EP0594668A1 - Optical signal processing - Google Patents
Optical signal processingInfo
- Publication number
- EP0594668A1 EP0594668A1 EP92914231A EP92914231A EP0594668A1 EP 0594668 A1 EP0594668 A1 EP 0594668A1 EP 92914231 A EP92914231 A EP 92914231A EP 92914231 A EP92914231 A EP 92914231A EP 0594668 A1 EP0594668 A1 EP 0594668A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- profile
- filter
- blf
- absorption
- detection system
- 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- Withdrawn
Links
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- 101710127406 Glycoprotein 5 Proteins 0.000 description 1
- DGAQECJNVWCQMB-PUAWFVPOSA-M Ilexoside XXIX Chemical compound C[C@@H]1CC[C@@]2(CC[C@@]3(C(=CC[C@H]4[C@]3(CC[C@@H]5[C@@]4(CC[C@@H](C5(C)C)OS(=O)(=O)[O-])C)C)[C@@H]2[C@]1(C)O)C)C(=O)O[C@H]6[C@@H]([C@H]([C@@H]([C@H](O6)CO)O)O)O.[Na+] DGAQECJNVWCQMB-PUAWFVPOSA-M 0.000 description 1
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- BJQHLKABXJIVAM-UHFFFAOYSA-N bis(2-ethylhexyl) phthalate Chemical compound CCCCC(CC)COC(=O)C1=CC=CC=C1C(=O)OCC(CC)CCCC BJQHLKABXJIVAM-UHFFFAOYSA-N 0.000 description 1
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- 229910052708 sodium Inorganic materials 0.000 description 1
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- 229910052724 xenon Inorganic materials 0.000 description 1
- FHNFHKCVQCLJFQ-UHFFFAOYSA-N xenon atom Chemical compound [Xe] FHNFHKCVQCLJFQ-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P3/00—Measuring linear or angular speed; Measuring differences of linear or angular speeds
- G01P3/36—Devices characterised by the use of optical means, e.g. using infrared, visible, or ultraviolet light
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
- G01C9/00—Measuring inclination, e.g. by clinometers, by levels
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/45—Interferometric spectrometry
- G01J3/453—Interferometric spectrometry by correlation of the amplitudes
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/42—Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry
-
- 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
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N2021/3185—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry typically monochromatic or band-limited
- G01N2021/3188—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry typically monochromatic or band-limited band-limited
Definitions
- the invention relates to optical detection systems and in particular to selective processing of an image signal field in the optical domain before signal detection so as to enhance the signal to noise ratio in the system.
- European Patent No 0155142 describes a remote gas detection system relying on signal processing in the optical domain using principles of optical transform image modulation (OTIM).
- OFTIM optical transform image modulation
- the object of the present invention is to provide a spectral pre-detection processing arrangement to enhance the performance of optical detection systems such as the above-mentioned remote gas sensor.
- the invention provides an optical detection system comprising a) means to receive radiation from a target within a field of view b) transform means to modulate the received radiation to sensitise the system to selected features dependent on the coherence function profile within the received optical field; and
- the transform means includes a spectral processor having: (i) a band limiting filter (BLF) ; and
- a modifying filter having a pass band at least partly overlapping the passband of the BLF;
- the characteristics of the BLF and the MF being selected to concentrate key information on the target radiation in a small region of the coherence function profile.
- the BLF and MF have Gaussian transmission profiles and the MF profile is centred in the BLF profile.
- the centre of the MF profile may be offset with respect to the centre of the BLF profile.
- the MF is arranged to have the same profile as an absorption band of the gas but centred at a different wavenumber. This arrangement leads to improved detection.
- the MF can have a transmission characteristic so as to produce a periodicity in the signal modulation of the coherence function.
- Detection of the transformed optical field may be enhanced by making one of the filters time dependent, for example by periodic movement of the filter.
