Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where V. Yu. Glebov is active.

Publication


Featured researches published by V. Yu. Glebov.


Review of Scientific Instruments | 2003

Spectrometry of charged particles from inertial-confinement-fusion plasmas

F. H. Seguin; J. A. Frenje; C. K. Li; Damien G. Hicks; S. Kurebayashi; J. R. Rygg; Barry E. Schwartz; R. D. Petrasso; S. Roberts; J. M. Soures; D. D. Meyerhofer; T. C. Sangster; J. P. Knauer; C. Sorce; V. Yu. Glebov; C. Stoeckl; Thomas W. Phillips; R. J. Leeper; Kurtis A. Fletcher; S. Padalino

High-resolution spectrometry of charged particles from inertial-confinement-fusion (ICF) experiments has become an important method of studying plasma conditions in laser-compressed capsules. In experiments at the 60-beam OMEGA laser facility [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)], utilizing capsules with D2, D3He, DT, or DTH fuel in a shell of plastic, glass, or D2 ice, we now routinely make spectral measurements of primary fusion products (p, D, T, 3He, α), secondary fusion products (p), “knock-on” particles (p, D, T) elastically scattered by primary neutrons, and ions from the shell. Use is made of several types of spectrometers that rely on detection and identification of particles with CR-39 nuclear track detectors in conjunction with magnets and/or special ranging filters. CR-39 is especially useful because of its insensitivity to electromagnetic noise and its ability to distinguish the types and energies of individual particles, as illustrated here by detailed calibrations of its respo...


Physics of Plasmas | 2011

The experimental plan for cryogenic layered target implosions on the National Ignition Facility—The inertial confinement approach to fusion

M. J. Edwards; J. D. Lindl; B. K. Spears; S. V. Weber; L. J. Atherton; D. L. Bleuel; David K. Bradley; D. A. Callahan; Charles Cerjan; D. S. Clark; G. W. Collins; J. Fair; R. J. Fortner; S. H. Glenzer; S. W. Haan; B. A. Hammel; Alex V. Hamza; S. P. Hatchett; N. Izumi; B. Jacoby; O. S. Jones; J. A. Koch; B. J. Kozioziemski; O. L. Landen; R. A. Lerche; B. J. MacGowan; A. J. Mackinnon; E. R. Mapoles; M. M. Marinak; M. J. Moran

Ignition requires precisely controlled, high convergence implosions to assemble a dense shell of deuterium-tritium (DT) fuel with ρR>∼1 g/cm2 surrounding a 10 keV hot spot with ρR ∼ 0.3 g/cm2. A working definition of ignition has been a yield of ∼1 MJ. At this yield the α-particle energy deposited in the fuel would have been ∼200 kJ, which is already ∼10 × more than the kinetic energy of a typical implosion. The National Ignition Campaign includes low yield implosions with dudded fuel layers to study and optimize the hydrodynamic assembly of the fuel in a diagnostics rich environment. The fuel is a mixture of tritium-hydrogen-deuterium (THD) with a density equivalent to DT. The fraction of D can be adjusted to control the neutron yield. Yields of ∼1014−15 14 MeV (primary) neutrons are adequate to diagnose the hot spot as well as the dense fuel properties via down scattering of the primary neutrons. X-ray imaging diagnostics can function in this low yield environment providing additional information about ...


Physics of Plasmas | 2005

Two-dimensional simulations of plastic-shell, direct-drive implosions on OMEGA

P. B. Radha; V.N. Goncharov; T.J.B. Collins; J. A. Delettrez; Y. Elbaz; V. Yu. Glebov; R. L. Keck; D. E. Keller; J. P. Knauer; J.A. Marozas; F. J. Marshall; P. W. McKenty; D. D. Meyerhofer; S. P. Regan; T. C. Sangster; D. Shvarts; S. Skupsky; Y. Srebro; R. P. J. Town; C. Stoeckl

