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Dive into the research topics where H.-S. Park is active.

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Featured researches published by H.-S. Park.


Nature | 2014

Fuel gain exceeding unity in an inertially confined fusion implosion

O. A. Hurricane; D. A. Callahan; D. T. Casey; Peter M. Celliers; C. Cerjan; E. L. Dewald; T. R. Dittrich; T. Döppner; D. E. Hinkel; L. Berzak Hopkins; J. L. Kline; S. Le Pape; T. Ma; A. G. MacPhee; J. L. Milovich; A. Pak; H.-S. Park; P. K. Patel; B. A. Remington; J. D. Salmonson; P. T. Springer; R. Tommasini

Ignition is needed to make fusion energy a viable alternative energy source, but has yet to be achieved. A key step on the way to ignition is to have the energy generated through fusion reactions in an inertially confined fusion plasma exceed the amount of energy deposited into the deuterium–tritium fusion fuel and hotspot during the implosion process, resulting in a fuel gain greater than unity. Here we report the achievement of fusion fuel gains exceeding unity on the US National Ignition Facility using a ‘high-foot’ implosion method, which is a manipulation of the laser pulse shape in a way that reduces instability in the implosion. These experiments show an order-of-magnitude improvement in yield performance over past deuterium–tritium implosion experiments. We also see a significant contribution to the yield from α-particle self-heating and evidence for the ‘bootstrapping’ required to accelerate the deuterium–tritium fusion burn to eventually ‘run away’ and ignite.


Physics of Plasmas | 2014

The high-foot implosion campaign on the National Ignition Facilitya)

O. A. Hurricane; D. A. Callahan; D. T. Casey; E. L. Dewald; T. R. Dittrich; T. Döppner; M. A. Barrios Garcia; D. E. Hinkel; L. Berzak Hopkins; P. Kervin; J. L. Kline; S. Le Pape; T. Ma; A. G. MacPhee; J. L. Milovich; J. D. Moody; A. Pak; P. K. Patel; H.-S. Park; B. A. Remington; H. F. Robey; J. D. Salmonson; P. T. Springer; R. Tommasini; L. R. Benedetti; J. A. Caggiano; Peter M. Celliers; C. Cerjan; Rebecca Dylla-Spears; D. H. Edgell

The “High-Foot” platform manipulates the laser pulse-shape coming from the National Ignition Facility laser to create an indirect drive 3-shock implosion that is significantly more robust against instability growth involving the ablator and also modestly reduces implosion convergence ratio. This strategy gives up on theoretical high-gain in an inertial confinement fusion implosion in order to obtain better control of the implosion and bring experimental performance in-line with calculated performance, yet keeps the absolute capsule performance relatively high. In this paper, we will cover the various experimental and theoretical motivations for the high-foot drive as well as cover the experimental results that have come out of the high-foot experimental campaign. At the time of this writing, the high-foot implosion has demonstrated record total deuterium-tritium yields (9.3×1015) with low levels of inferred mix, excellent agreement with implosion simulations, fuel energy gains exceeding unity, and evidenc...


Review of Scientific Instruments | 2012

Imaging of High-Energy X-Ray Emission from Cryogenic Thermonuclear Fuel Implosions on the NIF

T. Ma; N. Izumi; R. Tommasini; D. K. Bradley; P. M. Bell; C. Cerjan; S. N. Dixit; T. Döppner; O. S. Jones; J. L. Kline; G. A. Kyrala; O. L. Landen; S. LePape; A. J. Mackinnon; H.-S. Park; P. K. Patel; R. Prasad; J. E. Ralph; S. P. Regan; V. A. Smalyuk; P. T. Springer; L. J. Suter; R. P. J. Town; S. V. Weber; S. H. Glenzer

Accurately assessing and optimizing the implosion performance of inertial confinement fusion capsules is a crucial step to achieving ignition on the NIF. We have applied differential filtering (matched Ross filter pairs) to provide broadband time-integrated absolute x-ray self-emission images of the imploded core of cryogenic layered implosions. This diagnostic measures the temperature- and density-sensitive bremsstrahlung emission and provides estimates of hot spot mass, mix mass, and pressure.


Physics of Plasmas | 2013

Hohlraum energetics scaling to 520 TW on the National Ignition Facility

J. L. Kline; D. A. Callahan; S. H. Glenzer; N. B. Meezan; J. D. Moody; D. E. Hinkel; O. S. Jones; A. J. Mackinnon; R. Bennedetti; R. L. Berger; D. K. Bradley; E. L. Dewald; I. Bass; C. Bennett; M. W. Bowers; G. K. Brunton; J. Bude; S. C. Burkhart; A. Condor; J. M. Di Nicola; P. Di Nicola; S. N. Dixit; T. Doeppner; E. G. Dzenitis; G. V. Erbert; J. Folta; G. P. Grim; S. Glenn; Alex V. Hamza; S. W. Haan

Indirect drive experiments have now been carried out with laser powers and energies up to 520 TW and 1.9u2009MJ. These experiments show that the energy coupling to the target is nearly constant at 84%u2009±u20093% over a wide range of laser parameters from 350 to 520 TW and 1.2 to 1.9u2009MJ. Experiments at 520 TW with depleted uranium hohlraums achieve radiation temperatures of ∼330u2009±u20094u2009eV, enough to drive capsules 20 μm thicker than the ignition point design to velocities near the ignition goal of 370u2009km/s. A series of three symcap implosion experiments with nearly identical target, laser, and diagnostics configurations show the symmetry and drive are reproducible at the level of ±8.5% absolute and ±2% relative, respectively.


