Publications (45)103.7 Total impact

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ABSTRACT: Kinetic simulations of nonlinear electron plasma waves (EPW) are presented in 2D with the Vlasov code LOKI (2 space and 2 velocity dimensions; Banks et al., Phys. Plasmas 18, 052102 (2011)). Propagating EPWs are created with an external wave potential with uniform transverse amplitude. The evolution of the plasma wave field and its selfconsistent quasisteady distribution of trapped electrons is studied after the external drive is turned off. For finiteamplitude EPWs, the onset of the trappedelectroninduced filamentation instability (H. Rose, Phys. Plasmas 15, 042311 (2008)) and trapped electron sideband instability (S. Brunner and E. Valeo, PRL 93, 145003 (2004)) are studied as a function of wave amplitude and k0λDe, where k0 is the wavenumber of the external potential. We extend the theory of Kruer et al PRL 23, 1969 to 2D to find growth rates of both instabilities and compare these to the ones obtained from the simulations. In the nonlinear state, the distribution of resonant electrons is dramatically modified 
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ABSTRACT: We present results on the kinetic filamentation of finitewidth nonlinear electron plasma waves (EPW). Using 2D simulations with the PIC code BEPS, we excite a traveling EPW with a Gaussian transverse profile and a wavenumber k0λDe= 1/3. The transverse wavenumber spectrum broadens during transverse EPW localization for small width (but sufficiently large amplitude) waves, while the spectrum narrows to a dominant k as the initial EPW width increases to the planewave limit. For large EPW widths, filaments can grow and destroy the wave coherence before transverse localization destroys the wave; the filaments in turn evolve individually as selffocusing EPWs. Additionally, a transverse electric field develops that affects trapped electrons, and a beamlike distribution of untrapped electrons develops between filaments and on the sides of a localizing EPW. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DEAC5207NA27344 and funded by the Laboratory Research and Development Program at LLNL under project tracking code 12ERD061. Supported also under Grants DEFG5209NA29552 and NSFPhy0904039. Simulations were performed on UCLA's Hoffman2 and NERSC's Hopper. 
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ABSTRACT: Twodimensional Vlasov simulations of nonlinear electron plasma waves are presented, in which the interplay of linear and nonlinear kinetic effects is evident. The plasma wave is created with an external traveling wave potential with a transverse envelope of width Delta y such that thermal electrons transit the wave in a "sideloss" time, t(sl) similar to Delta(y)/v(e). Here, v(e) is the electron thermal velocity. The quasisteady distribution of trapped electrons and its selfconsistent plasma wave are studied after the external field is turned off. In cases of particular interest, the bounce frequency, omega(be) = k root e phi/m(e), satisfies the trapping condition omega(be)t(sl) > 2 pi such that the wave frequency is nonlinearly downshifted by an amount proportional to the number of trapped electrons. Here, k is the wavenumber of the plasma wave and phi is its electric potential. For sufficiently short times, the magnitude of the negative frequency shift is a local function of phi. Because the trapping frequency shift is negative, the phase of the wave on axis lags the offaxis phase if the trapping nonlinearity dominates linear wave diffraction. In this case, the phasefronts are curved in a focusing sense. In the opposite limit, the phasefronts are curved in a defocusing sense. Analysis and simulations in which the wave amplitude and transverse width are varied establish criteria for the development of each type of wavefront. The damping and trappedelectroninduced focusing of the finiteamplitude electron plasma wave are also simulated. The damping rate of the field energy of the wave is found to be about the sideloss rate, v(e) similar to t(sl)(1). For large wave amplitudes or widths Delta y, a trappinginduced selffocusing of the wave is demonstrated. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3577784]Physics of Plasmas 12/2011; 18:052102. DOI:10.1063/1.3577784 · 2.25 Impact Factor 
Article: TimeStep Considerations in Particle Simulation Algorithms for Coulomb Collisions in Plasmas
