IP Library Granted Patent US 7,664,149
Granted Patent B2
US 7,664,149 · App. 11/745,837 · Granted Feb 16, 2010

Auto-stabilization of lasers by means of resonant structures

Assignee: STC. UNM
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 7,664,149
App. No.
11/745,837
Granted
Feb 16, 2010
Kind
B2
Abstract

Apparatus, systems, and methods are provided that utilize a material inserted into a laser cavity such that the material has an optical length that varies as the laser cavity varies to keep the repetition rate constant. The material may provide auto-stabilization of the optical output form the laser cavity.

Claims (31)

1. An apparatus comprising:

a mode-locked laser, the mode-locked laser having a laser cavity, the laser cavity having a cavity length; and

a material disposed inside the laser cavity, the material having an optical length that varies to maintain a constant repetition rate as the cavity length fluctuates, the material having one or more properties to provide optically controlled auto-stabilization of the repetition rate.

2. The apparatus of claim 1 , wherein the material has an optical length that decreases as a repetition rate of an optical output of the laser cavity decreases.

3. The apparatus of claim 1 , wherein the material has a resonant optical transition at a frequency proportional to the repetition rate.

4. The apparatus of claim 1 , wherein the material includes rubidium.

5. The apparatus of claim 1 , wherein the material has a structure having at least three levels, to provide resonant coherent interaction, such that one level is separated from the two other levels by an optical transition corresponding to a laser frequency of the mode-locked laser.

6. The apparatus of claim 1 , wherein the material disposed in the laser cavity includes atomic vapors.

7. The apparatus of claim 1 , wherein the mode-locked laser is configured to mode-lock at about 795 nm with a repetition rate near a submultiple of a hyperfine splitting of a rubidium ground state.

8. The apparatus of claim 1 , wherein the apparatus includes another material having a structure to provide wavelength stabilization to an optical output.

9. A system comprising:

a laser apparatus including a mode-locked laser, the mode-locked laser having a material disposed in a laser cavity of the mode-locked laser, wherein the laser cavity is configured as a ring, the laser cavity having a cavity length, the material having an optical length that varies to maintain a constant repetition rate as the cavity length fluctuates, the material having one or more properties to provide optically controlled auto-stabilization of the repetition rate; and

a receiver unit to collect an output from the laser apparatus.

10. The system of claim 9 , wherein the material has an optical length that decreases as a repetition rate of an optical output of the laser cavity decreases.

11. The system of claim 9 , wherein the material has a resonant optical transition proportional to the repetition rate.

12. The system of claim 11 , wherein the material includes rubidium.

13. The system of claim 9 , wherein the material has a structure having at least a three levels to provide resonant coherent interaction.

14. The system of claim 9 , wherein the laser apparatus includes an external cavity configured to hold a test sample.

15. The system of claim 9 , wherein the laser apparatus is arranged as a spectroscopic tool.

16. The system of claim 10 , wherein the laser apparatus is arranged as a time standard.

17. A method comprising:

generating an optical pulse train from a laser source, the laser source being a mode-locked laser having a laser cavity in which a material is disposed, such that coherence is established between atomic levels of the material to auto-stabilize the pulse train optically, the material having an optical length that varies to maintain a constant repetition rate of the optical pulse train as the cavity length fluctuates; and

directing the optical pulse train to a receiver.

18. The method of claim 17 , wherein generating an optical pulse train includes mode-locking the laser source using a multiple quantum well saturable absorber.

19. The method of claim 17 , wherein the method includes using rubidium in the laser cavity to auto-stabilize the optical pulse train.

20. The method of claim 19 , wherein the method includes using calcium to provide wavelength stabilization to the optical pulse train.

21. The method of claim 17 , wherein the method includes using the auto-stabilized optical pulse train as a time standard.

22. The method of claim 17 , wherein the method includes:

forming a cavity including the laser source;

irradiating a sample with the optical pulse train; and

analyzing an output provided by the irradiating of the sample.

Assignments (3)
CONFIRMATORY LICENSE Recorded May 23, 2012
From: NEW MEXICO, UNIVERSITY OF
To: NAVY, SECRETARY OF THE UNITED STATES OF AMERICA
Reel/Frame 028314/0684 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Mar 18, 2010
From: ARISSIAN, LADAN M; DIELS, JEAN-CLAUDE
To: THE REGENTS OF THE UNIVERSITY OF NEW MEXICO C/O RESEARCH & TECHNOLOGY LAW
Reel/Frame 024099/0725 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Mar 18, 2010
From: THE REGENTS OF THE UNIVERSITY OF NEW MEXICO C/O RESEARCH & TECHNOLOGY LAW
To: STC.UNM
Reel/Frame 024099/0768 →
Continuity (2)
Provisional Application 6079847100 · May 8, 2006
Related Publication 20080225907A1 · Sep 18, 2008