WO1992011516A1 - Spectrometer - Google Patents

Spectrometer Download PDF

Info

Publication number
WO1992011516A1
WO1992011516A1 PCT/GB1991/002260 GB9102260W WO9211516A1 WO 1992011516 A1 WO1992011516 A1 WO 1992011516A1 GB 9102260 W GB9102260 W GB 9102260W WO 9211516 A1 WO9211516 A1 WO 9211516A1
Authority
WO
WIPO (PCT)
Prior art keywords
spectrometer
bundle
radiation
fibre
detector
Prior art date
Application number
PCT/GB1991/002260
Other languages
French (fr)
Inventor
Huw Prytherch
Leonard Morris
Original Assignee
Unicam Limited
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 Unicam Limited filed Critical Unicam Limited
Publication of WO1992011516A1 publication Critical patent/WO1992011516A1/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/12Generating the spectrum; Monochromators
    • G01J3/18Generating the spectrum; Monochromators using diffraction elements, e.g. grating
    • G01J3/1809Echelle gratings
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/02Details
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/02Details
    • G01J3/0205Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows
    • G01J3/0218Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows using optical fibers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/02Details
    • G01J3/0264Electrical interface; User interface
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/02Details
    • G01J3/0275Details making use of sensor-related data, e.g. for identification of sensor parts or optical elements
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/2803Investigating the spectrum using photoelectric array detector
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M11/00Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
    • G01M11/30Testing of optical devices, constituted by fibre optics or optical waveguides
    • G01M11/33Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/04Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings formed by bundles of fibres
    • G02B6/06Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings formed by bundles of fibres the relative position of the fibres being the same at both ends, e.g. for transporting images
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/12Generating the spectrum; Monochromators
    • G01J3/18Generating the spectrum; Monochromators using diffraction elements, e.g. grating
    • G01J2003/1828Generating the spectrum; Monochromators using diffraction elements, e.g. grating with order sorter or prefilter

