WikiPatents - Community Patent Review
Create Free Account  |  License or Sell Your Patent  |  WikiPatents Marketplace  |  WikiPatents Blog
Username:  Password:  
    
Advanced Search
Scattered total internal reflectance immunoassay system    
United States Patent5017009   
Link to this pagehttp://www.wikipatents.com/5017009.html
Inventor(s)Schutt; Ernest G. (Long Valley, NJ); Dondero; Richard S. (Riverdale, NJ); Hansen; William P. (Middleboro, MA); Hovorka; George B. (Hyde Park, MA); Meyer; Raymond E. (Arlington, MA); Utberg; Karin L. (Bridgewater, NJ); Greenwood; David L. (Bound Brook, NJ)
AbstractA new immunoassay system is provided for the detection of ligands or ligand binding partners in solution in a heterogeneous format. The invention relies upon the detection of back scattered light from an evanescent wave disturbed by the presence of a colloidal gold label brought to the interface by an immunological reaction. The evanescent wave existing at the interface in turn is the result of a totally internally reflected incident light wave. Placement of the detector at a back angle above the critical angle insures a superior signal-to-noise ratio.



 Title Information Submit all comments and votes
 
Patent Text Patent PDF Print Page Summary File History
Plain text PDF images Print Summary File History
Drawing from US Patent 5017009
Scattered total internal reflectance immunoassay system - US Patent 5017009 Drawing
Scattered total internal reflectance immunoassay system
Inventor     Schutt; Ernest G. (Long Valley, NJ); Dondero; Richard S. (Riverdale, NJ); Hansen; William P. (Middleboro, MA); Hovorka; George B. (Hyde Park, MA); Meyer; Raymond E. (Arlington, MA); Utberg; Karin L. (Bridgewater, NJ); Greenwood; David L. (Bound Brook, NJ)
Owner/Assignee     Ortho Diagnostic Systems, Inc. (Raritan, NJ)
Patent assignment
All assignments
Publication Date     May 21, 1991
Application Number     07/149,243
PAIR File History     Application Data   Transaction History
Image File Wrapper   Patent Term   Fees
Litigation
Filing Date     January 27, 1988
US Classification     356/338 422/82.05 436/527 436/807
Int'l Classification     G01N 021/49
Examiner     Rosenberger; Richard A.
Assistant Examiner    
Attorney/Law Firm     Michael, Matthews; Gale F. Stark;
Address
Parent Case     This application is a continuation-in-part of U.S. Ser. No. 879,236, filed June 26, 1986, now abandoned, the contents of which are hereby incorporated by reference into the subject application.
Priority Data    
USPTO Field of Search     356/336 356/338
Patent Tags     scattered total internal reflectance immunoassay
   
Enter a comma (,) or semicolon (;) between multiple tag words/phrases.
Describe this patent:
 Amusing   
 Clever   
 Complex   
 Efficient   
 Historic   
 Important   
 Innovative   
 Interesting   
 Practical   
 Simple   
[no votes]
Patent WIKI

Share information and news about this patent, including information and news about the technology, inventors, company, ligation and licensing.

 References Submit all comments and votes
 
*references marked with an asterisk below are user-added references
 U.S. References
 
Add a new US reference:  
ReferenceRelevancyCommentsReferenceRelevancyComments
4558014
Hirschfeld
436/527
Dec,1985

[0 after 0 votes]
4521522
Lundstrom
436/525
Jun,1985

[0 after 0 votes]
4456374
Langberg
356/237.2
Jun,1984

[0 after 0 votes]
4447546
Hirschfeld
436/527
May,1984

[0 after 0 votes]
4313734
Leuvering
436/525
Feb,1982

[0 after 0 votes]
4181441
Noller
356/414
Jan,1980

[0 after 0 votes]
3975084
Block
356/335
Aug,1976

[0 after 0 votes]
3939350
Kronick
250/365
Feb,1976

[0 after 0 votes]
 Foreign References
 Other References
 Market Review Submit all comments and votes
   
Market Size
Estimate the gross annual revenues of the relevant market sector:
> $10B
$5B - $10B
$2B - $5B
$500M - $2B
$100M - $500M
$10M - $100M
$1M - $10M
$500K - $1M
$100K - $500K
< $100K
[No votes]
$0
 