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ABSTRACT: The accuracy of firstorder Euler and higherorder timeintegration algorithms for gridbased Langevin equations collision models in a specific relaxation test problem is assessed. We show that statistical noise errors can overshadow timestep errors and argue that statistical noise errors can be conflated with timestep effects. Using a higherorder integration scheme may not achieve any benefit in accuracy for examples of practical interest. We also investigate the collisional relaxation of an initial electronion relative drift and the collisional relaxation to a resistive steadystate in which a quasisteady current is driven by a constant applied electric field, as functions of the time step used to resolve the collision processes using binary and gridbased, testparticle Langevin equations models. We compare results from two gridbased Langevin equations collision algorithms to results from a binary collision algorithm for modeling electronion collisions. Some guidance is provided on how large a time step can be used compared to the inverse of the characteristic collision frequency for specific relaxation processes.IEEE Transactions on Plasma Science 10/2010; DOI:10.1109/TPS.2010.2049589 · 0.95 Impact Factor 
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ABSTRACT: This paper shows work at Lawrence Livermore National Lab (LLNL) devoted to modeling the propagation of, and heating by, a relativistic electron beam in a idealized dense fuel assembly for fast ignition [1]. The implicit particleincell (PIC) code LSP is used. Experiments planned on the National Ignition Facility (NIF) in the next few years using the Advanced Radiography Capability (ARC) shortpulse laser motivate this work. We demonstrate significant improvement in the heating of dense fuel due to magnetic forces, increased beam collimation, and insertion of a finiteradius carbon region between the beam excitation and fuel regions.Journal of Physics Conference Series 09/2010; 244(2):022065. DOI:10.1088/17426596/244/2/022065 
Article: Simulation of laser–plasma interactions and fastelectron transport in inhomogeneous plasma
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ABSTRACT: A new framework is introduced for kinetic simulation of laser–plasma interactions in an inhomogeneous plasma motivated by the goal of performing integrated kinetic simulations of fastignition laser fusion. The algorithm addresses the propagation and absorption of an intense electromagnetic wave in an ionized plasma leading to the generation and transport of an energetic electron component. The energetic electrons propagate farther into the plasma to much higher densities where Coulomb collisions become important. The highdensity plasma supports an energetic electron current, return currents, selfconsistent electric fields associated with maintaining quasineutrality, and selfconsistent magnetic fields due to the currents. Collisions of the electrons and ions are calculated accurately to track the energetic electrons and model their interactions with the background plasma. Up to a density well above critical density, where the laser electromagnetic field is evanescent, Maxwell’s equations are solved with a conventional particlebased, finitedifference scheme. In the higherdensity plasma, Maxwell’s equations are solved using an Ohm’s law neglecting the inertia of the background electrons with the option of omitting the displacement current in Ampere’s law. Particle equations of motion with binary collisions are solved for all electrons and ions throughout the system using weighted particles to resolve the density gradient efficiently. The algorithm is analyzed and demonstrated in simulation examples. The simulation scheme introduced here achieves significantly improved efficiencies.Journal of Computational Physics 06/2010; DOI:10.1016/j.jcp.2010.03.001 · 2.49 Impact Factor 
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ABSTRACT: We present new results on the physics of shortpulse lasermatter interaction of kilojoulepicosecond pulses at full spatial and temporal scale using a new approach that combines a threedimensional collisional electromagnetic particleincell code with a magnetohydrodynamichybrid model of highdensity plasma. In the latter, collisions damp out plasma waves, and an Ohm’s law with electron inertia effects neglected determines the electric field. In addition to yielding orders of magnitude in speedup while avoiding numerical instabilities, this allows us to model the whole problem in a single unified framework: the laserplasma interaction at subcritical densities, energy deposition at relativistic critical densities, and fast electron transport in solid densities. Key questions such as the multipicosecond temporal evolution of the laser energy conversion into hot electrons, the impact of return currents on the laserplasma interaction, and the effect of selfgenerated electric and magnetic fields on electron transport will be addressed. We will report applications to current experiments.Physics of Plasmas 03/2010; 17(5):0567020567026. DOI:10.1063/1.3312825 · 2.25 Impact Factor 

