251 research outputs found
Coupled forward-backward trajectory approach for non-equilibrium electron-ion dynamics
We introduce a simple ansatz for the wavefunction of a many-body system based
on coupled forward and backward-propagating semiclassical trajectories. This
method is primarily aimed at, but not limited to, treating nonequilibrium
dynamics in electron-phonon systems. The time-evolution of the system is
obtained from the Euler-Lagrange variational principle, and we show that this
ansatz yields Ehrenfest mean field theory in the limit that the forward and
backward trajectories are orthogonal, and in the limit that they coalesce. We
investigate accuracy and performance of this method by simulating electronic
relaxation in the spin-boson model and the Holstein model. Although this method
involves only pairs of semiclassical trajectories, it shows a substantial
improvement over mean field theory, capturing quantum coherence of nuclear
dynamics as well as electron-nuclear correlations. This improvement is
particularly evident in nonadiabatic systems, where the accuracy of this
coupled trajectory method extends well beyond the perturbative electron-phonon
coupling regime. This approach thus provides an attractive route forward to the
ab-initio description of relaxation processes, such as thermalization, in
condensed phase systems
Nonlinear polarization evolution using time-dependent density functional theory
We propose a theoretical and computational approach to investigate temporal
behavior of a nonlinear polarization in perturbative regime induced by an
intense and ultrashort pulsed electric field. First-principles time-dependent
density functional theory is employed to describe the electron dynamics.
Temporal evolution of third-order nonlinear polarization is extracted from a
few calculations of electron dynamics induced by pulsed electric fields with
the same time profile but different amplitudes. We discuss characteristic
features of the nonlinear polarization evolution as well as an extraction of
nonlinear susceptibilities and time delays by fitting the polarization. We also
carry out a decomposition of temporal and spatial changes of the electron
density in power series with respect to the field amplitude. It helps to get
insight into the origin of the nonlinear polarization in atomic scale.Comment: 11 pages, 9 figure
Ab Initio Simulation of Electrical Currents Induced by Ultrafast Laser Excitation of Dielectric Materials
We theoretically investigate the generation of ultrafast currents in
insulators induced by strong few-cycle laser pulses. Ab initio simulations
based on time-dependent density functional theory give insight into the
atomic-scale properties of the induced current signifying a femtosecond-scale
insulator-metal transition. We observe the transition from nonlinear
polarization currents during the laser pulse at low intensities to
tunnelinglike excitation into the conduction band at higher laser intensities.
At high intensities, the current persists after the conclusion of the laser
pulse considered to be the precursor of the dielectric breakdown on the
femtosecond scale. We show that the transferred charge sensitively depends on
the orientation of the polarization axis relative to the crystal axis
suggesting that the induced charge separation reflects the anisotropic
electronic structure. We find good agreement with very recent experimental data
on the intensity and carrierenvelope phase dependence [A. Schiffrin et al.,
Nature (London) 493, 70 (2013)].Comment: Accepted versio
Controlling ultrafast currents by the non-linear photogalvanic effect
We theoretically investigate the effect of broken inversion symmetry on the
generation and control of ultrafast currents in a transparent dielectric (SiO2)
by strong femto-second optical laser pulses. Ab-initio simulations based on
time-dependent density functional theory predict ultrafast DC currents that can
be viewed as a non-linear photogalvanic effect. Most surprisingly, the
direction of the current undergoes a sudden reversal above a critical threshold
value of laser intensity I_c ~ 3.8*10^13 W/cm2. We trace this switching to the
transition from non-linear polarization currents to the tunneling excitation
regime. We demonstrate control of the ultrafast currents by the time delay
between two laser pulses. We find the ultrafast current control by the
non-linear photogalvanic effect to be remarkably robust and insensitive to
laser-pulse shape and carrier-envelope phase
Strain and process development for poly(3HB-co-3HP) fermentation by engineered Shimwellia blattae from glycerol
