Diode pumped low doped Nd 3+ glass laser

Claim 2

In a method for obtaining laser radiation, the steps of: optically pumping Nd 3+ lasant ions of a laser gain medium with the output optical radiation of a light emitting semiconductive diode; said gain medium comprises a glass member doped with the Nd 3+ lasant ions to a density of less than 10×10 20 cm -3 such that the laser gain medium has an optical loss at the wavelength of the lasant transition of less than 0.2 per meter and has a gain cross-section less than 8×10 -20 cm 2 ; resonating coherent lasant optical readiation emitted by a lasant transition of said optically pumped lasant Nd 3+ ions of said gain medium within an optical resonator containing said optically pumped gain medium and having at least one concave reflector to obtain output laser radiation; and focusing the resonant lasant radiation within said optical resonator and within said gain medium such that the predominant focusing mechanism for focusing the resonant radiation within said gain medium is focusing from a concave optical focusing element disposed on the optical axis of the optical resonator.

Claim 3

The method of claim 1 wherein the step of optically pumping the Nd 3+ ions of the laser gain medium comprises the steps of directing the optical pumping radiation into the laser gain medium in a direction generally collinearly with the optical axis of the optical resonator.

Claim 4

The method of claim 1 wherein the optical pumping radiation is coherent.

Claim 5

The method of claim 1 wherein the optical resonator is defined by faces of said laser gain medium.

Claim 6

The method of claim 1 including the step of incorporating an optically nonlinear material within said optical resonator for generating optical radiation of a wavelength harmonically related to the wavelength of the lasant transition of the optically pumped Nd 3+ ions.

Claim 7

The method of claim 1 wherein the optical pumping radiation has a substantial proportion of its energy falling within the band of wavelengths from 780 nm to 830 nm.

Claim 8

The method of claim 1 wherein the optical pumping radiation is continuous wave.

Claim 9

The method of claim 7 including the step of incorporating a pulser selected from the group consisting of electro-optic and acoustic-optic pulsers within said optical resonator and pulsing said pulser to obtain pulses of output laser radiation.

Claim 10

The method of claim 1 wherein said laser gain medium is a slab of Nd 3+ doped glass having a pair of mutually opposed broad side faces between which the resonant lasant radiation is reflected in a zig-zag path, and wherein the optical pumping radiation is directed into the slab through at least one of said broad side faces.

Claim 11

In a laser: gain medium means comprising a glass member doped with Nd 3+ lasant ions to a density of less than 5×10 20 cm -3 such that said laser gain medium means has an optical loss at the wavelength of the lasant transition of less than 0.2 per meter and has a gain cross-section less than 8×10 -20 cm 2 ; optical pumping means for optically pumping the Nd 3+ lasant ions of said laser gain medium means with the output optical radiation of a light-emitting semiconductor diode; optical resonator means for resonating coherent lasant optical radiation emitted by a lasant transition of said optically pumped lasant Nd 3+ ions of said gain medium means within said optical resonator means containing said optically pumped gain medium means to obtain output laser radiation; and focusing means for focusing the resonant lasant radiation within said optical resonator means and within the said gain medium means such that the predominant focusing mechanism for focusing the resonant radiation within said gain medium means is focusing from a concave optical focusing element disposed on the optical axis of the optical resonator means.

Claim 12

In a laser: gain medium means comprising a glass member doped with Nd 3+ lasant ions to a density of less than 5×10 20 cm -3 such that said laser gain medium means has an optical loss at the wavelength of the lasant transition of less than 0.2 per meter and has a gain cross-section less than 8×10 -20 cm 2 ; optical pumping means for optically pumping the Nd 3+ lasant ions of said laser gain medium means with the output optical radiation of a light-emitting semiconductor diode; optical resonator means for resonating coherent lasant optical radiation emitted by a lasant transition of said optically pumped lasant Nd 3+ ions of said gain medium means within said optical resonator means containing said optically pumped gain medium means to obtain output laser radiation; and focusing means for focusing the resonant lasant radiation within said optical resonator means and within the said gain medium means such that the predominant focusing mechanism for focusing the resonant radiation within said gain medium means is focusing from a concave optical focusing element disposed on the optical axis of the optical resonator means.

Claim 13

The laser of claim 10 wherein said optical pumping means includes means for directing the optical pumping radiation into said laser gain medium means in a direction generally collinearly with the optical axis of said optical resonator means.

Claim 14

The laser of claim 10 wherein said optical pumping means includes a semiconductor laser diode.

Claim 15

The laser of claim 10 wherein said optical resonator means is defined by faces of said laser gain medium means.

Claim 16

The laser of claim 10 including: nonlinear optic material disposed within said optical resonator means for interaction with said resonant lasant radiation for generating optical radiation of a wavelength harmonically related to the wavelength of the lasant transitions of the optically pumped Nd 3+ ions.

Claim 17

The laser of claim 10 including: pulser means selected from the group of electro-optic and acoustic-optic pulsers disposed within said optical resonator means for pulsing operation of the laser to obtain pulses of output laser radiation.

Claim 18

The laser of claim 10 wherein said laser gain medium means is a slab of Nd 3+ ion doped glass having a pair of mutually opposed broad side faces between which the resonant lasant radiation is reflected in a zig-zag path; and wherein the optical pumping radiation is directed into said slab through at least one of said broad side faces.