Publications (313)1111.28 Total impact
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ABSTRACT: We calculate the dielectric response of crystalline silicon following irradiation by a highintensity laser pulse, modeling the dynamics by the timedependent KohnSham equations in the presence of the laser field. Pumpprobe measurements of the response are numerically simulated by including both pump and probe externals fields in the simulation. As expected, the excited silicon shows features of an electronhole plasma of nonequilibrium phase in its response, characterized by a negative divergence in the real part of the dielectric function at small frequencies. The response to the probe pulse depends on the polarization of the pump pulse. We also find that the imaginary part of the dielectric function can be negative, particularly for the parallel polarization of pump and probe fields. We compare the calculated response with a simple Drude model. The real part of the dielectric function is well fitted by the model, treating the effective mass as a fitting parameter while taking electron density from the calculation. The fitted effective masses are consistent with carrierband dispersions.01/2014; 89(6).  [Show abstract] [Hide abstract]
ABSTRACT: Levels densities of independentparticle Hamiltonians can be calculated easily by using the realtime representation of the evolution operator together with the fast Fourier transform. We describe the method and implement it with a set of Python programs. Examples are provided for the total and partial levels densities of a heavy deformed nucleus (Dy164). The partial level densities that may be calculated are the projected ones on neutron number, proton number, azimuthal angular momentum, and parity.Computer Physics Communications. 01/2014;  [Show abstract] [Hide abstract]
ABSTRACT: The GallagherMoszkowski rule in the spectroscopy of oddodd nuclei imposes a new spin constraint on the energy functionals for selfconsistent mean field theory. The commonly used parameterization of the effective threebody interaction in the Gogny and Skyrme families of energy functionals is illsuited to satisfy the spin constraint. In particular, the Gogny parameterization of the threebody interaction has the opposite spin dependence to that required by the observed spectra. The twobody part has a correct sign, but in combination the rule is violated as often as not. We conclude that a new functional form is needed for the effective threebody interaction that can take into better account the different spinisospin channels of the interaction.10/2013; 89(2). 
Dataset: JChemPhys.134.144106