Definitions

  • the invention relates to a spectrometer comprisi means for gathering radiation emanating from or passi through a sample, means for selecting radiation of a giv band of wavelengths, and means for directing the select radiation onto a detector.
  • the invention is of particular though not exclusi use in an atomic emission spectrometer.
  • the wavelengths to be detected are common separated by means of an echelle monochromator.
  • This wi include an echelle grating and an order sorting prism that the different orders of diffraction coming from t echelle grating are dispersed at right angles by the ord sorting prism.
  • the spectra produced by the various orde of diffraction are then spaced across an output apertu plate.
  • the detector of radiation is photomultiplier tube which is mounted on a carriage whi can be moved to any point on the aperture plate so that selected aperture allows radiation of a given waveleng through to the photomultiplier tube.
  • this arrangeme it is only possible to detect a single wavelength or narr band of wavelengths at one time.
  • practice such an arrangement would be too expensive a bulky.
  • a spectrometer comprising means for gathering radiation emanating from or passing through a sample, means for selecting radiation of a given band of wavelengths, and means for directing the selected radiation onto a detector, is characterised in that the detector comprises an array of solid state detector elements and in that the means for directing the radiation onto the detector comprises a plurality of optical waveguides, each element of the array receiving radiation from one or more optical waveguides.
  • the plurality of optical waveguides preferably comprise an optical fibre bundle.
  • optical fibres to carry the radiation from the output of the radiation selecting means it is possible to locate the detectors more flexibly. Thus it is not necessary to be able to focus the radiation from the output of the monochromator onto the detector and there does not need to be a clear path to the detector.
  • the fibre optic bundles are compact and flexible it is possible to provide a plurality of bundles, on for example an echelle output plate, and if a corresponding plurality of detector arrays is provided then even greater flexibility in simultaneous measurement of a plurality of sample elements can be made.
  • the optical fibres may be clamped in a fixed orientation and position at each end, the position of individual fibres being the same at both ends.
  • the spectrum at the output slit is transferred to the detector array coherently, that is as though the exit slit was focused on the array.
  • the optical fibres of the bundle may be held in a fixed orientation and position at each end, the position of individual fibres at one end being randomly related to that of the corresponding fibre at the other end, the spectrometer further comprising means for determining which fibres correspond to a given wavelength of received radiation.
  • the determining means may comprise a microprocessor and memory means, the memory means containing data defining the positions of each individual fibre in the bundle at both ends.
  • the fibre bundle may have associates with it coding means which enables the data to be read into the memory means.
  • the data may be coded in machine readable form for example on a magnetic card, or may be in written form whereby the operator enters the information into the spectrometer via a keyboard.
  • Figure 1 shows in block schematic form a known atomic emission spectrometer
  • Figure 2 shows schematically a modification of the spectrometer of Figure 1 to produce a spectrometer in accordance with the invention
  • Figures 3 and 4 show first and second arrangements for determining the relative positions of individual fibres at each end of a fibre optic bundle
  • Figure 5 shows in block schematic form a spectrometer according to the invention.
  • Figure 1 shows in block schematic form an atomic emission spectrometer which comprises a source unit 1 and a detector unit 2.
  • the source unit 1 includes an inductively coupled plasma torch 3 in which the sample is atomised. Radiation emitted by the sample is passed to a focusing mirror 4 which focuses the radiation on the entrance slit 5 of an echelle monochromator. Radiation passes through the entrance slit 5 onto a collimating mirror 6 which directs the radiation to an echelle grating 7. Dispersed radiation from the echelle grating 7 passes through an order sorting prism and focusing lens 8 onto a plane mirror 9.
  • the plane mirror 9 reflects the dispersed radiation onto an aperture 10 which forms a plurality of exit slits from the monochromator.
  • a detector 11 in the form of a photomultiplier tube is arranged over a selected slit in the aperture plate 10 to detect radiation of a given wavelength.
  • the detector 11 is mounted on a carriage which is controlled so that it can place the detector over a selected slit on the plate.
