EP0620916A1 - Analytical device with light scattering - Google Patents

Analytical device with light scattering

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Publication number
EP0620916A1
EP0620916A1 EP93901849A EP93901849A EP0620916A1 EP 0620916 A1 EP0620916 A1 EP 0620916A1 EP 93901849 A EP93901849 A EP 93901849A EP 93901849 A EP93901849 A EP 93901849A EP 0620916 A1 EP0620916 A1 EP 0620916A1
Authority
EP
European Patent Office
Prior art keywords
light
sensor
detector
source
refractive index
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP93901849A
Other languages
German (de)
French (fr)
Inventor
Douglas Alastair Stewart
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fisons Ltd
Original Assignee
Fisons Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fisons Ltd filed Critical Fisons Ltd
Publication of EP0620916A1 publication Critical patent/EP0620916A1/en
Withdrawn legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/55—Specular reflectivity
    • G01N21/552—Attenuated total reflection
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/55—Specular reflectivity
    • G01N21/552—Attenuated total reflection
    • G01N21/553—Attenuated total reflection and using surface plasmons

Definitions

  • This invention relates to sensors, especially those termed biosensors, ie devices for the analysis of biologically active species such as antigens and antibodies in samples of biological origin.
  • the invention relates to biosensors based on resonant optical phenomena, eg surface plasmon resonance or resonant attenuated or frustrated total internal reflection.
  • biosensors include a sensitised coating layer which is located in the evanescent region of a resonant field.
  • Detection of the analyte typically utilizes optical techniques such as, for example, surface plasmon resonance (SPR), and is based on changes in the thickness and/or refractive index of the coating layer resulting from interaction of that layer with the analyte. This causes a change, eg in the angular position of the resonance.
  • SPR surface plasmon resonance
  • optical biosensors include a waveguide in which a beam of light is propagated. The optical characteristics of the device are influenced by changes occurring at the surface of the waveguide.
  • One form of optical biosensor is based on frustrated total reflection.
  • the principles of frustrated total reflection (FTR) are well-known; the technique is described, for example, by Bosa ⁇ chi and Oehrle [Applied Optics (1982), 21, 2167-2173].
  • An FTR device for use in immunoassay is disclosed in European Patent Application No 2205236A and comprises a cavity layer bounded on one side by the sample under investigation and on the other side by a spacer layer which in turn is mounted on a substrate.
  • the substrate-spacer layer interface is irradiated with monochromatic radiation such that total reflection occurs, the associated evanescent field penetrating through the spacer layer. If the thickness of the spacer layer is correct and the incident parallel wave vector matches one of the resonant mode propagation constants, the total reflection is frustrated and radiation is coupled into the cavity layer.
  • the cavity layer must be composed of material which has a higher refractive index than the spacer layer and which is transparent at the wavelength of the incident radiation.
  • the position of resonance may be monitored by scanning the angle at which monochromatic light is incident on the sensor.
  • the scanning of angle may be performed either sequentially or simultaneously ie by varying the angle of incidence of a parallel beam of light or by simultaneously irradiating over a range of angles using a fan- shaped beam of light as described (in connection with SPR) in European Patent Application No 0305109A.
  • prior proposals have involved a single-channel detector which is mechanically scanned over a range of angles? this necessitates synchronisation of the movement of the light source and the detector.
  • the second configuration in which a range of angles is irradiated simultaneously, requires relatively complex optics, which leads to relatively high manufacturing costs.
  • apparatus for the determination of a chemical or biochemical species comprising a resonant optical sensor disposed in a light path between a source of monochromatic light and a detector adapted to monitor some characteristic of the light, a light- scattering element being disposed in the light path between the source and the sensor.
  • the apparatus according to the invention is advantageous primarily in that it enables simultaneous irradiation at a range of angles, yet is of relatively simple and inexpensive construction, eg due to the absence of complex optics.
  • a laser Any convenient source of monochromatic light may be used but it is preferable to use a laser.
  • the choice of laser will depend inter alia on the particular form of sensor used.
  • 'light' may include not only visible light but also wavelengths above and below this range, eg in the ultra ⁇ violet and infra-red.
  • the light-scattering element is preferably a speckle plate or diffusion screen. To overcome the problem of speckle being transferred to the output, it may be necessary to translate or rotate the speckle plate rapidly, ie quicker than the integration time of the detector.
  • the speckle plate may be a separate component or it may be formed integrally with another component, eg as the output side of a half-wavelength plate comprising a mica sheet sandwiched between two glass sheets.
  • the light-scattering element is formed on the input side of the sensor, eg where the sensor is formed as a disposable unit.
  • the light source can be located very close to the sensor, enabling the use of a compact and inexpensive light source such as a laser diode.
  • the characteristic of the light which is monitored may be any characteristic which changes at resonance, eg the phase of reflected radiation or, in some cases, the intensity.
  • the sensor is preferably an FTR sensor.
  • Such a sensor will generally include an optical structure comprising a) a cavity layer of transparent dielectric material of refractive index n 3 , b) a dielectric substrate of refractive index n lf and c) interposed between the cavity layer and the substrate, a dielectric spacer layer of refractive index n 2 .