$0   $2.5B   $5B   $7.5B   $10B
Market Share
Estimate the percentage of the relevant market sector this invention will capture:
75% - 100%
50% - 74.99%
25% - 49.99%
10 - 24.99%
5 - 9.99%
2 - 4.99%
1 - 1.99%
< 1%
[No votes]
0.0%
 
0%   25%   50%   75%   100%
Reasonable Royalty
What percentage of gross sales should the inventor or assignee be paid?
75% - 100%
50% - 74.99%
25% - 49.99%
10 - 24.99%
5 - 9.99%
2 - 4.99%
1 - 1.99%
< 1%
[No votes]
0.0%
 
0%   25%   50%   75%   100%
Public's "Guesstimation" of Royalty Value
Market SizeN/A[No votes]
xMarket ShareN/A[No votes]
xReasonable RoyaltyN/A[No votes]

N/A

License Availablity
If you are NOT the owner or assignee, answer here:
Yes, license is available for purchase

No, license is not currently available



[No votes]
License Availablity
If you ARE the owner or assignee, answer here:
Yes, license is available for purchase

No, license is not currently available



[No votes]
Competitive Advantage
Does this invention have a significant competitive advantage over similar technologies?
Yes

No



[No votes]
Most helpful competitive advantage comment
[No comments]

Commercial Alternatives
Are there viable commercial alternatives for this invention?
Yes

No



[No votes]
Most helpful commercial alternative comment
[No comments]

 Technical Review Submit all comments and votes
 Claims Submit all comments and votes
 


What is claimed is:

1. An apparatus for detecting the presence of an analyte of interest inn a sample which comprises:

a light source;

housing means for receiving an optically transparent member having a sample contacting surface, said member in said housing means being disposed such that the sample contacting surface is illuminated with light emitted from said light source; and

photodetection means which excludes the detection of light which propagates in a geometric optical path from the light source, said photodetection means being capable of detecting elastically-scattered light which propagates through the optically transparent member from the illuminated sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle of the sample contacting surface; said photodetection means comprising a rotatable optical means comprising a first reflecting means and a second reflecting means whose optical axis is nearly coincident with the optical axis of said first reflecting means, whereby said elastically-scattered light is concentrated to facilitate detection thereof, said first reflecting means located to receive said elastically-scattered light and said second reflecting means located to receive light reflected from said first reflecting means.

2. An apparatus for detecting the presence of an analyte of interest in a sample which comprises:

a light source;

housing means for receiving an optically transparent member having a sample contacting surface, said member in said housing means being disposed such that the sample contacting surface is illuminated with light emitted from said light source which propagates through the optically transparent member at angles between the plane of the sample contacting surface and the critical angle for total internal reflectance; and

photodetection means which excludes the detection of light which propagates in a geometric optical path from the light source, said photodetection means being capable of detecting elastically--scattered light which propagates through the optically transparent member from the illuminates sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle; said photodetection means comprising a rotatable optical means comprising a first reflecting means and a second reflecting means whose optical axis is nearly coincident with the optical axis of said first reflecting means, whereby said elastically-scattered light is concentrated to facilitate detection thereof, said first reflecting means located to receive said elastically-scattered light and said second reflecting means located to receive light reflected from said first reflecting means.

3. The apparatus of claim 2 wherein said optically transparent member comprises a molded polymeric cuvette.

4. The apparatus of claim 3 wherein said sample contacting surface of said optically transparent member comprises one surface of a sample receiving cavity.

5. The apparatus of claim 3 wherein the first surface illuminated by light source is aligned to specularly reflected said light so that it is not detected by said photodetection means.

6. The apparatus of claim 2 wherein said first and second reflecting means are paraboloidal reflectors.

7. The apparatus of claim 6 wherein said paraboloidal reflectors are off-axis segments of said paraboloidal reflectors.

8. The apparatus of claim 2 further comprising:

a non-rotating first means to convert the light emitted from said light source from plane polarized light into circularly polarized light;

a second means located on said rotatable optical means to reconvert the polarized light received from said first means to plane polarized light.

