Method and apparatus for conducting heterodyne frequency-comb spectroscopy

Abstract

An apparatus and method are provided for conducting heterodyne frequency-comb spectroscopy. The apparatus includes a first and second frequency-comb generators for generating corresponding first and second continuous wave laser beams, respectively. The first beam defines a spectrum of light having a plurality of modes spaced by a first frequency. The second beam defines a spectrum of light having a plurality of modes spaced by a second frequency that is greater than the first frequency. The first and second beams are combined and the optical power of the combined beam is monitored with a data acquisition system to record a time trace. The recorded time trace is Fourier transformed such that each of spectrums of the first and second beams will exhibit a low-frequency comb. By superimposing the two combs, a beat frequency in a low-frequency region is assigned to an optical frequency.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

The drawings furnished herewith illustrate a preferred methodology of the present invention in which the above advantages and features are clearly disclosed as well as others which will be readily understood from the following description of the illustrated embodiment.

In the drawings:

FIG. 1 is a schematic view of an apparatus for conducting heterodyne frequency-comb spectroscopy in accordance with the present invention;

FIG. 2 is a schematic view of a frequency-comb generator for the apparatus of the present invention;

FIG. 3 is a graphical representation of the power versus the frequency of the frequency-combs generated by the frequency generators of the apparatus of the present invention;

FIG. 4 a is a graphical representation of an exemplary absorption spectroscopy showing the transmission intensity versus the frequency of the frequency-combs generated by the frequency generators of the apparatus of the present invention;

FIG. 4 b is a heterodyned graphical representation of the signal depicted in FIG. 4a showing the heterodyned signal versus the beat frequency;

FIG. 5 is a schematic view of an alternate embodiment of the apparatus for conducting heterodyne frequency-comb spectroscopy in accordance with the present invention;

FIG. 6 is a schematic view of a still further embodiment of the apparatus for conducting heterodyne frequency-comb spectroscopy in accordance with the present invention;

FIG. 7 is a graphical representation of the power versus the frequency of the frequency-combs generated by the apparatus of FIG. 6;

FIG. 8 a is a schematic view of a still further embodiment of the apparatus for conducting heterodyne frequency-comb spectroscopy in accordance with the present invention;

FIG. 8 b is a graphical representation of the power versus the frequency of the frequency-combs generated by the apparatus of FIG. 8a;

FIG. 8 c is a heterodyned graphical representation of the signal depicted in FIG. 8b showing the heterodyned signal versus the beat frequency;

FIG. 9 a is a schematic view of a still further embodiment of the apparatus for conducting heterodyne frequency-comb spectroscopy in accordance with the present invention;

FIG. 9 b is a graphical representation of the spectral power versus the optical frequency of the absorption spectrum generated by the apparatus of FIG. 9a; and

FIG. 8 c is a graphical representation of the down-converted signal depicted in FIG. 9b showing the spectral power versus the beat frequency in the radio frequency range.

Claims

1. An apparatus for conducting heterodyne frequency-comb spectroscopy, comprising: a first frequency-comb generator for generating a first continuous wave laser beam, the first beam defining a spectrum of light that includes a plurality of optical frequencies spaced by a first frequency;a second frequency-comb generator for generating a second continuous wave laser beam, the second beam defining a spectrum of light that includes a plurality of optical frequencies spaced by a second frequency; anda beam combiner operatively connected to the first and second frequency-comb generators, the beam combiner combining the first and second beams and providing the same as a combined beam having a plurality of beat frequencies dependent upon the optical frequencies of the spectrums of light defined by the first and second beams.

2. The apparatus of claim 1 wherein the first frequency-comb generator includes a filter having an input and an output, the filter controlling the spacing of the plurality of optical frequencies of the first beam.

3. The apparatus of claim 2 wherein the filter includes an etalon.

4. The apparatus of claim 3 wherein first frequency-comb generator includes a controller operatively connected to the filter, the controller controlling the temperature of the etalon, and wherein the spacing of the plurality of optical frequencies of the first beam is dependent on the temperature of the etalon.

5. The apparatus of claim 2 wherein the first frequency-comb generator includes an optical amplifier for generating an initial laser beam having predetermined optical power and an output coupler, the output coupler generating the first beam from a first output portion of the optical power and directing a feedback portion of the optical power to the input of the filter.

6. The apparatus of claim 5 wherein the first output portion of the optical power is generally equal to 2 percent of the optical power.

7. The apparatus of claim 5 wherein the first frequency-comb generator includes an isolator operatively connected to the optical amplifier and to the optical coupler, the isolator insuring the optical power propagates in a first direction.