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ABSTRACT: An investigation of the possible inflation of stimulated Brillouin backscattering (SBS) due to ion kinetic effects is presented using electromagnetic particle simulations and integrations of threewave coupledmode equations with linear and nonlinear models of the nonlinear ion physics. Electrostatic simulations of linear ion Landau damping in an ion acoustic wave, nonlinear reduction of damping due to ion trapping, and nonlinear frequency shifts due to ion trapping establish a baseline for modeling the electromagnetic SBS simulations. Systematic scans of the laser intensity have been undertaken with both onedimensional particle simulations and coupledmodeequations integrations, and two values of the electrontoion temperature ratio (to vary the linear ion Landau damping) are considered. Three of the four intensity scans have evidence of SBS inflation as determined by observing more reflectivity in the particle simulations than in the corresponding threewave modecoupling integrations with a linear ionwave model, and the particle simulations show evidence of ion trapping. Comment: 56 pages, 20 figuresPhysics of Plasmas 06/2007; 14(10). DOI:10.1063/1.2784449 · 2.25 Impact Factor 
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ABSTRACT: A first set of shock timing, laserplasma interaction, hohlraum energetics and hydrodynamic experiments have been performed using the first 4beams of the National Ignition Facility (NIF), in support of indirect drive Inertial Confinement Fusion (ICF) and High Energy Density Physics (HEDP). In parallel, a robust set of optical and Xray spectrometers, interferometer, calorimeters and imagers have been activated. The experiments have been undertaken with laser powers and energies of up to 8TW and 17kJ in flattop and shaped 1–9ns pulses focused with various beam smoothing options. The experiments have demonstrated excellent agreement between measured and predicted lasertarget coupling in foils and hohlraums, even when extended to a longer pulse regime unattainable at previous laser facilities, validated the predicted effects of beam smoothing on intense laser beam propagation in long scalelength plasmas and begun to test 3Dcodes by extending the study of laser driven hydrodynamic jets to 3Dgeometries.The European Physical Journal D 01/2007; 44(2):273281. DOI:10.1140/epjd/e2006001116 · 1.40 Impact Factor 
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ABSTRACT: Twodimensional simulations with the BZOHAR [B. I. Cohen, B. F. Lasinski, A. B. Langdon, and E. A. Williams, Phys. Plasmas 4, 956 (1997)] hybrid code (kinetic particle ions and Boltzmann fluid electrons) have been used to investigate the saturation of stimulated Brillouin backscatter (SBBS) instability, including the effects of ionion collisions and inhomogeneity. Two types of Langevinoperator, ionion collision models were implemented in the simulations. In both models the collisions are functions of the local ion temperature and density, but the collisions have no velocity dependence in the first model. In the second model the collisions are also functions of the energy of the ion that is being scattered so as to represent a more physical FokkerPlanck collision operator. Collisions decorrelate the ions from the acoustic waves in SBS, which disrupts ion trapping in the acoustic wave. Nevertheless, ion trapping leading to a hot ion tail and twodimensional physics that allows the SBS ion waves to nonlinearly scatter, remain important saturation mechanisms for SBBS in a highgain limit over a range of ion collisionality. Ionion collisions tend to increase ionwave dissipation, which decreases the gain exponent for stimulated Brillouin backscattering; and the peak Brillouin backscatter reflectivities decrease with increasing collisionality in the simulations for velocityindependent collisions and very weakly decrease for the range of FokkerPlanck collisionality considered. SBS backscatter in the presence of a spatially nonuniform plasma flow is also investigated. Simulations show that, depending on the sign of the spatial gradient of the flow relative to the backscatter, ion trapping effects that produce a nonlinear frequency shift can enhance (autoresonance) reflectivities relative to antiautoresonant configurations, in agreement with theoretical arguments.Physics of Plasmas 02/2006; 13(2):02270502270516. DOI:10.1063/1.2168405 · 2.25 Impact Factor 
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ABSTRACT: Experiments show that power is transferred between two copropagating 351 nm laser beams crossing in an Al plasma when the frequency of the driven ion wave is shifted by a Mach 1 flow. The resonant amplification of a lowintensity ( ⩽ 2.5×1014 W/cm2) beam intersected by a highintensity (7.0×1014 W/cm2) pump beam is determined by comparing the transmitted beam power to that measured in experiments where the plasma flow direction is reversed and the ion wave is evidently detuned. The polarization of the amplified light is also observed to align to the pump polarization consistent with ionwave scattering. The amplification is found to reduce with probebeam intensity demonstrating a nonlinear saturation mechanism that is effective when the ionwave damping is weak, which is modeled with a calculation including both the nonlinear ionwave frequency shifts due to ion trapping and wholebeam pump depletion.Physics of Plasmas 11/2005; 12(11):1127011127016. DOI:10.1063/1.2124508 · 2.25 Impact Factor 
