Gas laser and method of operation

Claim 2

In the method of operating a laser device having a lasing cavity having an optical axis and a gseous lasing medium having an upper lasing level disposed in said lasing cavity, the steps comprising: (a) pumping said lasing medium therein to produce population inversion and stimulated emission in the saturated regime wherein the rate of stimulated emission is at least not substantially less than the sum of all other rates at which population is transferred out of said upper lasing level; (b) causing the rate of collisions of lasing atoms and molecules occuring in said lasing medium during pumping to occur less rapidly than the sum of all the rates at which population is transferred out of said upper lasing level; (c) generating within said cavity a DC magnetic field having an axis having a first predetermined orientation at least a component of which is transverse to the optical axis and of amplitude sufficient to induce an electron precession rate large compared to the said transition rate out of said upper lasing level; and (d) polarizing laser light generated in said cavity to cause said light to have a predominate polarization orientated with respect to the axis of said magnetic field at angle of at least about 55° and less than 90°.

Claim 3

The method as defined in claim 1 wherein the laser device is an excimer laser.

Claim 4

The method as defined in claim 1 wherein the strength of said magnetic field is greater than 1,000 gauss.

Claim 5

The method as defined in claim 1 wherein the laser device is an excimer amplifier laser, the axis of the magnetic field is normal to the optical axis and the strength of the magnetic field is about 10,000 gauss.

Claim 6

The method as defined in claim 1 wherein said second orientation of said laser light is provided by Brewster windows.

Claim 7

The method as defined in claim 1 wherein the said second orientation of said laser light is provided by intracavity optics.

Claim 8

The method as defined in claim 1 wherein the laser device is an amplifier laser and an externally generated laser beam is introduced into said lasing cavity.

Claim 9

The method as defined in claim 7 wherein said external laser beam is generated to have said second predetermined orientation.

Claim 10

The method as defined in claim 1 wherein said second predetermined orientation lies in a plane normal to the optical axis.

Claim 11

In gas laser apparatus having a lasing cavity having an optical axis, a gaseous lasing medium having an upper lasing level disposed in said lasing cavity, and means for pumping said lasing medium therein to produce population inversion and stimulated emission in the saturated regime wherein the rate of stimulated emission is at least not substantially less than the sum of all other rates at which population is depleted from said upper laser level, the rate of collisions of lasing atoms and molecules during pumping occurring less rapidly than the transition rate at which said population is depleted from said upper lasing level, the combination comprising: (a) first means for generating within said cavity a DC magnetic field having an axis having a first predetermined orientation at least a component of which is transverse to the optical axis and having a field strength sufficient to induce an electron precession rate large compared to the said transition rate out of the upper lasing level of said gaseous medium; and (b) second means for providing laser light generated in said cavity to have predominate polarization having a second predetermined orientation, said first and second means providing said first and second orientations at an angle of at least about 55° one with another but less than 90°.

Claim 12

In gas laser apparatus having a lasing cavity having an optical axis, a gaseous lasing medium having an upper lasing level disposed in said lasing cavity, and means for pumping said lasing medium therein to produce population inversion and stimulated emission in the saturated regime wherein the rate of stimulated emission is at least not substantially less than the sum of all other rates at which population is depleted from said upper laser level, the rate of collisions of lasing atoms and molecules during pumping occurring less rapidly than the transition rate at which said population is depleted from said upper lasing level, the combination comprising: (a) first means for generating within said cavity a DC magnetic field having an axis having a first predetermined orientation at least a component of which is transverse to the optical axis and having a field strength sufficient to induce an electron precession rate large compared to the said transition rate out of the upper lasing level of said gaseous medium; and (b) second means for providing laser light generated in said cavity to have predominate polarization having a second predetermined orientation, said first and second means providing said first and second orientations at an angle of at least about 55° one with another but less than 90°.

Claim 13

The combination as defined in claim 10 wherein the strength of said magnetic field transverse to the optical axis is not less than 1,000 gauss.

Claim 14

The combination as defined in claim 10 wherein said first predetermined axis of said magnetic field is normal to the optical axis and the strength of said magnetic field is about 10,000 gauss.

Claim 15

The combination as defined in claim 10 wherein said second means comprises intracavity optic means.

Claim 16

The combination as defined in claim 10 wherein said lasing cavity is terminated by window means transparent to said stimulated emission and concentric about said optic axis, and additionally including third means for generating externally of said lasing cavity, a polarized laser beam having said second predetermined orientation and passing said laser beam through said lasing cavity along said optical axis.

Claim 17

The combination as defined in claim 10 wherein said first predetermined orientation at least substantially lies in a plane normal to the optical axis, and the second predetermined orientation lies in a plane normal to the optic axis.