Physics of Plasmas | 2015

Higher velocity, high-foot implosions on the National Ignition Facility lasera)

D. A. Callahan; O. A. Hurricane; D. E. Hinkel; T. Döppner; T. Ma; H.-S. Park; M. A. Barrios Garcia; L. Berzak Hopkins; D. T. Casey; C. Cerjan; E. L. Dewald; T. R. Dittrich; M. J. Edwards; S. W. Haan; Alex V. Hamza; J. L. Kline; J. P. Knauer; A. L. Kritcher; O. L. Landen; S. LePape; A. G. MacPhee; J. L. Milovich; A. Nikroo; A. Pak; P. K. Patel; J. R. Rygg; J. E. Ralph; J. D. Salmonson; B. K. Spears; P. T. Springer

By increasing the velocity in “high foot” implosions [Dittrich et al., Phys. Rev. Lett. 112, 055002 (2014); Park et al., Phys. Rev. Lett. 112, 055001 (2014); Hurricane et al., Nature 506, 343 (2014); Hurricane et al., Phys. Plasmas 21, 056314 (2014)] on the National Ignition Facility laser, we have nearly doubled the neutron yield and the hotspot pressure as compared to the implosions reported upon last year. The implosion velocity has been increased using a combination of the laser (higher power and energy), the hohlraum (depleted uranium wall material with higher opacity and lower specific heat than gold hohlraums), and the capsule (thinner capsules with less mass). We find that the neutron yield from these experiments scales systematically with a velocity-like parameter of the square root of the laser energy divided by the ablator mass. By connecting this parameter with the inferred implosion velocity ( v), we find that for shots with primary yield >1 × 1015 neutrons, the total yield ∼u2009v9.4. This incre...


The Journal of Neuroscience | 2014

Chronic Deep Cerebellar Stimulation Promotes Long-Term Potentiation, Microstructural Plasticity, and Reorganization of Perilesional Cortical Representation in a Rodent Model

Jessica Cooperrider; Havan Furmaga; Ela B. Plow; H.-S. Park; Zhihong Chen; Grahame Kidd; Kenneth B. Baker; John T. Gale; Andre G. Machado

Control over postinjury CNS plasticity is a major frontier of science that, if conquered, would open new avenues for treatment of neurological disorders. Here we investigate the functional, physiological, and structural changes in the cerebral cortex associated with chronic deep brain stimulation of the cerebellar output, a treatment approach that has been shown to improve postischemia motor recovery in a rodent model of cortical infarcts. Long–Evans rats were pretrained on the pasta-matrix retrieval task, followed by induction of focal cortical ischemia and implantation of a macroelectrode in the contralesional lateral cerebellar nucleus. Animals were assigned to one of three treatment groups pseudorandomly to balance severity of poststroke motor deficits: REGULAR stimulation, BURST stimulation, or SHAM. Treatment initiated 2 weeks post surgery and continued for 5 weeks. At the end, animals were randomly selected for perilesional intracortical microstimulation mapping and tissue sampling for Western blot analysis or contributed tissue for 3D electron microscopy. Evidence of enhanced cortical plasticity with therapeutically effective stimulation is shown, marked by greater perilesional reorganization in stimulation- treated animals versus SHAM. BURST stimulation was significantly effective for promoting distal forepaw cortical representation. Stimulation-treated animals showed a twofold increase in synaptic density compared with SHAM. In addition, treated animals demonstrated increased expression of synaptic markers of long-term potentiation and plasticity, including synaptophysin, NMDAR1, CaMKII, and PSD95. These findings provide a critical foundation of how deep cerebellar stimulation may guide plastic reparative reorganization after nonprogressive brain injury and indicate strong translational potential.


