Mode locked solid-state laser pumped by a non-diffraction-limited pumping source and method for generating pulsed laser radiation by pumping with a non-diffraction-limited pumping beam

• US 5,987,049 A
• Filed: 04/24/1998
• Issued: 11/16/1999
• Est. Priority Date: 04/24/1998
• Status: Expired due to Term

• Current Assignee: Lumentum Switzerland AG (Lumentum Holdings Inc.)
• Original Assignee: Time-Bandwidth Products AG (Lumentum Holdings Inc.)
• Inventors: Schusslbauer, Wolfgang, Weingarten, Kurt
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US09/066,509
• Time in Patent Office: 571 Days
• Field of Search: 372/70, 372/98, 372/18, 372/11, 372/99, 372/92
• US Class Current: 372/70
• CPC Class Codes: H01S 3/025 of solid state lasers, e.g. housings or mountings
• CPC Class Codes: H01S 3/0816 having 4 reflectors, e.g. Z-shaped resonators
• CPC Class Codes: H01S 3/0941 of a laser diode
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/1625 titanium

Abstract

A pulsed solid-state laser comprises an optical resonator and a solid-state laser medium placed inside the optical resonator. A saturable absorber, such as a semiconductor saturable absorber mirror device for passive mode locking is placed inside the optical resonator, and a pumping source is provided for exciting the laser gain medium to emit electromagnetic radiation. The pumping source emits pump radiation which impinges on the laser gain medium in the form of a non-diffraction-limited focused pumping beam. The product of the stimulated emission cross section times the spontaneous fluorescence lifetime is low for the laser medium, e.g., 0.1·10^-23 cm² s for Ti:sapphire; nevertheless, the laser yields a high output power of a few Watt even if pumped with a non-diffraction-limited pumping beam. Pumping with a non-diffraction-limited pumping beam makes feasible solid-state lasers with remarkably smaller sizes and lower costs, but with the same performance as known lasers.

Claims

1. A laser for emitting pulsed electromagnetic radiation, said laser comprising:

an optical resonator;

a solid-state laser gain medium placed inside said optical resonator, said laser gain medium having a defined stimulated emission cross section and a defined spontaneous fluorescence lifetime for a given optical wavelength;

means for passive mode locking placed inside said optical resonator; and

means for exciting said laser gain medium to emit electromagnetic radiation, said exciting means comprising a pumping source for emitting pumping radiation which impinges on said laser gain medium in the form of at least one non-diffraction-limited focused pumping beam with essentially one pumping wavelength;

the product of said cross-section and said fluorescence lifetime being equal to or smaller than 0.15·

10^-23 cm² s.

2. The laser according to claim 1 wherein the pumping-beam section inside said laser gain medium is equal to or smaller than two times the confocal parameter of said focused pumping beam.

3. The laser according to claim 1 wherein said laser gain medium has a defined absorption length for a given optical wavelength, and said absorption length is equal to or smaller than the pumping-beam section inside said laser gain medium at the pumping wavelength.

4. The laser of claim 1 wherein said solid-state laser gain medium contains transition-metal ions.

5. The laser of claim 4 wherein said solid-state laser gain medium is selected from the group consisting of Ti:

Al₂ O₃, Cr;

YAG, Cr;

Fo and Cr;

BeAl₂ O₄.

6. The laser of claim 5 wherein said solid-state laser gain medium is Ti:

Al₂ O₃ with a Ti₂ O₃ content higher than or equal to 0.25 percent in weight.

7. The laser of claim 1 wherein said pumping wavelength is shorter than 650 nm.

8. The laser of claim 7 wherein said pumping source is a frequency-doubled Nd:

YVO₄ laser, a frequency-doubled ND;

YAG laser or at least one laser diode.

9. The laser of claim 1 wherein the pumping beam has a coefficient of beam quality M² equal to or higher than 2.

10. The laser of claim 1 wherein the electromagnetic radiation emitted by said pumping source is directed into said laser gain medium in the form of two pumping beams from essentially opposite directions.

11. The laser of claim 1 wherein said means for mode locking comprise a saturable absorber.

12. The laser of claim 11 wherein said saturable absorber is a semiconductor saturable absorber mirror device.

13. A method for generating pulsed laser radiation, comprising the steps of:

generating at least one non-diffraction-limited focused pumping beam with essentially one pumping wavelength;

exciting a solid-state laser gain medium to emit electromagnetic radiation, by impinging said at least one pumping beam on said laser gain medium,

said laser gain medium having a defined stimulated emission cross section and a defined spontaneous fluorescence lifetime for a given optical wavelength and the product of said cross-section and said fluorescence lifetime being equal to or smaller than 0.15·

10^-23 cm² s;

recirculating said electromagnetic radiation in an optical resonator; and

passively mode locking said electromagnetic radiation.

14. The method of claim 13 wherein said pumping-beam section inside said laser gain medium is equal to or smaller than two times the confocal parameter of said focused pumping beam.

15. The method of claim 13 wherein said laser gain medium has a defined absorption length for a given optical wavelength, and said absorption length is equal to or smaller than the pumping-beam section inside said laser gain medium at the pumping wavelength.