Improved operation of the nonambipolar electron source.

Significant improvements have been made to the nonambipolar electron source (NES), a radio frequency (rf) plasma-based electron source that does not rely on electron emission at a cathode surface [B. Longmier, S. Baalrud, and N. Hershkowitz, Rev. Sci. Instrum. 77, 113504 (2006)]. A prototype NES has produced 30 A of continuous electron current, using 2 SCCM (SCCM denotes cubic centimeter per minute at STP) Xe, 1300 W rf power at 13.56 MHz, yielding a 180 times gas utilization factor. A helicon mode transition has also been identified during NES operation with an argon propellant, using 15 SCCM Ar, 1000 W rf, and 100 G magnetic field. This NES technology has the ability to replace hollow cathode electron sources and to enable high power electric propulsion missions, eliminating one of the lifetime restrictions that many ion thrusters have previously been faced with.

[1]  R. C. Weast CRC Handbook of Chemistry and Physics , 1973 .

[2]  Noah Hershkowitz,et al.  3 – How Langmuir Probes Work , 1989 .

[3]  James H. Gilland Mission and system optimization of nuclear electric propulsion vehicles for lunar and Mars missions , 1991 .

[4]  N. Hershkowitz,et al.  Radial control of the electrostatic potential in a tandem mirror with quadrupole end cells , 1992 .

[5]  J. Stevens 7 – Electron Cyclotron Resonance Plasma Sources , 1995 .

[6]  V. Godyak,et al.  The electron-energy distribution function in a shielded argon radiofrequency inductive discharge , 1995 .

[7]  Francis F. Chen Physics of helicon discharges , 1996 .

[8]  D. Korzec,et al.  Microwave plasma source for high current ion beam neutralization , 2000 .

[9]  Amy E. Wendt,et al.  High-density plasma sources , 2000 .

[10]  H. Kuninaka,et al.  Overdense Plasma Production in a Low-power Microwave Discharge Electron Source , 2001 .

[11]  B. Lindsay,et al.  Determination of the absolute partial and total cross sections for electron-impact ionization of the rare gases , 2002 .

[12]  K. P. Shamrai,et al.  Wave stimulated phenomena in inductively coupled magnetized plasmas , 2005 .

[13]  N. Hershkowitz,et al.  Nonambipolar electron source , 2006 .

[14]  N. Hershkowitz,et al.  Global nonambipolar flow: Plasma confinement where all electrons are lost to one boundary and all positive ions to another boundary , 2007 .

[15]  Francis F. Chen,et al.  Large-area helicon plasma source with permanent magnets , 2007 .