Method for the determination of species in solution with an optical wave-guide

• US RE33,064 E
• Filed: 10/09/1987
• Issued: 09/19/1989
• Est. Priority Date: 09/18/1981
• Status: Expired due to Term

• Current Assignee: Prutec Ltd. (Mutual Life Assurance Co. of Canada)
• Original Assignee: Prutec Ltd. (Mutual Life Assurance Co. of Canada)
• Inventors: Carter, Timothy J. N., Dahne, Claus, Place, John F.
• Primary Examiner(s): NOT, DEFINED
• Application Number:
  US07/107,763
• Time in Patent Office: 711 Days
• Field of Search: 356/440, 356/435, 356/436, 356/445, 356/448, 356/414, 356/417, 356/418, 422/55-60, 422/68, 422/73, 422/83, 422/86, 435/7, 436/34, 436/164, 436/165, 436/514, 436/527, 436/535, 436/805
• US Class Current: 436/34
• 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

An analyte in solution is made to react with a specific reactant coated on the wave-guide thus modifying the optical properties thereof. The index of refraction of the wave-guide material is higher than that of the reaction medium which ensures that a light signal injected into said guide be carried by multiple total reflection, the distance of penetration of the evanescent wave associated with the totally reflected signal being of the same order of magnitude or greater than the thickness of the analyte-reactant product layer.

Claims

1. A method of determining the presence .Iadd.and concentration .Iaddend.of an analyte in solution, which comprises the steps of:

(a) applying a film of a reaction to a surface of an optical waveguide .Iadd.core .Iaddend.having a refractive index n₁ ;

(b) .[.injecting a light signal of a wave length λ

into said waveguide at one end thereof and measuring at another end of said waveguide a light signal modification resulting from an evanescent light component associated with said signal in said waveguide, said light signal being internally reflected at an angle θ

of internal reflection.]. .Iadd.contacting said film with a solution of an analyte in a liquid phase of refractive index n₂ less than n₁, whereby said analyte reacts with said reaction to form an analyte/reactant reaction product layer at the surface of said waveguide core, .Iaddend.

(c) .[.contacting said film with a solution of an analyte in a liquid phase of refractive index n₂ less than n₁ whereby said analyte reacts with said reactance to form a layer of analyte-reactant product on said waveguide of a thickness less than λ

; and

.]. .Iadd.injecting a light signal of waveguide λ

into said waveguide core at an input thereof, whereby said light signal is internally reflected through said waveguide core at an angle θ

of internal reflection and evanescent wave component of said light signal interacts with said analyte/reactant product at the surface of said waveguide core which interaction results in a modification of said light signal representing presence and concentration of said analyte, .Iaddend.

(d) controlling the depth of penetration dp of said evanescent .[.light.]. .Iadd.wave .Iaddend.component .[.associated with said signal in said waveguide.]. .Iadd.into said liquid phase .Iaddend.in accordance with the relation;

##EQU3## so that said depth of penetration dp substantially matches or exceeds the thickness of said .[.analyte-reactant.]. .Iadd.analyte/reactant .Iaddend.product layer .[.and the measurement in step (b) takes place while the reaction occurs without interference from spurious signals from the liquid phase surrounding said layer..]..Iadd., and

(e) measuring at an output of the waveguide core said light signal modification while the reaction occurs without interference from spurious signals from the liquid phase surrounding said layer.Iaddend..

2. The method defined in claim 1 wherein .[.the.]. .Iadd.said evanescent component has an .Iaddend.electric field .[.E of said evanescent component .Iadd.having a value E .Iaddend.at a depth of penetration dp corresponding to the thickness of said reactant product layer .[.is.]..Iadd., said value being .Iaddend.at least 0.1 of the value Eo of the electric field at zero depth.

3. The method defined in claim 1 in which said modification .[.refers to.]. .Iadd.is .Iaddend.the absorption of the light signal, .Iadd.said light signal being injected into one end of said waveguide core and said output being at another end of said waveguide core, .Iaddend.said modification leading to a decrease with time of the light signal measured at .[.an.]. .Iadd.said .Iaddend.output of said waveguide core.