- FIGS 1 to 3 show spectral profiles of a band limiting filter (BLF), received radiation with a single target gas absorption line within the band of the BLF, and the spectrally processed signal after transmission through the BLF;
- BLF band limiting filter
- Figure 4 is a graph of the coherence envelope function y(L);
- Figure 5 shows graphs of measurable parameters from changes in the coherence envelope with gas concentration
- Figures 6-8 show graphs illustrating the effect of use of a BNF whose centre frequency is offset relative to the peak in a target gas absorption line;
- Figure 9 is a graph of the real part of the coherence envelope
- Figure 10 is a table giving developments of different pre-detection spectral processing
- Figures 11a and lib show an alternative filter approach, with and without gas absorption.
- Figure 12 shows how a comb filter may be used for spectral sampling
- the Band-Limiting Filter This is the relatively broad-band filter which sets the spectral acceptance range of the system. Strictly speaking it also includes the spectral response of the detector/detectors and the spectral transmission of the optics; and some aspects of atmospheric transmission.
- the Modifying Filter or Filters are additional spectral filters with their significant profile within the band-pass of the BLF.
- Band-Pass Region over which spectral transmission is approximately 50% of the peak transmission.
- Centre-Wavelength/Wavenumbers This is the characteristic wavelength/wavenumber of the filters which can be defined in many ways for different filter types. For example, it can be the wavelength/wavenumber at peak transmission, or the point midway between the 3dB points. The exact definition will be explained in each case that is considered.
- Spectral Profile Description of the shape of the filters e.g. Gaussian, rectangular or periodic.
- Peak Transmission Highest transmission of the filter across its band-pass.
- Spectral Processing will include the manipulation of:
- OTIM optical transform image modulation
- ⁇ ( ⁇ , ⁇ ) is the received spectral profile
- the aim is to concentrate the key information about the presence of the wanted gas to a small region of the coherence function profile.
- a movement of a specific null in the coherence function, or the value of the visibility at a particular path difference can be employed, together with high performance post-detector processing (e.g. correlation or matched filtering).
- high performance post-detector processing e.g. correlation or matched filtering.
- the objective is to maximise the change in some aspect (or feature) of the coherence function ⁇ (L;T) so that the smallest possible concentration of the wanted gas, causes a significant change in the electronic output.
- Case 1 An extension of Case 1 is to off-set the centre-wavelength 21 of the BLF with respect to the gas absorption line 10 to give the intensity profile 31 as shown respectively in Figures 6, 7 and 8.
- the spectral profile I(k) is given by
- Figure 10 illustrates the principle of the present invention.
- Light 101 101 received from a field of view in which a target gas might be present is received by the optical detector system 102.
- the received light passes through a band limiting filter BLF 103 and then a modifying filter MF 104. Further optical processing may then take place in a pre-detector optical processor 105 before detection (106).
- the signal from the detector 108 is then connected to an electronic processor 107
- Figure 12(a) shows an intensity profile 120 with two filter lines of ⁇ k separation and with no gas present, and it can be deduced that there will be a periodic structure in the coherence function proportional to 1/ ⁇ k.
- the gas absorption line 121 is seen to appear midway between the two modifying filter lines 122, 123.
- the coherence function will now have a periodicity proportional to 2/ ⁇ k. This, in effect re-distributes the modulation efficiency, so the sensitivity of detection at a particular path difference is enhanced.
- the concept of double filter absorption lines can be extended to include multiple lines where the gas feature is in effect sampled at a number of specific wavenumbers.
- the MF could appear as a spectral comb function consisting of many absorption bands 130, periodically spaced at wavenumbers intervals ⁇ where ⁇ ⁇ 1 (the gas feature (121) bandwidth). This situation is sketched in Figure 13.
- the spectral profile of the light after passage through the filter is in effect the product of the gas absorption profile and the filter transmission.
- the resulting coherence function (the Fourier transform of the spectral profile) is a convolution of the absorption line coherence function with the Fourier transform of the filter transmission, ie a replication of the absorption line coherence function with period 1/ ⁇ . It is therefore possible to sample various features of the gas coherence profile in a simultaneous fashion (say by multiple folding of one arm in the interferometer).
- the structure of the coherence envelope is more dependent on the gas absorption line because G(L) (the Fourier transform of A( ⁇ )) decreases more quickly with respect to L than with a Gaussian line of notionally the same spectral width.