9. The apparatus of claim 8 wherein said means to convert said light comprise one-quarter wave retardation plates.

10. The apparatus of claim 8 wherein:

said housing means is adapted to receive a plurality of said optically transparent members arranged in a circle above said rotatable optical means, which circle is centered on the rotational axis of said rotatable optical means,

each of said optically transparent members comprising a molded polymeric cuvette having a sample contacting surface which can be illuminated by said light source and aligned to specularly reflect said light so that it is not detected by said photodetection means,

said rotatable optical means adapted to present polarized light to each cuvette in turn, and

said photodetection means further comprising an optical encoder coupled to the rotatable optical means.

11. The apparatus of claim 2 further comprising:

a non-rotating first means to convert the light emitted from said light source from plane polarized light into circulatory polarized light;

a second means located on said rotatable optical means to reconvert the polarized light received from said first means to plane polarized light; and

a third means to optimize said polarization achieved by said first and second means.

12. The apparatus of claim 11 wherein said non-rotating means to convert said light comprise one-quarter wave retardation plates.

13. The apparatus of claim 2 further comprising an aperture whereby other than said elastically-scattered light is substantially excluded.

14. The apparatus of claim 13 wherein said aperture comprises a rotating aperture which rotates with said rotatable optical means.

15. The apparatus of claim 2 further comprising an optical encoder coupled to the rotatable optical means.

16. A method for detecting the presence of a light scattering molecule on the surface of an optically transparent material which comprises illuminating said light scattering molecule from light through rotating optical reflectors detecting light scattered elastically by said light scattering molecule which propagates through said optically transparent material between the plane of the surface of the optically transparent material on which the light scattering molecule is located and the total internal reflectance critical angle of the surface on which the light scattering molecule is located, and correlating detected, elastically-scattered light to the presence of the light scattering molecule on the surface of the optically transparent material.

17. A method for detecting the presence of a light scattering molecule on the surface of an optically transparent material which comprises illuminating said light scattering molecule with an evanescent wave resulting from a light wave which propagates through said optically transparent material from light through rotating optical reflectors, detecting light scattered elastically by said light scattering molecule which propagates through said optically transparent material between the plane of the surface of the optically transparent material on which the light scattering molecule is located and the total internal reflectance critical angle of the surface on which the light scattering molecule is located, and correlating detected, elastically-scattered light to the presence of the light scattering molecule on the surface of the optically transparent material.

18. The method of claim 17 wherein the detecting step further comprises:

obtaining a plurality of readings of said elastically-scattered light by moving said light source across said sample contacting surface and recording said readings at discrete locations identified by means of an encoder.

19. The method of claim 18 wherein the step of obtaining a plurality of readings is performed once per revolution of said rotating optical reflectors.
 Description Submit all comments and votes
 


FIELD OF THE INVENTION

This invention relates to immunoassays generally and more particularly provides a new system for performing virtual homogeneous immunoassaYs employing colloidal gold.

BACKGROUND OF THE INVENTION

Many human disease states are identified on the basis of immunoassay techniques which rely upon the specificity between immunoglobulin, whether monoclonal or polyclonal, and their respective binding partners, which may be haptens, antigens, or other analytes, all of which may hereafter be collectively and interchangeably referred to herein as "ligands" and "ligand binding partners." Furthermore, "ligand" also means any molecule having an affinity to bind or complex with a "ligand binding partner", including chelators, immunobinders, nucleic acid strands, bioreceptors, and hydrophobic binders. Over the past fifteen or so years, there has been a substantial amount of effort involved in the development of immunoassay techniques utilizing the so-called sandwich and competitive techniques. The sandwich technique involves the immobilization of an antigen by one antibody and then subsequent labeling by attachment of a second antibody having associated therewith a detectable label. Reverse immunoassays for the detection of antibody are similar but instead put antigen on the surface for reaction with the sample antibody. Competitive techniques are useful for antigens having only a single epitopic site for reaction with an antibody. Accordingly, and as the name implies, such techniques rely upon the competition of the antigen with another labeled antigen for a binding site on an immobilized antibody. The substitutions necessary for antibody detection tests are obvious and need not be covered here in any great detail.

Of great importance in the laboratory is the development of highly sensitive techniques which can be run in either batch random access, panel, or stat modes. Preferably, such techniques will be homogeneous in nature, i.e., and as used herein, they will be conducted solely within one container without any accompanying requirement to physically separate out components following reactions during the assay.