Poly(3-hydroxybytyrate-co-3-hydroxypropionate), poly(3HB-co-3HP), is a possible alternative to synthetic polymers such as polypropylene, polystyrene and polyethylene due to its low crystallinity and fragility. We already reported that recombinant strains of Shimwellia blattae expressing 1,3-propanediol dehydrogenase DhaT as well as aldehyde dehydrogenase AldD of Pseudomonas putida KT2442, propionate-CoA transferase Pct of Clostridium propionicum X2 and PHA synthase PhaC1 of Ralstonia eutropha H16 are able to accumulate up to 14.5% (wtPHA/wtCDW) of poly(3-hydroxypropionate), poly(3HP), homopolymer from glycerol as a sole carbon source (Appl Microbiol Biotechnol 98:7409-7422, 2014a). However, the cell density was rather low. In this study, we optimized the medium aiming at a more efficient PHA synthesis, and we engineered a S. blattae strain accumulating poly(3HB-co-3HP) with varying contents of the constituent 3-hydroxypropionate (3HP) depending on the cultivation conditions. Consequently, 7.12, 0.77 and 0.32 gPHA/L of poly(3HB-co-3HP) containing 2.1, 8.3 and 18.1 mol% 3HP under anaerobic/aerobic (the first 24 hours under anaerobic condition, thereafter, aerobic condition), low aeration/agitation (the minimum stirring rate required in medium mixing and small amount of aeration) and anaerobic conditions (the minimum stirring rate required in medium mixing without aeration), respectively, were synthesized from glycerol by the genetically modified S. blattae ATCC33430 strains in optimized culture medium
Local SiC photoluminescence evidence of non-mutualistic hot spot formation and sub-THz coherent emission from a rectangular BiSrCaCuO mesa
From the photoluminescence of SiC microcrystals uniformly covering a
rectangular mesa of the high transition temperature superconductor
BiSrCaCuO, the local surface temperature
was directly measured during simultaneous sub-THz emission from the
intrinsic Josephson junctions (IJJs) in the mesa. At high bias currents and
low bath temperatures K, the center of a large
elliptical hot spot with jumps dramatically with little
current-voltage characteristic changes. The hot spot doesn't alter the
ubiquitous primary and secondary emission conditions: the ac Josephson relation
and the electromagnetic cavity resonance excitation, respectively. Since the
intense sub-THz emission was observed for high K in
the low bias regime where hot spots are absent, hot spots can not provide
the primary mechanisms for increasing the output power, the tunability, or for
promoting the synchronization of the IJJs for the sub-THz emission, but can
at best coexist non-mutualistically with the emission. No standing
waves were observed
Observation of molecular dipole excitations by attosecond self-streaking
We propose a protocol to probe the ultrafast evolution and dephasing of
coherent electronic excitation in molecules in the time domain by the intrinsic
streaking field generated by the molecule itself. Coherent electronic motion in
the endohedral fullerene \Necsixty~is initiated by a moderately intense
femtosecond UV-VIS pulse leading to coherent oscillations of the molecular
dipole moment that persist after the end of the laser pulse. The resulting
time-dependent molecular near-field is probed through the momentum modulation
of photoemission from the central neon atom by a time-delayed attosecond XUV
pulse. Our ab-initio time-dependent density functional theory and classical
trajectory simulations predict that this self-streaking signal accurately
traces the molecular dipole oscillations in real time. We discuss the
underlying processes and give an analytical model that captures the essence of
our ab-initio simulations
Ab-initio multi-scale simulation of high-harmonic generation in solids
High-harmonic generation by a highly non-linear interaction of infrared laser
fields with matter allows for the generation of attosecond pulses in the XUV
spectral regime. This process, well established for atoms, has been recently
extended to the condensed phase. Remarkably well pronounced harmonics up to
order ~30 have been observed for dielectrics. We present the first ab-initio
multi-scale simulation of solid-state high-harmonic generation. We find that
mesoscopic effects of the extended system, in particular the realistic sampling
of the entire Brillouin zone, the pulse propagation in the dense medium, and
the inhomogeneous illumination of the crystal have a strong effect on the
formation of clean harmonic spectra. Our results provide a novel explanation
for the formation of clean harmonics and have implications for a wide range of
non-linear optical processes in dense media
Frequency-resolved microscopic current density analysis of linear and nonlinear optical phenomena in solids
We perform a frequency-resolved analysis of electron dynamics in solids to
obtain microscopic insight into linear and nonlinear optical phenomena. For the
analysis, we first compute the electron dynamics under optical electric fields
and evaluate the microscopic current density as a function of time and space.
Subsequently, we perform the Fourier transformation on the microscopic current
density and obtain the corresponding quantity in the frequency domain. The
frequency-resolved microscopic current density provides insight into the
microscopic electron dynamics in real-space at the frequency of linear and
nonlinear optical responses. We apply frequency-resolved microscopic current
density analysis to light-induced electron dynamics in aluminum, silicon, and
diamond based on the first-principles electron dynamics simulation according to
the time-dependent density functional theory. Consequently, the nature of
delocalized electrons in metals and bound electrons in semiconductors and
insulators is suitably captured by the developed scheme
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