Optical sensing based on overlapping optical modes in optical resonator sensors and interferometric sensors

• US 8,111,402 B2
• Filed: 04/03/2009
• Issued: 02/07/2012
• Est. Priority Date: 04/03/2008
• Status: Active Grant

• Current Assignee: California Institute of Technology, Oewaves Incorporated, University of Southern California
• Original Assignee: California Institute of Technology, Oewaves Incorporated, University of Southern California
• Inventors: Le, Thanh M., Yu, Nan, Maleki, Lutfollah, Savchenkov, Anatoliy, Steier, William H.
• Primary Examiner(s): LEE, HWA S
• Application Number:
  US12/418,525
• Publication Number:
  US 20090251705A1
• Time in Patent Office: 1,040 Days
• Field of Search: 356/461, 356/460, 356/459, 356/480, 356/481, 356/491, 356/517, 356/437, 356/432
• US Class Current: 356/491
• CPC Class Codes: G01N 2021/7779 interferometric
• CPC Class Codes: G01N 2021/7789 Cavity or resonator
• CPC Class Codes: G01N 21/7703 using reagent-clad optical fibres or optical waveguides using measurement of total internal reflection or attenuated total reflection G01N21/552; optical fibres or waveguides per se G02B

Abstract

Techniques and devices based on transverse magnetic (TM) and transverse electric (TE) modes in an optical resonator or interferometer to provide sensitive optical detection with insensitivity to a change in temperature. A shift in a difference between a first resonance wavelength of a TE optical mode and a second resonance wavelength of a TM optical mode is measured to measure a change in a sample that is in optical interaction with the optical resonator or interferometer. For example, the detected shift can be used to measure a change in a refractive index of the sample.

Claims

1. An optical sensing device, comprising:

a laser that produces a laser probe beam;

an optical resonator in an optical path of the laser probe beam to receive light of the laser probe beam in a transverse magnetic (TM) mode and a transverse electric (TE) mode and to support both TM and TE optical modes that spatially overlap, the optical resonator located adjacent to or in contact with a sample to cause optical interaction between the sample and the light in the TM and TE optical modes; and

a detection unit that is coupled to the optical resonator to detect a shift in a difference between a first resonance wavelength of a TE optical mode and a second resonance wavelength of a TM optical mode and to measure a change in the sample from the detected shift.

2. The device as in claim 1, comprising:

an optical polarization controller located in the optical path between the laser and the optical resonator to control an optical polarization of the laser probe beam at the optical resonator for coupling the light of the laser probe beam into light of the TM and TE optical modes inside the optical resonator.

3. The device as in claim 1, wherein:

the detection unit includes a photodetector that receives light from the optical resonator.

4. The device as in claim 1, wherein:

the detection unit processes the detected shift to measure a change in a refractive index of the sample.

5. The device as in claim 1, wherein:

the detection unit processes the detected shift to measure a change in a concentration of a substance in the sample.

6. The device as in claim 1, comprising:

an optical coupler optically coupled to the optical resonator to evanescently couple light of the laser probe beam into the optical resonator.

7. The device as in claim 1, wherein:

the optical resonator is a whispering gallery mode (WGM) resonator and the TE and TM optical modes are TE and TM whispering gallery modes, respectively.

8. The device as in claim 1, wherein:

the optical resonator is a ring resonator.

9. The device as in claim 8, wherein:

the ring resonator comprises an optical waveguide forming a closed ring.

10. The device as in claim 9, wherein:

the optical waveguide is an optical waveguide integrated on a substrate.

11. The device as in claim 9, comprising:

a separate waveguide located adjacent to the ring resonator to be in evanescent coupling with the ring resonator to provide optical coupling with the ring resonator.

12. The device as in claim 1, wherein:

the optical resonator has an exterior surface that is functionalized to selectively bond with a target biological substance.

13. The device as in claim 3, wherein the detection unit is coupled to the laser to sweep an optical frequency of the laser probe beam over the first resonance wavelength of the TE optical mode and the second resonance wavelength of the TM optical mode to obtain spectrum of the light that is from the optical resonator and is received at the photodetector.

14. The device as in claim 13, wherein the detection unit includes a ramp signal function generator that produces a ram signal for sweeping the optical frequency of the laser probe beam.

15. The device as in claim 13, wherein the detection unit includes a lock-in amplifier that receives a detector output signal from the photodetector and processes the detector output signal with respect to a reference.

16. The device as in claim 15, wherein the detection unit operates the lock-in amplifier to produce a derivative signal from the detector output signal of the photodetector.

17. The device as in claim 13, wherein the detection unit includes a computer that receives the spectrum of the light that is from the optical resonator and is received at the photodetector.

