Heterodyne photomixer spectrometer with receiver photomixer driven at different frequency than source photomixer
View Patent ↗A heterodyne photomixer spectrometer comprises a receiver photomixer that is driven at a different frequency than the source photomixer, thereby maintaining the coherent nature of the detection, eliminating etalon effects, and providing not only the amplitude but also the phase of the received signal. The heterodyne technique can be applied where the source and receiver elements are components of a waveguide thereby forming an on-chip heterodyne spectrometer.
1. A heterodyne photomixer spectrometer, comprising:
a first laser generating a first laser beam,
a second laser generating a second laser beam at a frequency having a stable difference, δ, from the frequency of the first laser beam,
a third laser generating a third laser beam swept in frequency,
a source photomixer receiving the first laser beam and third laser beam and outputting light onto a sample, and
a receiver photomixer receiving the second laser beam and third laser beam and detecting the light transmitted reflected, or guided through the sample.
2. The heterodyne photomixer spectrometer of claim 1 , further comprising a spectrum analyzer connected to the receiver photomixer to measure the amplitude of the frequency response at the difference frequency.
3. The heterodyne photomixer spectrometer of claim 1 , further comprising an electronic filter centered on the response of the receiver photomixer at the difference frequency to pass only the difference frequency.
4. The heterodyne photomixer spectrometer of claim 3 , further comprising a power meter to measure the amplitude of the passed response of the electronic filter.
5. The heterodyne photomixer spectrometer of claim 1 , wherein the stable frequency difference is between approximately 1 MHz and 1 GHz.
6. The heterodyne photomixer spectrometer of claim 1 , wherein the first and second lasers are visible lasers.
7. The heterodyne photomixer spectrometer of claim 1 , wherein the first and second lasers are near-infrared lasers.
8. The heterodyne photomixer spectrometer of claim 1 , wherein the second laser beam is generated by passing a portion of the first laser beam through an acousto-optic modulator (AOM) driven at the desired difference frequency, δ, to generate a weaker laser beam at ν 1 +δ and wherein this weaker laser beam is amplified to generate the second laser beam at ν 1 +δ.
9. The heterodyne photomixer spectrometer of claim 8 , wherein the amplifier used to generate the second laser beam is a Master-Oscillator-Power-Amplifier (MOPA).
10. The heterodyne photomixer spectrometer of claim 1 , wherein the second laser beam is generated by passing a portion of the first laser beam through an electro-optic modulator (EOM) driven at the desired difference frequency, δ, to generate the second laser beam at ν 1 +δ.
11. The heterodyne photomixer spectrometer of claim 10 , wherein a Master-Oscillator-Power-Amplifier (MOPA) boosts the power of the second laser beam.
12. The heterodyne photomixer spectrometer of claim 1 , wherein the sample comprises a gas.
13. The heterodyne photomixer spectrometer of claim 12 , wherein the gas is contained in a gas cell.
14. The heterodyne photomixer spectrometer of claim 1 , wherein the source and receiver photomixers are both on the same chip and connected via an on chip waveguide.
15. The heterodyne photomixer spectrometer of claim 14 , wherein the source or receiver photomixer comprises an optoelectronic switch.
16. The heterodyne photomixer spectrometer of claim 14 , wherein the waveguide comprises a coplanar waveguide, coplanar transmission line, or microstrip.
17. The heterodyne photomixer spectrometer of claim 14 , wherein the sample is placed close to or on the waveguide so that the fringing fields of the electromagnetic wave propagating between the source and receiver photomixers interact with the sample.