Optical sensing based on whispering-gallery-mode microcavity

• US 6,490,039 B2
• Filed: 08/08/2001
• Issued: 12/03/2002
• Est. Priority Date: 08/08/2000
• Status: Expired due to Term

• Current Assignee: California Institute of Technology
• Original Assignee: California Institute of Technology
• Inventors: Ilchenko, Vladimir, Maleki, Luftollah
• Primary Examiner(s): Font, Frank G.
• Assistant Examiner(s): Punnoose, Roy M.
• Application Number:
  US09/925,713
• Publication Number:
  US 20020097401A1
• Time in Patent Office: 482 Days
• Field of Search: 356/436, 356/440, 356/442, 385/28, 385/30, 372/98, 372/108
• US Class Current: 356/436
• CPC Class Codes: G01N 21/552 Attenuated total reflection
• CPC Class Codes: G01N 21/7746 the waveguide coupled to a cavity resonator
• CPC Class Codes: G02B 6/29341 Loop resonators operating in a whispering gallery mode evanescently coupled to a light guide, e.g. sphere or disk or cylinder evanescent coupling for sensing fluorescence G01N21/648
• CPC Class Codes: H01S 5/1075 Disk lasers with special modes, e.g. whispering gallery lasers

Abstract

Techniques and devices for sensing a sample by using a whispering gallery mode resonator.

Claims

1. A device, comprising:

an optical resonator to support a whispering gallery mode of an electromagnetic field;

an optical coupler positioned adjacent to said optical resonator and having an interfacing surface to evanescently couple optical energy into or out of said optical resonator in said whispering gallery mode;

a sample unit disposed relative to said optical resonator to supply a sample to a spatial region within a reach of and to interact with said electromagnetic field of said whispering gallery mode to produce a change in said optical energy in said optical resonator;

an optical detector located relative to said optical coupler to receive an output from said optical coupler and measure said change during a transient period before said optical resonator reaches an equilibrium state in interaction with the sample; and

a signal processor coupled to said optical detector to process an output from said optical detector to extract information on the sample.

2. The device as in claim 1, wherein said optical resonator includes a spherical portion of a sphere that comprises an equator.

3. The device as in claim 1, wherein said optical resonator has a non-spherical shape to provide a two-dimensional confinement.

4. The device as in claim 3, wherein said optical resonator is a spheroid.

5. The device as in claim 1, wherein said optical resonator has an exterior coated to bind a selected substance.

6. The device as in claim 1, wherein said interfacing surface of said optical coupler is coated to bind a selected substance.

7. A method, comprising:

measuring a first value of a property of an output optical signal from an optical resonator that supports a whispering gallery mode in absence of a sample;

measuring a second value of the property of the output optical signal from the optical resonator when the sample is present within a reach of the whispering gallery mode; and

extracting information of the sample from a difference between the first and the second value.

8. The method as in claim 7, wherein the property includes a decay time of the optical resonator.

9. The method as in claim 7, wherein the property includes a frequency shift in a mode frequency of the whispering gallery mode.

10. The method as in claim 7, wherein the property includes a change in a line width of a resonance of the optical resonator.

11. The method as in claim 7, wherein the property includes a change in a mode coupling efficiency associated with the whispering gallery mode.

12. The method as in claim 7, wherein said first value is measured when said optical resonator is in an equilibrium state in absence of the sample, and said second value is measured when said optical resonator in another equilibrium state in presence of the sample.

13. The method as in claim 7, wherein said first and said second value are measured during a transient period when said optical resonator is in a non-equilibrium state due to an interaction with the sample.

14. A device, comprising:

an optical resonator having a geometry of an oblate spheroid to support a whispering gallery mode;

an optical coupler positioned adjacent to said optical resonator to evanescently couple optical energy into said optical resonator in said whispering gallery mode or out of said optical resonator to produce an output signal;

a sample unit disposed adjacent to said optical resonator to supply a sample to a spatial region within a reach of an electromagnetic field of said whispering gallery mode to interact with said electromagnetic field to produce a change in said output signal;

an optical detector located relative to said optical coupler to measure said change in said output signal; and

a signal processor coupled to said optical detector to process an output from said optical detector to extract information on the sample.

15. The device as in claim 14, wherein said optical detector is configured to measure a frequency shift in said whispering gallery mode.

16. The device as in claim 14, wherein said optical detector is configured to measure a decay time of said optical resonator.

17. The device as in claim 14, wherein said optical detector is configured to measure a change in a linewidth of a resonance of said optical resonator.

18. The device as in claim 14, wherein said optical detector is configured to measure a change in a mode coupling efficiency associated with said whispering gallery mode.

19. The device as in claim 14, wherein said optical detector is configured to measure a change in a frequency shift in said whispering gallery mode during a transient period when said optical resonator is in a non-equilibrium state due to an interaction with the sample.

20. A device, comprising:

an optical resonator having a dielectric hollow shell with a thickness less than on wavelength of an optical signal and a medium filled in said hollow shell with a refractive index greater than a refractive index of said hollow shell, said optical resonator configured to support a whispering gallery mode;

an optical coupler positioned adjacent to said optical resonator and having an interfacing surface to evanescently couple said optical signal into said optical resonator in a whispering gallery mode or to couple energy out of said optical resonator to produce an output signal;

a sample unit coupled to said optical resonator to supply a sample into said medium within a reach of an electromagnetic field of said whispering gallery mode to interact with said electromagnetic field to produce a change in said output signal;

an optical detector positioned relative to said optical coupler to receive said output signal and to measure said change; and

a signal processor coupled to said optical detector to process an output from said optical detector to extract information on the sample.

21. The device as in claim 20, wherein said optical resonator includes a spherical portion of a hollow sphere that comprises an equator.

22. The device as in claim 20, wherein said optical resonator is a hollow spheroid.

23. The device as in claim 20, wherein said optical resonator has an exterior coated to bind a selected substance.

24. The device as in claim 20, wherein said interfacing surface of said optical coupler is coated to bind a selected substance.

25. A method, comprising:

causing a measurement of a first value of a property of an output optical signal from an optical resonator that supports a whispering gallery mode in absence of a sample;

causing a measurement of a second value of the property of the output optical signal from the optical resonator when the sample is present within a reach of the whispering gallery mode; and

causing a difference between the first and the second value to be processed to extract information of the sample.

26. The method as in claim 25, wherein said first value is measured when said optical resonator is in an equilibrium state in absence of the sample, and said second value is measured when said optical resonator in another equilibrium state in presence of the sample.

27. The method as in claim 25, wherein said first and said second value are measured during a transient period when said optical resonator is in a non-equilibrium state due to an interaction with the sample.

28. The method as in claim 27, wherein the property includes a frequency shift in a mode frequency of the whispering gallery mode.