It is one object of the present invention to provide a new immunoassay system which is highly sensitive and which is homogeneous in nature.

U.S. Pat. 3,939,350 to Kronick and the Kronick citations therein referenced describe an immunoassay system which allows for the measurement of biochemical analytes by fluorescence in a liquid sample. Kronick employs a physical phenomenon known under the name of total internal reflectance. This optical phenomenon occurs wherein light, when directed through a high refractive index material toward the interface of that material with a second material having a lower refractive index at greater than a critical angle, all light is reflected from that interface save for a microscopic evanescent wave which propagates into the second material for only a short distance. The second material may, for instance, be water or another aqueous medium in which an assay is being conducted. Kronick noted that when he brought materials which had been fluorescently labeled down to the interface and within the field of the evanescent wave, he could energize the fluorescent molecules and detect fluorescence which then emanated into the overlying solution. The Kronick system, however, looks at fluorescence which cannot be readily modified by alteration of the fluorescent labels in order to suit the system under study. Due to the nature of the specificity of the fluorescent label with respect to the wavelength of the excitation frequency, one is limited to a discrete light source providing the critical excitation frequency. To date, most investigators favor the He-Ne laser light source due to its reliability and low cost as well as the low cost of associated optics. Such a light source, however, brings concomitant difficulties in tailoring fluorescent molecules to be excited by the He-Ne laser output. The organic, inorganic, and bio-organic techniques required are especially difficult to control in the immunoassay arena. Further, Kronick's reliance on fluorescence is accompanied by additional disadvantages associated with bleaching of the fluorescent molecules and generally critical matching of fluorescent molecule excitation wavelength with laser output wavelength necessary to obtain good quantum efficiency.

It is an object of the present invention to provide a new immunoassay system which avoids the disadvantages associated with fluorescent labels and the criticality associated with matching an excitation source.

It is another object of the present invention to employ the principles of total internal reflection but with far greater flexibility regarding the choice of illumination sources. U.S. Pat. 4,181,441 to Noller describes a system similar to that of Kronick. Noller, however, taught that the assay should be conducted by measurement of light absorption in a liquid sample which could then be correlated to the presence of biochemical analytes. Although the Noller system employs different physical principles than the Kronick system, light absorption measurements are similarly subject to poorer signal-to-noise ratios due to small differences in large light signals thereby making such a system inherently less sensitive than desired. It is another object of the present invention to avoid employing light absorption measurements while still gaining the advantages to be provided by the total internal reflectance phenomenon.

U.S. Pat. No. 4,521,522 to Lundstrom teaches yet another immunoassay based upon reflectance and the use of Brewster s angle. This system relies upon a different optical phenomenon wherein directing a light beam, polarized in the plane of incidence, upon an interface, for example that formed between plastic and liquid, results in the transmission of a strong light beam into the liquid when such light strikes the interface at the Brewster angle. At the Brewster angle, substantially no light is reflected.

The Brewster angle is a function of the refractive indices of the two materials as well as the direction of polarization. Lundstrom noted that upon the growth of a biochemical layer at the interface, the Brewster angle condition would be disrupted resulting in increasing light reflectance, particularly at angles less than the Brewster angle. Unfortunately, the Lundstrom assay only works effictively with a wash step since the transmission of the beam into the liquid also results in the generation of light scatter and thus a spurious signal.

It is another object of the present invention to utilize light scatter but to avoid light scatter generated by the transmission of light into the liquid which occurs naturally when light is directed at an interface at the Brewster angle. Accordingly, it is yet another object of the present invention to avoid employing a Brewster angle condition.

SUMMARY OF THE INVENTION

In accordance with various aspects and the principles of the present invention, there is provided an immunoassay system which utilizes scattered total internal reflectance (STIR) as a measure of the presence of particular ligands to be determined in an aqueous solution. The invention relies in part upon the identification of the critical angle associated with total internal reflectance. The angle is largely a function of the refractive index of the material through which an incident light wave is directed, e.g. plastic, and the relatively lower refractive index of the material in which the immunoassay is being conducted, e.g. an aqueous solution. It is measured from a line perpendicular to the interface between the two materials, and thus at its maximum, 90.degree. , will lie in the plane of the interface.

