METHOD AND DEVICE FOR STABILIZING THE SPECTRUM OF A PULSED COHERENT OPTICAL SOURCE

• US 20100329287A1
• Filed: 02/20/2009
• Published: 12/30/2010
• Est. Priority Date: 02/22/2008
• Status: Abandoned Application

• Current Assignee: CSEM Centre Suisse D'Electronique et de Microtechnique SA
• Original Assignee: CSEM Centre Suisse D'Electronique et de Microtechnique SA
• Inventors: Lecomte, Steve
• Application Number:
  US12/918,956
• Publication Number:
  US 20100329287A1
• Time in Patent Office: Days
• US Class Current: 372/3
• CPC Class Codes: H01S 3/1106 Mode locking
• CPC Class Codes: H01S 3/1305 Feedback control systems
• CPC Class Codes: H01S 3/137 for stabilising of frequency
• CPC Class Codes: H01S 3/1392 by using a passive reference, e.g. absorption cell H01S3/1396, H01S3/1398 take precedence
• CPC Class Codes: H01S 3/1394 by using an active reference, e.g. second laser, klystron or other standard frequency source
• CPC Class Codes: H01S 5/0657 Mode locking, i.e. generation of pulses at a frequency corresponding to a roundtrip in the cavity
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser

Abstract

The invention relates to a method for stabilizing the spectrum of a pulsed coherent optical source that comprises controlling the offset frequency ω₀ and the repetition rate ω_r in order to stabilize the frequencies of the comb lines constituting the optical spectrum thereof. The method comprises forming, from the pulsed coherent optical source (S₁), a beam that is directed onto a reference resonant optical cavity (CR), and using the signal generated by the reference resonant optical cavity (CR) for controlling the offset frequency ω_o or the repetition rate ω_r, and probing, using a comb line, an atomic or molecular transition (AMT) in order to generate a driving signal for the repetition rate ω_r or the offset frequency ω₀.

Claims

1. A method for stabilizing the spectrum of a pulsed coherent optical source according to which the offset frequency ω

₀ and the repetition rate ω

_r are slaved so as to slave the frequencies of the comb lines which make up its optical spectrum, characterized in that a beam that is directed onto a reference resonant optical cavity is formed on the basis of the pulsed coherent optical source and the signal formed by the reference resonant optical cavity is used to slave the offset frequency ω

₀ or the repetition rate ω

_r and an atomic or molecular transition is probed by means of a comb line so as to form a signal for slaving the repetition rate ω

_r or the offset frequency ω

₀.

3. The method as claimed in claim 1 according to which various colors of the spectrum of the optical comb are spatially split.

4. The method as claimed in claim 1, according to which the frequency of the optical region of the pulsed coherent optical source at the microwave region is divided by the repetition rate ω

_r of the stabilized pulsed coherent optical source.

5. The method as claimed in claim 1, according to which the offset frequency ω

₀ or the repetition rate ω

_r is stabilized with the aid of a phase modulator by a slaving of Pound-Drever-Hall type.

6. A device for the implementation of the method as claimed in claim 1, comprising a pulsed coherent light source (S₁) of volume less than 10.10⁻

4 cm³ and of power less than 1 W and an ultrastable reference resonant cavity (CR) of volume less than 0.2 cm³.

8. The device as claimed in claim 6, comprising at least one optical element (L_s) for splitting various colors of the optical spectrum of the pulsed coherent optical source (S₁).

9. The device as claimed in claim 8 in which the optical element (L_s) for splitting various colors of the optical spectrum of the pulsed coherent optical source (S₁) is chosen from among the following elements:

planar selective grating, interleaver, glass plate with dielectric coating whose reflectivity varies as a function of wavelength, diffraction grating, low-finesse resonant optical cavity with wide free spectral region.

10. The device as claimed in claim 6, in which the pulsed coherent light source (S₁) is chosen from among the following sources:

edge-emitting quantum well multi-section laser with saturable absorber, edge-emitting quantum dot multi-section laser with saturable absorber, vertical-cavity surface-emitting laser (VECSEL) with saturable absorber not integrated into the structure generating the optical gain, an external-cavity surface-emitting mode-locked integrated laser (MIXSEL), a fiber laser, a Raman laser, a solid-state laser with mode locked by a saturable absorbent based on a semiconductor (SESAM), a microtoroid resonator pumped by continuous light, an optical-fiber resonator pumped by continuous light.