  • a spectrometer as describ with reference to Figure 1 has been manufactured and so by Unicam Limited under the type number PU 7000.
  • FIG. 2 shows how this spectrometer may be modifi according to the invention.
  • the aperture plate 10 inste of having a large number of small apertures, each of whi lets through a single wavelength, or narrow band wavelengths, is provided with a plurality of slots 2 21,22,23 each of which is dimensioned so that a fu spectrum of a given order is let through.
  • An optical fib bundle 24 is clamped at one end 25 and located over t slot 23.
  • a similar clamping arrangement 26 at the oth end is located over a diode array detector 27.
  • ea individual fibre and its associated element of the dio array detector 27 corresponds to the slit a photomultiplier tube of the arrangement of Figure l.
  • the bundle is coherent, that is, the positions of the en of individual fibres correspond at both ends of the bundl then a plurality of fibres may be coupled to each eleme of the diode array 27. This eases alignment problems as is not essential that a given fibre completely alig itself with a single element of the array. However, if t optical fibre bundle 24 is not coherent, that is t positions of the ends of a single fibre do not correspo at both ends of the bundle, it is then necessary that on a single fibre is coupled to a given detector element.
  • a coherent fibre optic bundle is provided t spectrometer becomes equivalent to one where the dio array is either mounted on the output slit or has an ima of the output slit focused on it and standard diode arr detection electronics can be used.
  • a bundl is expensive to produce and it would be advantageous if non-coherent bundle could be manufactured and used.
  • T enable such a bundle to be used it is proposed t determined the position, at each end of the bundle, of th end of each fibre and to use this information to modify th processing of the signal produced by the detector.
  • Figures 3 and 4 illustrate two methods of determining the relative positions of the fibre ends. As shown in Figure 3 a stationary light source 30 provides radiation which is directed onto one end 31 of a fibre optic bundle 32.
  • a shutter 33 Between the radiation source 30 and the end 31 of the fibre optic bundle 32 is a shutter 33.
  • the shutter is moved to expose in turn the ends of each of the optical fibres in the bundle 32.
  • a detector 35 is positioned at the other end 34 of the fibre optic bundle.
  • This may be a standard diode array detector of the form which will be used in the spectrometer.
  • Figure 4 shows an alternative way of calibrating the fibre optic bundle. This uses a moveable radiation source 40 and a coherent bundle 41 of optical fibres.
  • the bundle has one end 42 splayed out so that individual fibres are relatively widely separated and another end 43 which is clamped so that the ends of the fibres align with the ends 44 of a non-coherent optical fibre bundle 42.
  • the other end 45 of the non-coherent bundle 42 is coupled to a diode array detector 46.
  • a label which contains the calibration information may be, for example, in the form of a magnetically encoded card or may have the information printed so that an operator can key appropriate instructions into the spectrometer manually. If a magnetically or optically encoded card is used this can then be inserted into a card reader on the spectrometer an the information automatically read by the reader an entered into the spectrometer without requiring th intervention of an operator other than to insert the car 5 in a reader.
  • Figure 5 shows in block schematic form an embodimen of a spectrometer according to the invention. It comprise a source unit 1 and detector unit 2 which are as describe with reference to Figure 1 except that the aperture plat
  • 10 10 is of the form shown in Figure 2.
  • One end 51 of a optical fibre bundle 52 is aligned over one of the slots i the aperture plate 10 and its other end 53 is aligned wit a diode array detector 54.
  • the diode array detector i connected to a control and read out circuit 55 whic
  • a card reader 58 is arranged to rea information from a card 59 which is attached to the bundl
  • This information is stored in a memory 61, which i also attached to the bus 56, under the control of th microprocessor 56. Also attached to the bus 56 is keyboard 62 and display unit 63. The microprocessor memor and keyboard are also used to control other functions o
  • the spectrometer in a known manner and to analyse th results for display on the display unit 63 or to send th results to a printer (not shown) which provides a hard cop version of the results.
  • the detector array 54 need not be a photodiode array but could be a charge coupled device array or any other convenient array of detector elements.
  • the invention is not limited to use in atomic emission spectrometers but could be used in any spectrometer which used an array of detector elements.