Multidimensional hydrodynamic properties of high-adiabat direct-drive plastic-shell implosions on the OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] are investigated using the multidimensional hydrodynamic code, DRACO [D. Keller et al., Bull. Am. Phys. Soc. 44, 37 (1999)]. Multimode simulations including the effects of nonuniform illumination and target roughness indicate that shell stability during the acceleration phase plays a critical role in determining target performance. For thick shells that remain integral during the acceleration phase, target yields are significantly reduced by the combination of the long-wavelength (l<10) modes due to surface roughness and beam imbalance and the intermediate modes (20⩽l⩽50) due to single-beam nonuniformities. The neutron-production rate for these thick shells truncates relative to one-dimensional (1D) predictions. The yield degradation in the thin shells is mainly due to shell breakup at short wavelengths (λ∼Δ, where Δ is the in-flight s...


Physics of Plasmas | 2005

Multidimensional analysis of direct-drive, plastic-shell implosions on OMEGA

P. B. Radha; T.J.B. Collins; J. A. Delettrez; Y. Elbaz; R. Epstein; V. Yu. Glebov; V.N. Goncharov; R. L. Keck; J. P. Knauer; J.A. Marozas; F. J. Marshall; R. L. McCrory; P.W. McKenty; D. D. Meyerhofer; S. P. Regan; T. C. Sangster; W. Seka; D. Shvarts; S. Skupsky; Y. Srebro; C. Stoeckl

Direct-drive, plastic shells imploded on the OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] with a 1ns square pulse are simulated using the multidimensional hydrodynamic code DRACO in yield degradation in “thin” shells is primarily caused by shell breakup during the acceleration phase due to short-wavelength (l>50, where l is the Legendre mode number) perturbation growth, whereas “thick” shell performance is influenced primarily by long and intermediate modes (l⩽50). Simulation yields, temporal history of neutron production, areal densities, and x-ray images of the core compare well with experimental observations. In particular, the thin-shell neutron production history falls off less steeply than one-dimensional predictions due to shell-breakup-induced undercompression and delayed stagnation. Thicker, more-stable shells show burn truncation due to instability-induced mass flow into the colder bubbles. Estimates of small-scale mix indicate that turbulent mixing does not influence p...


Review of Scientific Instruments | 2012

Neutron spectrometry--an essential tool for diagnosing implosions at the National Ignition Facility (invited).

M. Gatu Johnson; J. A. Frenje; D. T. Casey; C. K. Li; F. H. Séguin; R. D. Petrasso; R. C. Ashabranner; R. Bionta; D. L. Bleuel; E. Bond; J. A. Caggiano; A. Carpenter; C. Cerjan; T. J. Clancy; T. Doeppner; M. J. Eckart; M. J. Edwards; S. Friedrich; S. H. Glenzer; S. W. Haan; Edward P. Hartouni; R. Hatarik; S. P. Hatchett; O. S. Jones; G. A. Kyrala; S. Le Pape; R. A. Lerche; O. L. Landen; T. Ma; A. J. Mackinnon

DT neutron yield (Y(n)), ion temperature (T(i)), and down-scatter ratio (dsr) determined from measured neutron spectra are essential metrics for diagnosing the performance of inertial confinement fusion (ICF) implosions at the National Ignition Facility (NIF). A suite of neutron-time-of-flight (nTOF) spectrometers and a magnetic recoil spectrometer (MRS) have been implemented in different locations around the NIF target chamber, providing good implosion coverage and the complementarity required for reliable measurements of Y(n), T(i), and dsr. From the measured dsr value, an areal density (ρR) is determined through the relationship ρR(tot) (g∕cm(2)) = (20.4 ± 0.6) × dsr(10-12 MeV). The proportionality constant is determined considering implosion geometry, neutron attenuation, and energy range used for the dsr measurement. To ensure high accuracy in the measurements, a series of commissioning experiments using exploding pushers have been used for in situ calibration of the as-built spectrometers, which are now performing to the required accuracy. Recent data obtained with the MRS and nTOFs indicate that the implosion performance of cryogenically layered DT implosions, characterized by the experimental ignition threshold factor (ITFx), which is a function of dsr (or fuel ρR) and Y(n), has improved almost two orders of magnitude since the first shot in September, 2010.


