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Dive into the research topics where Martyn T. Swinhoe is active.

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Featured researches published by Martyn T. Swinhoe.


Archive | 2013

Final Technical Report for the Neutron Detection without Helium-3 Project

James H. Ely; Mary Bliss; Richard T. Kouzes; Azaree T. Lintereur; Sean M. Robinson; Edward R. Siciliano; Martyn T. Swinhoe; Mitchell L. Woodring

This report details the results of the research and development work accomplished for the ‘Neutron Detection without Helium-3’ project conducted during the 2011-2013 fiscal years. The primary focus of the project was to investigate commercially available technologies that might be used in safeguards applications in the relatively near term. Other technologies that are being developed may be more applicable in the future, but were outside the scope of this study.


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 ...


Archive | 2013

Modeling and Simulation Optimization and Feasibility Studies for the Neutron Detection without Helium-3 Project

James H. Ely; Edward R. Siciliano; Martyn T. Swinhoe; Azaree T. Lintereur

This report details the results of the modeling and simulation work accomplished for the ‘Neutron Detection without Helium-3’ project during the 2011 and 2012 fiscal years. The primary focus of the project is to investigate commercially available technologies that might be used in safeguards applications in the relatively near term. Other technologies that are being developed may be more applicable in the future, but are outside the scope of this study.


Nuclear Technology | 2013

Development of Self-Interrogation Neutron Resonance Densitometry to Improve Detection of Possible Diversions for PWR Spent Fuel Assemblies

Adrienne M. LaFleur; William S. Charlton; Howard O. Menlove; Martyn T. Swinhoe; Alain R. Lebrun

A new nondestructive assay technique called self-interrogation neutron resonance densitometry (SINRD) is currently being developed at Los Alamos National Laboratory to improve existing nuclear safeguards and material accountability measurements for light water reactor fuel assemblies. The viability of using SINRD to improve the detection of possible diversion scenarios for pressurized water reactor 17 × 17 spent low-enriched uranium (LEU) and mixed oxide (MOX) fuel assemblies was investigated via Monte Carlo N-Particle eXtended transport code (MCNPX) simulations. The following capabilities were assessed: (a) verification of the burnup of a spent fuel assembly, (b) ability to distinguish fresh and one-cycle spent MOX fuel from three- and four-cycle spent LEU fuel, and (c) sensitivity and penetrability to the removal of fuel pins. SINRD utilizes 244Cm spontaneous-fission neutrons to self-interrogate the spent fuel pins. The amount of resonance absorption of these neutrons in the fuel can be quantified using a set of fission chambers (FCs) placed adjacent to the assembly. The sensitivity of SINRD is based on using the same fissile materials in the FCs as are present in the fuel because the effect of resonance absorption lines in the transmitted flux is amplified by the corresponding (n, f) reaction peaks in the FC. SINRD requires calibration with a reference assembly of similar geometry in a similar measurement configuration with the same surrounding moderator as the spent fuel assemblies. However, this densitometry method uses ratios of different detectors so that several systematic errors related to calibration and positioning cancel in the ratios.


Nuclear Science and Engineering | 2012

Development of Self-Interrogation Neutron Resonance Densitometry to Quantify the Fissile Content in PWR Spent LEU and MOX Assemblies

Adrienne M. LaFleur; William S. Charlton; Howard O. Menlove; Martyn T. Swinhoe

Abstract A new nondestructive assay technique called self-interrogation neutron resonance densitometry (SINRD) is currently being developed at Los Alamos National Laboratory to improve existing nuclear safeguards and material accountability measurements for light water reactor fuel assemblies. The viability of using SINRD to quantify the fissile content (235U and 239Pu) in pressurized water reactor 17 × 17 spent low-enriched uranium and mixed-oxide fuel assemblies in water was investigated via Monte Carlo N-particle extended transport code simulations. SINRD utilizes 244Cm spontaneous fission neutrons to self-interrogate the fuel pins. The amount of resonance absorption of these neutrons in the fuel can be quantified using 235U and 239Pu fission chambers placed adjacent to the assembly. The sensitivity of this technique is based on using the same fissile materials in the fission chambers as are present in the fuel because the effect of resonance absorption lines in the transmitted flux is amplified by the corresponding (n,f) reaction peaks in the fission chamber. SINRD requires calibration with a reference assembly of similar geometry. However, this densitometry method uses ratios of different fission chambers so that most systematic errors related to calibration and positioning cancel in the ratios.


international conference on advancements in nuclear instrumentation, measurement methods and their applications | 2011

