J. A. Brown
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View article: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>12</mml:mn></mml:mmultiscripts></mml:math>(<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:msubsup><mml:mi>n</mml:mi><mml:mn>1</mml:mn><mml:mo>′</mml:mo></mml:msubsup><mml:mi>γ</mml:mi></mml:mrow></mml:math>) partial <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>γ</mml:mi></mml:math>-ray cross section measured using the GENESIS array
() partial -ray cross section measured using the GENESIS array Open
Improved neutron inelastic scattering cross sections have repeatedly been identified as a top priority nuclear data need, important for basic science and a range of applications in nuclear energy, stockpile stewardship, and proliferation d…
View article: Identifying Suitable Front Contacts for Cd(Se, Te) Solar Cells on Space-Qualified Cover Glass
Identifying Suitable Front Contacts for Cd(Se, Te) Solar Cells on Space-Qualified Cover Glass Open
To employ solar cells in space, achieving high specific power (W/kg) and radiation hardness is crucial. CdTe thin-film solar cells are expected to demonstrate the capability of achieving high specific power and radiation hardness comparabl…
View article: Measurement of the energy-differential <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Cl</mml:mi><mml:mprescripts/><mml:none/><mml:mn>35</mml:mn></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mmultiscripts><mml:mi mathvariant="normal">S</mml:mi><mml:mprescripts/><mml:none/><mml:mn>35</mml:mn></mml:mmultiscripts></mml:mrow></mml:math> cross section via the ratio with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Li</mml:mi><mml:mprescripts/><mml:none/><mml:mn>6</mml:mn></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>α</mml:mi><mml:mo>)</mml:mo><mml:mmultiscripts><mml:mi mathvariant="normal">H</mml:mi><mml:mprescripts/><mml:none/><mml:mn>3</mml:mn></mml:mmultiscripts></mml:mrow></mml:math>
Measurement of the energy-differential cross section via the ratio with Open
Knowledge of the neutron-induced 35Cl (n, x) cross sections is vital to the design and certification of molten chloride fast reactors (MCFRs) since the 35Cl (n, p0) 35S reaction is believed to b…
View article: Proton discrimination in CLYC for fast neutron spectroscopy
Proton discrimination in CLYC for fast neutron spectroscopy Open
View article: Characterization of a SiPM-based monolithic neutron scatter camera using dark counts
Characterization of a SiPM-based monolithic neutron scatter camera using dark counts Open
The Single Volume Scatter Camera (SVSC) Collaboration aims to develop portable neutron imaging systems for a variety of applications in nuclear non-proliferation. Conventional double-scatter neutron imagers are composed of several separate…
View article: PANDA-FES: Portable and Adaptable Neutron Diagnostics for Advancing Fusion Energy Science
PANDA-FES: Portable and Adaptable Neutron Diagnostics for Advancing Fusion Energy Science Open
Nuclear fusion is a potential source of carbon-free electricity with many concepts in development. The Portable and Adaptable Neutron Diagnostics for Advancing Fusion Energy Science (PANDA-FES) suite has been deployed since 2021 to measure…
View article: GENESIS: Gamma Energy Neutron Energy Spectrometer for Inelastic Scattering
GENESIS: Gamma Energy Neutron Energy Spectrometer for Inelastic Scattering Open
Improved neutron inelastic scattering cross section data are needed to inform integral benchmark studies and advance applications in a wide variety of areas including nuclear energy, stockpile stewardship, nonproliferation, and space explo…
View article: Characterization of a SiPM-based monolithic neutron scatter camera using dark counts
Characterization of a SiPM-based monolithic neutron scatter camera using dark counts Open
We report on the design and characterization of a prototype monolithic neutron scatter camera that is intended to significantly improve upon the geometrical shortcomings of conventional neutron cameras. The detector consists of a 50 mm $\t…
View article: Secondary neutron production from thick target deuteron breakup
Secondary neutron production from thick target deuteron breakup Open
Thick target deuteron breakup is a variable-energy accelerator-based source of high-energy neutrons, with applications in fundamental and applied nuclear science and engineering. However, the breakup mechanism remains poorly understood, an…
View article: Absolute light yield of the EJ-204 plastic scintillator
Absolute light yield of the EJ-204 plastic scintillator Open
The absolute light yield of a scintillator, defined as the number of scintillation photons produced per unit energy deposited, is a useful quantity for scintillator development, research, and applications. Yet, literature data on the absol…
View article: Measurement of proton light yield of water-based liquid scintillator
Measurement of proton light yield of water-based liquid scintillator Open
View article: Secondary Neutron Production from Thick Target Deuteron Breakup
Secondary Neutron Production from Thick Target Deuteron Breakup Open
Thick target deuteron breakup is a variable-energy accelerator-based source of high-energy neutrons, with applications in fundamental and applied nuclear science and engineering. However, the breakup mechanism remains poorly understood, an…
View article: The 40Ar(d,p)41Ar cross section between 3–7 MeV
The 40Ar(d,p)41Ar cross section between 3–7 MeV Open
View article: Modeling ionization quenching in organic scintillators
Modeling ionization quenching in organic scintillators Open
Ionization quenching models were assessed by evaluating light yield data from multiple organic scintillators and recoil ions over a fission spectrum neutron energy range, important for basic science and applications.