18. A method for optically sensing a sample, comprising:

placing an optical resonator, which is structured to support transverse magnetic (TM) and transverse electric (TE) optical modes that spatially overlap, adjacent to or in contact with a sample to cause optical interaction between the sample and optical fields of light in the TM and TE optical modes;

coupling probe light into the optical resonator to cause the probe light in the TM and TE optical modes to interact with the sample; and

detecting a shift in a difference between a first resonance wavelength of a TE optical mode and a second resonance wavelength of a TM optical mode of the optical resonator to measure a change in the sample to reduce noise in the detected shift caused by thermal fluctuations in the optical resonator and the sample.

19. The method as in claim 18, comprising:

processing the detected shift in the difference between the first resonance wavelength of the TM optical mode and the second resonance wavelength of the TE optical mode to measure a change in a refractive index of the sample.

20. The method as in claim 18, comprising:

processing the detected shift in the difference between the first resonance wavelength of the TM optical mode and the second resonance wavelength of the TE optical mode to measure a change in a concentration of a chemical or biological substance in the sample.

21. The method as in claim 18, comprising:

controlling polarization of the probe light at the optical resonator to couple the probe light into the optical resonator both of the TM and TE optical modes to achieve resonances at the first resonance wavelength of the TM optical mode and at the second resonance wavelength of the TE optical mode.

22. The method as in claim 18, wherein:

the optical resonator is a whispering gallery mode resonator, and the method further includes operating an optical coupler to provide evanescent optical coupling to the whispering gallery mode resonator to couple the probe light into the whispering gallery mode resonator.

23. The method as in claim 18, wherein:

the optical resonator is a ring resonator formed by an optical waveguide, and the method further includes providing evanescent optical coupling to the optical waveguide to couple the probe light into the optical waveguide.

24. The method as in claim 18, further comprising:

sweeping an optical frequency of the laser probe beam over the first resonance wavelength of the TE optical mode and the second resonance wavelength of the TM optical mode to obtain spectrum of light that is coupled out of the optical resonator, and

using the obtained spectrum of light coupled out of the optical resonator to detect the shift in the difference between the first resonance wavelength of the TE optical mode and the second resonance wavelength of the TM optical mode of the optical resonator.

25. An optical sensing device, comprising:

an optical input module to provide laser light linearly polarized at an input polarization;

a waveguide structured to support transverse magnetic (TM) and transverse electric (TE) optical modes linearly polarized along first and second orthogonal polarizations, respectively, and located adjacent to or in contact with a sample to cause optical interaction between the sample and the light in waveguide, the waveguide placed in an optical path of the laser light from the optical input module to receive the laser light and oriented relative to the optical input module to form a 45-degree angle between and input polarization and each of the first and second orthogonal polarizations;

an output polarizer polarized at an output polarization which is at 45 degrees with respect to each of the first and second orthogonal polarizations of the waveguide and located in an optical path of light output by the waveguide to cause optical interference between a portion of light in the TE mode from the waveguide and a portion of light in the TM mode from the waveguide; and

a detection unit to receive light from the output polarizer to detect a difference between a phase shift of light in the TE mode and light in the TM mode in the output of the waveguide from the optical interference and to measure a change in the sample.

26. The device as in claim 25, comprising:

a laser that produces the laser light directed into the waveguide,

wherein the optical input module controls a polarization of the laser light from the laser to be in the input polarization.

27. A method for optically sensing a sample, comprising:

placing an optical resonator that supports two or more different optical modes relative to a sample in optical interaction between the sample and the optical resonator;

coupling probe light into the optical resonator to produce first and second different optical modes that spatially overlap with each other, the first and second optical modes having first and second optical resonances at a first resonance wavelength and a second resonance wavelength, respectively;

sweeping an optical frequency of the probe light over the first and second resonance wavelengths of the first and second optical modes;

detecting light coupled out of the optical resonator to measure a spectrum of the light coupled out of the optical resonator or waveguide based on sweeping of the optical frequency of the probe light;

using the obtained spectrum of light to obtain a difference between the first resonance wavelength of the first optical mode and the second resonance wavelength of the second optical mode; and

using the difference between the first resonance wavelength and the second resonance wavelength to determine a change in the sample while suppressing a noise caused by a temperature change.

28. The method as in claim 27, comprising:

obtaining a shift in the difference between the first resonance wavelength and the second resonance wavelength that is caused by a refractive index of the sample;

using the shift to measure a change in the refractive index of the sample.

29. The method as in claim 27, comprising:

obtaining a shift in the difference between the first resonance wavelength and the second resonance wavelength caused by a change in a concentration of a chemical or biological substance in the sample; and

using the shift to measure a change in the concentration of the chemical or biological substance in the sample.

30. The method as in claim 27, comprising:

controlling polarization of the probe light at the optical resonator to in producing the first and second different optical modes that spatially overlap with each other.