# US 4,397,025 A · Dual frequency laser

> Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt

- Number: US 4,397,025 A
- Document ID: US4397025A
- Status: Granted
- Kind: A
- Application number: 06/195,241
- Filed: 1980-10-08
- Granted: 1983-08-02
- Earliest claimed: 1980-10-08
- Assignees: Environmental Research & Technology, Inc.
- Inventors: Paul L. Kebabian
- Web page: https://patentgrep.com/patent/US4397025A

## CPC

- H01S 3/102: by controlling the active medium, e.g. by controlling the processes or apparatus for excitation (H01S3/13 takes precedence)
- H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL

## Abstract

A method and apparatus for operating a dual-frequency gas laser so as to controllably switch between frequencies makes use of a cavity so tuned that the comb of resonant frequencies is not commensurate with the frequency difference between the laser operating frequencies, and, in a preferred embodiment, with one of the resonant frequencies tuned to coincide with one of the operating frequencies. The cavity length and overall gain at each frequency are so selected that the spacing between resonant frequencies is greater than the breadth above unity gain of the individual peaks of the gain vs. frequency curve. The active material is subjected to a magnetic field which may be varied in a controlled manner. In a preferred embodiment, this field is applied normal to the optical axis of the resonant cavity, and an optical element within the cavity is arranged to act as a plane polarizer with its plane of polarization normal to the magnetic field.

## Claims

### Claim 1

In a laser oscillator having a resonant optical cavity including an optical axis, at least a portion of said cavity containing an active gaseous material capable of supporting laser action over a first limited frequency range and a second limited frequency range remote from one another and centered respectively at a first center frequency and a second center frequency, said cavity being tuned such that simultaneously (a) adjacent resonant frequencies thereof are spaced apart by a frequency spacing which has a magnitude at least of the order of one of said limited frequency ranges, (b) the difference in frequency between said first center frequency and said second center frequency is a non-integral multiple of said frequency spacing, and (c) one of said resonant frequencies substantially coincides with said first center frequency; the improvement comprising,
means for providing a magnetic field in said active gaseous material so as to produce Zeeman-splitting which characteristically serves to divide each of said limited frequency ranges into a plurality of similar secondary frequency ranges, said magnetic field having an operating field strength sufficient simultaneously to frequency-shift ones of said secondary frequency ranges centered at said first center frequency away from said first center frequency by a frequency increment on the order of at least half of said first limited frequency range, and to frequency-shift ones of said secondary frequency ranges centered at said second center frequency away from said second center frequency by a frequency increment on the order of at least the frequency difference between said second center frequency and an adjacent one of said resonant frequencies; and
means for varying said magnetic field so as to control the intensity and frequency of electromagnetic radiation generated by said laser oscillator.

### Claim 2 (depends on 1)

The improvement in a laser oscillator according to claim 1 wherein said means for varying constitutes means for alternatively selecting the frequencies of said radiation at either said first center frequency or at said one of said resonant frequencies adjacent said second center frequency.

### Claim 3 (depends on 1)

The improvement in a laser oscillator according to claim 1 wherein said means for varying said magnetic field can vary said field strength between substantially zero and at least said operating field strength, said means for providing said field being disposed to produce said magnetic field with a predominant field direction fixed in a first direction relative to said optical axis at said portion of said optical cavity.

### Claim 4 (depends on 3)

The improvement in a laser oscillator according to claim 3 wherein said first direction is substantially normal to said optical axis within said portion of said cavity and wherein additionally said optical cavity is provided with polarizing means for selectively removing from interaction within said optical cavity such electromagnetic radiation generated by said active gaseous material and propagating parallel to said optical axis as has an electric field vector parallel to said first direction.

### Claim 5 (depends on 3)

The improvement in a laser oscillator according to claim 3 wherein said first direction is substantially parallel to said optical axis within said portion of said optical cavity.

### Claim 6 (depends on 1)

The improvement in a laser oscillator according to claim 1 wherein said optical cavity is provided with polarizing means for selectively removing from interaction within said optical cavity such electromagnetic radiation generated by said active gaseous material and propagating parallel to said optical axis as has an electric field vector oriented in a given direction, wherein said means for producing said magnetic field can provide a substantially constant magnetic field strength with a predominant field direction, and wherein said means for varying said magnetic field can alter said predominant field direction relative to said polarizing means so as to alternately bring said predominant field direction parallel to and normal to said given direction.

### Claim 7

A laser oscillator comprising in combination:
a resonant optical cavity including an optical axis, at least a portion of said cavity containing an active gaseous material capable of supporting laser action over a first limited frequency range and a second limited frequency range centered respectively at a first center frequency and a second center frequency remote from one another and equidistant from a third frequency, said cavity being tuned such that simultaneously (a) adjacent resonant frequencies thereof are spaced apart by a frequency spacing which has a magnitude at least on the order of one of said limited frequency ranges, (b) said resonant frequencies respectively nearest said first and second center frequencies are respectively disposed to be displaced therefrom by equal frequency differences on the order of at least one quarter of said one of said limited frequency range, and (c) said resonant frequencies are disposed substantially symmetrically about said third frequency;
means for providing a magnetic field in said active gaseous material so as to product Zeeman-splitting which characteristically serves to divide each of said limited frequency ranges into a plurality of similar secondary frequency ranges, said magnetic field having a predominant field direction substantially parallel to said optical axis within said portion of said cavity and having an operating field strength sufficient to frequency-shift ones of said secondary frequency ranges away from the respective said first and second center frequencies a frequency increment on the order of at least the frequency difference between said first and second center frequencies and the respectively nearest resonant frequencies; and
means for varying said magnetic field so that said predominant field direction may be selectively reversed relative to said optical axis.