Review of Scientific Instruments | 2012

A novel particle time of flight diagnostic for measurements of shock- and compression-bang times in D3He and DT implosions at the NIF

H. G. Rinderknecht; M. Gatu Johnson; A. Zylstra; N. Sinenian; M. Rosenberg; J. A. Frenje; C. Waugh; C. K. Li; F. H. Séguin; R. D. Petrasso; J. R. Rygg; J. R. Kimbrough; A. G. MacPhee; G. W. Collins; Damien G. Hicks; A. J. Mackinnon; P. Bell; R. Bionta; Thomas E. Clancy; R. A. Zacharias; T. Döppner; H.-S. Park; S. LePape; O. L. Landen; N. B. Meezan; E. I. Moses; V. U. Glebov; C. Stoeckl; T. C. Sangster; R.E. Olson

The particle-time-of-flight (pTOF) diagnostic, fielded alongside a wedge range-filter (WRF) proton spectrometer, will provide an absolute timing for the shock-burn weighted ρR measurements that will validate the modeling of implosion dynamics at the National Ignition Facility (NIF). In the first phase of the project, pTOF has recorded accurate bang times in cryogenic DT, DT exploding pusher, and D(3)He implosions using DD or DT neutrons with an accuracy better than ±70 ps. In the second phase of the project, a deflecting magnet will be incorporated into the pTOF design for simultaneous measurements of shock- and compression-bang times in D(3)He-filled surrogate implosions using D(3)He protons and DD-neutrons, respectively.


Review of Scientific Instruments | 2012

Invited Article: Relation between electric and magnetic field structures and their proton-beam images

Nathan Kugland; D. D. Ryutov; C. Plechaty; Jeffrey S. Ross; H.-S. Park

Proton imaging is commonly used to reveal the electric and magnetic fields that are found in high energy density plasmas. Presented here is an analysis of this technique that is directed towards developing additional insight into the underlying physics. This approach considers: formation of images in the limits of weak and strong intensity variations; caustic formation and structure; image inversion to obtain line-integrated field characteristics; direct relations between images and electric or magnetic field structures in a plasma; imaging of sharp features such as Debye sheaths and shocks. Limitations on spatial and temporal resolution are assessed, and similarities with optical shadowgraphy are noted. Synthetic proton images are presented to illustrate the analysis. These results will be useful for quantitatively analyzing experimental proton imaging data and verifying numerical codes.


Review of Scientific Instruments | 2012

Measuring the absolute deuterium-tritium neutron yield using the magnetic recoil spectrometer at OMEGA and the NIF.

D. T. Casey; J. A. Frenje; M. Gatu Johnson; F. H. Séguin; C. K. Li; R. D. Petrasso; V. Yu. Glebov; Joseph Katz; J. P. Knauer; D. D. Meyerhofer; T. C. Sangster; R. Bionta; D. L. Bleuel; T. Döppner; S. H. Glenzer; Edward P. Hartouni; S. P. Hatchett; S. Le Pape; T. Ma; A. J. Mackinnon; M. McKernan; M. J. Moran; Eric K. Moses; H.-S. Park; J. E. Ralph; B. A. Remington; V. A. Smalyuk; C. B. Yeamans; J. L. Kline; G. A. Kyrala

A magnetic recoil spectrometer (MRS) has been installed and extensively used on OMEGA and the National Ignition Facility (NIF) for measurements of the absolute neutron spectrum from inertial confinement fusion implosions. From the neutron spectrum measured with the MRS, many critical implosion parameters are determined including the primary DT neutron yield, the ion temperature, and the down-scattered neutron yield. As the MRS detection efficiency is determined from first principles, the absolute DT neutron yield is obtained without cross-calibration to other techniques. The MRS primary DT neutron measurements at OMEGA and the NIF are shown to be in excellent agreement with previously established yield diagnostics on OMEGA, and with the newly commissioned nuclear activation diagnostics on the NIF.


Physics of Plasmas | 2013

Magnetic field advection in two interpenetrating plasma streams

D. D. Ryutov; N. L. Kugland; M. C. Levy; C. Plechaty; J. S. Ross; H.-S. Park

Laser-generated colliding plasma streams can serve as a test-bed for the study of various astrophysical phenomena and the general physics of self-organization. For streams of a sufficiently high kinetic energy, collisions between the ions of one stream with the ions of the other stream are negligible, and the streams can penetrate through each other. On the other hand, the intra-stream collisions for high-Mach-number flows can still be very frequent, so that each stream can be described hydrodynamically. This paper presents an analytical study of the effects that these interpenetrating streams have on large-scale magnetic fields either introduced by external coils or generated in the plasma near the laser targets. Specifically, a problem of the frozen-in constraint is assessed and paradoxical features of the field advection in this system are revealed. A possibility of using this system for studies of magnetic reconnection is mentioned.

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D. A. Callahan

Lawrence Livermore National Laboratory

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B. A. Remington

Lawrence Livermore National Laboratory

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T. Ma

University of Washington

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D. T. Casey

Lawrence Livermore National Laboratory

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D. E. Hinkel

Lawrence Livermore National Laboratory

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O. A. Hurricane

Lawrence Livermore National Laboratory

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S. W. Haan

Lawrence Livermore National Laboratory

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T. R. Dittrich

Lawrence Livermore National Laboratory

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E. L. Dewald

Lawrence Livermore National Laboratory

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P. K. Patel

Lawrence Livermore National Laboratory

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