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ABSTRACT: The first experiments on the National Ignition Facility (NIF) have employed the first four beams to measure propagation and laser backscattering losses in large ignitionsize plasmas. Gasfilled targets between 2 and 7 mm length have been heated from one side by overlapping the focal spots of the four beams from one quad operated at 351 nm (3ω) with a total intensity of 2 × 1015 W cm−2. The targets were filled with 1 atm of CO2 producing up to 7 mm long homogeneously heated plasmas with densities of ne = 6 × 1020 cm−3 and temperatures of Te = 2 keV. The high energy in an NIF quad of beams of 16 kJ, illuminating the target from one direction, creates unique conditions for the study of laser–plasma interactions at scale lengths not previously accessible. The propagation through the largescale plasma was measured with a gated xray imager that was filtered for 3.5 keV xrays. These data indicate that the beams interact with the full length of this ignitionscale plasma during the last ~1 ns of the experiment. During that time, the full aperture measurements of the stimulated Brillouin scattering and stimulated Raman scattering show scattering into the four focusing lenses of 3% for the smallest length (~2 mm), increasing to 10–12% for ~7 mm. These results demonstrate the NIF experimental capabilities and further provide a benchmark for threedimensional modelling of the laser–plasma interactions at ignitionsize scale lengths.Nuclear Fusion 11/2004; 44(12):S185. DOI:10.1088/00295515/44/12/S08 · 3.24 Impact Factor 
Article: Saturation of Stimulated Brillouin Backscattering in Twodimensional Kinetic Ion Simulations
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ABSTRACT: Twodimensional (2D) simulations with the BZOHAR[1] hybrid code (kinetic PIC ions and Boltzmann fluid electrons)are used to study saturation of stimulated Brillouin backscatter (SBBS). The simulations give a firstprinciples description of SBBS nonlinearities: ion wave breaking and trapping (and the nonlinear frequency shift and relaxation of the collisionless dissipation), twoionwavedecay instability, harmonic generation, and pump depletion.[1] The simulations address the affects of these nonlinearities on SBBS as a function of ZTe/Ti for a single ion species. Laser transverse nonuniformity, the spatially nonuniform detuning of the SBBS ion wave due to ion trapping[2], and ponderomotive filamentation have influence. Peak SBBS reflectivities in 2D are less than in 1D. High 2D reflectivities and ion wave amplitudes relax to small values in times corresponding to less than 40 ps in experimentally relevant conditions, while in 1D with the same parameters high reflectivities and ion wave amplitudes are sustained for longer times. Ion wave dissipation is higher in 2D. [1] B.I. Cohen, et al., Phys. Plas. 4, 956 (1997). [2] L. Divol, et al., Phys. Plas. 10, 1822 (2003).Physics of Plasmas 10/2004; 1(5):1076P. DOI:10.1063/1.1878792 · 2.25 Impact Factor 
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ABSTRACT: We present the first direct experimental observation of the parametric twoion decay instability of ionacoustic waves driven by a high intensity (5 x 10(15) W cm(2)) laser beam in a laser produced highZ plasma. Using two separate Thomson scattering diagnostics simultaneously, we directly measure the scattering from thermal ionacoustic fluctuations, the primary ion waves that are driven to large amplitudes by the high intensity beam, and the twoion decay products. The decay products are shown to be present only where the interaction takes place and their k spectrum is broad.Physical Review Letters 08/2004; 93(4):045004. DOI:10.1103/PhysRevLett.93.045004 · 7.73 Impact Factor 
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ABSTRACT: A new electromagnetic kinetic electron δf particle simulation model has been demonstrated to work well at large values of plasma β times the iontoelectron mass ratio [Y. Chen and S. E. Parker, J. Comput. Phys. 198, 463 (2003)]. The simulation is threedimensional using toroidal fluxtube geometry and includes electronion collisions. The model shows accurate shear Alfvén wave damping and microtearing physics. Zonal flows with kinetic electrons are found to be turbulent with the spectrum peaking at zero and having a width in the frequency range of the driving turbulence. This is in contrast with adiabatic electron cases where the zonal flows are near stationary, even though the linear behavior of the zonal flow is not significantly affected by kinetic electrons. Zonal fields are found to be very weak, consistent with theoretical predictions for β below the kinetic ballooning limit. Detailed spectral analysis of the turbulence data is presented in the various limits. © 2004 American Institute of Physics.Physics of Plasmas 04/2004; 11(5):25942599. DOI:10.1063/1.1689668 · 2.25 Impact Factor 
