Magnetic field profile for improved ion laser performance

Coherent light generators – Having an applied magnetic field

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372 61, 372 62, 372 67, H01S 300, H01S 303

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049742280

ABSTRACT:
An ion laser is constructed with means for generating a magnetic confinement field operating in the cathode transition region of the laser. The magnetic confinement field is preferably generated by first and second magnetic windings, each axially aligned with the laser volume, but disposed so as to generate first and second magnetic fields which are of opposite polarity. The first and second magnetic fields of opposite polarity combine to create a region of zero axial magnetic field, which in a preferred embodiment is located substantially within the cathode transition region of the laser. In an alternate embodiment, the first and second magnetic fields are of the same polarity, and therefore generate a region of minimized axial magnetic field, preferably located substantially within the cathode transition region of the laser.

REFERENCES:
patent: 3670262 (1972-06-01), Hallock et al.
patent: 3993965 (1976-11-01), Alves et al.
patent: 4649547 (1987-03-01), Carlson et al.
patent: 4715039 (1987-12-01), Miller et al.
patent: 4811355 (1989-03-01), Krueger et al.
patent: 4847841 (1989-08-01), Lamprecht et al.
Ferdinand F. Cap, "Handbook on Plasma Instabilities", vol. I, (Academic Press, N.Y., 1976), Chapter 8, Plasma Containment, pp. 131-153.
Kobayashi et al., "Power Enhancement for Argon II Narow Tube Lasers by a Traverse Magnetic Field", (Appl. Phys. Lett. 40 (19), May 15, 1985) pp. 925-927.
Kobayashi et al., "Power Enhancement in Argon II Narrow-Tube Lasers Due to Zeeman Effect by a Transverse Magnetic Field", (IEEE Journal of Quantum Electronics, vol. QE-23, No. 5, May 1987) pp. 633-640.
The Lexel Laser pamphlet (Feb. 16, 1989).

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