  • the interface between the substrate and the spacer layer is irradiated with light such that internal reflection occurs. Resonant propagation of a guided mode in the cavity layer will occur, for a given wavelength, at a particular angle of incidence.
  • the wavelength at which the resonant effect occurs depends on various parameters of the sensor device, such as the refractive indices and thicknesses of the various layers. In general, it is a pre-requisite that the refractive index n 3 of the cavity layer and the refractive index n x of the substrate should both exceed the refractive index n 2 of the spacer layer. Also, since at least one mode must exist in the cavity to achieve resonance, the cavity layer must exceed a certain minimum thickness.
  • the cavity layer is preferably a thin-film of dielectric material. Suitable materials for the cavity layer include zirconium dioxide, titanium dioxide, aluminium oxide and tantalum oxide.
  • the cavity layer may be prepared by known techniques, eg vacuum evaporation, sputtering, chemical vapour deposition or in-diffusion.
  • the dielectric spacer layer must have a lower refractive index than both the cavity layer and the substrate.
  • the layer may, for example, comprise an evaporated or sputtered layer of magnesium fluoride.
  • suitable materials include lithium fluoride and silicon dioxide.
  • the spacer layer may be deposited on the substrate by a sol-gel process, or be formed by chemical reaction with the substrate.
  • the sol-gel process is particularly preferred where the spacer layer is of silicon dioxide.
  • the refractive index of the substrate (n must be greater than that (n 2 ) of the spacer layer but the thickness of the substrate is generally not critical.
  • the spacer layer will typically have a thickness of the order of several hundred nanometres, say from about 200nm to 2000nm, more preferably 500 to 1500nm, eg lOOOnm.
  • the cavity layer typically has a thickness of a few tens of nanometres, say 10 to 200nm, more preferably 30 to 150nm, eg lOOnm.
  • the cavity layer has a thickness of 30 to 150nm and comprises a material selected from zirconium dioxide, titanium dioxide, tantalum oxide and aluminium oxide
  • the spacer layer has a thickness of 500 to 1500nm and comprises a material selected from magnesium fluoride, lithium fluoride and silicon dioxide, the choice of materials being such that the refractive index of the spacer layer is less than that of the cavity layer.
  • Preferred materials for the cavity layer and the spacer layer are tantalum oxide and silicon dioxide respectively.
  • the incident light is coupled into the cavity layer by FTR, propagates a certain distance along the cavity layer, and couples back out (also by FTR) .
  • the propagation distance depends on the various device parameters but is typically of the order of 1 or 2mm.
  • the surface of the sensor ie the surface of the cavity layer in the case of an FTR sensor
  • the immobilised biochemicals may be covalently bound to the sensor surface by methods which are well known to those skilled in the art.
  • Figure 1 is a schematic view (not to scale) of an apparatus according to the invention
  • Figure 2 depicts the dependence of the intensity of the detected light on the angle of incidence
  • Figure 3 is a schematic view of part of a second embodiment of an apparatus according to the invention.
  • a biosensor comprises a glass prism 1 coated over an area of its base with a first coating 2 of magnesium fluoride and a second coating 3 of titanium dioxide.
  • the prism 1 and first and second coatings 2,3 together constitute a resonant optical structure, the first coating 2 acting as a spacer layer and the second coating 3 as a cavity layer.
  • the first coating 2 has a thickness of approximately lOOOnm and the second coating 3 a thickness of approximately lOOnm.
  • Immobilised on the surface of the second coating 3 is a layer 4 of immobilised biochemicals, which act as specific binding partner for the analyte under test.
  • the interface between the base of the prism 1 and the first coating 2 is irradiated by a beam of monochromatic light from a laser 5.
  • Light from the laser 5 is collimated by optics 6 and passes through a speckle plate 7 and a polariser 8.
  • the polariser 8 is arranged to produce linearly polarised light with two components : transverse electric (TE) and transverse magnetic (TM) .
  • the polariser is set at 45° to the TE and TM transmission axes and thus provides equal components of TE and TM light.
  • the laser 5 is arranged to maximise the intensity of the light transmitted through the polariser 8 ie with the polarisation axis aligned with that of the polariser 8.
  • the effect of the speckle plate 7 is to present light at a range of angles (including the angle at which resonance occurs) across the whole length of the interface between the base of the prism 1 and the first coating 2. This is a major advantage of this technique, avoiding errors due to imperfections such as dust or scratches on the surface as may occur when a narrow beam of light is used.
  • the reflected light is passed through a compensator 9 to a polarisation analyser 10.
  • the compensator 9 which may be of any conventional form, is manually adjusted to remove any phase difference which is introduced into the TE and TM components on reflection and by birefringence in the optical path.
  • the compensator 9 is adjusted to allow for the difference in phase change occurring on reflection of the TE and TM components.
  • An approximately plane-polarised beam of light is therefore incident on the analyser 10 and this is adjusted to give zero transmission to a detector 12. This will apply for all angles except near resonance. Near resonance of either component, the phase shift produced by reflection will vary rapidly with angle, resulting in maximum throughput of light through the analyser 10 at resonance.
  • the lens 11 is telecentric, ie located at one focal length from the prism 1 and one focal length from the detector 12. This minimises the effects of positioning errors.
  • FIG. 1 shows a plot of the measured signal intensity against angle before and (dotted line) after complexation of the immobilised biochemicals with the analyte.
  • the resonant optical sensor (comprising the layers 2,3,4) is formed on a disposable glass block 31, the input window 32 of which is formed as a diffusion screen.
  • the light source is a laser diode 33 located, in use, very close to the screen 32 and aligned so as to give the major plane of polarisation at 45° to the TE and TM transmission axes.