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Human Computer Interaction (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Abstract

The spectrometer comprises a radiation source (1) whose radiation is focused on an entrance slit (5) of an echelle monochromator (6, 7, 8, 9, 10). A fibre optic bundle (52) has one end (51) located above a slot on the output plate (10) of the echelle monochromator and its other end (53) located adjacent an array detector (54). The fibre optic bundle (52) has a card (59) attached to it which specifies the respective positions of the ends of each fibre within the bundle. A card reader (58) reads this information and passes it to a memory (61). A microprocessor (57) is used to relate the outputs of a given detector element to a given wavelength of radiation using the information read from the card (59).

Description

BACKGROUND OF THE INVENTION
The invention relates to a spectrometer comprisi means for gathering radiation emanating from or passi through a sample, means for selecting radiation of a giv band of wavelengths, and means for directing the select radiation onto a detector.
The invention is of particular though not exclusi use in an atomic emission spectrometer. In su instruments the wavelengths to be detected are common separated by means of an echelle monochromator. This wi include an echelle grating and an order sorting prism that the different orders of diffraction coming from t echelle grating are dispersed at right angles by the ord sorting prism. The spectra produced by the various orde of diffraction are then spaced across an output apertu plate. DESCRIPTION OF PRIOR ART
In a known spectrometer of this type, an example which is the Unicam PU 7000 ICP atomic emissi spectrometer, the detector of radiation is photomultiplier tube which is mounted on a carriage whi can be moved to any point on the aperture plate so that selected aperture allows radiation of a given waveleng through to the photomultiplier tube. With this arrangeme it is only possible to detect a single wavelength or narr band of wavelengths at one time. In principle it would possible to provide a plurality of photomultiplier tub each with their own separate carriage so that more than o wavelength could be detected simultaneously. However practice such an arrangement would be too expensive a bulky.
Another construction for an atomic emissi spectrometer which has been proposed is to focus t echelle output spectrum onto a two dimensional array charge coupled devices (CCDs) . Such arrays are readi available since they are commonly used as sensors for vid cameras. However this requires accurate focusing of the echelle output image onto the CCD array and places certain restraints on the physical layout of the instrument. SUMMARY OF THE INVENTION According to this invention a spectrometer comprising means for gathering radiation emanating from or passing through a sample, means for selecting radiation of a given band of wavelengths, and means for directing the selected radiation onto a detector, is characterised in that the detector comprises an array of solid state detector elements and in that the means for directing the radiation onto the detector comprises a plurality of optical waveguides, each element of the array receiving radiation from one or more optical waveguides. An advantage of this invention is that it enables a dispersed spectrum of radiation to be detected by an array detector while allowing greater flexibility of instrument layout.
The plurality of optical waveguides preferably comprise an optical fibre bundle.
By using optical fibres to carry the radiation from the output of the radiation selecting means it is possible to locate the detectors more flexibly. Thus it is not necessary to be able to focus the radiation from the output of the monochromator onto the detector and there does not need to be a clear path to the detector. By providing a bundle of optical fibres coupled to an array detector it is possible to detect simultaneously a band of wavelengths and consequently in an atomic emission, absorption, or fluorescence spectrometer simultaneous measurements for a number of elements may be made. As the fibre optic bundles are compact and flexible it is possible to provide a plurality of bundles, on for example an echelle output plate, and if a corresponding plurality of detector arrays is provided then even greater flexibility in simultaneous measurement of a plurality of sample elements can be made. The optical fibres may be clamped in a fixed orientation and position at each end, the position of individual fibres being the same at both ends. Thus the spectrum at the output slit is transferred to the detector array coherently, that is as though the exit slit was focused on the array. In this case it is not necessary for there to be a single optical fibre corresponding to a single detector element and in particular, a plurality of fibres could be coupled to each detector element. This eases alignment problems between the end of the optical fibre bundle and the detector.
The optical fibres of the bundle may be held in a fixed orientation and position at each end, the position of individual fibres at one end being randomly related to that of the corresponding fibre at the other end, the spectrometer further comprising means for determining which fibres correspond to a given wavelength of received radiation.
Constructing bundles of fibre optic cables which are coherent, that is where the fibre position at one end corresponds to that at the other end is relatively expensive whereas if the fibres are allowed to arrange themselves randomly a much less expensive manufacturing method can be used to construct the fibre bundle. By determining the relative alignments of the fibres at each end and providing in the spectrometer means for correcting the input signal from the detector in accordance with the position of the fibres, it is possible to use relatively inexpensive fibre optic bundles. The determining means may comprise a microprocessor and memory means, the memory means containing data defining the positions of each individual fibre in the bundle at both ends. The fibre bundle may have associates with it coding means which enables the data to be read into the memory means.
The data may be coded in machine readable form for example on a magnetic card, or may be in written form whereby the operator enters the information into the spectrometer via a keyboard. BRIEF DESCRIPTION OF DRAWINGS
The above and other features of the invention will become more apparent from the following detailed description of embodiments of the invention, which is given by way of example, with reference to the accompanying drawings, in which:-
Figure 1 shows in block schematic form a known atomic emission spectrometer;
Figure 2 shows schematically a modification of the spectrometer of Figure 1 to produce a spectrometer in accordance with the invention;
Figures 3 and 4 show first and second arrangements for determining the relative positions of individual fibres at each end of a fibre optic bundle; and,
