Kinetic simulation of thermonuclear-neutron production by a 107-A deuterium Z pinch

Fully kinetic simulations have demonstrated that at sufficiently high currents, half of the neutrons produced by a deuterium Z-pinch are thermonuclear in origin. At 150-kA pinch current, O. A. Anderson et al. [Phys. Rev. 110, 1375 (1958)] clearly shows that essentially all of the neutrons produced by a deuterium pinch are not thermonuclear, but are initiated by an instability that creates beam-target neutrons. Since this paper, many subsequent authors have supported this result while others have claimed that pinch neutrons are, on the contrary, thermonuclear. To resolve this issue, fully kinetic, collisional, and electromagnetic simulations of the complete time evolution of a deuterium pinch have been performed. The simulations were performed with the implicit particle-in-cell code LSP, as described in D. R. Welch et al. [Phys. Rev. Lett. 103, 255002 (2009)]. At 106 -A pinch currents, most of the neutrons are, indeed, beam-target in origin. At 15-MA current, half of the neutrons are thermonuclear and half...

[1]  J. Leboeuf,et al.  Development of global magnetohydrodynamic instabilities in Z-pinch plasmas in the presence of nonideal effects , 2004 .

[2]  M. Cuneo,et al.  Architecture of petawatt-class z-pinch accelerators. , 2007 .

[3]  G. Gerdin,et al.  Particle beams generated by a 6–12.5 kJ dense plasma focus , 1982 .

[4]  J. Huba NRL: Plasma Formulary , 2004 .

[5]  W. Stygar,et al.  Optimized transmission-line impedance transformers for petawatt-class pulsed-power accelerators , 2008 .

[6]  J. Meyer-ter-Vehn,et al.  The physics of inertial fusion - Hydrodynamics, dense plasma physics, beam-plasma interaction , 2004 .

[7]  Robert W. Clark,et al.  Neutron production and implosion characteristics of a deuterium gas-puff Z pinch , 2007 .

[8]  G. Cooper,et al.  Deuterium gas-puff Z-pinch implosions on the Z acceleratora) , 2006 .

[9]  T. A. Mehlhorn,et al.  Integrated simulation of the generation and transport of proton beams from laser-target interaction , 2006 .

[10]  H. Yousefi,et al.  Simulation of high-energy proton production by fast magnetosonic shock waves in pinched plasma discharges , 2007 .

[11]  Robert W. Clark,et al.  Z-pinch plasma neutron sources , 2007 .

[12]  Michael H Frese MACH2: A two-dimensional magnetohydrodynamic simulation code for complex experimental configurations , 1987 .

[13]  Shigeru Yonemura,et al.  Weighted Particles in Coulomb Collision Simulations Based on the Theory of a Cumulative Scattering Angle , 1998 .

[14]  R J Leeper,et al.  Fully kinetic particle-in-cell simulations of a deuterium gas puff z pinch. , 2009, Physical review letters.

[15]  S. Colgate,et al.  Neutron Production in Linear Deuterium Pinches , 1958 .

[16]  Gerber,et al.  Enhanced stability and neutron production in a dense Z-pinch plasma formed from a frozen deuterium fiber. , 1987, Physical review letters.

[17]  H. Yousefi,et al.  Simulation of high-energy particle production through sausage and kink instabilities in pinched plasma discharges , 2006 .

[18]  A. Dangor,et al.  Snowplow-like behavior in the implosion phase of wire array Z pinches , 2002 .

[19]  Arber Td Hybrid Simulation of the Nonlinear Evolution of a Collisionless, Large Larmor Radius Z Pinch. , 1996 .

[20]  C. W. Barnes,et al.  Principles and capabilities of 3-D, E-M particle simulations , 1980 .

[21]  L. Juha,et al.  Neutron Energy Distribution Function Reconstructed From Time-of-Flight Signals in Deuterium Gas-Puff $Z$-Pinch , 2009, IEEE Transactions on Plasma Science.