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  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

L'appareil pour la détermination d'un composé chimique ou biochimique comprend un détecteur optique résonant (1-4) disposé sur le trajet optique entre une source de lumière monochromatique (5) et un détecteur (12) conçu pour mesurer une caractéristique particulière de la lumière. Un élément diffractant la lumière (7) est disposé sur le trajet optique entre la source (5) et le détecteur (1-4). L'élément diffractant la lumière peut être une plaque à tavelures ou un écran de diffusion et il est de préférence formé sur le côté entrée du détecteur, qui peut être une unité que l'on jette après usage.The apparatus for the determination of a chemical or biochemical compound comprises a resonant optical detector (1-4) disposed in the optical path between a monochromatic light source (5) and a detector (12) adapted to measure a particular characteristic of the light. A light diffracting element (7) is disposed in the optical path between the source (5) and the detector (1-4). The light scattering element may be a speckle plate or a scattering screen and is preferably formed on the input side of the detector, which may be a discarded unit after use.

Description

Title : Analytical Device with Light Scattering
This invention relates to sensors, especially those termed biosensors, ie devices for the analysis of biologically active species such as antigens and antibodies in samples of biological origin. In particular, the invention relates to biosensors based on resonant optical phenomena, eg surface plasmon resonance or resonant attenuated or frustrated total internal reflection.
Many devices for the automatic determination of biochemical analytes in solution have been proposed in recent years. Typically, such devices (biosensors) include a sensitised coating layer which is located in the evanescent region of a resonant field. Detection of the analyte typically utilizes optical techniques such as, for example, surface plasmon resonance (SPR), and is based on changes in the thickness and/or refractive index of the coating layer resulting from interaction of that layer with the analyte. This causes a change, eg in the angular position of the resonance.
Other optical biosensors include a waveguide in which a beam of light is propagated. The optical characteristics of the device are influenced by changes occurring at the surface of the waveguide. One form of optical biosensor is based on frustrated total reflection. The principles of frustrated total reflection (FTR) are well-known; the technique is described, for example, by Bosaσchi and Oehrle [Applied Optics (1982), 21, 2167-2173]. An FTR device for use in immunoassay is disclosed in European Patent Application No 2205236A and comprises a cavity layer bounded on one side by the sample under investigation and on the other side by a spacer layer which in turn is mounted on a substrate. The substrate-spacer layer interface is irradiated with monochromatic radiation such that total reflection occurs, the associated evanescent field penetrating through the spacer layer. If the thickness of the spacer layer is correct and the incident parallel wave vector matches one of the resonant mode propagation constants, the total reflection is frustrated and radiation is coupled into the cavity layer. The cavity layer must be composed of material which has a higher refractive index than the spacer layer and which is transparent at the wavelength of the incident radiation.
In devices of this kind, the position of resonance may be monitored by scanning the angle at which monochromatic light is incident on the sensor. The scanning of angle may be performed either sequentially or simultaneously ie by varying the angle of incidence of a parallel beam of light or by simultaneously irradiating over a range of angles using a fan- shaped beam of light as described (in connection with SPR) in European Patent Application No 0305109A. In the first configuration, prior proposals have involved a single-channel detector which is mechanically scanned over a range of angles? this necessitates synchronisation of the movement of the light source and the detector. The second configuration, in which a range of angles is irradiated simultaneously, requires relatively complex optics, which leads to relatively high manufacturing costs.
There has now been devised an apparatus involving the use of a resonant optical sensor for the determination of a chemical or biochemical species, which overcomes or substantially mitigates some or all of the disadvantages of the prior art arrangements described above.
According to the invention, there is provided apparatus for the determination of a chemical or biochemical species, comprising a resonant optical sensor disposed in a light path between a source of monochromatic light and a detector adapted to monitor some characteristic of the light, a light- scattering element being disposed in the light path between the source and the sensor. The apparatus according to the invention is advantageous primarily in that it enables simultaneous irradiation at a range of angles, yet is of relatively simple and inexpensive construction, eg due to the absence of complex optics.
