Waveguide sensors optimized for discrimination against non-specific binding

• US 20080220440A1
• Filed: 04/13/2001
• Published: 09/11/2008
• Est. Priority Date: 07/25/2000
• Status: Abandoned Application

• Current Assignee: Trustees of Boston University
• Original Assignee: Trustees of Boston University
• Inventors: Worth, Colin, Unlu, M Selim, Goldberg, Bennett B
• Application Number:
  US10/333,864
• Publication Number:
  US 20080220440A1
• Time in Patent Office: Days
• US Class Current: 435/7.1
• 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
• CPC Class Codes: G01N 33/54373 involving physiochemical end-point determination, e.g. wave-guides, FETS, gratings

Abstract

A system for interferometrically detecting the present of bound material using a wave propagating waveguide and the influence on propagation time of bound material in the proximity of the waveguide. The waveguide layer thickness and the radiation wavelength λ are selected so that the effects on phase difference between the two radiations applied in the beam are minimal in the region directly adjacent the surface of the waveguide, so as to unmask the influence of the more distant bound materials.

Claims

1. A method for detecting a target material located within a first range of distances, above the surface of a waveguide of predetermined dimensions, and in the presence of a non target material in a second range of distances close to the waveguide surface, said first and second ranges being sufficiently close for material to effect therewithin propagation of radiation in said waveguide, said method comprising the steps of:

directing a first radiation of a selected wavelength and phase through said waveguide;

directing a second radiation of a selected wavelength and phase through said waveguide;

interferometrically detecting a phase difference between the first radiation and the second radiation as the first radiation and the second radiation are directed through said waveguide;

the detected phase difference having a relatively low first component effect provided by the selected wavelength of the first radiation and the selected wavelength of the second radiation cooperating with said predetermined dimensions of the waveguide to act on the phase difference caused by the non target material;

the detected phase difference having a relatively large second component effect provided by the selected wavelength of the first radiation and the selected wavelength of the second radiation cooperating with said predetermined dimensions of the waveguide to act on the phase difference caused by the target material; and

detecting the target material by comparing the first component effect and the second component effect.

2. The method of claim 1 further including the step of sensitizing said waveguide surface to bind said target materials.

3. The method of claim 2 wherein said sensitizing step includes sensitizing said surface to bio-materials which bind to the sensitized surface with at least a portion of said biomaterials within said first range of distances.

4. The method of claim 1 further including the step of directing a fluid containing said target materials across the surface of the waveguide.

5. The method of claim 4 wherein said fluid directing step includes the step of applying in sequence as a fluid across the waveguide surface a first applied buffer fluid, the target material containing fluid, and a second applied buffer fluid.

6. The method of claim 5 wherein said step of detecting a phase difference includes the step of detecting a phase difference shift between conditions of the first and second applied buffer fluids.

7. The method of claim 6 wherein said first and second applied buffer fluids are the same.

8. The method of claim 1 further including the step of applying the directed first and second radiations through gratings into said waveguide.

9. The method of claim 1 further including the step of forming said waveguide from a thin film dielectric material.

10. The method of claim 9 wherein said dielectric material is silicon, doped glass, or silicon-oxynitride.

11. The method of claim 10 wherein said waveguide is at least partially bordered other than at said surface by layers with substantially different indices of refraction thereby to substantially confine the directed first and second radiation to said waveguide.

12. The method of claim 10 wherein said waveguide is formed of silicon nitride silicon dioxide and has a thickness of at least 0.08 nm.

13. The method of claim 12 wherein said first and second radiations are the TE₀ and TM₀ modes.

14. The method of claim 1 wherein said detecting step further includes forming an interference pattern between the first and second radiations exiting said waveguide.

15. The method of claim 14 further including the step of detecting the phase difference as a shift in the interference pattern against a standard condition of substantially no bound target material.

16. The method of claim 1 wherein said directing step includes the step of directing said first and second radiations to a waveguide having a ridged cross section.

