Thermal Imaging System

This invention relates to imaging systems, particularly thermal imaging systems. Such systems are well known per se, e.g., see "Thermal Imaging Systems" by J. M. Lloyd, Plenum Press, 1975, and "Thermal Imaging With Real Time Picture Presentation" by Sven-Bertel Borg, Applied Optics, Vol. 7, No. 9, pp 1697-1703, September 1968 (and the bibliography therein), and "Wide-Angle Infrared Camera For Industry and Medicine" by E. Sundstrom, Applied Optics, Vol. 7, No. 9, pp 1763-1768, September 1968. These systems operate in the visible or infra red (I.R.) part of the electromagnetic spectrum by collecting radiation from a scene and focussing it onto a detector which gives an electrical output proportional to radiation received. The detector output is displayed on a cathode ray tube in a conventional manner. In some systems a single small detector is effectively swept over the scene in a raster manner i.e. in a manner similar to that used in a television picture. One way of raster scanning requires a rotor having reflecting surfaces to sweep the scene image line by line onto the detector, successive surfaces having a differing inclination so that each surface sweeps successive lines. A disadvantage with this is the high rotor speed necessary to obtain a good quality display. An alternative system uses a reflecting rotor to scan a line onto the detector and an oscillating mirror to direct successive lines onto the detector. Again rotor speeds can be very high; also synchronism between rotor and mirror causes unwanted problems.

According to this invention, in an imaging system in which visible or infra red radiation from a scene is focussed onto a rotor to sweep an image of the scene onto a detector for subsequent reproduction of the scene on a display, the rotor includes a plurality of visible or infra red radiation transmitting fibres arranged for transferring radiation between different parts of the rotor's surface.

The rotor may be of cylindrical shape with a single bundle of fibres arranged diagonally, or a plurality of bundles each having one end staggered along the length of the rotor's curved surface and the other end lying in a common plane on the rotor's curved surface.

A correction plate comprising a plurality of visible or infra red radiation transmitting fibres may be arranged adjacent the rotor for directing radiation into the fibres in the rotor; such a plate may have a flat or slightly curved front surface and a rear surface which is complementary to the curved surface of the rotor and spaced a short distance from it.

The fibres used to transmit infra red are similar in principle and construction to those used in visible fibre optics except that the material used in the fibres must be capable of transmitting infra red radiation.

One such material is a glass, described in a co-pending patent application by A. H. Lettington and J. A. Savage (U.S. Ser. No. 811,414 filed June 29, 1977, for Infra Red Transmitting Glasses), which has up to 30 atomic percent of telluride substituted for selenide in a glass having a composition within the following range

germanium 10-35 atomic percent

arsenic 9-45 atomic percent

selenide 45-70 atomic percent

Preferably the glass range is within the area defined and bounded by the lines joining the following compositions in the GeAsSe ternary diagram expressed in atomic percentages Ge.sub.22 As.sub.9 Se.sub.69, Ge.sub.35 As.sub.9 Se.sub.56, Ge.sub.35 As.sub.20 Se.sub.45, Ge.sub.15 As.sub.40 Se.sub.45.

Typical fibre diameters are 50.mu. and the binding matrix an epoxy resin. The ends of the fibres on the rotor and correction plate are preferably coated with a single or multi-layer anti-reflection coating such as a single layer of cerium flouride.

Various detectors may be used and cooled in conventional manner e.g. by liquid nitrogen. For example the detector material may be Cadmium Mercury Telluride (C.M.T.) described in U.S. Pat. No. 2,953,690, or Lead Tin Telluride (L.T.T.).

The invention will now be described by way of example only, with reference to the accompanying drawings of which:

FIG. 1 is a schematic plan view of an infra red system constructed in accordance with the present invention;

FIG. 2 is a sectional side view of part of the system shown in FIG. 1;

FIG. 3 is a view of an alternate construction of rotor which gives vertical and horizontal scanning of a scene;

FIG. 4 is a developed view of the rotor of FIG. 3;

FIG. 5 is a plan view of the rotor of FIGS. 3 and 4; and

FIG. 6 illustrates a modification of the system shown in FIG. 2, for use as a picture generator.