Any convenient source of monochromatic light may be used but it is preferable to use a laser. The choice of laser will depend inter alia on the particular form of sensor used. In this context, 'light' may include not only visible light but also wavelengths above and below this range, eg in the ultra¬ violet and infra-red.
The light-scattering element is preferably a speckle plate or diffusion screen. To overcome the problem of speckle being transferred to the output, it may be necessary to translate or rotate the speckle plate rapidly, ie quicker than the integration time of the detector.
The speckle plate may be a separate component or it may be formed integrally with another component, eg as the output side of a half-wavelength plate comprising a mica sheet sandwiched between two glass sheets.
In a particularly preferred embodiment, the light-scattering element is formed on the input side of the sensor, eg where the sensor is formed as a disposable unit. In this case, the light source can be located very close to the sensor, enabling the use of a compact and inexpensive light source such as a laser diode.
The characteristic of the light which is monitored may be any characteristic which changes at resonance, eg the phase of reflected radiation or, in some cases, the intensity.
The sensor is preferably an FTR sensor. Such a sensor will generally include an optical structure comprising a) a cavity layer of transparent dielectric material of refractive index n3, b) a dielectric substrate of refractive index nlf and c) interposed between the cavity layer and the substrate, a dielectric spacer layer of refractive index n2.
In use, the interface between the substrate and the spacer layer is irradiated with light such that internal reflection occurs. Resonant propagation of a guided mode in the cavity layer will occur, for a given wavelength, at a particular angle of incidence.
The wavelength at which the resonant effect occurs depends on various parameters of the sensor device, such as the refractive indices and thicknesses of the various layers. In general, it is a pre-requisite that the refractive index n3 of the cavity layer and the refractive index nx of the substrate should both exceed the refractive index n2 of the spacer layer. Also, since at least one mode must exist in the cavity to achieve resonance, the cavity layer must exceed a certain minimum thickness.
The cavity layer is preferably a thin-film of dielectric material. Suitable materials for the cavity layer include zirconium dioxide, titanium dioxide, aluminium oxide and tantalum oxide.
The cavity layer may be prepared by known techniques, eg vacuum evaporation, sputtering, chemical vapour deposition or in-diffusion.
The dielectric spacer layer must have a lower refractive index than both the cavity layer and the substrate. The layer may, for example, comprise an evaporated or sputtered layer of magnesium fluoride. Other suitable materials include lithium fluoride and silicon dioxide. Apart from the evaporation and sputtering techniques mentioned above, the spacer layer may be deposited on the substrate by a sol-gel process, or be formed by chemical reaction with the substrate.
The sol-gel process is particularly preferred where the spacer layer is of silicon dioxide.
The refractive index of the substrate (n must be greater than that (n2) of the spacer layer but the thickness of the substrate is generally not critical.
By contrast, the thickness of the cavity layer must be so chosen that resonance occurs within an appropriate range of coupling angles. The spacer layer will typically have a thickness of the order of several hundred nanometres, say from about 200nm to 2000nm, more preferably 500 to 1500nm, eg lOOOnm. The cavity layer typically has a thickness of a few tens of nanometres, say 10 to 200nm, more preferably 30 to 150nm, eg lOOnm.
It is particularly preferred that the cavity layer has a thickness of 30 to 150nm and comprises a material selected from zirconium dioxide, titanium dioxide, tantalum oxide and aluminium oxide, and the spacer layer has a thickness of 500 to 1500nm and comprises a material selected from magnesium fluoride, lithium fluoride and silicon dioxide, the choice of materials being such that the refractive index of the spacer layer is less than that of the cavity layer.
Preferred materials for the cavity layer and the spacer layer are tantalum oxide and silicon dioxide respectively.
At resonance, the incident light is coupled into the cavity layer by FTR, propagates a certain distance along the cavity layer, and couples back out (also by FTR) . The propagation distance depends on the various device parameters but is typically of the order of 1 or 2mm.
At resonance the reflected light will undergo a phase change, and it is this which may be detected.
In general, it is necessary for suitable optical components to be used to prevent non-resonant reflected light reaching the detector. This prevents the technique being used with conventional SPR, or with FTR as described in our co-pending International Patent Application No PCT/GB91/01161 in which the cavity layer and/or spacer layer absorbs at resonance, unless augmented with suitable optics as described in our co- pending International Patent Application No PCT/GB91/01466.
