IP Library Granted Patent US 7,426,040
Granted Patent B2
US 7,426,040 · App. 11/206,900 · Granted Sep 16, 2008

Chip-scale optical spectrum analyzers with enhanced resolution

Assignee: University of Pittsburgh
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 7,426,040
App. No.
11/206,900
Granted
Sep 16, 2008
Kind
B2
Abstract

A Fabry-Perot cavity filter includes a first mirror and a second mirror. A gap between the first and the second mirror monotonically varies as a function of width of the filter. This filter may be used with photodetector and a channel selection filter in an optical device, such as a spectrum analyzer. The channel selection filter may be a metal nanooptic filter array which includes plurality of subwavelength apertures in a metal film or between metal islands.

Claims (49)

1. A device comprising:

a Fabry-Perot cavity filter comprising a first mirror and a second mirror, wherein a gap between the first and the second mirror monotonically varies as a function of width of the filter; and

a channel selection filter comprising a metal nanooptic filter array based on plasmon resonance,

wherein the channel selection filter has a wider wavelength passband width than the Fabry-Perot cavity filter and

wherein the metal nanooptic filter array comprises a plurality of subwavelength apertures in a metal film or between metal islands, such that a distance between the apertures in different regions of the metal nanooptic filter array is different.

2. The device of claim 1 , wherein the first mirror is tilted with respect to the second mirror such that the gap varies in a continuous fashion along the width of the filter.

3. The device of claim 1 , wherein the first mirror and the second mirror comprise flat mirrors.

4. The device of claim 1 , wherein:

the gap comprises an air filled gap; and

the first mirror is tilted with respect to the second mirror such that the gap between the first and the second mirror monotonically varies.

5. The device of claim 1 , wherein:

a tapered spacer material is located in the gap; and

the first and the second mirrors contact the tapered spacer material such that the gap between the first and the second mirror monotonically varies.

6. The device of claim 1 , further comprising a photodetector, wherein a first photodetector pixel is adapted to detect radiation from the Fabry-Perot cavity filter position having a first gap height and a second photodetector pixel is adapted to detect radiation from the Fabry-Perot cavity filter position having a second gap height different from the first gap height.

7. A device, comprising:

a Fabry-Perot cavity filter comprising a first mirror and a second mirror wherein a gap between the first and the second mirror is variable; and

a photodetector array, wherein a first photodetector pixel is adapted to detect radiation from the Fabry-Perot cavity filter position having a first gap height and a second photodetector pixel is adapted to detect radiation from the Fabry-Perot cavity filter position having a second gap height different from the first gap height;

a channel selection filter array positioned such that only one peak from the Fabry-Perot cavity filter is incident on each pixel of the photodetector array;

wherein the channel selection filter comprises a metal nanooptic filter array based on plasmon resonance;

wherein the channel selection filter has a wider wavelength passband width than the Fabry-Perot cavity filter; and

wherein the metal nanooptic filter array comprises a plurality of subwavelength apertures in a metal film or between metal islands, such that a distance between the apertures in different regions of the metal nanooptic filter array is different.

8. The device of claim 7 , wherein:

the photodetector array comprises a plurality of pixels; and

each detector pixel is adapted to detect radiation from a different Fabry-Perot cavity filter position having different gap height.

9. The device of claim 7 , wherein:

the channel selection filter is positioned between the photodetector array and the Fabry-Perot cavity filter.

10. The device of claim 7 , wherein:

the first mirror is tilted with respect to the second mirror such that the gap varies in a continuous fashion as a function of width of the Fabry-Perot cavity filter; and

the first mirror and the second mirror comprise flat mirrors.

11. The device of claim 7 , wherein the device comprises a color camera, a spectrum analyzer, a monochromator or an optical analyte detection system.

12. An optical filtering method, comprising:

passing incident radiation through a Fabry-Perot cavity filter comprising a first mirror and a second mirror, wherein a gap between the first and the second mirror monotonically varies as a function of width of the filter;

passing the incident radiation through a channel selection filter such that only one peak from the incident radiation that passes through Fabry-Perot cavity filter is incident on each pixel of a photodetector;

wherein the channel selection filter comprises a metal nanooptic filter array which comprises a plurality of subwavelength apertures in a metal film or between metal islands, such that a distance between the apertures in different regions of the metal nanooptic filter array is different; and

wherein the incident radiation is filtered by the channel selection filter based on plasmon resonance between the incident radiation and the metal film or metal islands of the channel selection filter.

13. The method of claim 12 , wherein the first mirror is tilted with respect to the second mirror such that the gap varies in a continuous fashion along the width of the filter.

14. The method of claim 12 , wherein the channel selection filter has a wider wavelength passband width than the Fabry-Perot cavity filter.

15. The method of claim 12 , further comprising:

detecting radiation from the Fabry-Perot cavity filter position having a first gap height at a first photodetector pixel; and

detecting radiation from the Fabry-Perot cavity filter position having a second gap height different from the first gap height at a second photodetector pixel.

16. The method of claim 12 , wherein the method comprises a spectrum analysis method, a color image formation method, a wavelength separation method or an optical analyte detection method.

17. The method of claim 12 , wherein the incident radiation first passes through the Fabry-Perot filter and then through channel selection filter.

18. The device of claim 1 , wherein the metal nanooptic filter array comprises a metal film.

19. The device of claim 7 , wherein the metal nanooptic filter array comprises a metal film.

20. The device of claim 1 , wherein the metal nanooptic filter array comprises metal islands.

21. The device of claim 7 , wherein the metal nanooptic filter array comprises metal islands.

22. The method of claim 12 , wherein the metal nanooptic filter array comprises a metal film.

23. The method of claim 12 , wherein the metal nanooptic filter array comprises metal islands.

24. The method of claim 12 , wherein at each location on the metal nanooptic filter array and on the Fabry-Perot cavity filter corresponding to one photodetector pixel, the Fabry-Perot cavity filter passes a set of wavelength peaks and the metal nanooptic filter array passes a wavelength band that overlaps with only one of the Fabry-Perot wavelength peaks.

Assignments (2)
CONFIRMATORY LICENSE Recorded Nov 29, 2006
From: UNIVERSITY OF PITTSBURGH
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 018560/0675 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 19, 2005
From: KIM, HONG KOO; SUN, ZHIJUN; JUNG, YUN SUK
To: PITTSBURGH, UNIVERSITY OF
Reel/Frame 016908/0465 →
Continuity (2)
Provisional Application 6060262300 · Aug 19, 2004
Related Publication 20060209413A1 · Sep 21, 2006