Light directed through the plastic toward the interface formed by the aqueous sample and plastic materials at the critical angle will result in total internal reflectance of the light within the plastic. It is recognized that no materials in the real world are perfect and accordingly, it is preferred that the incident light be directed toward the interface at an angle several degrees greater than the critical angle, most preferably in the range of approximately 6.degree. greater in order to ensure that the basic conditions of total internal reflectance are met. At such an angle, the incident collimated light, preferably from a laser, is totally internally reflected within the plastic save for the propagation of the evanescent wave parallel to the surface of the plastic and approximately 1/4.lambda. from the surface. Similarly, smooth surfaces at the interface are preferred for optimum signal quality. Unlike conventional fluorescent techniques including those of Kronick, the present assay system is flexible with respect to light wavelength since particle size may be readily adjusted to match the available light source (or vice versa) to provide acceptable light scatter. Fluorescent molecules are not readily adjustable with respect to excitation wavelength.

Most ideally, the light source will be a He-Ne light source, however, other lasers with different wavelength outputs have been used and still other sources suggest themselves including light emitting diodes and other nonlaser light sources.

Applicants' immunoassay system further relies upon conventional immunoassay techniques. However, applicants' immunoassay system also employs a particulate label having a higher refractive index than that of the solution, and most preferably also higher than the first light transmissive material, e.g. plastic in the foregoing example. Such Particles would include, for instance, red blood cells, other materials having a highly reflective surface such as metallic particles, and nonmetallic substances such as glass or plastics, e.g. latex particles, and the like. Most preferably, colloidal gold is used as a label for the solution phase immunologically active component. While the use of colloidal gold as a label is known, see for example U.S. Pat. No. 4,313,734 Leuvering, almost no nonagglutination related uses of the label have been made to date due to the difficulties associated with its detection, particularly in homogeneous type systems. It was surprisingly discovered by the inventors hereof that the unique combination of STIR with colloidal gold has resulted in an extremely efficient and sensitive homogeneous assay system. It is believed, but not known for certain that this is due primarily to the interaction of the colloidal gold particles with the evanescent wave. Indeed, experience implies that particles having an increasingly higher index of refraction than that of the underlying solid generally increasingly scatter light. While particles with indices of refraction less than the underlying solid, providing they are also not equal to that of the aqueous medium, would also scatter light, such are less preferred.

Assuming for the moment a conventional sandwich technique, one immunoglobulin or ligand binding partner is immobilized on the surface and binds antigen or other ligand to be determined. Thereafter, (or simultaneously, or if not previously) a second immunoglobulin, directed at a second epitopic site on the ligand, and labeled directly or indirectly with colloidal gold, binds to the ligand creating the so-called "sandwich". In this arrangement, the presence of the colloidal gold disrupts the propagation of the evanescent wave resulting in scattered light which may be detected by a photomultiplier or other light sensor to provide a responsive signal. Another important aspect of the present invention involves the physical location of the detector. The detector is ideally placed at an angle greater than the critical angle and in a location whereby only light scattered backward toward the light source is detected. This location thereby ideally avoids the detection of spurious scattered light within the bulk liquid medium.

Another feature of the instant invention is that the immunoassays are diffusion rate controlled and not particularly temperature dependent. This is in strong contrast to ELISA and various other immunoassay techniques wherein temperature control is critical since small changes in temperature in such systems results in wide variations in assay results per unit of time.

It was surprisingly found by the inventors hereof, that as a result of the combination of these elements, rapid, sensitive results could be obtained in a homogeneous environment without requiring the complicated equipment previously associated with colloidal gold assay techniques.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 depicts an optically transparent member 53 with refractive index n.sub.2 having a fluid contacting surface 52 in contact with fluid 54 having a refractive index n.sub.1 which is less than n.sub.2. The total internal reflectance critical angle 55 measured from a line 50 perpendicular to the plane of the fluid contacting surface 51 is the minimum angle of illumination required to provide total internal reflectance at surface 52. This angle is defined by the equation ##EQU1## The critical angle, .theta..sub.c, is only defined in the higher refractive index medium and can range from 0.degree. to 90.degree. . Light propagating from a point on the fluid contacting surface 58 at the total internal reflectance critical angle 55 would follow the path depicted as 57. All light propagating through the optically transparent member 53 from a point on the fluid contacting surface 58 between the plane of the sample fluid contacting surface 51 and the total internal reflectance critical angle 55 of the fluid contacting surface, will propagate in the range depicted as 56.