Dataset: JChemPhys.134.144106
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ABSTRACT: We have been developing a theoretical framework to describe electron dynamics in a crystalline solid under an ultrashort laser pulse. We rely upon the timedependent density functional theory, solving the timedependent KohnSham equation in realtime and realspace. Using our method, it is possible to describe both linear and nonlinear lightmatter interactions in a unified way. In my presentation, I will focus on the application to coherent phonon generation, a coherent atomic oscillation over a macroscopic volume. I will show applications to two material, semiconductor Si and semimetal Sb. For Si, we have found that the TDDFT is capable of describe two distinct mechanisms of the coherent phonon generation. When the laser frequency is below the direct bandgap, virtual electronic excitation induces impulsive force to atoms. When the laser frequency is above the gap, real electronic excitation causes the atomic motion. For Sb, we study the frequency dependence of the coherent phonon generation and compare our results with phenomenological theories.03/2013; 
Article: Erratum: "Nonadiabatic generation of coherent phonons" [J. Chem. Phys. 137, 22A527 (2012)].
The Journal of Chemical Physics 01/2013; 138(2):029903. · 3.12 Impact Factor 
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ABSTRACT: As part of a program to study oddA nuclei in the HartreeFockBogoliubov (HFB) theory, we have developed a new calculational tool to find the HFB minima of oddA nuclei based on the gradient method and using interactions of Gogny's form. The HFB minimization includes both timeeven and timeodd fields in the energy functional, avoiding the commonly used "filling approximation". Here we apply the method to calculate neutron pairing gaps in some representative isotope chains of spherical and deformed nuclei, namely the Z=8,50 and 82 spherical chains and the Z=62 and 92 deformed chains. We find that the gradient method is quite robust, permitting us to carry out systematic surveys involving many nuclei. We find that the timeodd field does not have large effect on the pairing gaps calculated with the Gogny D1S interaction. Typically, adding the Todd field as a perturbation increases the pairing gap by ~100 keV, but the reminimization brings the gap back down. This outcome is very similar to results reported for the Skyrme family of nuclear energy density functionals. Comparing the calculated gaps with the experimental ones, we find that the theoretical errors have both signs implying that the D1S interaction has a reasonable overall strength. However, we find some systematic deficiencies comparing spherical and deformed chains and comparing the lighter chains with the heavier ones. The gaps for heavy spherical nuclei are too high, while those for deformed nuclei tend to be too low. The calculated gaps of spherical nuclei show hardly any Adependence, contrary to the data. Inclusion of the Todd component of the interaction does not change these qualitative findings.Physical Review C 10/2012; 86(6). · 3.72 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: The timedependent density functional theory (TDDFT) is the leading computationally feasible theory to treat excitations by strong electromagnetic fields. Here the theory is applied to coherent optical phonon generation produced by intense laser pulses. We examine the process in the crystalline semimetal antimony (Sb), where nonadiabatic coupling is very important. This material is of particular interest because it exhibits strong phonon coupling and optical phonons of different symmetries can be observed. The TDDFT is able to account for a number of qualitative features of the observed coherent phonons, despite its unsatisfactory performance on reproducing the observed dielectric functions of Sb. A simple dielectric model for nonadiabatic coherent phonon generation is also examined and compared with the TDDFT calculations.The Journal of Chemical Physics 08/2012; 137(22):22A527. · 3.12 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: Spectroscopic observables such as electromagnetic transitions strengths can be related to the properties of the intrinsic meanfield wave function when the latter are strongly deformed, but the standard rotational formulas break down when the deformation decreases. Nevertheless there is a welldefined, nonzero, spherical limit that can be evaluated in terms of overlaps of meanfield intrinsic deformed wave functions. We examine the transition between the spherical limit and strongly deformed one for a range of nuclei comparing the two limiting formulas with exact projection results. We find a simple criterion for the validity of the rotational formula depending on $<\Delta \vec{J}^2>$, the mean square fluctuation in the angular momentum of the intrinsic state. We also propose an interpolation formula which describes the transition strengths over the entire range of deformations, reducing to the two simple expressions in the appropriate limits.Physical Review C 06/2012; 86(5). · 3.72 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: The HartreeFockBogoliubov approximation is very useful for treating both long and shortrange correlations in finite quantum fermion systems, but it must be extended in order to describe detailed spectroscopic properties. One problem is the symmetrybreaking character of the HFB approximation. We present a general and systematic way to restore symmetries and to extend the configuration space using pfaffian formulas for the manybody matrix elements. The advantage of those formulas is that the sign of the matrix elements is unambiguously determined. It is also helpful to extend the space of configurations by constraining the HFB solutions in some way. A powerful method for finding these constrained solutions is the gradient method, based on the generalized Thouless transformation. The gradient method also preserves the number parity of the Bogoliubov transformation, which facilitates the application of the theory to systems with odd particle number.05/2012;  [Show abstract] [Hide abstract]
ABSTRACT: We show that longrange correlations for nuclear masses have a significant effect on the synthesis of heavy elements by the r process. As calculated by Delaroche et al. [Phys. Rev. C 81, 014303 (2010)], these correlations suppress magic number effects associated with minor shells. This impacts the calculated abundances before the third rprocess peak (at mass number A≈195), where the abundances are low and form a trough. This trough and the position of the third abundance peak are strongly affected by the masses of nuclei in the transition region between deformed and spherical. Based on different astrophysical environments, our results demonstrate that a microscopic theory of nuclear masses including correlations naturally smoothens the separation energies, thus reducing the trough and improving the agreement with observed solar system abundances.Physical Review Letters 04/2012; 108(15):151101. · 7.73 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: I review the phenomena associated with pairing in nuclear physics, most prominently the ubiquitous presence of oddeven mass differences and the properties of the excitation spectra, very different for eveneven and oddA nuclei. There are also significant dynamical effects of pairing, visible in the inertias associated with nuclear rotation and largeamplitude shape deformation.03/2012;  [Show abstract] [Hide abstract]
ABSTRACT: We analyze the effect of pairing on particle transport in timedependent theories based on the HartreeFockBogoliubov (HFB) or BCS approximations. The equations of motion for the HFB density matrices are unique and the theory respects the usual conservation laws defined by commutators of the conserved quantity with the Hamiltonian. In contrast, the theories based on the BCS approximation are more problematic. In the usual formulation of TDHF+BCS, the equation of continuity is violated and one sees unphysical oscillations in particle densities. This can be ameliorated by freezing the occupation numbers during the evolution in TDHF+BCS, but there are other problems with the BCS that make it doubtful for reaction dynamics. We also compare different numerical implementations of the timedependent HFB equations. The equations of motion for the $U$ and $V$ Bogoliubov transformations are not unique, but it appears that the usual formulation is also the most efficient. Finally, we compare the timedependent HFB solutions with numerically exact solutions of the twoparticle Schrodinger equation. Depending on the treatment of the initial state, the HFB dynamics produces a particle emission rate at short times similar to that of the Schrodinger equation. At long times, the total particle emission can be quite different, due to inherent meanfield approximation of the HFB theory.Physical Review C 02/2012; 85(3). · 3.72 Impact Factor 
Article: Timedependent density functional theory for strong electromagnetic fields in crystalline solids
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ABSTRACT: We apply the coupled dynamics of timedependent density functional theory and Maxwell equations to the interaction of intense laser pulses with crystalline silicon. As a function of electromagnetic field intensity, we see several regions in the response. At the lowest intensities, the pulse is reflected and transmitted in accord with the dielectric response, and the characteristics of the energy deposition are consistent with twophoton absorption. The absorption process begins to deviate from that at laser intensities of ∼1013 W/cm2, where the energy deposited is of the order of 1 eV per atom. Changes in the reflectivity are seen as a function of intensity. When it passes a threshold of about 3×1012 W/cm2, there is a small decrease. At higher intensities, above 2×1013 W/cm2, the reflectivity increases strongly. This behavior can be understood qualitatively in a model treating the excited electronhole pairs as a plasma.Physical Review B 01/2012; 85(4):045134. · 3.66 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We present a Pfaffian formula for projection and symmetry restoration for wave functions of the general Bogoliubov form, including quasiparticle excited states and linear combinations of them. This solves a longstanding problem in calculating states of good symmetry, arising from the sign ambiguity of the commonly used determinant formula. A simple example is given of projecting a good particle number and angular momentum from a Bogoliubov wave function in the Fock space of a single jshell.Physical Review Letters 01/2012; 108(4):042505. · 7.73 Impact Factor 
Conference Paper: Theoretical investigation for coherent phonon generation studied with firstprinciples calculation
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ABSTRACT: We investigate mechanisms of coherent phonon generation in timedependent density functional theory. It is shown that stimulated Raman and displacive excitation mechanisms are understood in a unified way.Lasers and ElectroOptics (CLEO), 2012 Conference on; 01/2012  [Show abstract] [Hide abstract]
ABSTRACT: We recently proposed a nonlocal form for the 3body induced interaction that is consistent with the Fock space representation of interaction operators but leads to a fractional power dependence on the density. Here we examine the implications of the nonlocality for the excitation spectrum. In the twocomponent weakly interacting Fermi gas, we find that it gives an effective mass that is comparable to the one in manybody perturbation theory. Applying the interaction to nuclear matter, it predicts a huge enhancement to the effective mass. Since the saturation of nuclear matter is partly due to the induced 3body interaction, fitted functionals should treat the effective mass as a free parameter, unless the 2 and 3body contributions are determined from basic theory.Physical Review C 11/2011; 85(3). · 3.72 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We present a computational methodology for a theory of the lowest octupole excitations applicable to all eveneven nuclei beyond the lightest. The theory is the wellknown generatorcoordinate extension (GCM) of the HartreeFockBogoliubov selfconsistent mean field theory (HFB). We use the discretebasis HillWheel method (HW) to compute the wave functions with an interaction from the Gogny family of Hamiltonians. Comparing to the compiled experimental data on octupole excitations, we find that the performance of the theory depends on the deformation characteristics of the nucleus. For nondeformed nuclei, the theory reproduces the energies to about 20 % apart from an overall scale factor of about 1.6. The performance is somewhat poorer for (quadrupole) deformed nuclei, and for both together the dispersion of the scaled energies about the experimental values is about 25 %. This compares favorably with the performance of similar theories of the quadrupole excitations. Nuclei having static octupole deformations in HFB form a special category. These nuclei have the smallest measured octupole excitation energies as well as the smallest predicted energies. However, in these cases the energies are seriously underpredicted by the theory. We find that a simple twoconfiguration approximation, the Minimization After Projection method, (MAP) is almost as accurate as the full HW treatment, provided that the octupoledeformed nuclei are omitted from the comparison. This article is accompanied by a tabulation of the predicted octupole excitations for 818 nuclei extending from dripline to dripline, computed with several variants of the Gogny interaction.Physical Review C 07/2011; 84(5). · 3.72 Impact Factor
Publication Stats
11k  Citations  
1,111.28  Total Impact Points  
Top Journals
 Physical Review C (93)
 Nuclear Physics A (27)
 Physics Letters B (25)
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Institutions

