Broadband laser source

• US 5,255,274 A
• Filed: 06/08/1992
• Issued: 10/19/1993
• Est. Priority Date: 09/06/1989
• Status: Expired due to Term

• Current Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Inventors: Digonnet, Michel J. F., Wysocki, Paul F., Kim, Byoung Y.
• Primary Examiner(s): Gonzalez, Frank
• Application Number:
  US07/895,602
• Time in Patent Office: 498 Days
• Field of Search: 356/345, 356/350, 356/351, 372/6, 372/20, 372/21, 372/26, 372/28, 372/32, 372/27, 359/326, 359/328, 359/331, 359/332, 385/12
• US Class Current: 372/26
• CPC Class Codes: H01S 3/06795 with superfluorescent emission, e.g. amplified spontaneous emission sources for fibre laser gyrometers fibre laser gyrometers per se G01C19/72

Abstract

A laser source comprises an optical fiber doped with a homogeneously broadened lasing medium, preferably with Erbium, pumped by a laser pump source and an intracavity acousto-optic modulator. When the acousto-optic modulator is driven by a variable frequency source, the Erbium fluorescence line emitted by the Erbium-doped optical fiber can be electronically tuned. In another embodiment, an electronic sweep waveform is used to frequency modulate the acoustic signal produced by the acousto-optic modulator. Without the low-rate frequency modulation, Erbium in a silica optical fiber is a mostly homogeneously broadened gain medium with a narrow laser linewidth. When measured on a long time scale, low-rate frequency modulation provides a broader spectral width, on the order of 19 nm, which makes such a source an ideal source for certain optical applications such as fiber optic gyroscopes.

Claims

1. An optical sensor for sensing an ambient effect, said optical sensor having an integration time, comprising:

a loop comprising an optical fiber having two polarization modes, each of said polarization modes propagating light at a different velocity, thereby providing an effective optical path length difference for said two modes for light traversing said loop; and

a broadband laser source having a cavity, said source being optically coupled to introduce light into said loop, said cavity having a lasing medium which emits radiation in an emission spectrum in response to application of pump energy to said lasing medium, said laser source further comprising a frequency modulator for shifting the frequency of said radiation by a predetermined frequency and for modulating said radiation shifted by said predetermined frequency, said frequency modulator sweeping across a substantial portion of said emission spectrum in a period shorter than the integration time of said sensor.

2. An optical sensor for sensing an ambient effect as claimed in claim 1, wherein said ambient effect is rotation of said loop.

3. An optical sensor for sensing an ambient effect as claimed in claim 1, wherein the radiation emitted by said laser has a coherence length which is less than said optical path length difference.

4. An apparatus, comprising:

a light source which, at a predetermined instant in time, emits radiation having a frequency bandwidth, said light source including a medium which emits radiation in response to a pump signal;

a frequency shifter which frequency shifts said radiation through a range of optical frequencies over a predetermined period of time beginning at said predetermined instant in time to produce optical frequencies outside said bandwidth, said frequency shifter being optically coupled to receive radiation emitted by said light source;

a detector which detects said radiation and integrates said radiation over a time at least as great as said predetermined period of time to generate a signal having a bandwidth greater than said frequency bandwidth, said detector being optically coupled to receive light that has been frequency shifted by said frequency shifter.

5. The apparatus of claim 4, wherein said light source comprises a laser having a resonant cavity, said frequency shifter being disposed to frequency shift radiation inside said cavity.

6. The apparatus of claim 4, additionally comprising an interferometer loop connected to receive radiation from said light source and to output said radiation to said detector.

7. The apparatus of claim 4, wherein said light source comprises an optical fiber which emits radiation in response to optical pumping.

8. The apparatus of claim 4, wherein said frequency shifting is periodic, said predetermined period of time being equal to one half of the period of the frequency shifting.

9. A method of supplying broadband radiation to an interferometer having a detection system with an integration time, comprising the steps of:

providing a medium which emits radiation in response to pumping at a pump wavelength;

pumping said medium at said pump wavelength to cause said medium to emit radiation at least at one emission wavelength;

modulating the frequency of at least a portion of said radiation, including radiation at said emission wavelength, said modulating step comprising the step of shifting the frequency of said portion of radiation by a predetermined frequency and the step of sweeping said frequency at a predetermined rate;

coupling the frequency modulated radiation to said interferometer, and using the detection system to detect the frequency modulated radiation; and

selecting said sweeping rate and said integration time such that the detection system generates a signal having a bandwidth substantially greater than that of the radiation detected by the detection system.

10. The method as claimed in claim 9, wherein the modulating step comprises the step of passing radiation through a Bragg cell deflector.

11. A method of generating a broadband signal, comprising:

using a detector to detect radiation from a light source which, at a predetermined instant in time, emits radiation having a frequency bandwidth;

frequency shifting said radiation, prior to said detection, through a range of optical frequencies over a predetermined period of time beginning at said predetermined instant in time to produce frequencies outside said bandwidth;

integrating an output of the detector over a time which is greater than said period of time to generate a signal having a bandwidth greater than said frequency bandwidth.