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Neutron Energy Distribution Function Reconstructed From Time-of-Flight Signals in Deuterium Gas-Puff $Z$-Pinch
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Citations
21
References
2009
Year
EngineeringNuclear PhysicsFusion PowerFusion MaterialsPeak Neutron EnergyFusion NeutronsControlled Nuclear FusionFusion Reactor MaterialNuclear ReactorsHigh-energy Nuclear ReactionPhysicsNeutron SourceNuclear ReactionsNeutron TransportNuclear EngineeringNuclear AstrophysicsDeuterium Gas-puffNuclear EnergyTime-of-flight SignalsExperimental Nuclear PhysicsNatural SciencesFast DeuteronsApplied PhysicsNeutron Scattering
The implosion of a solid deuterium gas-puff <i xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">Z</i> -pinch was studied on the S-300 pulsed power generator [A. S. Chernenko, , Proceedings of 11th Int. Conf. on High Power Particle Beams, 154 (1996)]. The peak neutron yield above 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">10</sup> was achieved on the current level of 2 MA. The fusion neutrons were generated at about 150 ns after the current onset, i.e., during the stagnation and at the beginning of the expansion of a plasma column. The neutron emission lasted on average 25 ns. The neutron energy distribution function was reconstructed from 12 neutron time-of-flight signals by the Monte Carlo simulation. The side-on neutron energy spectra peaked at 2.42 plusmn 0.04 MeV with about 450-keV FWHM. In the downstream direction (i.e., the direction of the current flow from the anode toward the cathode), the peak neutron energy and the width of a neutron spectrum were 2.6 plusmn 0.1 MeV and 400 keV, respectively. The average kinetic energy of fast deuterons, which produced fusion neutrons, was about 100 keV. The generalized beam-target model probably fits best to the obtained experimental data.
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