FIG. 2 is a simplified elevation view of the cuvette and the rotating optics mechanism used to illuminate and read it.

FIG. 3 is cross-section of a cuvette.

FIG. 4 is a perspective view of a cuvette and a paraboloidal reflector which is the first component of the receiving optics.

FIG. 5 depicts an apparatus with laser illumination above critical angle.

FIG. 6 depicts illumination and detection light paths used when illumination is above the critical angle.

FIG. 7 shows data obtained with the apparatus of FIG. 5.

FIG. 8 depicts an apparatus with light emitting diode illumination above the critical angle.

FIG. 9 shows data obtained with the apparatus of FIG. 8.

DETAILED DESCRIPTION OF THE INVENTION AND BEST MODE

The present invention provides an apparatus for detecting the presence of an analyte of interest in a sample. This apparatus comprises a light source; housing means for receiving an optically transparent member having a sample contacting surface, said member in said housing means being disposed such that the sample contacting surface is illuminated with light emitted from said light source; and photodetection means which excludes the detection of light which propagates in a geometric optical path from the light source, said photodetection means being capable of detecting elastically-scattered light which propagates through the optically transparent member from the illuminated sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle of the sample contacting surface. Within this application, "photodetection means" is defined as a system for detecting photons having a wavelength equal to the wavelength of the illuminating light, and includes combinations of photon detectors (e.g. photomultiplier tubes), lenses, mirrors, light filters, optical fibers, prisms, apertures, and masks. A geometric optical path is the path that a family of light rays will follow based on first order reflection and refraction of idealized surfaces (imperfection free) and ignoring the effects of surface and bulk material imperfections, diffraction, interference, scatter, and partial reflection at surfaces. Further, within this application, "elastically-scattered light" (also referrred to herein as "scatter" and "scattered light") means incident light which has been redirected by an object without changing the wavelength of the light, by means other than dopler shifting, due to the difference in the refractive index of the object and its surrounding medium. Fluorescence, also known as inelastic scatter, is the light emitted by a light absorbing molecule after the molecule has absorbed a photon of light. The wavelength of the absorbed light is less than the wavelength of the emitted light. Flouorescent light is always of a wavelength different from the light incident on the light absorbing molecule.

"Critical angle", also referred to herein as "total internal reflectance critical angle", is the angle (less than 90.degree. ) measured from the line perpendicular to an interface between materials of different refractive indexes, beyond which total internal reflection can occur, and is defined by the equation ##EQU2## wherein n.sub.1 is the lower refractive index and n.sub.2 is the higher refractive index of the two mediums forming the interface. The critical angle can only exist in the higher refractive index medium. Light which illuminates the interface from the lower refractive index material at any angle (0.degree. to 90.degree. ) cannot be refracted into the higher refractive index medium at an angle greater than or equal to the critical angle. Total internal reflection occurs exclusively when an interface between materials of different refractive indexes is illuminated from the higher refractive index medium beyond the critical angel, causing all the incident illumination to be reflected at the interface unless it is perturbed by diffraction, scatter, or absorption.

The present invention also provides another apparatus for detecting the presence of an analyte of interest in a sample. This apparatus comprises a light source; housing means for receiving an optically transparent member having a sample contacting surface, said member in said housing means being disposed such that the sample contacting surface is illuminated with light emitted from said light source which propagates through the optically transparent member at angles between the plane of the sample contacting surface and the critical angle for total internal reflectance; and photodetection means which excludes the detection of light which propagates in a geometric optical path from the light source, said photodetection means being capable of detecting elastically-scattered light which propagates through the optically transparent member from the illuminated sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle.

Suitable light sources for the apparatuses of the present invention provide collimated or uncollimated light, polarized or unpolarized light, or monochromatic or polychromatic light. Preferred light sources include lasers (e.g., He-Ne lasers), light emitting diodes (LEDs), flash lamps, arc lamps, incandescent lamps, and fluorescent discharge lamps.