Physics of Plasmas | 2010

Probing high areal-density cryogenic deuterium-tritium implosions using downscattered neutron spectra measured by the magnetic recoil spectrometer

J. A. Frenje; D. T. Casey; C. K. Li; F. H. Séguin; R. D. Petrasso; V. Yu. Glebov; P. B. Radha; T. C. Sangster; D. D. Meyerhofer; S. P. Hatchett; S. W. Haan; Charles Cerjan; O. L. Landen; K. Fletcher; R. J. Leeper

For the first time high areal-density (ρR) cryogenic deuterium-tritium (DT) implosions have been probed using downscattered neutron spectra measured with the magnetic recoil spectrometer (MRS) [J. A. Frenje et al., Rev. Sci. Instrum. 79, 10E502 (2008)], recently installed and commissioned on OMEGA [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)]. The ρR data obtained with the MRS have been essential for understanding how the fuel is assembled and for guiding the cryogenic program at the Laboratory for Laser Energetics (LLE) to ρR values up to ∼300 mg/cm2. The ρR data obtained from well-established charged particle spectrometry techniques [C. K. Li et al., Phys. Plasmas 8, 4902 (2001)] were used to authenticate the MRS data for low-ρR plastic capsule implosions, and the ρR values inferred from these techniques are in excellent agreement, indicating that the MRS technique provides high-fidelity data. Recent OMEGA-MRS data and Monte Carlo simulations have shown that the MRS on the NIF [G. H. Miller et al....


Review of Scientific Instruments | 2006

Development of nuclear diagnostics for the National Ignition Facility (invited)

V. Yu. Glebov; D. D. Meyerhofer; T. C. Sangster; C. Stoeckl; S. Roberts; C. A. Barrera; J. Celeste; Charles Cerjan; Lucile S. Dauffy; David C. Eder; R. L. Griffith; S. W. Haan; B. A. Hammel; S. P. Hatchett; N. Izumi; J. R. Kimbrough; J. A. Koch; O. L. Landen; R. A. Lerche; B. J. MacGowan; M. J. Moran; E. W. Ng; Thomas W. Phillips; P. Song; R. Tommasini; B. K. Young; S. E. Caldwell; Gary P. Grim; S. C. Evans; J. M. Mack

The National Ignition Facility (NIF) will provide up to 1.8MJ of laser energy for imploding inertial confinement fusion (ICF) targets. Ignited NIF targets are expected to produce up to 1019 DT neutrons. This will provide unprecedented opportunities and challenges for the use of nuclear diagnostics in ICF experiments. In 2005, the suite of nuclear-ignition diagnostics for the NIF was defined and they are under development through collaborative efforts at several institutions. This suite includes PROTEX and copper activation for primary yield measurements, a magnetic recoil spectrometer and carbon activation for fuel areal density, neutron time-of-flight detectors for yield and ion temperature, a gamma bang time detector, and neutron imaging systems for primary and downscattered neutrons. An overview of the conceptual design, the developmental status, and recent results of prototype tests on the OMEGA laser will be presented.


Physics of Plasmas | 2014

Improving the hot-spot pressure and demonstrating ignition hydrodynamic equivalence in cryogenic deuterium–tritium implosions on OMEGAa)

V.N. Goncharov; T. C. Sangster; R. Betti; T. R. Boehly; M.J. Bonino; T.J.B. Collins; R. S. Craxton; J. A. Delettrez; D. H. Edgell; R. Epstein; R.K. Follett; C.J. Forrest; D. H. Froula; V. Yu. Glebov; D. R. Harding; R.J. Henchen; S. X. Hu; I.V. Igumenshchev; R. Janezic; J. H. Kelly; Thomas Kessler; T. Z. Kosc; S. J. Loucks; J.A. Marozas; F. J. Marshall; A. V. Maximov; R.L. McCrory; P.W. McKenty; D. D. Meyerhofer; D.T. Michel