Figure 5 shows in block schematic form a spectrometer according to the invention. DESCRIPTION OF PREFERRED EMBODIMENT Figure 1 shows in block schematic form an atomic emission spectrometer which comprises a source unit 1 and a detector unit 2. The source unit 1 includes an inductively coupled plasma torch 3 in which the sample is atomised. Radiation emitted by the sample is passed to a focusing mirror 4 which focuses the radiation on the entrance slit 5 of an echelle monochromator. Radiation passes through the entrance slit 5 onto a collimating mirror 6 which directs the radiation to an echelle grating 7. Dispersed radiation from the echelle grating 7 passes through an order sorting prism and focusing lens 8 onto a plane mirror 9. The plane mirror 9 reflects the dispersed radiation onto an aperture 10 which forms a plurality of exit slits from the monochromator. A detector 11 in the form of a photomultiplier tube is arranged over a selected slit in the aperture plate 10 to detect radiation of a given wavelength. The detector 11 is mounted on a carriage which is controlled so that it can place the detector over a selected slit on the plate. A spectrometer as describ with reference to Figure 1 has been manufactured and so by Unicam Limited under the type number PU 7000.
Figure 2 shows how this spectrometer may be modifi according to the invention. The aperture plate 10 inste of having a large number of small apertures, each of whi lets through a single wavelength, or narrow band wavelengths, is provided with a plurality of slots 2 21,22,23 each of which is dimensioned so that a fu spectrum of a given order is let through. An optical fib bundle 24 is clamped at one end 25 and located over t slot 23. A similar clamping arrangement 26 at the oth end is located over a diode array detector 27. Thus ea individual fibre and its associated element of the dio array detector 27 corresponds to the slit a photomultiplier tube of the arrangement of Figure l. the bundle is coherent, that is, the positions of the en of individual fibres correspond at both ends of the bundl then a plurality of fibres may be coupled to each eleme of the diode array 27. This eases alignment problems as is not essential that a given fibre completely alig itself with a single element of the array. However, if t optical fibre bundle 24 is not coherent, that is t positions of the ends of a single fibre do not correspo at both ends of the bundle, it is then necessary that on a single fibre is coupled to a given detector element.
If a coherent fibre optic bundle is provided t spectrometer becomes equivalent to one where the dio array is either mounted on the output slit or has an ima of the output slit focused on it and standard diode arr detection electronics can be used. However such a bundl is expensive to produce and it would be advantageous if non-coherent bundle could be manufactured and used. T enable such a bundle to be used it is proposed t determined the position, at each end of the bundle, of th end of each fibre and to use this information to modify th processing of the signal produced by the detector. Figures 3 and 4 illustrate two methods of determining the relative positions of the fibre ends. As shown in Figure 3 a stationary light source 30 provides radiation which is directed onto one end 31 of a fibre optic bundle 32. Between the radiation source 30 and the end 31 of the fibre optic bundle 32 is a shutter 33. The shutter is moved to expose in turn the ends of each of the optical fibres in the bundle 32. A detector 35 is positioned at the other end 34 of the fibre optic bundle. This may be a standard diode array detector of the form which will be used in the spectrometer. By moving the shutter 33 and monitoring at the detector 35 which elements are illuminated as the shutter is moved, the corresponding positions of the ends of the fibres at each end of the bundle can be determined. This information can then be stored and used to calibrate the spectrometer. Figure 4 shows an alternative way of calibrating the fibre optic bundle. This uses a moveable radiation source 40 and a coherent bundle 41 of optical fibres. The bundle has one end 42 splayed out so that individual fibres are relatively widely separated and another end 43 which is clamped so that the ends of the fibres align with the ends 44 of a non-coherent optical fibre bundle 42. The other end 45 of the non-coherent bundle 42 is coupled to a diode array detector 46. By aligning the radiation source 40 with each individual fibre at the end 42 in turn and detecting which element of the diode array 46 received radiation, positions of the ends of each optical fibre in the bundle 42 can be determined. This information can then be stored and used to calibrate the spectrometer.
When the fibre optic bundle has been calibrated, it is possible to attach to it a label which contains the calibration information. This may be, for example, in the form of a magnetically encoded card or may have the information printed so that an operator can key appropriate instructions into the spectrometer manually. If a magnetically or optically encoded card is used this can then be inserted into a card reader on the spectrometer an the information automatically read by the reader an entered into the spectrometer without requiring th intervention of an operator other than to insert the car 5 in a reader.
Figure 5 shows in block schematic form an embodimen of a spectrometer according to the invention. It comprise a source unit 1 and detector unit 2 which are as describe with reference to Figure 1 except that the aperture plat
10 10 is of the form shown in Figure 2. One end 51 of a optical fibre bundle 52 is aligned over one of the slots i the aperture plate 10 and its other end 53 is aligned wit a diode array detector 54. The diode array detector i connected to a control and read out circuit 55 whic
15 contains the electronics for scanning the diode array an converting the signals read out from the diode array int digital form so that it can then be passed via a bus 56 t a microprocessor 57. A card reader 58 is arranged to rea information from a card 59 which is attached to the bundl
20 52. This information is stored in a memory 61, which i also attached to the bus 56, under the control of th microprocessor 56. Also attached to the bus 56 is keyboard 62 and display unit 63. The microprocessor memor and keyboard are also used to control other functions o
25 the spectrometer in a known manner and to analyse th results for display on the display unit 63 or to send th results to a printer (not shown) which provides a hard cop version of the results.
It would be possible to modify the arrangement show
30 in Figure 5 by providing a plurality of bundles of optica fibres with a corresponding plurality of detector arrays. Alternatively if a single two dimensional detector arra was used the fibre optic bundles could be aligned wit different parts of the array. Either a plurality of car
35 readers could be employed or a single card reader could b used to read the cards attached to each of the optical fibre bundles in turn during the initial setting setting u procedures of the instrument. Clearly the detector array 54 need not be a photodiode array but could be a charge coupled device array or any other convenient array of detector elements. The invention is not limited to use in atomic emission spectrometers but could be used in any spectrometer which used an array of detector elements.
As an alternative to the methods of determining the position of the individual fibres of the bundle described with reference to Figures 3 and 4 it would be possible to calibrate the spectrometer directly. For example one end of the bundle could be traversed across a narrow output slit of the monochromator in the spectrometer and the order of illumination of detector elements read directly into the memory 61. This would eliminate the need for a card reader or for manual entry of the information. An interlock could be built in to ensure that when a fibre optic bundle was changed the calibration operation has to be repeated.