Suitable optically transparent members, e.g., cuvettes, are comprised of glass, quartz, silicon, plastics such as polycarbonate, acrylic, or polystyrene, or oils comprising silicone or high molecular weight hydrocarbons.

Suitable photodetection means comprise photon detectors such as photomultiplier tubes, photodiodes (e.g., PIN diodes and gallium-aluminum-arsenide diodes), cadmium sulfide photoresistive cells, phototubes, and pyrolytic detectors. Also provided is a method for detecting the presence of a light scattering molecule on the surface of an optically transparent material. This method comprises illuminating said light scattering molecule, detecting light scattered elastically by said light scattering molecule which propagates through said optically transparent material between the plane of the surface of the optically transparent material on which the light scattering molecule is located and the total internal reflectance critical angle of the surface on which the light scattering molecule is located, and correlating detected, elastically-scattered light to the presence of the light scattering molecule on the surface of the optically transparent material. Within this application, an "evanescent wave" means a nonpropagating light wave such as a wave in the region of a surface on the side of the surface opposite the side of illumination, produced when the illuminating light undergoes total internal reflection. Also within this application a "light scattering molecule" means a molecule which causes incident light to be elastically scattered. "Molecule" includes, in the case of crystalline and elemental materials, two or more atoms.

Still further, the present invention provides a method for detecting the presence of a light scattering molecule on the surface of an optically transparent material. This method comprises illuminating said light scattering molecule with an evanescent wave resulting from a light wave which propagates through said optically transparent material, detecting light scattered elastically by said light scattering molecule which propagates through said optically transparent material between the plane of the surface of the optically transparent material on which the light scattering molecule is located and the total internal reflectance critical angle of the surface on which the light scattering molecule is located, and correlating detected, elastically-scattered light to the presence of the light scattering molecule on the surface of the optically transparent material.

Further provided is a method for detecting an analyte in a fluid sample wherein said analyte is a ligand of a ligand - ligand binding partner pair. This method comprises the steps of:

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of ligand binding partners of said ligand - ligand binding partner pair are immobilized;

b) further providing light scattering particle-labeled ligands capable of forming complexes with said immobilized ligand binding partners;

c) contacting said fluid sample and said light scattering particle-labeled ligands with said sample contacting surface under conditions such that said analyte and said light scattering particle-labeled ligands each form complexes with said immobilized ligand binding partners;

d) illuminating said complexes with an evanescent wave resulting from a light wave which propagates through said optically transparent material;

e) detecting light scattered elastically by said light scattering particles of said complexes;

f) correlating elastically-scattered light to the presence of complexes on said sample contacting surface; and

g) comparing the presence of complexes on the sample contacting surface with the presence of complexes on a sample contacting surface for a standard control, thereby detecting the analyte in the fluid sample.

Within this application, "particle" means one or more molecules. "Labeled" means directly linked, e.g., conjugated, cross-linked, or adsorbed, or indirectly linked, e.g., linked via an antibody.

Further yet is provided a method for detecting an analyte in a fluid sample wherein said analyte is a ligand of a ligand - ligand binding partner pair. This method comprises the steps of:

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of ligand binding partners of said ligand - ligand binding partner pair are immobilized;

b) further providing light scattering ligands caPable of forming complexes with said immobilized ligand binding partners;

c) contacting said fluid sample and said light scattering ligands with said sample contacting surface under conditions such that said analyte and said light scattering ligands each form complexes with said immobilized ligand binding partners;

d) illuminating said complexes;

e) detecting light scattered elastically by light scattering ligands of said complexes and which propagates through said optically transparent material from the sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle of the sample contacting surface;

f) correlating elastically-scattered light to the presence of complexes on said sample contacting surface; and

g) comparing the presence of complexes on the sample contacting surface with the presence of complexes on a sample contacting surface for a standard control, thereby detecting the analyte in the fluid sample.

Within this application, "light scattering ligands" means ligands or light scattering particle-labeled ligands which cause incident light to be elastically scattered.