### Claim 8 (depends on 7)

Apparatus according to claim 7 and further including means for selecting circularly polarized electromagnetic radiation of a given handedness generated by said gaseous material and initially propagating parallel to said optical axis within said portion.

### Claim 9

A method for controlling the output of a laser oscillator including a resonant optical cavity having an optical axis, at least a portion of said cavity containing an active gaseous material capable of supporting laser action over a first limited frequency range and a second limited frequency range remote from one another and centered respectively at a first center frequency and a second center frequency, said method comprising the steps of:
(1) tuning said cavity such that simultaneously (a) adjacent resonant frequencies thereof are spaced apart by a frequency spacing which has a magnitude at least of the order of one of said limited frequency ranges, (b) the difference in frequency between said first center frequency and said second center frequency is a non-integral multiple of said frequency spacing, and (c) one of said resonant frequencies substantially coincides with said first center frequency;
(2) subjecting said active gaseous material in said cavity to a magnetic field so as to divide each of said limited frequency ranges into a plurality of similar secondary frequency ranges by Zeeman-splitting, said magnetic field having an operating field strength sufficient simultaneously to frequency-shift ones of said secondary frequency ranges centered at said first center frequency away from said first center frequency by a frequency increment on the order of at least half of said first limited frequency range, and to frequency-shift ones of said secondary frequency ranges centered at said second center frequency away from said second center frequency a frequency increment on the order of at least the frequency difference between said second center frequency and an adjacent one of said resonant frequencies; and
(3) varying said magnetic field so that the intensity and frequency of the electromagnetic radiation generated by said laser oscillator may be controlled.

### Claim 10 (depends on 9)

The method according to claim 9 wherein selective control of said electromagnetic radiation includes alternative selection of frequencies of said radiation to be at said first center frequency and at said one of said resonant frequencies adjacent said second center frequency.

### Claim 11 (depends on 9)

The method according to claim 9 wherein the step of varying said magnetic field comprises varying the field strength of said magnetic field between substantially zero and at least said operating field strength, said magnetic field being disposed with a predominant field direction fixed relative to said optical axis at said portion of said optical cavity.

### Claim 12 (depends on 11)

The method according to claim 11 wherein said predominant field direction is disposed substantially normal to said optical axis within said portion, said method further including the step of selectively removing from interaction with said optical cavity electromagnetic radiation generated by said active gaseous material propagating parallel to said optical axis and having an electric field vector parallel to said predominant field direction.

### Claim 13 (depends on 11)

The method according to claim 11 wherein said predominant field direction is disposed substantially parallel to said optical axis within said portion.

### Claim 14 (depends on 9)

The method according to claim 9 wherein said magnetic field has a constant magnetic field strength substantially equal to said operating field strength and is disposed with a predominant field direction normal to said optical axis at said portion of said cavity, said method further including the step of selectively removing from interaction within said optical cavity electromagnetic radiation generated by said active gaseous material propagating parallel to said optical axis and having an electric field vector oriented in a given direction, said step of varying said magnetic field comprising alternately bringing said predominant field direction substantially parallel to and normal to said given direction.

### Claim 15

A method for controlling the output of a laser oscillator including a resonant optical cavity having an optical axis, at least a portion of said cavity containing an active gaseous material capable of supporting laser action over a first limited frequency range and a second limited frequency range remote from one another and centered respectively at a first center frequency and a second center frequency and equidistant from a third frequency, said method comprising the steps of:
(1) tuning said cavity such that simultaneously (a) adjacent resonant frequencies are spaced apart by a frequency spacing which has a magnitude at least on the order of one of said limited frequency ranges, (b) said resonant frequencies respectively nearest said first and second center frequencies are respectively displaced therefrom by substantially equal frequency differences of a magnitude on the order of at least one quarter of one said limited frequency range, and (c) said resonant frequencies are disposed symmetrically about said third frequency;
(2) subjecting said active gaseous material in said cavity to a magnetic field so as to divide each of said first and second limited frequency ranges into a plurality of similar secondary frequency ranges by Zeeman-splitting, wherein said magnetic field has a predominant field direction substantially parallel said optical axis within said portion and has an operating field strength sufficient to frequency-shift ones of said secondary frequency ranges respectively centered at said first and second center frequencies away from the respective first and second center frequencies a frequency increment on the order of at least the frequency difference between said first and second center frequencies and respective adjacent ones of said resonant frequencies; and
(3) substantially reversing the direction of said magnetic field.

### Claim 16 (depends on 15)

The method according to claim 15 and further including the step of selecting circularly polarized electromagnetic radiation of a given handedness generated by said active gaseous material and initially propagating parallel to said optical axis.