1994–2014

University of Washington Seattle
 • Institute for Nuclear Theory
 • Department of Physics
Seattle, Washington, United States


2006–2013

University of Tsukuba
 Centre for Computational Sciences
Tsukuba, Ibarakiken, Japan


2012

Universität Basel
 Department of Physics
Basel, BS, Switzerland


2009

University of Alcalá
 Department of Physics and Mathematics
Alcalá de Henares, Madrid, Spain


2002

Trinity Washington University
Washington, Washington, D.C., United States


1998

Tohoku University
Japan


1973–1998

Michigan State University
 Department of Physics and Astronomy
East Lansing, MI, United States


1995

University of Everett Washington
Seattle, Washington, United States


1988

McGill University
 Department of Physics
Montréal, Quebec, Canada


1985–1986

The University of Tennessee Medical Center at Knoxville
Knoxville, Tennessee, United States 
Oak Ridge National Laboratory
 Physics Division
Oak Ridge, FL, United States 
University of Tennessee
Knoxville, Tennessee, United States 
Argonne National Laboratory
 Division of Physics
Lemont, Illinois, United States 
Joint Institute for Heavy Ion Research
Oak Ridge, Tennessee, United States


1967–1979

University of Copenhagen
 Niels Bohr Institute
Copenhagen, Capital Region, Denmark