8. The apparatus of claim 5 wherein the first frequency-comb generator includes: an optical attenuator having an input operatively connected to the output of the filter and an output; anda polarization cavity having an input operatively connected to the output of the optical attenuator and an output operatively connected to the input of the optical actuator; wherein:the optical attenuator controls the optical power of the initial laser beam; andthe polarization cavity maintains the linear polarization of the feedback portion of the optical power.

9. The apparatus of claim 1 further comprising a spectrum analyzer operatively connected to the beam combiner, the spectrum analyzer recording the combined beam.

10. The apparatus of claim 1 further comprising an enclosure for receiving the first and second frequency-comb generators therein.

11. An apparatus for conducting heterodyne frequency-comb spectroscopy, comprising: first and second frequency-comb generators, each frequency-comb generator including: a laser cavity for propagating optical power traveling therein;an output coupler optically communicating with the laser cavity for receiving the optical power and generating a continuous wave laser beam from a first output portion of the optical power, the continuous wave laser beam defining a spectrum of light including a plurality of optical frequencies spaced by a frequency;a beam combiner operatively connected to the first and second frequency-comb generators, the beam combiner combining the first and second continuous wave laser beams generated by the first and second frequency-comb generators and providing the same as a combined beam having a plurality of beat frequencies dependent upon the optical frequencies of the spectrums of light defined by the first and second continuous wave laser beams.

12. The apparatus of claim 11 wherein each frequency-comb generator includes a filter optically communicating with the laser cavity, the filter receiving a feedback portion of the optical power from the output coupler and spacing the optical frequencies of the spectrum of light by the frequency.

13. The apparatus of claim 12 wherein the filter includes an etalon.

14. The apparatus of claim 13 wherein each frequency-comb generator includes a controller operatively connected to the filter, the controller controlling the temperature of the etalon, and wherein the spacing of the plurality of optical frequencies of the spectrum of light is dependent on the temperature of the etalon.

15. The apparatus of claim 11 wherein the first output portion of the optical power is generally equal to 2 percent of the optical power.

16. The apparatus of claim 11 further comprising a spectrum analyzer operatively connected to the beam combiner, the optical spectrum analyzer recording the combined beam.

20. A method for conducting heterodyne frequency-comb spectroscopy, comprising the steps of: generating at least one continuous wave comb defined by a plurality of optical frequencies;down-converting the optical frequencies of the at least one continuous wave comb; anddetermining an optical spectrum for the at least one continuous wave comb from the down-converted optical frequencies.

21. The method of claim 20 wherein the step of generating the at least one continuous wave comb includes the steps of: generating a first continuous wave laser beam having a plurality of optical frequencies spaced by a first frequency that define a first continuous wave comb; andgenerating a second continuous wave laser beam having a plurality of optical frequencies spaced by a second frequency that define a second continuous wave comb.

22. The method of claim 20 wherein the step of down-converting the optical frequencies includes the step of superimposing the first and second continuous wave combs to determine a beat spectrum.

23. The method of claim 21 wherein the step of generating the first continuous wave laser beam includes the steps of: generating optical power having a spectrum;filtering at least a portion of the optical power so that the spectrum has the plurality of optical frequencies spaced by the first frequency; andgenerating the first continuous wave laser beam in response to the spectrum.

24. The method of claim 23 wherein the step of filtering at least a portion of the optical power includes the additional step of passing the portion of the optical power through an etalon.

25. The method of claim 24 wherein the etalon has a temperature and wherein the step of filtering at least a portion of the optical power includes the additional step of tuning the first frequency by adjusting the temperature of the etalon.

26. The method of claim 21 wherein the second frequency is greater than the first frequency.

27. The method of claim 20 wherein the step of down-converting the frequencies includes the steps of: designating the plurality of optical frequencies to generate modulations at lower beating frequencies; anddetecting the lower beating frequencies to observe the optical spectrum.

28. A method for conducting heterodyne frequency-comb spectroscopy, comprising the steps of: generating at least one continuous wave comb defined by a plurality of optical frequencies;designating the plurality of optical frequencies to generate modulations at lower beating frequencies; anddetecting the lower beating frequencies to observe an optical spectrum.

29. The method of claim 28 comprising the additional step of exposing the at least one continuous wave comb to a predetermined stimulus.

30. The method of claim 29 wherein the step of exposing the at least one continuous wave comb to a predetermined stimulus includes the step of passing the at least one continuous wave comb through a sample.

31. The method of claim 28 wherein the step of generating the at least one continuous wave comb includes the steps of: generating a first continuous wave laser beam having a plurality of optical frequencies spaced by a first frequency that define a first continuous wave comb; andgenerating a second continuous wave laser beam having a plurality of optical frequencies spaced by a second frequency that define a second continuous wave comb.

32. The method of claim 31 wherein the step of designating the plurality of optical frequencies includes the step of superimposing the first and second continuous wave combs to generate the lower beating frequencies.