UV and X-ray Spectral Lines of FeXXIII Ion for Plasma DiagnosticsWe have calculated X-ray and UV spectra of Be-like Fe (FeXXIII) ion in collisional-radiative model including all fine-structure transitions among the 2s2, 2s2p, 2p2, 2snl, and 2pnl levels where n=3…Izumi Murakami, Takako Kato·May 15, 1996SaveLearn
Problems with Standard Semiclassical Stark Broadening TheoryIn this work we study in detail the NeVII 2s3p-2s3s singlet line, which was also the object of a recent experiment. The standard perturbative impact theory predictions are tested against a fully…S. Alexiou·May 10, 1996SaveLearn
Frequency Separation for Relaxation ProblemsThe modern era in spectral line broadening began with the understanding that the slow(quasistatic) ion and fast(impact) electron perturbers could be treated separately. The problem remained of…S. Alexiou·May 10, 1996SaveLearn
Ionization of the hydrogen atom in strong magnetic fields: beyond the adiabatic approximationHigh magnetic fields in neutron stars, B ~ 1011 - 1013 G, substantially modify the properties of atoms and their interaction with radiation. In particular, the photoionization cross section…A. Y. Potekhin, G. G. Pavlov, J. Ventura·May 5, 1996SaveLearn
Right-unitary transformation theory and applicationsWe develop a new transformation theory in quantum physics, where the transformation operators, defined in the infinite dimensional Hilbert space, have right-unitary inverses only. Through several…Zhong Tang·Apr 30, 1996SaveLearn
Interaction of a slow monopole with a hydrogen atomThe electric dipole moment of the hydrogen-like atom induced by a monopole moving outside the electron shell is calculated. The correction to the energy of the ground state of the hydrogen atom due…Ya. M. Shnir·Apr 29, 1996SaveLearn
Electromagnetic modes of Maxwell fisheye lensWe provide an analysis of the radial structure of TE and TM modes of the Maxwell fisheye lens, by means of Maxwell equations as applied to the fisheye case. Choosing a lens of size R = 1 cm, we plot…H. C. Rosu, M. Reyes·Apr 25, 1996SaveLearn
Limits on the monopole magnetic field from measurements of the electric dipole moments of atoms, molecules and the neutronA radial magnetic field can induce a time invariance violating electric dipole moment (EDM) in quantum systems. The EDMs of the Tl, Cs, Xe and Hg atoms and the neutron that are produced by such a…V. V. Flambaum, D. W. Murray·Apr 22, 1996SaveLearn
Evanescent wave diffraction of multi-level atomsDiffraction of multi-level atoms by an evanescent wave reflective diffraction grating is modeled by numerically solving the time-dependent Schrödinger equation. We are able to explain the diffraction…D. Gordon, C. M. Savage·Apr 19, 1996SaveLearn
Atomic Data for Permitted Resonance Lines of Atoms and Ions from H to Si, and S, Ar, Ca and FeWe list vacuum wavelengths, energy levels, statistical weights, transition probabilities and oscillator strengths for permitted resonance spectral lines of all ions of 18 astrophysically important…D. A. Verner, E. M. Verner, G. J. Ferland·Apr 10, 1996SaveLearn
An Atom Laser Based on Raman TransitionsIn this paper we present an atom laser scheme using a Raman transition for the output coupling of atoms. A beam of thermal atoms (bosons) in a metastable atomic state |1 > are pumped into a…G. M. Moy, J. J. Hope, C. M. Savage·Apr 4, 1996SaveLearn
Hall-Effect for Neutral AtomsIt is shown that polarizable neutral systems can drift in crossed magnetic and electric fileds. The drift velocity is perpendicular to both fields, but contrary to the drif t velocity of a charged…A. P. Kasantsev, A. M. Dykhne, V. L. Pokrovsky·Apr 4, 1996SaveLearn