Claims

1. A spectrometer comprising means (4,5) for gatherin radiation emanating from or passing through a sample, mean (6,7,8,9,10) for selecting radiation of a given band o wavelengths and means for directing the selected radiatio onto a detector (27,54); characterised in that the mean for directing the radiation onto the detector (27,54) comprises a plurality of optical waveguides (24,52), eac element of the array receiving radiation from one or mor optical waveguides (24,52).
2. A spectrometer as claimed in claim 1, wherein th plurality of optical waveguides comprises a fibre opti bundle (24,52).
3. A spectrometer as claimed in claim 2, wherein at eac end of the bundle (24,52) the optical fibres are clamped i a fixed orientation and position, the relative position of each individual fibre being the same at both ends.
4. A spectrometer as claimed in claim 2, wherein at each end of the bundle (24,52) the optical fibres are held in a fixed orientation and position, the relative position of individual fibres at one end being randomly related to that at the other end, the spectrometer further comprising means (56,58,59,61) for determining which fibre corresponds to a given wavelength of received radiation.
5. A spectrometer as claimed in claim 4, wherein the determining means comprises a microprocessor (56) and memory means (61) , the memory means (61) containing data defining the positions of the individual fibres in the bundle (24,52).
6. A spectrometer as claim in claim 5, in which the optical fibre bundle (24,52) has associated with it coding means (59) which enables the data to be read into the memory means (61) .
7. A spectrometer as claimed in claim 6, in which the coding means comprises a magnetic card (59) and the spectrometer further comprises a magnetic card reader (58) .
PCT/GB1991/002260 1990-12-21 1991-12-18 Spectrometer WO1992011516A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB909027831A GB9027831D0 (en) 1990-12-21 1990-12-21 Spectrometer
GB9027831.8 1990-12-21

Publications (1)

Publication Number Publication Date
WO1992011516A1 true WO1992011516A1 (en) 1992-07-09

Family

ID=10687458

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/GB1991/002260 WO1992011516A1 (en) 1990-12-21 1991-12-18 Spectrometer

Country Status (3)

Country Link
AU (1) AU9104791A (en)
GB (1) GB9027831D0 (en)
WO (1) WO1992011516A1 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996028748A2 (en) * 1995-03-14 1996-09-19 Maechler Meinrad Optical system with wide measuring ranges
WO2003024011A2 (en) * 2001-09-12 2003-03-20 Lnl Optenia Inc. Optical performance monitor
US7272276B2 (en) 2001-09-12 2007-09-18 Enablence Inc. Optical performance monitor

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2097106A1 (en) * 1970-07-01 1972-03-03 Coats J Et P Ltd
US4711572A (en) * 1983-12-01 1987-12-08 Jenoptik Jena Gmbh Method and arrangement for multielement analyse
US4812646A (en) * 1987-11-03 1989-03-14 Photon Devices, Ltd. Optical fiber initialization method and apparatus
EP0362562A2 (en) * 1988-10-03 1990-04-11 Fried. Krupp AG Hoesch-Krupp Spectrometer for the simultaneous measurement of intensity in several spectral ranges

