OPTIMIZED METHOD FOR LID BIOSENSOR RESONANCE DETECTION

• US 20090138205A1
• Filed: 11/06/2008
• Published: 05/28/2009
• Est. Priority Date: 03/10/2006
• Status: Active Grant

• Current Assignee: Corning Incorporated
• Original Assignee: Corning Incorporated
• Inventors: Gollier, Jacques, Piech, Garrett A., Webb, Michael B., Wu, Qi
• Granted Patent: US 7,979,241 B2
• Time in Patent Office: Days
• US Class Current: 702/19
• CPC Class Codes: G01J 3/02 Details
• CPC Class Codes: G01J 3/0218 using optical fibers
• CPC Class Codes: G01J 3/1895 using fiber Bragg gratings or gratings integrated in a waveguide
• CPC Class Codes: G01J 3/28 Investigating the spectrum using colour filters G01J3/51
• CPC Class Codes: G01J 3/2803 using photoelectric array detector
• CPC Class Codes: G01N 21/7743 the reagent-coated grating coupling light in or out of the waveguide

Abstract

An optical interrogation system is described herein that can interrogate a label-independent-detection (LID) biosensor and monitor a biological event on top of the biosensor without suffering from problematical parasitic reflections and/or problematical pixelation effects. In one embodiment, the optical interrogation system is capable of interrogating a biosensor and using a low pass filter algorithm to digitally remove problematic parasitic reflections contained in the spectrum of an optical resonance which makes it easier to determine whether or not a biological event occurred on the biosensor. In another embodiment, the optical interrogation system is capable of interrogating a biosensor and using an oversampling/smoothing algorithm to reduce oscillations in the estimated location of an optical resonance caused by the problematical pixelation effect which makes it easier to determine whether or not a biological event occurred on the biosensor.

Claims

1. An optical interrogation system comprising:

a launch system that emits an optical beam towards a biosensor;

a receive system that collects an optical beam from the biosensor and then outputs a signal which corresponds to the collected optical beam; and

a processor that applies a low pass filter to the signal to digitally remove a plurality of problematic parasitic reflections located on each side of an optical resonance represented within the signal.

2. The optical interrogation system of claim 1, wherein said low pass filter is represented as follows:

Y′

=Gy

where;

y is the signal;

represents a convolution product;

G is a filter function; and

Y′

is a filtered signal.

3. The optical interrogation system of claim 2, wherein the filter function is:

a Gaussian function;

a rectangular function;

or a sinc function.

4. The optical interrogation system of claim 1, wherein said low pass filter is represented as follows:

Y1=G*FFT(y); and

Y′

=FFT<sup>−

1</sup>(Y1)

where;

y is the signal;

G is a filter function;

FFT is a Fourier transform;

FFT<sup>−

1</sup> is an inverse Fourier transform; and

Y′

is a filtered signal.

5. The optical interrogation system of claim 4, wherein the filter function is:

a Gaussian function;

a rectangular function;

or

a sinc function.

6. The optical interrogation system of claim 1, further comprising an optical isolator located between the biosensor and both a lensed fiber of the launch system and a lensed fiber of the receive system, wherein the optical isolator filters out the parasitic reflections caused by a part of the optical beam reflected from a face of a substrate of the biosensor, and wherein the optical isolator does not filter out the parasitic reflections caused by the optical beam which passes through the substrate and is reflected from a top surface of the biosensor.

7. The optical interrogation system of claim 1, wherein the low pass filter filters out the parasitic reflections caused by the optical beam which passes through a substrate of the biosensor and is then reflected from a top surface of the biosensor, and wherein the low pass filter does not filter out the parasitic reflections caused by a part of the optical beam reflected from a face of the substrate of the biosensor.

8. The optical interrogation system of claim 1, wherein the receive system includes a spectrometer which has a misaligned entrance spectrometer slit or fiber.

9. The optical interrogation system of claim 1, wherein the low pass filter has a width sized to suppress detrimental effects of the parasitic reflections.

10. The optical interrogation system of claim 1, wherein the optical resonance includes a spectral resonance with a width that is larger than a period of parasitic fringes.

11. The optical interrogation system of claim 1, wherein the receive system samples the optical beam collected from the biosensor at a period lower than a period of parasitic fringes which are on each side of the optical resonance.

12. A method for interrogating a biosensor, said method comprising the steps of:

emitting an optical beam towards the biosensor;

collecting an optical beam from the biosensor;

generating a signal which corresponds to the collected optical beam; and

applying a low pass filter to the signal to digitally remove a plurality of problematic parasitic reflections located on each side of an optical resonance represented within the signal.

13. The method of claim 12, wherein said low pass filter is represented as follows:

Y′

=Gy

where;

y is the signal;

represents a convolution product;

G is a filter function; and

Y′

is a filtered signal.

14. The method of claim 13, wherein the filter function is:

a Gaussian function;

a rectangular function;

or

a sinc function.

15. The method of claim 12, wherein said low pass filter is represented as follows:

Y1=G*FFT(y); and

Y′

=FFT<sup>−

1</sup>(Y1)

where;

y is the signal;

G is a filter function;

FFT is a Fourier transform;

FFT<sup>−

1</sup> is an inverse Fourier transform; and

Y′

is a filtered signal.

16. The method of claim 15, wherein the filter function is:

a Gaussian function;

a rectangular function;

or

a sinc function.

17. The method of claim 12, further comprising a step of using an optical isolator to filter out the parasitic reflections caused by a part of the optical beam reflected from a face of a substrate of the biosensor while the optical isolator does not filter out the parasitic reflections caused by the optical beam which passes through the substrate is reflected from a top surface of the biosensor.

18. The method of claim 12, wherein the low pass filter filters out the parasitic reflections caused by the optical beam which passes through a substrate of the biosensor and is then reflected from a top surface of the biosensor, and wherein the low pass filter does not filter out the parasitic reflections caused by a part of the optical beam reflected from a face of the substrate of the biosensor.

19. The method of claim 12, wherein the optical resonance include a spectral resonance with a width that is larger than a period of parasitic fringes.

20. The method of claim 12, wherein the collecting step includes a step of sampling the optical beam collected from the biosensor at a period lower than a period of parasitic fringes which are on each side of the optical resonance.