Decoherence in Ion Trap Quantum ComputersThe intrinsic decoherence from vibrational coupling of the ions in the Cirac-Zoller quantum computer [Phys. Rev. Lett. 74, 4091 (1995)] is considered. Starting from a state in which the…Anupam Garg·Mar 29, 1996SaveLearn
Some remarks on the two-electron atomNew, approximate, two-electron wavefunctions are introduced for the two-electron atoms (cations), which account remarkably well for the ground-state energies and the lowest-excxited states (where…M. Apostol·Mar 25, 1996SaveLearn
TM-Surface Waves along the Boundary between two Nonlinear Anisotropic DielectricsIt is shown that the Maxwell's equations for surface electromagnetic TM-waves, propagating along the plane boundary between two nonlinear dielectrics with arbitrary diagonal tensor of dielectric…Yu. P. Rybakov, B. Saha·Mar 22, 1996SaveLearn
Giant Coulomb broadening and Raman lasing on ionic transitionsCW generation of anti-Stokes Raman laser on a number of blue-green argon-ion lines (4p-4s, 4p-3d) has been demonstrated with optical pumping from metastable levels 3d'2G, 3d4F. It is found,…A. A. Apolonsky, S. A. Babin, A. I. Chernykh et al.·Mar 22, 1996SaveLearn
Density Matrix Functional Calculations for Matter in Strong Magnetic Fields: I. Atomic PropertiesWe report on a numerical study of the density matrix functional introduced by Lieb, Solovej and Yngvason for the investigation of heavy atoms in high magnetic fields. This functional describes …Kristinn Johnsen, Jakob Yngvason·Mar 21, 1996SaveLearn
Interaction of Charged 3D Soliton with Coulomb CenterThe Einstein - de Broglie particle-soliton concept is applied to simulate stationary states of an electron in a hydrogen atom. According to this concept, the electron is described by the localized…Yu. P. Rybakov, B. Saha·Mar 21, 1996SaveLearn
Direct Probing of Quantum Phase Space by Photon CountingWe propose a very simple experimental setup to measure, via photon counting, the overlap of the Wigner functions characterizing two single mode light beams. We show that this scheme can be applied to…Konrad Banaszek, Krzysztof Wodkiewicz·Mar 19, 1996SaveLearn
Quantum Reservoir EngineeringWe show how to design different couplings between a single ion trapped in a harmonic potential and an environment. This will provide the basis for the experimental study of the process of decoherence…J. F. Poyatos, J. I. Cirac, P. Zoller·Mar 15, 1996SaveLearn
Ionization of hydrogen and hydrogenic ions by antiprotonsPresented here is a description of the ionization of hydrogen and hydrogenic ions by antiproton-impact, based on very large scale numerical solutions of the time-dependent Schrödinger equation in…D. R. Schultz, P. S. Krstic, C. O. Reinhold et al.·Mar 4, 1996SaveLearn
Stimulated Enhancement of Cross-Section by a Bose-Einstein CondensateThis paper examines the feasibility of constructing an experiment which detects the atomic stimulation of a photon emission process. A beam of atoms (bosons) in an excited state is passed over an…J. J. Hope, C. M. Savage·Feb 27, 1996SaveLearn
Prospects for Parity Non-conservation Experiments with Highly Charged Heavy IonsWe discuss the prospects for parity non-conservation experiments with highly charged heavy ions. Energy levels and parity mixing for heavy ions with two to five electrons are calculated. We…M. Maul, A. Schäfer, W. Greiner et al.·Feb 23, 1996SaveLearn
Atomic Data and Databases on the Internet: Entering 1996In this report the current situation with availability and management of atomic data on the Internet is reviewed.Yu. V. Ralchenko·Jan 23, 1996SaveLearn
Dynamics, correlations and phases of the micromaserThe micromaser possesses a variety of dynamical phase transitions parametrized by the flux of atoms and the time-of-flight of the atom within the cavity. We discuss how these phases may be revealed…Per Elmfors, Benny Lautrup, Bo-Sture Skagerstam·Jan 21, 1996SaveLearn