Optics: measuring and testing – Refraction testing – Prism engaging specimen
Reexamination Certificate
2002-03-08
2004-04-06
Pham, Hoa Q. (Department: 2877)
Optics: measuring and testing
Refraction testing
Prism engaging specimen
Reexamination Certificate
active
06717663
ABSTRACT:
BACKGROUND OF THE INVENTION
I. Field of the Invention
The present invention relates generally to optical instruments for measuring refractive index of a substance, and more particularly to an optical configuration and method for measuring a difference in refractive index between a test sample and a reference sample. The present invention is applicable to differential refractometers and surface plasmon resonance (SPR) biosensor devices.
II. Description of the Related Art
Refractometers measure the critical angle of total reflection by directing an obliquely incident non-collimated beam of light at a surface-to-surface boundary between a high refractive index prism and a sample to allow a portion of the light to be observed after interaction at the boundary. In transmitted light refractometers, light that is transmitted through the sample and prism is observed, while in reflected light refractometers, the light that is reflected due to total reflection at the surface-to-surface boundary is observed. In either case, an illuminated region is produced over a portion of a detection field of view, and the location of the shadowline between the illuminated region and an adjacent dark region in the detection field of view allows the sample refractive index to be deduced geometrically. Differential refractometers, for example that disclosed in U.S. Pat. No. 5,157,454, have been developed for measuring a difference in refractive index between a test sample and a known reference sample, whereby variable test conditions effecting the measurement result, such as sample temperature, illumination level, etc., can be “subtracted out” to yield a more accurate and precise measurement result. The prior art differential refractometers known to applicants involve moving parts which malfunction or wear out over time, and/or are restricted to the transmitted light variety so as to prevent measurement of samples having relatively high opacity.
Optical biosensor devices designed to analyze binding of analyte molecules to a binding layer by observing changes in internal reflection at a sensing interface are also part of the related prior art. More specifically, U.S. Pat. No. 5,313,264 to Ivarsson et al. describes an optical biosensor system that comprises a plurality of side-by-side sensing surfaces 39A-D illuminated by a streak of light
5
extending transversely across the sensing surfaces, and an anamorphic lens system
6
by which rays of light reflected from the respective sensing surfaces are imaged on corresponding columns of a two-dimensional array
7
of photosensitive elements. Accordingly, the signals from the photosensitive elements can be processed to determine a minimum reflectance associated with the resonance angle at each sensing surface. Although the system described in U.S. Pat. No. 5,313,264 avoids the use of moving parts, it is nevertheless optically complex and requires a two-dimensional array, factors that are accompanied by an increase in cost.
Finally, it is noted that one-dimensional (linear) arrays of photosensitive elements cells are commonly used in automatic refractometers designed to take non-differential readings with respect to a single test sample. Examples can be found in U.S. Pat. Nos. 4,640,616 (Michalik) and 6,172,746 (Byrne et al.). However, applicants are unaware of any critical angle optical device for differential refractive index measurements that operates using a linear array, despite the recognized economy offered by this type of array.
BRIEF SUMMARY OF THE INVENTION
Therefore, it is an object of the present invention to provide an optical configuration for differential refractive index measurements wherein a test sample and a reference sample are illuminated by a single illuminating beam.
It is another object of the present invention to provide an optical configuration for differential refractive index measurements that does not rely on moving parts.
It is a further object of the present invention to provide an optical configuration for differential refractive index measurements wherein detected light has been reflected rather than transmitted at an optical interface of the configuration.
It is a further object of the present invention to provide an optical configuration for critical angle differential refractive index measurements wherein light interacting at first and second optical interfaces corresponding to a test sample and a reference sample is detected by a single linear scanned array of photoelectric cells.
It is a further object of the present invention to provide an optical configuration for differential refractive index measurements in accordance with the objects stated above, and which operates based on surface plasmon resonance principles for use in a biosensor device.
An optical configuration formed in accordance with a first embodiment of the present invention comprises an optical path defining a meridional plane of the configuration. A high index prism in the optical path includes a sample surface divided by a partition residing in the meridional plane, such that a test sample and a reference sample supported by the sample surface are located on opposite sides of the meridional plane to establish a first optical interface associated with the test sample and a second optical interface associated with the reference sample. An illumination beam traveling along the optical path illuminates both optical interfaces simultaneously to provide a first partial beam defined by the refractive index of the test sample and a second partial beam defined by the refractive index of the reference sample. Optical means direct the first and second partial beams to illuminate different respective segments of a linear scanned array of photoelectric cells aligned in the meridional plane, whereby a difference in refractive index can be determined by a difference in shadowline location on the array. In the first embodiment, optical means includes a single wedge affixed to an exit surface of the prism in the path of the first partial beam to cause deflection thereof relative to the second partial beam.
In a second embodiment similar to the first embodiment, another wedge is affixed to the exit surface of the prism in the path of the second partial beam and in opposite orientation relative to the first wedge to achieve greater separation between the partial beams.
A third embodiment based on the first and second embodiments is an adaptation of the basic configuration in order to observe molecular interactions, particularly specific binding of analyte molecules to a binding layer, using the principles of surface plasmon resonance. In accordance with the third embodiment, a thin metallic film is applied to a slide placed on the sample surface or directly to the sample surface, and the test sample and reference sample are brought into contact with the metallic film to define first and second evanescent wave optical interfaces. In this embodiment, the locations of resonance minimums exhibited by the first and second partial beams are detected.
As taught in a fourth embodiment of the present invention, the optical means may include a pair of two-axis wedges arranged in opposite fashion in the paths of the first and second partial beams for both separating the partial beams along an axis of the linear scanned array and converging the partial beams toward the meridional plane to arrive at the linear scanned array. As an alternative to using two-axis wedges, a pair of single axis wedges may be used in combination with a cylinder lens or biprism between the prism and linear scanned array.
The present invention further encompasses methods for measuring a difference in refractive index between a test sample and a reference sample based on the specified optical configurations.
REFERENCES:
patent: 4042304 (1977-08-01), Martin et al.
patent: 4126393 (1978-11-01), Sumikama et al.
patent: 4640616 (1987-02-01), Michalik
patent: 4834104 (1989-05-01), Kreinick et al.
patent: 4952055 (1990-08-01), Wyatt
patent: 5157454 (1992-10-01), Oka et al.
patent: 5305071 (1994-04-01), Wyatt
paten
Atkinson Robert C.
Byrne Michael J.
Ryan Thomas E.
Sharma Keshav
Hodgson & Russ LLP
Pham Hoa Q.
Reichert, Inc.
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