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ABSTRACT: A new electromagnetic kinetic electron simulation model that uses a generalized splitweight scheme, where the adiabatic part is adjustable, along with a parallel canonical momentum formulation has been developed in threedimensional toroidal fluxtube geometry. This model includes electron–ion collisional effects and has been linearly benchmarked. It is found that for Hmode parameters, the nonadiabatic effects of kinetic electrons increase linear growth rates of the iontemperaturegradientdriven (ITG) modes, mainly due to trappedelectron drive. The ion heat transport is also increased from that obtained with adiabatic electrons. The linear behaviour of the zonal flow is not significantly affected by kinetic electrons. The ion heat transport decreases to below the adiabatic electron level when finite plasma β is included due to finiteβ stabilization of the ITG modes. This work is being carried out using the 'Summit Framework'.Nuclear Fusion 09/2003; 43(10):1121. DOI:10.1088/00295515/43/10/013 · 3.24 Impact Factor 
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ABSTRACT: The nonlinear saturation of stimulated Brillouin scattering (SBS) in long beryllium plasmas (500 μm) and for long time (500 ps) is studied in detail through welldiagnosed onedimensional (1D) hybrid particleincell (PIC) simulations done using BZOHAR [B. I. Cohen, B. F. Lasinski, A. B. Langdon, and E. A. Williams, Phys. Plasmas 4, 956 (1997)]. Under conditions of interest, when the linear gain associated with the SBS growth is large, it is shown that following a first phase of large and bursty SBS reflectivity, SBS is suppressed by a selfinduced spatial detuning due to inhomogeneous modifications of the (locally averaged) ion distribution function. This nonlinear evolution was observed over a range of laser intensities and plasma parameters. © 2003 American Institute of Physics.Physics of Plasmas 08/2003; 10(9):37283732. DOI:10.1063/1.1601223 · 2.25 Impact Factor 
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ABSTRACT: Thomson scattering has been used to measure the time resolved spectrum of ion wave decay products from two instabilities which can limit the growth of stimulated Raman scattering (SRS). This experiment detected ion wave decay products far above the thermal level and demonstrates that SRS produced Langmuir waves undergo the Langmuir decay instability in ignition relevant plasmas. Product waves of the electromagnetic decay instability were not detected. © 2003 American Institute of Physics.Physics of Plasmas 07/2003; 10(8):34223425. DOI:10.1063/1.1590317 · 2.25 Impact Factor 
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ABSTRACT: An experimental study of the stimulated Brillouin scattering (SBS) instability has investigated the effects of velocity gradients and kinetic effects on the saturation of ionacoustic waves in a plasma. For intensities less than I<1.5×1015 W cm−2, SBS is in a linear regime and is moderated primarily by velocity gradients, while for intensities above this threshold, nonlinear trapping is relevant. Direct evidence of detuning of SBS by a velocity gradient was achieved by directly measuring the frequency of the SBSdriven acoustic wave relative to the local resonant acoustic frequency. The frequency and amplitude of the ionacoustic wave directly responsible for SBS has been measured as a function of space using a 3ω 200 ps Thomsonscattering probe beam. Furthermore, direct evidence of kinetic effects associated with the SBS process in the nonlinear regime has been investigated through a novel use of Thomson scattering. Specifically, a measured twofold increase in the ion temperature has been linked with ionacoustic waves that have been driven to large amplitudes by the SBS instability. Ionacoustic waves were excited to large amplitude with a 2ω 1.2nslong interaction beam with intensities up to 7×1015 W cm−2. The measured twofold increase in the ion temperature and its correlation with SBS reflectivity measurements provides quantitative evidence of hot ions created by ion trapping in laser plasmas. These detailed and accurate measurements in wellcharacterized plasma conditions allow a direct test of linear and nonlinear models of the saturation of SBS. © 2003 American Institute of Physics.Physics of Plasmas 04/2003; 10(5):18461853. DOI:10.1063/1.1542887 · 2.25 Impact Factor
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672  Citations  
103.70  Total Impact Points  
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1995–2011

Lawrence Livermore National Laboratory
 Physics Division
Livermore, California, United States
