R. C. Mock
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View article: Temporal control of radiation pulse using gas filled drift cells on HERMES III
Temporal control of radiation pulse using gas filled drift cells on HERMES III Open
Significant erosion of the front of the HERMES-III electron beam in drift cells filled with N[sub 2] gas is measured for pressures greater than 100 Torr (as much as 10 ns [3 m] at 630 Torr for 11-m length cells). Little rise time (RT) shar…
View article: Comparative properties of the interior and blowoff plasmas in a dynamic hohlraum
Comparative properties of the interior and blowoff plasmas in a dynamic hohlraum Open
A Dynamic Hohlraum (DH) is formed when arrays of tungsten wires driven by a high-current pulse implode and compress a cylindrical foam target. The resulting radiation is confined by the wire plasma and forms an intense, ∼200–250eV Planckia…
View article: Compound-lens diode for hermes III
Compound-lens diode for hermes III Open
Significantly improved spatial uniformity of bremsstrahlung radiation, relative to a diode with a planar anode, is predicted for the HERMES III accelerator when a compound-lens diode is used to actively control the high-power electron beam…
View article: Photoneutron Production on HERMES III Using an Intense Bremsstrahlung Source
Photoneutron Production on HERMES III Using an Intense Bremsstrahlung Source Open
An intense reusable source of pulsed photoneutrons has been developed for HERMES III, delivering 0.5 to 1 {times} 10{sup 14} n/pulse with an average kinetic-energy of 1.8 to 1.3 MeV, respectively, over a useful area of 150 cm{sup 2} in a p…
View article: Progress in z-pinch driven dynamic-hohlraums for high-temperature radiation-flow and ICF experiments at Sandia National Laboratories
Progress in z-pinch driven dynamic-hohlraums for high-temperature radiation-flow and ICF experiments at Sandia National Laboratories Open
Progress in understanding the physics of dynamic-hohlraums is reviewed for a system capable of generating 13 TW of axial radiation for high temperature (>200 eV) radiation-flow experiments and ICF capsule implosions.
View article: THE APPLICATION OF 2-D SIMULATIONS TO Z-PINCH EXPERIMENT DESIGN AND ANALYSIS
THE APPLICATION OF 2-D SIMULATIONS TO Z-PINCH EXPERIMENT DESIGN AND ANALYSIS Open
The successful 2-D simulations of z-pinch experiments (reproducing such features as the measured experimental current drive, radiation pulse shape, peak power and total radiated energy) can lead to a better understanding of the underlying …
View article: Dynamics of a Z-pinch x-ray source for heating inertial-confinement-fusion relevant hohlraums to 120–160 eV
Dynamics of a Z-pinch x-ray source for heating inertial-confinement-fusion relevant hohlraums to 120–160 eV Open
A Z-pinch radiation source has been developed that generates 60±20 kJ of x rays with a peak power of 13±4 TW through a 4-mm-diam axial aperture on the Z facility. The source has heated National Ignition Facility-scale (6-mm-diam by 7-mm-hi…
View article: Characteristics of ICF Relevant Hohlraums Driven by X-Rays from a Z-Pinch
Characteristics of ICF Relevant Hohlraums Driven by X-Rays from a Z-Pinch Open
Radiation environments characteristic of those encountered during the low-temperature foot pulse and subsequent higher-temperature early-step pulses (without the foot pulse) required for indirect-drive ICF ignition on the National ignition…
View article: Z-Pinch Generated X-Rays Demonstrate Indirect-Drive ICF Potential
Z-Pinch Generated X-Rays Demonstrate Indirect-Drive ICF Potential Open
Hohlraums (measuring 6-mm in diameter by 7-mm in height) have been heated by x-rays from a z-pinch. Over measured x-ray input powers P of 0.7 to 13 TW, the hohlraum radiation temperature T increases from {approximately}55 to {approximately…
View article: High-temperature dynamic hohlraums on the pulsed power driver <i>Z</i>
High-temperature dynamic hohlraums on the pulsed power driver <i>Z</i> Open
In the concept of the dynamic hohlraum an imploding Z pinch is optically thick to its own radiation. Radiation may be trapped inside the pinch to give a radiation temperature inside the pinch greater than that outside the pinch. The radiat…
View article: Wire array Z-pinch insights for enhanced x-ray production
Wire array Z-pinch insights for enhanced x-ray production Open