For use in the determination of biochemical species, the surface of the sensor, ie the surface of the cavity layer in the case of an FTR sensor, will generally be sensitised by having biomolecules, eg specific binding partners for the analyte(s) under test, immobilised upon it. The immobilised biochemicals may be covalently bound to the sensor surface by methods which are well known to those skilled in the art.
The invention will now be described in more detail, by way of illustration only, with reference to the accompanying drawings in which
Figure 1 is a schematic view (not to scale) of an apparatus according to the invention,
Figure 2 depicts the dependence of the intensity of the detected light on the angle of incidence, and
Figure 3 is a schematic view of part of a second embodiment of an apparatus according to the invention.
Referring first to Figure 1, a biosensor comprises a glass prism 1 coated over an area of its base with a first coating 2 of magnesium fluoride and a second coating 3 of titanium dioxide. The prism 1 and first and second coatings 2,3 together constitute a resonant optical structure, the first coating 2 acting as a spacer layer and the second coating 3 as a cavity layer. The first coating 2 has a thickness of approximately lOOOnm and the second coating 3 a thickness of approximately lOOnm.
Immobilised on the surface of the second coating 3 is a layer 4 of immobilised biochemicals, which act as specific binding partner for the analyte under test.
The interface between the base of the prism 1 and the first coating 2 is irradiated by a beam of monochromatic light from a laser 5. Light from the laser 5 is collimated by optics 6 and passes through a speckle plate 7 and a polariser 8.
The polariser 8 is arranged to produce linearly polarised light with two components : transverse electric (TE) and transverse magnetic (TM) . The polariser is set at 45° to the TE and TM transmission axes and thus provides equal components of TE and TM light.
The laser 5 is arranged to maximise the intensity of the light transmitted through the polariser 8 ie with the polarisation axis aligned with that of the polariser 8.
The effect of the speckle plate 7 is to present light at a range of angles (including the angle at which resonance occurs) across the whole length of the interface between the base of the prism 1 and the first coating 2. This is a major advantage of this technique, avoiding errors due to imperfections such as dust or scratches on the surface as may occur when a narrow beam of light is used.
All the light incident on the interface between the base of the prism 1 and the first coating 2 is reflected, resonance being detected as a change of phase of the reflected light.
The reflected light is passed through a compensator 9 to a polarisation analyser 10. The compensator 9, which may be of any conventional form, is manually adjusted to remove any phase difference which is introduced into the TE and TM components on reflection and by birefringence in the optical path.
Away from the resonant angle, the compensator 9 is adjusted to allow for the difference in phase change occurring on reflection of the TE and TM components. An approximately plane-polarised beam of light is therefore incident on the analyser 10 and this is adjusted to give zero transmission to a detector 12. This will apply for all angles except near resonance. Near resonance of either component, the phase shift produced by reflection will vary rapidly with angle, resulting in maximum throughput of light through the analyser 10 at resonance.
Light passing through the analyser 10 is focussed by a cylindrical lens 11 onto a detector 12. The lens 11 is telecentric, ie located at one focal length from the prism 1 and one focal length from the detector 12. This minimises the effects of positioning errors.
In use, light is incident on the interface between the base of the prism 1 and the first coating layer 2 simultaneously at a range of angles, including the resonant angle. Off-resonance no light intensity is detected at the detector 12; as resonance is approached, the detected light intensity increases and then falls.
When the layer of immobilised biochemicals 4 is contacted with a sample containing the analyte under test, specific binding occurs between the biochemicals and the analyte molecules, resulting in a change in the refractive index in the vicinity of the surface of the device. This in turn results in a shift in the position of the resonance. Figure 2 shows a plot of the measured signal intensity against angle before and (dotted line) after complexation of the immobilised biochemicals with the analyte.
In the embodiment shown in Figure 3, the resonant optical sensor (comprising the layers 2,3,4) is formed on a disposable glass block 31, the input window 32 of which is formed as a diffusion screen. The light source is a laser diode 33 located, in use, very close to the screen 32 and aligned so as to give the major plane of polarisation at 45° to the TE and TM transmission axes.

