Continuously variable laser output coupler

• US 4,187,475 A
• Filed: 01/05/1978
• Issued: 02/05/1980
• Est. Priority Date: 01/05/1978
• Status: Expired due to Term

• Current Assignee: Irwin Wieder
• Original Assignee: Analytical Radiation Corporation
• Inventors: Wieder, Irwin
• Primary Examiner(s): Sikes, William L.
• Application Number:
  US05/867,005
• Time in Patent Office: 761 Days
• Field of Search: 331/94.5 C, 331/94.5 D, 331/94.5 M, 331/94.5 S, 350/164, 350/315
• US Class Current: 372/31
• CPC Class Codes: H01S 3/08004 incorporating a dispersive element, e.g. a prism for wavelength selection H01S3/0811, H01S3/08022 take precedence
• CPC Class Codes: H01S 3/139 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity length

Abstract

The output power of any laser is optimized by providing an output mirror with a transmission which varies as a function of position on the mirror and transmitted wavelength. The transmission which corresponds to the optimum output for a given laser wavelength is chosen by monitoring laser output and moving the output mirror in at least one direction essentially perpendicular to the laser beam axis while maintaining the orientation of its reflecting surface perpendicular to the laser beam axis, and locating the mirror position corresponding to optimum laser output.

Claims

1. A method for optimizing the output of a laser comprising:

providing as part of a laser cavity an output mirror with a range of transmission values, said transmission values varying in a known way as a function of wavelength and position along a gradient,

monitoring the output power of said laser, and

moving said output mirror along a gradient in the plane of said output mirror so that said plane remains essentially perpendicular to the laser beam axis, and until said monitored output power is optimized.

2. The method of claim 1 wherein said output mirror is a linear filter wedge with a thickness gradient of dielectric layers along a linear axis.

3. The method of claim 1 wherein said output mirror is a circular filter wedge with a thickness gradient of dielectric layers along a circumference of said wedge.

4. A method for stabilizing the output power of a laser, said method comprising:

providing as part of a laser cavity an output mirror with a range of transmission values, said transmission values varying in a known way as a function of wavelength and position along a gradient,

monitoring the output power of said laser, and,

moving said output mirror along a gradient in the plane of said output mirror so that said plane remains essentially perpendicular to the laser beam axis, and until said monitored output power is stabilized to a predetermined level.

5. The method of claim 4 wherein said output mirror is a linear filter wedge with a thickness gradient of dielectric layers along a linear axis.

6. The method of claim 4 wherein said output mirror is a circular filter wedge with a thickness gradient of dielectric layers along a circumference of said wedge.

7. A laser apparatus comprising:

an active laser medium having pumping means operatively associated therewith,

an optical resonator disposed about said laser medium, said resonator including at least one output mirror for transmitting an output beam wherein the output mirror of said optical resonator is a wedge filter having servo controlled mechanical means supporting said wedge filter, said mechanical means for moving said wedge in a direction in the plane of said wedge and along a thickness gradient of said wedge, said mechanical means maintaining the orientation of said plane of said wedge essentially perpendicular to said output beam of said laser, and,

means disposed in the path of the output beam for monitoring the output of said laser, said monitoring means generating a control signal electrically transmitted to said servo for controlling the position of said wedge filter.

8. The laser apparatus of claim 7 wherein said optical resonator includes a frequency tunable element other than said wedge filter.

9. The laser apparatus of claim 8, wherein said frequency tunable element other than said wedge filter is a reflection grating.

10. The laser apparatus of claim 7 wherein said laser medium has variable gain.

11. The apparatus of claim 7 wherein said servo means is adapted to hunt for maximum beam output.

12. The apparatus of claim 7 wherein said servo means is adapted to hunt for a preset level of beam output.