17. The method of claim 1 wherein said directing step includes the step of applying said first and second radiations in a beam of smaller cross section dimensions than that of the cross section dimensions of said waveguide.

18. The method of claim 1 further including the step of forming said first and second radiations by separating the radiation in a laser beam into different modes.

19. The method of claim 18 wherein said different modes are the TE₀ and TM₀ modes.

20. Apparatus for use in the method of claim 1 including:

a thin film waveguide having a transverse wave supporting channel;

a surface bordering said waveguide for exposure to target material;

said surface partially transmissive to transverse waves and thereby causing a phase sensitive delay in the transmission of said transverse waves in said waveguide as a function of target material beyond said surface and not immediately adjacent to said surface.

21. The apparatus of claim 20 further including a fluid path adjacent said surface for applying material into the vicinity of said surface to thereby effect a delay in the propagation of said transverse waves to a degree representative of the target material.

22. The apparatus of claim 20 further including a sensitized layer on said waveguide surface to bind said target materials.

23. The apparatus of claim 20 wherein said surface is sensitized to bio-materials which bind to the sensitized surface within said first range of distances.

24. The apparatus of claim 20 further including means for directing a fluid containing said target materials across the surface of the waveguide.

25. The apparatus of claim 24 wherein said fluid directing means includes means for applying in sequence as a fluid across the waveguide surface a first applied buffer fluid, the target material containing fluid, and a second applied buffer fluid.

26. The apparatus of claim 25 further including means detecting a phase difference shift between conditions of the application of the first and second applied buffer fluids.

27. The apparatus of claim 20 wherein said first and second applied buffer fluids are the same.

28. The apparatus of claim 20 further including gratings for applying the directed first and second radiations into said waveguide.

29. The apparatus of claim 20 wherein said waveguide is a thin film dielectric material.

30. The apparatus of claim 29 wherein said dielectric material is silicon, doped glass or silicon-oxynitride.

31. The apparatus of claim 30 wherein said waveguide is at least partially bordered other than at said surface by layers with substantially different indices of refraction thereby to substantially confine the directed first and second radiation to said waveguide.

32. The apparatus of claim 30 wherein said waveguide material is silicon nitride silicon dioxide and has a thickness of at least 0.08 nm.

33. The apparatus of claim 32 wherein said first and second radiations are the TE₀ and TM₀ modes.

34. The apparatus of claim 20 further including means for forming an interference pattern between the first and second radiations exiting said waveguide.

35. The apparatus of claim 34 further including means for detecting a phase difference representative of the presence of a target material as a shift in the interference pattern against a standard condition of substantially no bound target material.

36. The apparatus of claim 20 wherein said waveguide has a ridged cross section.

37. The apparatus of claims 20 wherein said first and second radiations are in a beam of smaller cross section dimensions that the cross section dimensions of said waveguide.

38. The apparatus of claim 20 further including means for separating the radiation In a laser beam into different modes.

39. The apparatus of claim 38 wherein said different modes are the TE₀ and TM₀ modes.

40. The method of claim 1 wherein said target materials are bio specimens.

41. The apparatus of claim 20 wherein said target materials are bio specimens.

42. A method for detecting a presence of a target material at a distance from a surface of a waveguide in a presence of a non target material closer to said surface comprising the steps of:

selecting a wavelength of a radiation;

selecting a thickness of said waveguide;

having the non target material bound to said surface more closely than a target material bound to said surface;

applying the radiation in a TE₀ mode to said waveguide;

applying the radiation in a TE_M mode to said waveguide;

combining the radiation in the TE₀ mode and the radiation in a TE_M mode to create an interference pattern;

the waveguide thickness being selected to enhance an effect of target material on said interference pattern relative to an effect of non target material; and

detecting the presence of the target material based on the interference pattern.

44. The method of claim 42 wherein the step of detecting includes a step of detecting the presence of the non target material based on the interference pattern.

43. (canceled)