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Dive into the research topics where N. Guler is active.

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Featured researches published by N. Guler.


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 | 2014

Neutron source reconstruction from pinhole imaging at National Ignition Facility

Petr L. Volegov; C. R. Danly; D. N. Fittinghoff; G. P. Grim; N. Guler; N. Izumi; T. Ma; F. E. Merrill; A. L. Warrick; C. H. Wilde; D. C. Wilson

The neutron imaging system at the National Ignition Facility (NIF) is an important diagnostic tool for measuring the two-dimensional size and shape of the neutrons produced in the burning deuterium-tritium plasma during the ignition stage of inertial confinement fusion (ICF) implosions at NIF. Since the neutron source is small (∼100 μm) and neutrons are deeply penetrating (>3 cm) in all materials, the apertures used to achieve the desired 10-μm resolution are 20-cm long, single-sided tapers in gold. These apertures, which have triangular cross sections, produce distortions in the image, and the extended nature of the pinhole results in a non-stationary or spatially varying point spread function across the pinhole field of view. In this work, we have used iterative Maximum Likelihood techniques to remove the non-stationary distortions introduced by the aperture to reconstruct the underlying neutron source distributions. We present the detailed algorithms used for these reconstructions, the stopping criteria used and reconstructed sources from data collected at NIF with a discussion of the neutron imaging performance in light of other diagnostics.


Physics of Plasmas | 2014

Development of the CD Symcap platform to study gas-shell mix in implosions at the National Ignition Facility

D. T. Casey; V. A. Smalyuk; Robert Tipton; J. Pino; Gary P. Grim; B. A. Remington; Dana P. Rowley; S. V. Weber; M. A. Barrios; L. R. Benedetti; D. L. Bleuel; E. Bond; David K. Bradley; J. A. Caggiano; D. A. Callahan; Charles Cerjan; K. C. Chen; D. H. Edgell; M. J. Edwards; D. N. Fittinghoff; J. A. Frenje; M. Gatu-Johnson; Vladimir Yu. Glebov; S. Glenn; N. Guler; S. W. Haan; Alex V. Hamza; R. Hatarik; H. W. Herrmann; D. Hoover

Surrogate implosions play an important role at the National Ignition Facility (NIF) for isolating aspects of the complex physical processes associated with fully integrated ignition experiments. The newly developed CD Symcap platform has been designed to study gas-shell mix in indirectly driven, pure T2-gas filled CH-shell implosions equipped with 4 μm thick CD layers. This configuration provides a direct nuclear signature of mix as the DT yield (above a characterized D contamination background) is produced by D from the CD layer in the shell, mixing into the T-gas core. The CD layer can be placed at different locations within the CH shell to probe the depth and extent of mix. CD layers placed flush with the gas-shell interface and recessed up to 8 μm have shown that most of the mix occurs at the inner-shell surface. In addition, time-gated x-ray images of the hotspot show large brightly radiating objects traversing through the hotspot around bang-time, which are likely chunks of CH/CD plastic. This platf...


Physics of Plasmas | 2013

Characterization of a novel, short pulse laser-driven neutron source

D. Jung; Katerina Falk; N. Guler; O. Deppert; M. Devlin; Andrea Favalli; Juan C. Fernandez; D. C. Gautier; Matthias Geissel; R. Haight; Christopher E. Hamilton; B. M. Hegelich; R. P. Johnson; F. E. Merrill; G. Schaumann; Kurt F. Schoenberg; M. Schollmeier; T. Shimada; T.N. Taddeucci; J. L. Tybo; S.A. Wender; C. H. Wilde; G. A. Wurden; Markus Roth

We present a full characterization of a short pulse laser-driven neutron source. Neutrons are produced by nuclear reactions of laser-driven ions deposited in a secondary target. The emission of neutrons is a superposition of an isotropic component into 4π and a forward directed, jet-like contribution, with energies ranging up to 80 MeV. A maximum flux of 4.4 × 109 neutrons/sr has been observed and used for fast neutron radiography. On-shot characterization of the ion driver and neutron beam has been done with a variety of different diagnostics, including particle detectors, nuclear reaction, and time-of-flight methods. The results are of great value for future optimization of this novel technique and implementation in advanced applications.


Journal of Applied Physics | 2016

Neutron imaging with the short-pulse laser driven neutron source at the Trident laser facility

N. Guler; Petr L. Volegov; Andrea Favalli; F. E. Merrill; Katerina Falk; D. Jung; J. L. Tybo; C. H. Wilde; Stephen Croft; C. R. Danly; O. Deppert; M. Devlin; Juan C. Fernandez; D. C. Gautier; Matthias Geissel; R. Haight; Christopher E. Hamilton; B. M. Hegelich; Daniela Henzlova; R. P. Johnson; G. Schaumann; Kurt F. Schoenberg; M. Schollmeier; Tsutomu Shimada; Martyn T. Swinhoe; T.N. Taddeucci; S.A. Wender; G. A. Wurden; Markus Roth

Emerging approaches to short-pulse laser-driven neutron production offer a possible gateway to compact, low cost, and intense broad spectrum sources for a wide variety of applications. They are based on energetic ions, driven by an intense short-pulse laser, interacting with a converter material to produce neutrons via breakup and nuclear reactions. Recent experiments performed with the high-contrast laser at the Trident laser facility of Los Alamos National Laboratory have demonstrated a laser-driven ion acceleration mechanism operating in the regime of relativistic transparency, featuring a volumetric laser-plasma interaction. This mechanism is distinct from previously studied ones that accelerate ions at the laser-target surface. The Trident experiments produced an intense beam of deuterons with an energy distribution extending above 100 MeV. This deuteron beam, when directed at a beryllium converter, produces a forward-directed neutron beam with ∼5 × 109 n/sr, in a single laser shot, primarily due to ...