4. The method defined in claim 1 in which said modification is the generation of a fluorescent light signal, said fluorescent light signal increasing with time as measured at .[.an.]. .Iadd.said .Iaddend.output of said waveguide .Iadd.core.Iaddend..

5. The method defined in claim 1 in said .Iadd.said .Iaddend.modification is the scattering of said light wave signal, the extent of such scattering increasing with time and being measurable partly laterally of the scattering region and partly at .[.an.]. .Iadd.said .Iaddend.output of the waveguide .Iadd.core.Iaddend..

6. The method defined in claim 1 in which a polarized light signal is used and in which said modification affects elliptical polarization parameters of said signal.

7. The method defined in claim 1 in which the waveguide .Iadd.core .Iaddend.is selected from .[.the.]. .Iadd.a .Iaddend.light transparent plate, rod or fiber with refractive index of at least 1.4.

8. The method defined in claim 1 in which the waveguide g core is a single mode or multi-mode optical fiber.

9. The method defined in claim 1 in which a multi-mode fiber is used as said waveguide .Iadd.core.Iaddend., and comprising using modes sufficiently shallow, with regard to .Iadd.an axis of .Iaddend.the fiber .[.axis.]., to ensure total reflection and sufficiently steep to ensure a high linear density of light signal/coating interaction sites.

10. The method defined in claim 1 in which the waveguide .Iadd.core .Iaddend.is a multi-mode fiber and in which the modes are selected with an initial reflecting angle close to the critical angle, whereby in the course of the reaction a slight change in the refractive index N₂ n₂ of .[.the.]. .Iadd.a .Iaddend.rare medium that occurs due to the growing of the analyte-reactant product will result in at least partial refraction of the .Iadd.signal .Iaddend.outside the waveguide .Iadd.core.Iaddend..

11. The method defined in claim 1 wherein the light signal modification in step (b) is monitored with time, and .[.the.]. rate data so obtained is correlated with corresponding standard reference rate data obtained in a similar manner from calibrating samples of said analyte.

12. The method defined in claim 11 wherein a reference quantity of the analyte is contacted with said film while adding beforehand or simultaneously therewith a reference amount of reactant for causing the latter to competitively react with the analyte in the solution and said reference quantity on the surface .Iadd.of said waveguide core.Iaddend..

13. The method defined in claim 11 in which there is added in the analyte solution a tracer quantity of pure analyte in labelled form, the presence of a label in the reactant analyte product layer on the waveguide surface causing the said modification to the light signal travelling through said waveguide core, the magnitude of said modification being in direct relation with the ratio of labelled analyte in the solution.

14. The method defined in claim 11 wherein said film of said reactant on said surface is in excess of that stoichiometrically needed for binding the analyte in the solution to be determined, contacting said .[.coated.]. surface .Iadd.having said film thereon .Iaddend.with the analyte solution for totally binding said analyte to be determined, adding to the analyte solution a reference amount of analyte in pure labelled form to react with the still unused excess of reactant, the presence of said label in the reactant analyte product causing the said light signal modification occurring to the light signal, the magnitude of said modification being in direct proportion to the ratio of the labelled analyte to the analyte originally in the solution.

15. The method defined in claim 11 in which the analyte .[.prossesses.]. .Iadd.possesses .Iaddend.more than one binding side for specifically binding more than one kind of reactant, comprising contacting said surface coated with a first reactant with said analyte solution, adding a reference quantity of a second reactant for having said second reactant to bind to a second binding site of said analyte, the said light signal modification being the result of the binding of said second reactant on the said second binding site of the analyte bonded by a first binding site on said first reactant on the surface.

16. The method defined in claim 11 .[.in which.]. .Iadd.comprising interpreting .Iaddend.said rate data are interpreted in terms of the slope of the rate curves pertaining to the reaction under test and .[.can be extrapolated.]. .Iadd.extrapolating the rate curves .Iaddend.to determine equilibrium conditions.