Claims

Claims
1. Apparatus for the determination of a chemical or biochemical species, comprising a resonant optical sensor (1-4) disposed in a light path between a source (5) of monochromatic light and a detector (12) adapted to monitor some characteristic of the light, a light-scattering element (7) being disposed in the light path between the source (5) and the sensor (1-4).
2. Apparatus as claimed in Claim 1, wherein the source (5) of monochromatic light is a laser.
3. Apparatus as claimed in Claim 1 or Claim 2, wherein the light-scattering element is a speckle plate (7) .
4. Apparatus as claimed in Claim 1 or Claim 2, wherein the light-scattering element is a diffusion screen.
5. Apparatus as claimed in Claim 3, wherein the speckle plate can be translated or rotated more quickly than the integration time of the detector.
6. Apparatus as claimed in any preceding claim, wherein the speckle plate is formed integrally with another component, eg as the output side of a half-wavelength plate comprising a mica sheet sandwiched between two glass sheets.
7. Apparatus as claimed in any one of Claims 1 to 5, wherein the light-scattering element (32) is formed on the input side of the sensor (31) .
8. Apparatus as claimed in Claim 7, wherein the sensor (31) is a disposable unit.
9. Apparatus as claimed in Claim 8, wherein the source of monochromatic light is a laser diode (33).
10. Apparatus as claimed in any preceding claim, wherein the sensor (1-4) is an FTR sensor comprising a) a cavity layer (3) of transparent dielectric material of refractive index n3, b) a dielectric substrate (1) of refractive index πα, and c) interposed between the cavity layer (3) and the substrate (1) , a dielectric spacer layer (2) of refractive index n2.
EP93901849A 1992-01-11 1993-01-08 Analytical device with light scattering Withdrawn EP0620916A1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
GB9200563 1992-01-11
GB929200563A GB9200563D0 (en) 1992-01-11 1992-01-11 Analytical device with light scattering
PCT/GB1993/000027 WO1993014393A1 (en) 1992-01-11 1993-01-08 Analytical device with light scattering

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EP0620916A1 true EP0620916A1 (en) 1994-10-26

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GB9200563D0 (en) 1992-03-11
JPH07502815A (en) 1995-03-23
WO1993014393A1 (en) 1993-07-22

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