Physics of Plasmas | 2017

The role of hot spot mix in the low-foot and high-foot implosions on the NIF

T. Ma; P. K. Patel; N. Izumi; P. T. Springer; M.H. Key; L. J. Atherton; M. A. Barrios; L. R. Benedetti; R. Bionta; E. Bond; D. K. Bradley; J. A. Caggiano; D. A. Callahan; D. T. Casey; Peter M. Celliers; C. Cerjan; J. A. Church; D. S. Clark; E. L. Dewald; T. R. Dittrich; S. Dixit; T. Döppner; Rebecca Dylla-Spears; D. H. Edgell; R. Epstein; J. E. Field; D. N. Fittinghoff; J. A. Frenje; M. Gatu Johnson; S. Glenn

Hydrodynamic mix of the ablator into the DT fuel layer and hot spot can be a critical performance limitation in inertial confinement fusion implosions. This mix results in increased radiation loss, cooling of the hot spot, and reduced neutron yield. To quantify the level of mix, we have developed a simple model that infers the level of contamination using the ratio of the measured x-ray emission to the neutron yield. The principal source for the performance limitation of the “low-foot” class of implosions appears to have been mix. Lower convergence “high-foot” implosions are found to be less susceptible to mix, allowing velocities of >380 km/s to be achieved.


Review of Scientific Instruments | 2012

Simultaneous usage of pinhole and penumbral apertures for imaging small scale neutron sources from inertial confinement fusion experiments.

N. Guler; Petr L. Volegov; C. R. Danly; G. P. Grim; F. E. Merrill; C. H. Wilde

Inertial confinement fusion experiments at the National Ignition Facility are designed to understand the basic principles of creating self-sustaining fusion reactions by laser driven compression of deuterium-tritium (DT) filled cryogenic plastic capsules. The neutron imaging diagnostic provides information on the distribution of the central fusion reaction region and the surrounding DT fuel by observing neutron images in two different energy bands for primary (13-17 MeV) and down-scattered (6-12 MeV) neutrons. From this, the final shape and size of the compressed capsule can be estimated and the symmetry of the compression can be inferred. These experiments provide small sources with high yield neutron flux. An aperture design that includes an array of pinholes and penumbral apertures has provided the opportunity to image the same source with two different techniques. This allows for an evaluation of these different aperture designs and reconstruction algorithms.


Review of Scientific Instruments | 2012

The Neutron Imaging Diagnostic at NIF

F. E. Merrill; Robert A. Buckles; Deborah J. Clark; C. R. Danly; Owen B. Drury; J M Dzenitis; V E Fatherly; D. N. Fittinghoff; R. Gallegos; Gary P. Grim; N. Guler; E. N. Loomis; S Lutz; Robert M. Malone; D D Martinson; D Mares; D J Morley; George L. Morgan; John A. Oertel; I.L. Tregillis; Petr L. Volegov; P B Weiss; C. H. Wilde; D. C. Wilson

A neutron imaging diagnostic has recently been commissioned at the National Ignition Facility (NIF). This new system is an important diagnostic tool for inertial fusion studies at the NIF for measuring the size and shape of the burning DT plasma during the ignition stage of Inertial Confinement Fusion (ICF) implosions. The imaging technique utilizes a pinhole neutron aperture, placed between the neutron source and a neutron detector. The detection system measures the two dimensional distribution of neutrons passing through the pinhole. This diagnostic has been designed to collect two images at two times. The long flight path for this diagnostic, 28 m, results in a chromatic separation of the neutrons, allowing the independently timed images to measure the source distribution for two neutron energies. Typically the first image measures the distribution of the 14 MeV neutrons and the second image of the 6-12 MeV neutrons. The combination of these two images has provided data on the size and shape of the burning plasma within the compressed capsule, as well as a measure of the quantity and spatial distribution of the cold fuel surrounding this core.A neutron imaging diagnostic has recently been commissioned at the National Ignition Facility (NIF). This new system is an important diagnostic tool for inertial fusion studies at the NIF for measuring the size and shape of the burning DT plasma during the ignition stage of Inertial Confinement Fusion (ICF) implosions. The imaging technique utilizes a pinhole neutron aperture, placed between the neutron source and a neutron detector. The detection system measures the two dimensional distribution of neutrons passing through the pinhole. This diagnostic has been designed to collect two images at two times. The long flight path for this diagnostic, 28 m, results in a chromatic separation of the neutrons, allowing the independently timed images to measure the source distribution for two neutron energies. Typically the first image measures the distribution of the 14 MeV neutrons and the second image of the 6-12 MeV neutrons. The combination of these two images has provided data on the size and shape of the burning plasma within the compressed capsule, as well as a measure of the quantity and spatial distribution of the cold fuel surrounding this core.