A priori precision estimation for neutron Triples counting

Stephen Croft; Martyn T. Swinhoe; Vladimir Henzl

The nondestructive assay of Plutonium bearing items for criticality, safety, security, safeguards, inventory balance, process control, waste management and compliance is often undertaken using correlated neutron counting. In particular Multiplicity Shift Register analysis allows one to extract autocorrelation parameters from the pulse train which can, within the framework of a simple interpretational model, be related to the effective 240Pu spontaneous fission mass present. The effective 240Pu mass is a weighted sum of the 238Pu, 240Pu and 242Pu masses so if the relative isotopic composition of the Pu can be established from the measured 240Pu effective mass one can estimate the total Pu mass and also the masses of the individual isotopes, example the fissile species 239Pu and 241Pu. In multiplicity counting three counting rates are obtained. These are the Singles, Doubles and Triples rates. The Singles rate is just the gross, totals or trigger rate. The Doubles and Triples rates are calculated from factorial moments of the observed signal triggered neutron multiplicity distributions following spontaneous fission in the item and can be thought of as the rate of observed coincident pairs and coincident triplets on the pulse train. Coincident events come about because the spontaneous fission and induced fission chains taking place in the item result in bursts of neutrons. These remain time correlated during the detection process and so retain information, through the burst size distribution, about the Pu content. In designing and assessing the performance of a detector system to meet a given goal it is necessary to make a priori estimates of the counting precision for all three kinds of rates. This is non-trivial because the counting does not obey the familiar rules of a Poissonian counting experiment because the pulse train has time correlated events on it and the train is sampled by event triggered gates that may overlap. For Singles and Doubles simple approximate analytical empirical rules for how to estimate the variance have been developed guided by theory and refined by experiment. However, for Triples no equivalent rules have been put forward and tested until now. In this work we propose an analytical expression, the CSH relation, for the variance on the Triples count and exercise it against experimental data gathered for Pu items measured in the Los Alamos National Laboratorys Epithermal Neutron Multiplicity Counter (ENMC). Preliminary results are encouraging and reasonable agreement with observation, considered fit for scoping studies, is obtained. We have also looked at the behavior using Monte Carlo simulations.


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.


IEEE Transactions on Nuclear Science | 2013

Pulse Shape Discrimination Properties of Neutron-Sensitive Organic Scintillators

Andrea Favalli; M. L. Iliev; K. Chung; C. Hurlbut; H. P. Martinez; Martyn T. Swinhoe; Natalia P. Zaitseva; Kiril Dimitrov Ianakiev

The new plastic scintillators with n/γ pulse shape discrimination (PSD) properties being developed by the Lawrence Livermore National Laboratory (LLNL) and commercialized by Eljen Technology are addressing the toxicity and flammability issues of liquid scintillators, thus enabling a much wider range of practical applications for the detection of neutrons. These scintillation materials use multiple dyes, the concentration of which can vary, and therefore the light output and PSD properties of these new materials are expected to vary as well. In this paper, we compare the light signal time profiles of a liquid scintillator and two samples (one from LLNL and one from Eljen Technology) of new plastic scintillators with PSD properties. We acquired the light signal time profiles using both γ sources (60Co, 137Cs, 241Am) and neutrons calibrated in electron-equivalent by the gamma sources. The n/γ PSD properties for time profiles collected are analyzed and discussed with respect to charge integration time.


ieee nuclear science symposium | 2008

New generation enrichment monitoring technology for gas centrifuge enrichment plants

Kiril Dimitrov Ianakiev; Boian S. Alexandrov; Brian D Boyer; T. R. Hill; D.W. MacArthur; Thomas Marks; Calvin E. Moss; Blake P Nolen; Mark T. Paffett; Gregg A Sheppard; Martyn T. Swinhoe

We report our progress toward development of new generation on-line enrichment monitoring technology for UF6 gas centrifuge plants based on a transmission source and a NaI spectrometer. We use an X-ray tube with transmission filters instead of a decaying isotopic transmission source to eliminate the costly replacement of this source. The UF6 gas density measurement is based on the energy dependency of the mass attenuation for two characteristic X-ray lines generated by the transmission filters. An analytical expression for the UF6 density is derived and criteria for the selection of transmission energies are discussed. Because of the differential method of measurement, the UF6 gas density does not depend on the intensity of the X-ray source. We describe a design of a sealed UF6 gas test stand for development testing and calibration of various on-line enrichment monitoring instruments. The sealed source is intended to replace a UF6 gaseous loop currently used for calibration.


Filtration & Separation | 2004

Large area neutron detector based on /sup 6/Li ionization chamber with integrated body-moderator of high density polyethylene

Kiril Dimitrov Ianakiev; Martyn T. Swinhoe; Kiwhan Chung; E.A. McKigney

We describe the development of a large area neutron detector based on a pulse-mode ionization chamber lined with /sup 6/Li foil in a low-cost housing of HDPE (high density polyethylene) that serves as the moderator. The use of inexpensive materials, technology for mass production and simple construction, which integrates the basic components of the sensor together, results in a substantial cost reduction. For a given sensor size, detection efficiency, or counting time, the proposed detector is expected to provide an order-of magnitude cost reduction compared to current neutron detection technology. This paper describes the detection concept including the optimization of the design using neutron transport calculations. It also gives experimental results on some prototype units using neutron and gamma sources. The properties affecting long term counting stability are discussed. An approach to reduce the effect of outgassing from the HDPE body is suggested.

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Howard O. Menlove

Los Alamos National Laboratory

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Stephen J. Tobin

Los Alamos National Laboratory

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Kiril Dimitrov Ianakiev

Los Alamos National Laboratory

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Stephen Croft

Los Alamos National Laboratory

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Johnna B Marlow

Los Alamos National Laboratory

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Andrea Favalli

Los Alamos National Laboratory

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Vladimir Henzl

Los Alamos National Laboratory

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Louise G Evans

Los Alamos National Laboratory

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Daniela Henzlova

Los Alamos National Laboratory

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Carlos D. Rael

Los Alamos National Laboratory

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