jagdish Rai·Oct 5, 1995SaveLearn
Quantum state diffusion with a moving basis: computing quantum-optical spectraQuantum state diffusion (QSD) as a tool to solve quantum-optical master equations by stochastic simulation can be made several orders of magnitude more efficient if states in Hilbert space are…R. Schack, T. A. Brun, I. C. Percival·Oct 3, 1995SaveLearn
Electron impact excitation cross sections for allowed transitions in atomsWe present a semiempirical Gaunt factor for widely used Van Regemorter formula [Astrophys. J. 136, 906 (1962)] for the case of allowed transitions in atoms with the LS coupling scheme. Cross sections…V. Fisher, V. Bernshtam, H. Golten et al.·Sep 28, 1995SaveLearn
Squeezing in the interaction of radiation with two-level atomsWe propose a simple experimental procedure to produce squeezing and other non-classical properties like photon antibunching of radiation, and amplification without population inversion. The method…Abir Bandyopadhyay, Jagdish Rai·Sep 25, 1995SaveLearn
Hyperspherical Close-Coupling Calculation of D-wave Positronium Formation and Excitation Cross Sections in Positron-Hydrogen ScatteringHyperspherical close-coupling method is used to calculate the elastic, positronium formation and excitation cross sections for positron collisions with atomic hydrogen at energies below the H(n=4)…Yan Zhou, C. D. Lin·Sep 22, 1995SaveLearn
Nuclear spin--rotation interaction in the hydrogen molecular ionThe nuclear spin--rotation interaction in the hyperfine structure of the hydrogen molecular ion is investigated. The interaction constants are determined and are found to differ in sign and magnitude…James F. Babb·Sep 20, 1995SaveLearn
Conventional Quantum Chemical Correlation Energy versus Density-Functional Correlation EnergyWe analyze the difference between the correlation energy as defined within the conventional quantum chemistry framework and its namesake in density-functional theory. Both quantities are rigorously…E. K. U. Gross, M. Petersilka, T. Grabo·Sep 19, 1995SaveLearn
2-2 and 2-3 Intercombination Transitions in Be-like IonsWe report here on calculation of probabilities of intercombination transitions 2s2 1S0 - 2s2p 3P1, 2s3p 3P1 for Be-like ions along the isoelectronic sequence for large range of…Yu. V. Ralchenko, L. A. Vainshtein·Sep 16, 1995SaveLearn