- the rectangular spectral profile introduces elements of ⁇ phase shift into the coherence profile which can further advantageously modify the coherence function.
- the principle of the modulation techniques is to ensure that one or more unique features of the coherence characteristic are selectively modulated prior to detection, thereby maximising the immunity of the system to interferant species and the effects of background duties.
- ⁇ m centre wavelength
- TAOF Tunable Acousto-Optic Filter
- ⁇ m can be varied by changing the frequency of the TAOF electrical driving signal.
- the depth of absorption of the TAOF at ⁇ m can be varied by changing the amplitude of the electrical driving signal.
- the depth of absorption can be varied using "conventional" (interference or dye) filters by changing the area of filter inserted into the optical path.
- gas cell filters can be amplitude modulated by controlling the amount of absorptive gas in the active region of the cell. Centre frequency or depth of absorption modulation can be applied to any or all of the filters employed (broad band-pass or narrow band pre-processing filters). Furthermore, the use of such filter modulation does not preclude the other forms of modulation such as phase modulation via variation of interferometer path difference. Note also that pressure modulation of gas cells will lead to variable spectral width; modulating the width of the TAOF has the same effect. In all cases it is important to remember that both the real and imaginary components are available.
- the types of active illumination sources can include lasers, band-limited white light, fluorescence stimulating, spectral discharge lamps (e.g. sodium or xenon), solid state devices (e.g. LEDs) etc.
- spectral discharge lamps e.g. sodium or xenon
- solid state devices e.g. LEDs
- spectral profiles are available by combining the natural line shape of the emitted light and the transmission profile of the spectral filters (BLF or MF).
- the sensor can employ any of the sources individually or in any combination that is desirable.
- solar radiation can be regarded as one of the possible sources.
- the system is essentially linear in its spectral processing (ie the filters can be placed at any point in the system) it can be advantageous for certain purposes to position some (or all) of the spectral processing at or near the source and not (as so far discussed) in the receiver.
- This may well be beneficial where a number of low-cost receivers are needed and therefore only one unit (the transmitter) needs contain the relatively complex manipulation.
- the same philosophy applies if a number of low cost transmitters are needed with only one or a few higher value receivers; in this case the receivers contain the spectral processing.
- the invention has been based on the application of spectral pre-detector processing to gas detection.
- the principles can however be applied to a wider class of problems. For example, if it is required to remotely measure tilt or more generally movement of an object (e.g. rotation of a shaft), angular dependent spectral changes can be detected. This could be noted by observing spectral variations from an interference filter fitted to the object or even by exploiting the wavelength dependence of reflectivity (ie Fresnel reflectance which depends on object refractive index which is a function of wavelength).
- the spectral changes associated with thin films or animal/vegetable layers could lead to applications in the maritime (oil pollution) environment or more generally resource and health monitoring.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- Electromagnetism (AREA)
- Power Engineering (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
Un système de détection optique, composé d'un dispositif de transformation modulant le rayonnement reçu de façon à sensibiliser le système à des caractéristiques sélectionnées dépendant du profil de la fonction de cohérence dans le champ optique reçu, comprend un processeur spectral. Le processeur spectral possède un filtre limiteur de bande (BLF) et un filtre modificateur (MF) ayant une bande passante recouvrant au moins partiellement la bande passante du BLF (103). Le BLF et le MF sont sélectionnés de manière à concentrer l'information clé sur le rayonnement cible dans une petite région du profil de la fonction de cohérence. De préférence, le BLF a un profil de transmission rectangulaire et le MF a un profil gaussien, correpondant à celui de la ligne d'absorption du gaz à détecter. Le centre du profil d'absorption du