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2097106A1 (en) * 1970-07-01 1972-03-03 Coats J Et P Ltd
US4711572A (en) * 1983-12-01 1987-12-08 Jenoptik Jena Gmbh Method and arrangement for multielement analyse
US4812646A (en) * 1987-11-03 1989-03-14 Photon Devices, Ltd. Optical fiber initialization method and apparatus
EP0362562A2 (en) * 1988-10-03 1990-04-11 Fried. Krupp AG Hoesch-Krupp Spectrometer for the simultaneous measurement of intensity in several spectral ranges

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
APPLIED OPTICS vol. 7, no. 5, 1 May 1968, pages 857 - 859; L.COMBES ET AL.: 'FIBER OPTIC POLYCHROMATOR' *
REVIEW OF SCIENTIFIC INSTRUMENTS vol. 57, no. 8, 1 August 1986, pages 1816 - 1818; R.KINDSFATHER ET AL.: 'TWO DIMENSIONAL THOMSON SCATTERING SYSTEM' *
REVIEW OF SCIENTIFIC INSTRUMENTS vol. 57, no. 8, 1 August 1986, pages 2035 - 2037; N.HAWKES ET AL.: 'MULTICHANNEL DETECTOR FOR UV' *
REVIEW OF SCIENTIFIC INSTRUMENTS vol. 59, no. 1, 1 January 1988, pages 125 - 127; J.CASTRACANE ET AL.: 'SIX CHANNEL GRATING SPECTROMETER' *

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996028748A2 (en) * 1995-03-14 1996-09-19 Maechler Meinrad Optical system with wide measuring ranges
WO1996028748A3 (en) * 1995-03-14 1996-11-07 Meinrad Maechler Optical system with wide measuring ranges
WO2003024011A2 (en) * 2001-09-12 2003-03-20 Lnl Optenia Inc. Optical performance monitor
WO2003024011A3 (en) * 2001-09-12 2003-12-11 Lnl Optenia Inc Optical performance monitor
US7272276B2 (en) 2001-09-12 2007-09-18 Enablence Inc. Optical performance monitor

Also Published As

Publication number Publication date
GB9027831D0 (en) 1991-02-13
AU9104791A (en) 1992-07-22

Similar Documents

Publication Publication Date Title
EP1144965B1 (en) Spectrometer
US5528050A (en) Compact scan head with multiple scanning modalities
US4919535A (en) Reflectance measuring apparatus for making contactless measurements
US4932779A (en) Color measuring instrument with integrating sphere
US4993834A (en) Spectrometer for the simultaneous measurement of intensity in various spectral regions
US5424841A (en) Apparatus for measuring spatial distribution of fluorescence on a substrate
US5042893A (en) Direct mount coupling to a spectrophotometer
US5604594A (en) Device and method for determining the color value of a light
US5615008A (en) Optical waveguide integrated spectrometer
US6905258B2 (en) Miniature imaging encoder readhead using fiber optic receiver channels
US5424826A (en) Wideband optical micro-spectrometer system
JP2001527214A (en) Detector with transmission grating beam splitter for multi-wavelength sample analysis
US4636074A (en) Optics system for emission spectrometer
US4375919A (en) Multiple entrance aperture dispersive optical spectrometer
US6208413B1 (en) Hadamard spectrometer
US4049353A (en) Spectrometric system and cassette
KR102075053B1 (en) Optical measuring device
US4494872A (en) Multiple entrance aperture dispersive optical spectrometer
EP0340915A2 (en) Optical system for a multidetector array spectrograph
EP1054244A2 (en) Optical scanning spectrometer.
US4566792A (en) Multi-channel spectrophotometric measuring device
CN101467182B (en) Apparatus and method for optically examining security documents
WO1992011516A1 (en) Spectrometer
EP0994341B1 (en) Method of measuring distribution of internal refractive index for optical fibre preform and measuring device
US20020126280A1 (en) Holographic grating spectrum analyzer

Legal Events

Date Code Title Description
AK Designated states

Kind code of ref document: A1

Designated state(s): AU US

AL Designated countries for regional patents

Kind code of ref document: A1

Designated state(s): AT BE CH DE DK ES FR GB GR IT LU MC NL SE