Design and initial results from a kilojoule level Dense Plasma Focus with hollow anode and cylindrically symmetric gas puff.

We have designed and built a Dense Plasma Focus (DPF) Z-pinch device using a kJ-level capacitor bank and a hollow anode, and fueled by a cylindrically symmetric gas puff. Using this device, we have measured peak deuteron beam energies of up to 400 keV at 0.8 kJ capacitor bank energy and pinch lengths of ∼6 mm, indicating accelerating fields greater than 50 MV/m. Neutron yields of on the order of 10(7) per shot were measured during deuterium operation. The cylindrical gas puff system permitted simultaneous operation of DPF with a radiofrequency quadrupole accelerator for beam-into-plasma experiments. This paper describes the machine design, the diagnostic systems, and our first results.

[1]  G. Gerdin,et al.  Faraday cup analysis of ion beams produced by a dense plasma focus , 1981 .

[2]  J. Frenje,et al.  Compact multichannel neutral particle analyzer for measurement of energetic charge-exchanged neutrals in Alcator C-Mod , 2006 .

[3]  Cesar H. Moreno,et al.  Conceptual engineering of plasma-focus thermonuclear pulsors , 2000 .

[4]  A. Clausse,et al.  A lumped parameter model of plasma focus , 2004, IEEE Transactions on Plasma Science.

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

[6]  A. Clausse,et al.  Modeling of the Dynamic Plasma Pinch in Plasma Focus Discharges Based in Von Karman Approximations , 2009, IEEE Transactions on Plasma Science.

[7]  H. Schmidt,et al.  Gas-puff target experiments with the Poseidon plasma focus facility , 1994 .

[8]  C. Grant,et al.  Spatiotemporal temperature and density characterization of high-power atmospheric flashover discharges over inert poly(methyl methacrylate) and energetic pentaerythritol tetranitrate dielectric surfaces , 2012 .

[9]  J. Mather Investigation of the High‐Energy Acceleration Mode in the Coaxial Gun , 1964 .

[10]  M. Mathuthu,et al.  The three-phase theory for plasma focus devices , 1997 .

[11]  G. Murtaza,et al.  ROLE OF ANODE LENGTH IN A MATHER-TYPE PLASMA FOCUS , 1992 .

[12]  K. Schönbach,et al.  Neutron-, ion-, and electron-energy spectra in a 1 kJ plasma focus , 1975 .

[13]  Plasma focus based repetitive source of fusion neutrons and hard x-rays , 2008, 0901.2007.

[14]  W. Kies,et al.  High performance 300 kV driver speed 2 for MA pinch discharges , 1986 .

[15]  E. L. Jacobs,et al.  The Lead Activation Technique for High Energy Neutron Measurement , 1965 .

[16]  T. L. Tan,et al.  Drive Parameter as a Design Consideration for Mather and Filippov Types of Plasma Focus , 2006, IEEE Transactions on Plasma Science.

[17]  W. Kies Power limits for dynamical pinch discharges , 1986 .

[18]  W. Bostick,et al.  CORRIGENDUM: Time resolved energy spectrum of the axial ion beam generated in plasma focus discharges , 1993 .

[19]  D. Welch,et al.  Fully kinetic simulations of dense plasma focus Z-pinch devices. , 2012, Physical review letters.

[20]  L. Soto New trends and future perspectives on plasma focus research , 2005 .

[21]  W. Kies,et al.  The first and the final fifty nanoseconds of a fast focus discharge , 1983 .

[22]  Yves Peysson,et al.  Hard x-ray diagnostic for lower hybrid experiments on Alcator C-Mod , 2006 .

[23]  K. Koshelev,et al.  Pinch modes produced in the SPEED2 plasma focus , 2000 .