Comparisons of measured total radiated x-ray power from annular wire-array z-pinches with a variety of models as a function of wire number, array mass, and load radius are reviewed. The data, which are comprehensive, have provided importan…
View article: Z-Pinch Driven Inertial Confinement Fusion Target Physics Research at Sandia National Laboratories
Z-Pinch Driven Inertial Confinement Fusion Target Physics Research at Sandia National Laboratories Open
Three hohlraum concepts are being pursued at Sandia National Laboratories (SNL) to investigate the possibility of using pulsed power driven magnetic implosions (z-pinches) to drive high gain targets capable of yields in the range of 200-10…
View article: Variation of high-power aluminum-wire array Z-pinch dynamics with wire number, array radius, and load mass
Variation of high-power aluminum-wire array Z-pinch dynamics with wire number, array radius, and load mass Open
A systematic study of annular aluminum-wire z-pinches on the Saturn accelerator shows that the quality of the implosion, including the radiated power, increases with wire number. Radiation magnetohydrodynamic (RMEC) xy simulations suggest …
View article: Time-dependent electron temperature diagnostics for high-power, aluminum z-pinch plasmas
Time-dependent electron temperature diagnostics for high-power, aluminum z-pinch plasmas Open
Time-resolved x-ray pinhole photographs and time-integrated radially-resolved x-ray crystal spectrometer measurements of azimuthally-symmetric aluminum-wire implosions suggest that the final pinch is composed of a hot dense plasma core sur…
View article: Intense electron-beam transport in the ion-focused regime through the collision-dominated regime
Intense electron-beam transport in the ion-focused regime through the collision-dominated regime Open
This paper reviews the transport of the 19-MeV, 700-kA, 25-ns Hermes-III electron beam in long gas cells filled with N{sub 2} gas spanning six decades in pressure from 10{sup 3} to {approximately}10{sup 3} Torr. We show through measurement…
View article: Preradiation studies for non-thermal Z-pinch wire load experiments on Saturn
Preradiation studies for non-thermal Z-pinch wire load experiments on Saturn Open
The implosion dynamics of compact wire arrays on Saturn are explored as a function of wire mass m, wire length {ell}, wire radii R, and radial power-flow feed geometry using the ZORK code. Electron losses and the likelihood of arcing in th…
View article: Compound-lens injector for a pulsed 13-TW electron beam
Compound-lens injector for a pulsed 13-TW electron beam Open
A robust injector capable of controlling the radius and angle of incidence of the pulsed, intense, annular electron beam extracted from the HERMES III accelerator is described. The injector, called the compound lens, uses a tapered anode t…
View article: Generation, control, and transport of a 19-MeV, 700-kA pulsed electron beam
Generation, control, and transport of a 19-MeV, 700-kA pulsed electron beam Open
We show experimentally and theoretically that the generation of the 13-TW Hermes III electron beam can be accurately monitored, and that the beam can be accurately directed onto a high-Z target to produce a wide variety of bremsstrahlung p…
View article: Production and measurement of flash X-ray dose rates in excess of 10/sup 13/ RAD (CaF/sub 2/)/s
Production and measurement of flash X-ray dose rates in excess of 10/sup 13/ RAD (CaF/sub 2/)/s Open
The radiation field from an intense reusable source of flash x-rays that delivers a measured peak dose and dose rate of 370 {plus_minus} 60 krad (CaF{sub 2}) and (3.5 {plus_minus} 0.7) {times} 10{sup 13} rad (CaF{sub 2})/s over a useful ar…
View article: Dose-rate field of the HERMES III flash X-ray source
Dose-rate field of the HERMES III flash X-ray source Open
Measurements show that the HERMES III flash x-ray source produces a peak dose-rate radiation field of (5 {plus minus} 0.5) {times} 10{sup 12} rad(Si)/s over a useful area of 1000 cm{sup 2}, with a pulse width of {approximately}20 ns. Numer…
View article: Temporal characterization of the 19-MV, 700-kA HERMES III electron beam
Temporal characterization of the 19-MV, 700-kA HERMES III electron beam Open
The shot-to-shot variation of the HERMES III Accelerator parameters at the electron-beam diode, the time dependence of the electron flow in the diode, and the time dependence of the subsequent radiation produced from the bremsstrahlung tar…