Physics of Plasmas | 2014

Simulations of indirectly driven gas-filled capsules at the National Ignition Facility

S. V. Weber; D. T. Casey; David C. Eder; J. D. Kilkenny; J. Pino; V. A. Smalyuk; Gary P. Grim; B. A. Remington; Dana P. Rowley; C. B. Yeamans; Robert Tipton; M. A. Barrios; R. Benedetti; L. Berzak Hopkins; D. L. Bleuel; E. Bond; David K. Bradley; J. A. Caggiano; D. A. Callahan; Charles Cerjan; D. S. Clark; L. Divol; D. H. Edgell; M. J. Edwards; M. J. Eckart; D. N. Fittinghoff; J. A. Frenje; M. Gatu-Johnson; Vladimir Yu. Glebov; S. Glenn

Gas-filled capsules imploded with indirect drive on the National Ignition Facility have been employed as symmetry surrogates for cryogenic-layered ignition capsules and to explore interfacial mix. Plastic capsules containing deuterated layers and filled with tritium gas provide a direct measure of mix of ablator into the gas fuel. Other plastic capsules have employed DT or D3He gas fill. We present the results of two-dimensional simulations of gas-filled capsule implosions with known degradation sources represented as in modeling of inertial confinement fusion ignition designs; these are time-dependent drive asymmetry, the capsule support tent, roughness at material interfaces, and prescribed gas-ablator interface mix. Unlike the case of cryogenic-layered implosions, many observables of gas-filled implosions are in reasonable agreement with predictions of these simulations. Yields of TT and DT neutrons as well as other x-ray and nuclear diagnostics are matched for CD-layered implosions. Yields of DT-fille...


Physics of Plasmas | 2017

Laser-plasmas in the relativistic-transparency regime: Science and applications

Juan C. Fernandez; D. Cort Gautier; Chengkung Huang; S. Palaniyappan; B. J. Albright; W. Bang; G. Dyer; Andrea Favalli; James F. Hunter; Jacob Mendez; Markus Roth; Martyn T. Swinhoe; P. A. Bradley; O. Deppert; Michelle A. Espy; Katerina Falk; N. Guler; Christopher E. Hamilton; B. M. Hegelich; Daniela Henzlova; Kiril Dimitrov Ianakiev; Metodi Iliev; R. P. Johnson; A. Kleinschmidt; Adrian S. Losko; E. McCary; M. Mocko; R. O. Nelson; R. Roycroft; Miguel A. Santiago Cordoba

Laser-plasma interactions in the novel regime of relativistically induced transparency (RIT) have been harnessed to generate intense ion beams efficiently with average energies exceeding 10 MeV/nucleon (>100 MeV for protons) at “table-top” scales in experiments at the LANL Trident Laser. By further optimization of the laser and target, the RIT regime has been extended into a self-organized plasma mode. This mode yields an ion beam with much narrower energy spread while maintaining high ion energy and conversion efficiency. This mode involves self-generation of persistent high magnetic fields (∼104 T, according to particle-in-cell simulations of the experiments) at the rear-side of the plasma. These magnetic fields trap the laser-heated multi-MeV electrons, which generate a high localized electrostatic field (∼0.1 T V/m). After the laser exits the plasma, this electric field acts on a highly structured ion-beam distribution in phase space to reduce the energy spread, thus separating acceleration and energy-spread reduction. Thus, ion beams with narrow energy peaks at up to 18 MeV/nucleon are generated reproducibly with high efficiency (≈5%). The experimental demonstration has been done with 0.12 PW, high-contrast, 0.6 ps Gaussian 1.053 μm laser pulses irradiating planar foils up to 250 nm thick at 2–8 × 1020 W/cm2. These ion beams with co-propagating electrons have been used on Trident for uniform volumetric isochoric heating to generate and study warm-dense matter at high densities. These beam plasmas have been directed also at a thick Ta disk to generate a directed, intense point-like Bremsstrahlung source of photons peaked at ∼2 MeV and used it for point projection radiography of thick high density objects. In addition, prior work on the intense neutron beam driven by an intense deuterium beam generated in the RIT regime has been extended. Neutron spectral control by means of a flexible converter-disk design has been demonstrated, and the neutron beam has been used for point-projection imaging of thick objects. The plans and prospects for further improvements and applications are also discussed.

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F. E. Merrill

Los Alamos National Laboratory

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D. N. Fittinghoff

Lawrence Livermore National Laboratory

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C. H. Wilde

Los Alamos National Laboratory

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C. R. Danly

Los Alamos National Laboratory

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Gary P. Grim

Los Alamos National Laboratory

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Andrea Favalli

Los Alamos National Laboratory

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Juan C. Fernandez

Los Alamos National Laboratory

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Katerina Falk

Los Alamos National Laboratory

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Markus Roth

Technische Universität Darmstadt

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