MF est décalé par rapport au centre du profil du BLF. Dans d'autres configurations, le MF peut être tel qu'il produit deux ou plusieurs profils d'absorption (122, 123) dans le profil du BLF. La fonction de transmission d'un des filtres peut être dépendante du temps de manière à améliorer la détection du champ optique transformé. Cette dépendance est obtenue grâce au mouvement périodique du filtre produit par la variation de l'angle d'inclinaison d'un filtre d'interférence pour moduler la fréquence centrale du profil de transmission du filtre par un système faisant en sorte que la surface du filtre périodiquement déplacé, inséré dans le chemin optique du système, varie de manière à moduler périodiquement la profondeur d'absorption du filtre.An optical detection system, composed of a transformation device modulating the received radiation so as to sensitize the system to selected characteristics depending on the profile of the coherence function in the received optical field, comprises a spectral processor. The spectral processor has a band limiting filter (BLF) and a modifying filter (MF) having a bandwidth at least partially overlapping the bandwidth of the BLF (103). The BLF and MF are selected in such a way as to concentrate the key information about the target radiation in a small region of the profile of the coherence function. Preferably, the BLF has a rectangular transmission profile and the MF has a Gaussian profile, corresponding to that of the absorption line of the gas to be detected. The center of the MF absorption profile is offset from the center of the BLF profile. In other configurations, the MF may be such that it produces two or more absorption profiles (122, 123) in the profile of the BLF. The transmission function of one of the filters can be time-dependent so as to improve the detection of the transformed optical field. This dependence is obtained thanks to the periodic movement of the filter produced by the variation of the angle of inclination of an interference filter to modulate the center frequency of the transmission profile of the filter by a system ensuring that the surface of the filter periodically moved, inserted in the optical path of the system, varies so as to periodically modulate the depth of absorption of the filter.
Description
Claims
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB9115158 | 1991-07-12 | ||
GB919115158A GB9115158D0 (en) | 1991-07-12 | 1991-07-12 | Optical signal processing |
PCT/GB1992/001177 WO1993001477A1 (en) | 1991-07-12 | 1992-06-29 | Optical signal processing |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0594668A1 true EP0594668A1 (en) | 1994-05-04 |
Family
ID=10698321
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP92914231A Withdrawn EP0594668A1 (en) | 1991-07-12 | 1992-06-29 | Optical signal processing |
Country Status (5)
Country | Link |
---|---|
EP (1) | EP0594668A1 (en) |
JP (1) | JPH06509169A (en) |
CA (1) | CA2113270A1 (en) |
GB (2) | GB9115158D0 (en) |
WO (1) | WO1993001477A1 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5488876A (en) * | 1992-09-30 | 1996-02-06 | Precision Sampling Incorporated | Soil sampling system with sample container ridgidly coupled to drive casing |
JP5910139B2 (en) * | 2012-02-10 | 2016-04-27 | 株式会社島津製作所 | Laser gas analyzer |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2106665A (en) * | 1981-09-23 | 1983-04-13 | Spectron Developments Limited | Spectroscopic analysis |
GB8406690D0 (en) * | 1984-03-14 | 1984-04-18 | Secr Defence | Remote sensing of gases &c |
US5076699A (en) * | 1989-05-01 | 1991-12-31 | Rosemount Analytical Inc. | Method and apparatus for remotely and portably measuring a gas of interest |
-
1991
- 1991-07-12 GB GB919115158A patent/GB9115158D0/en active Pending
-
1992
- 1992-06-29 JP JP5502055A patent/JPH06509169A/en active Pending
- 1992-06-29 CA CA002113270A patent/CA2113270A1/en not_active Abandoned
- 1992-06-29 EP EP92914231A patent/EP0594668A1/en not_active Withdrawn
- 1992-06-29 WO PCT/GB1992/001177 patent/WO1993001477A1/en not_active Application Discontinuation
-
1994
- 1994-01-10 GB GB9400341A patent/GB2272765B/en not_active Expired - Fee Related
Non-Patent Citations (1)
Title |
---|
See references of WO9301477A1 * |
Also Published As
Publication number | Publication date |
---|---|
JPH06509169A (en) | 1994-10-13 |
GB9400341D0 (en) | 1994-03-16 |
CA2113270A1 (en) | 1993-01-21 |
WO1993001477A1 (en) | 1993-01-21 |
GB9115158D0 (en) | 1991-08-28 |
GB2272765B (en) | 1995-04-05 |
GB2272765A (en) | 1994-05-25 |
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