Reaching ignition in direct-drive (DD) inertial confinement fusion implosions requires achieving central pressures in excess of 100 Gbar. The OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] is used to study the physics of implosions that are hydrodynamically equivalent to the ignition designs on the National Ignition Facility (NIF) [J. A. Paisner et al., Laser Focus World 30, 75 (1994)]. It is shown that the highest hot-spot pressures (up to 40 Gbar) are achieved in target designs with a fuel adiabat of α ≃ 4, an implosion velocity of 3.8 × 107 cm/s, and a laser intensity of ∼1015 W/cm2. These moderate-adiabat implosions are well understood using two-dimensional hydrocode simulations. The performance of lower-adiabat implosions is significantly degraded relative to code predictions, a common feature between DD implosions on OMEGA and indirect-drive cryogenic implosions on the NIF. Simplified theoretical models are developed to gain physical understanding of the implosion dynamics th...


Review of Scientific Instruments | 2008

First measurements of the absolute neutron spectrum using the magnetic recoil spectrometer at OMEGA (invited).

J. A. Frenje; D. T. Casey; C. K. Li; J. R. Rygg; F. H. Séguin; R. D. Petrasso; V. Yu. Glebov; D. D. Meyerhofer; T. C. Sangster; S. P. Hatchett; S. W. Haan; Charles Cerjan; O. L. Landen; M. J. Moran; P. Song; D. C. Wilson; R. J. Leeper

A neutron spectrometer, called a magnetic recoil spectrometer (MRS), has been built and implemented at the OMEGA laser facility [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] for absolute measurements of the neutron spectrum in the range of 6-30 MeV, from which fuel areal density (rhoR), ion temperature (T(i)), and yield (Y(n)) can be determined. The results from the first MRS measurements of the absolute neutron spectrum are presented. In addition, measuring rhoR at the National Ignition Facility (NIF) [G. H. Miller et al., Nucl. Fusion 44, S228 (2004)] will be essential for assessing implosion performance during all stages of development from surrogate implosions to cryogenic fizzles to ignited implosions. To accomplish this, we are also developing an MRS for the NIF. As much of the research and development and instrument optimization of the MRS at OMEGA are directly applicable to the MRS at the NIF, a description of the design and characterization of the MRS on the NIF is discussed as well.


Physics of Plasmas | 2001

Core performance and mix in direct-drive spherical implosions with high uniformity

D. D. Meyerhofer; J. A. Delettrez; R. Epstein; V. Yu. Glebov; V.N. Goncharov; R. L. Keck; R. L. McCrory; P.W. McKenty; F. J. Marshall; P. B. Radha; S. P. Regan; S. Roberts; W. Seka; S. Skupsky; V. A. Smalyuk; C. Sorce; C. Stoeckl; J. M. Soures; R. P. J. Town; B. Yaakobi; Jonathan D. Zuegel; J. A. Frenje; C. K. Li; R. D. Petrasso; F. H. Séguin; Kurtis A. Fletcher; Stephen Padalino; C. Freeman; N. Izumi; R. A. Lerche

The performance of gas-filled, plastic-shell implosions has significantly improved with advances in on-target uniformity on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton et al., Opt. Commun. 133, 495 (1997)]. Polarization smoothing (PS) with birefringent wedges and 1-THz-bandwidth smoothing by spectral dispersion (SSD) have been installed on OMEGA. The beam-to-beam power imbalance is ⩽5% rms. Implosions of 20-μm-thick CH shells (15 atm fill) using full beam smoothing (1-THz SSD and PS) have primary neutron yields and fuel areal densities that are ∼70% larger than those driven with 0.35-THz SSD without PS. They also produce ∼35% of the predicted one-dimensional neutron yield. The results described here suggest that individual-beam nonuniformity is no longer the primary cause of nonideal target performance. A highly constrained model of the core conditions and fuel–shell mix has been developed. It suggests that there is a “clean” fuel region, surrounded by a mixed region, that acc...

Collaboration


Dive into the V. Yu. Glebov's collaboration.

Researchain Logo
Decentralizing Knowledge