Further still is provided a method for detecting an analyte in a fluid sample wherein said analyte is a ligand of a ligand - ligand binding partner pair. This method comprises

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of ligand binding partners of said ligand - ligand binding partner pair are immobilized;

b) further providing light scattering ligands capable of forming complexes with said immobilized ligand binding partners;

c) contacting said fluid sample and said light scattering ligands with said sample contacting surface under conditions such that said analyte and said light scattering ligands each form complexes with said immobilized ligand binding partners;

d) illuminating said complexes with an evanescent wave resulting from a light wave which propagates through said optically transparent material;

e) detecting light scattered elastically by light scattering ligands of said complexes and which propagates through said optically transparent material from the sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle of the sample contacting surface;

f) correlating elastically-scattered light to the presence of complexes on said sample contacting surface; and

g) comparing the presence of complexes on the sample contacting surface with the presence of complexes on a sample contacting surface for a standard control, thereby detecting the analyte in the fluid sample.

In one embodiment of the invention, the methods provided herein may be performed wherein the sample contacting surface is contacted .with the fluid sample before being contacted with the ligands<In another embodiment of the invention, the sample contacting surface is contacted with the ligands before being contacted with the fluid sample. In yet a further embodiment of the invention, the sample contacting surface is simultaneously contacted with said fluid sample and the ligands. In still another embodiment of the invention, the sample is mixed with the ligands so as to form a mixture, and the mixture is contacted with the sample contacting surface.

Furthermore, in a preferred embodiment of the invention, light scattering particle-labeled ligands comprise ligands labeled with colloidal gold particles.

In still another embodiment of the invention, a method is provided for detecting an analyte in a fluid sample. In this method the analyte is a ligand having an epitope for which a first ligand binding partner is specific and an epitope for which a second ligand binding partner is specific. The method comprises:

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of first ligand binding partners are immobilized;

b) further providing light scattering particle-labeled second ligand binding partners;

c) contacting said fluid sample and said light scattering particle-labeled second ligand binding partners with said sample contacting surface under conditions such that immobilized first ligand binding partner : analyte : light scattering particle-labeled second ligand binding partner complexes are formed;

d) illuminating said complexes with an evanescent wave resulting from a light wave which propagates through said optically transparent material;

e) detecting light scattered elastically by said light scattering particles of said complexes;

f) correlating elastically-scattered light to the presence of complexes on said sample contacting surface; and

g) comparing the presence of complexes on the sample contacting surface with the presence of complexes on a sample contacting surface for a standard control, thereby detecting the analyte in the fluid sample.

Still another method is provided for detecting an analyte in a fluid sample, wherein said analyte is a ligand having an epitope for which a first ligand binding partner is specific and an epitope for which a second ligand binding partner is specific. This method comprises:

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of first ligand binding partners are immobilized;

b) further providing light scattering second ligand binding partners;

c) contacting said fluid sample and said light scattering second ligand binding partners with said sample contacting surface under conditions such that immobilized first ligand binding partner : analyte : light scattering second ligand binding partner complexes are formed;

d) illuminating said complexes;

e) detecting light scattered elastically by said light scattering second ligand binding partners of said complexes and which propagates through said optically transparent material from the sample contacting surface between the plane of the sample contacting surface and the total internal reflectance critical angle of the sample contacting surface;

f) correlating elastically-scattered light to the presence of complexes on said sample contacting surface; and

g) comparing the presence of complexes on the sample contacting surface with the presence of complexes on a sample contacting surface for a standard control, thereby detecting the analyte in the fluid sample.

Within this application, "light scattering second ligand binding partners" means second ligand binding partners or particle labeled second ligand binding partners which cause incident light to be elastically scattered.

Still further is provided a method for detecting an analyte in a fluid sample wherein said analyte is a ligand having an epitope for which a first ligand binding partner is specific and an epitope for which a second ligand binding partner is specific. This method comprises:

a) providing an optically transparent material having a refractive index greater than the refractive index of said fluid sample, said optically transparent material having a sample contacting surface to which a plurality of first ligand binding partners are immobilized;

b) further providing light scattering second ligand binding partners;

c) contacting said fluid sample and said light scattering second ligand binding Partners with said sample contacting surface under conditions such that immobilized first ligand binding partner : analyte: light scattering second ligand binding Partner complexes are formed;

d) illuminating said complexes with an evanescent wave