View article: Thermonuclear neutron emission from a sheared-flow stabilized Z-pinch
Thermonuclear neutron emission from a sheared-flow stabilized Z-pinch Open
The fusion Z-pinch experiment (FuZE) is a sheared-flow stabilized Z-pinch designed to study the effects of flow stabilization on deuterium plasmas with densities and temperatures high enough to drive nuclear fusion reactions. Results from …
View article: Simultaneous measurement of organic scintillator response to carbon and proton recoils
Simultaneous measurement of organic scintillator response to carbon and proton recoils Open
Organic scintillators are widely used for neutron detection in both basic nuclear physics and applications. While the proton light yield of organic scintillators has been extensively studied, measurements of the light yield from neutron in…
View article: Comparative scintillation performance of EJ-309, EJ-276, and a novel organic glass
Comparative scintillation performance of EJ-309, EJ-276, and a novel organic glass Open
An organic glass scintillator developed by Sandia National Laboratories was characterized in terms of its light output and pulse shape discrimination (PSD) properties and compared to commercial liquid (EJ-309) and plastic (EJ-276) organic …
View article: The Single-Volume Scatter Camera
The Single-Volume Scatter Camera Open
The multi-institution Single-Volume Scatter Camera (SVSC) collaboration led by Sandia National Laboratories (SNL) is developing a compact, high-efficiency double-scatter neutron imaging system. Kinematic emission imaging of fission-energy …
View article: Scintillator light yield measurements with waveform digitizers
Scintillator light yield measurements with waveform digitizers Open
View article: Publisher's Note: Statistical properties of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi>Pu</mml:mi><mml:mprescripts/><mml:none/><mml:mn>243</mml:mn></mml:mmultiscripts></mml:math>, and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi>Pu</mml:mi><mml:mprescripts/><mml:none/><mml:mn>242</mml:mn></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math> cross section calculation [Phys. Rev. C <b>93</b>, 014323 (2016)]
Publisher's Note: Statistical properties of , and cross section calculation [Phys. Rev. C <b>93</b>, 014323 (2016)] Open
Received 4 September 2019DOI:https://doi.org/10.1103/PhysRevC.100.039901©2019 American Physical SocietyPhysics Subject Headings (PhySH)A ≥ 220PropertiesNuclear mass rangesA ≥ 220Research AreasCollective levelsEnergy levelsResonance reactio…
View article: SCEMA: a high channel density electronics module for fast waveform capture
SCEMA: a high channel density electronics module for fast waveform capture Open
The development of fast, highly pixelated photodetectors with single-photon sensitivity has the potential to enable a variety of new radiation detection concepts. Systems that desire to employ these detectors without loss of information de…
View article: Interaction position, time, and energy resolution in organic scintillator bars with dual-ended readout
Interaction position, time, and energy resolution in organic scintillator bars with dual-ended readout Open
View article: Performance evaluation of an energy tuning assembly for neutron spectral shaping
Performance evaluation of an energy tuning assembly for neutron spectral shaping Open
View article: Low energy light yield of fast plastic scintillators
Low energy light yield of fast plastic scintillators Open
View article: FIER: Software for analytical modeling of delayed gamma-ray spectra
FIER: Software for analytical modeling of delayed gamma-ray spectra Open
View article: Neutron Spectroscopy for pulsed beams with frame overlap using a double time-of-flight technique
Neutron Spectroscopy for pulsed beams with frame overlap using a double time-of-flight technique Open
View article: The 88-Inch Cyclotron: A one-stop facility for electronics radiation and detector testing
The 88-Inch Cyclotron: A one-stop facility for electronics radiation and detector testing Open
View article: Neutron transfer in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts><mml:mo>+</mml:mo><mml:mmultiscripts><mml:mi>Au</mml:mi><mml:mprescripts/><mml:none/><mml:mn>197</mml:mn></mml:mmultiscripts></mml:mrow></mml:math> reaction from gold isotope residuals
Neutron transfer in the reaction from gold isotope residuals Open
Residual gold nuclei were produced in this paper via neutron transfer at multiple energies using a 130-MeV 13C beam incident on a stacked-foil target consisting of alternating layers of 197Au and 27Al. Prod…
View article: Energy dependence of the prompt<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>γ</mml:mi></mml:math>-ray emission from the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mo>(</mml:mo><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math>-induced fission of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">U</mml:mi><mml:none/><mml:mo>*</mml:mo><mml:mprescripts/><mml:none/><mml:mn>234</mml:mn></mml:mmultiscripts></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi>Pu</mml:mi><mml:none/><mml:mo>*</mml:mo><mml:mprescripts/><mml:none/><mml:mn>240</mml:mn></mml:mmultiscripts></mml:math>
Energy dependence of the prompt-ray emission from the-induced fission ofand Open
Prompt-fission γ rays are responsible for approximately 5% of the total energy released in fission, and therefore important to understand when modeling nuclear reactors. In this work we present prompt γ-ray emission characteristics in fiss…
View article: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi mathvariant="bold">La</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>137</mml:mn><mml:mo>,</mml:mo><mml:mn>138</mml:mn><mml:mo>,</mml:mo><mml:mn>139</mml:mn></mml:mrow></mml:mmultiscripts><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math> cross sections constrained with statistical decay properties of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="bold">La</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>138</mml:mn><mml:mo>,</mml:mo><mml:mn>139</mml:mn><mml:mo>,</mml:mo><mml:mn>140</mml:mn></mml:mrow></mml:mmultiscripts></mml:math> nuclei
cross sections constrained with statistical decay properties of nuclei Open
The nuclear level densities and $\\gamma$-ray strength functions of\n$^{138,139,140}$La were measured using the $^{139}$La($^{3}$He, $\\alpha$),\n$^{139}$La($^{3}$He, $^{3}$He$^\\prime$) and $^{139}$La(d, p) reactions. The\nparticle-$\\gam…