11. The device as claimed in claim 6, in which the ultrastable reference resonant cavity (CR) is chosen from among the following elements:

monolithic glass gauge with ultra low expansion of ULE type whose faces comprise dielectric mirrors with reflectivity greater than 99%, the same glass gauge but with a hollow cavity, an ultracompact resonator of annular type with quality factor greater than 10⁶, an ultracompact optical resonator made of a mechanically structured material and based on the photonic bandgap effect.

12. The device as claimed in claim 6, in which the various elements of which it is composed are linked by optical-fiber waveguides or channel waveguides made of materials chosen from among the following materials:

silicon oxide, silicon nitride, silicon, polymers or equivalents, so as to ensure the coupling and the decoupling of the laser beam between these various elements.

13. The device as claimed in claim 6, in which an optically non-linear spectral widening element is placed directly at the output of the pulsed coherent optical source, this spectral widening element being chosen from among the following components:

highly non-linear optical fiber of standard single-mode type or of photonic crystal type, waveguide with a geometry of conical type.

15. The device as claimed in claim 6, in which at least a part of the optical components is made using integrated optics.

2. A method for stabilizing the spectrum of a pulsed coherent optical source according to which the offset frequency ω

₀ and the repetition rate ω

_r are slaved so as to slave the frequencies of the comb lines which make up its optical spectrum, characterized in that a pulsed beam that is directed onto a reference resonant optical cavity is formed on the basis of the pulsed coherent optical source and the signal formed by the reference resonant cavity is used to slave the offset frequency ω

₀ or the repetition rate ω

_r and a continuous coherent optical source is used to form a continuous beam that is directed onto an atomic or molecular transition, the signal from which is used to slave the continuous coherent optical source and the difference in frequency between the pulsed and continuous optical beams is detected so as to slave the repetition rate ω

_r or the offset frequency ω

₀.

7. A device for the implementation of the method as claimed in claim 2, comprising a pulsed coherent light source (S₁) of volume less than 10.10⁻

4 cm³ and of power less than 1 W, an ultrastable reference resonant cavity (CR) of volume less than 0.2 cm³ and a continuous coherent light source (S₂) of volume less than 10.10<sup>−

4</sup> cm³ and of a power less than 0.5 W.

14. The device as claimed in claim 7, in which the spectral width of the continuous coherent optical source (S₂) is less than 1 MHz and is formed by one of the following lasers:

semiconductor laser of DFB type with distributed feedback or DBR laser with distributed Bragg reflector, semiconductor laser of Fabry-Pé

rot type with extended cavity, laser of toroidal resonator type, fiber laser.

16. The method as claimed in claim 2, according to which various colors of the spectrum of the optical comb are spatially split.

17. The method as claimed in claim 2, according to which the frequency of the optical region of the pulsed coherent optical source at the microwave region is divided by the repetition rate ω

_r of the stabilized pulsed coherent optical source.

18. The method as claimed in claim 2, according to which the offset frequency ω

₀ or the repetition rate ω

_r is stabilized with the aid of a phase modulator by a slaving of Pound-Drever-Hall type.

19. The device as claimed in claim 7, comprising at least one optical element (L_s) for splitting various colors of the optical spectrum of the pulsed coherent optical source (S₁).

20. The device as claimed in claim 7, in which the pulsed coherent light source (S₁) is chosen from among the following sources:

edge-emitting quantum well multi-section laser with saturable absorber, edge-emitting quantum dot multi-section laser with saturable absorber, vertical-cavity surface-emitting laser (VECSEL) with saturable absorber not integrated into the structure generating the optical gain, an external-cavity surface-emitting mode-locked integrated laser (MIXSEL), a fiber laser, a Raman laser, a solid-state laser with mode locked by a saturable absorbent based on a semiconductor (SESAM), a microtoroid resonator pumped by continuous light, an optical-fiber resonator pumped by continuous light.