As shown in FIGS. 1 and 2 infra red radiation from a scene is collected and focussed by a lens 1 onto a fibre optic correction plate 2. This plate 2 comprises numerous fibres of infra red transmitting glass held parallel to one another in a glass binder with the fibres lengths perpendicular to the flat front face 3 of the plate. The rear face 4 of the plate 2 is of a cylindrical curvature. Behind the plate 2 is a cylindrically shaped rotor 5 comprising a bundle 6 of infra red transmitting fibre arranged parallel to one another in a binder. The remainder of the rotor 5 is of lightweight plastics material mounted on a rotor spindle 7 for rotation by an electric motor 8. The direction of rotation of rotor 2 is immaterial.

Behind the rotor 5 is a lens 9 which focusses images from the rotor 5 onto a linear detector array 10 whose output is used to form a display in a conventional manner e.g. on a cathode ray tube 11. The number of elements in the detector array 10 is equal to the number of lines in the scene, thus for a clear display as large a number as possible is used, typically 200 detector elements.

When the rotor 5 is rotated, the image on the correction plate 2 is swept across the detector array 10 twice per revolution. The rotor periphery is equispaced from the rear face 4 of the plate 2 resulting in good transmission of the image between the plate 2 and rotor 5 because the image leaves and enters the fibres normal to their end surfaces. The displayed scene may be interlaced by tilting the axis of the fibres 6 relative to the normal to the axis of the rotor 5.

As shown the rotor diameter is about .sqroot.2 x width of the image on the correction plate 2, the width of the fibre bundle is about half the image width, and the height of the fibre bundle is the height of the image. Such a rotor has a dead time of about 75%. For a smaller drum, equal to the image width on the plate 2, the dead time is about 50% but a loss in definition can occur at the edge of the displayed image.

As an alternative to the system shown in FIGS. 1 and 2, a single detector element may be used and an additional vertical scanning mirror or rotor used to obtain a vertical sweeping the image. If a vertical scanning rotor is used, it is arranged orthogonal to the rotor of FIGS. 1, 2 and a double curved fibre optical correction plate is located between the two rotors.

One drawback of the rotor shown in FIGS. 1, 2 is the dead time i.e. the period during which no image is transmitted between the plate and detector array and the large number of detector elements needed for a good quality display.

One rotor 14 which avoids this dead time and which produces a vertical scan, thereby reducing the number of detector elements, is shown in FIGS. 3, 4 and 5. For simplicity of illustration the image on the correction plate 2 is swept in six bands. Six bundles 15, 16, 17, 18, 19, 20 of parallel spaced fibres are arranged with one end 15a to 20a spaced around the curved surface of the rotor 14 equispaced in a vertical direction collectively covering the total height of the image formed on the correction plate 2. The other ends 15b to 20b of the bundles are arranged diametrically opposite to the ends 15a to 20a respectively but in a common plane on the rotor circumference. Each bundle 15 to 20 has a width equal to half the image (on the plate 2) width and a height equal to the band height, i.e., one-sixth of the correction plate image height. Output from the rotor is through a lens 21 to a detector array 22 which only requires a number of elements large enough to give a good quality display for one band height.

In operation with the rotor 14 rotating, the top sixth of the image is scanned by the fibre bundle 15 onto the detector array 22, followed by scanning of the next lower sixth of the image by the fibre bundle 16, and so on until the whole image is scanned. This process is repeated once for each revolution of the rotor 14.

As an example of a rotor 14 constructed according to FIGS. 3, 4 and 5, the number n of bands was 28, the width w of the image was 2cm, and the rotor diameter was therefore nw/2.pi. = 8.91 cm.

The correction plate 2 may be replaced by a lens for some applications when losses associated with the infra red image not entering the rotor fibres normal to their ends may be accepted.

The lens 9, or 21 may be replaced by infra red transmitting fibres. This allows considerable freedom in placing the detector e.g. away from the rotor 5 and in a cooled chamber.

Since the imaging system may also be operated using visible light it may be used as a picture generator i.e. the reverse of that described above with reference to FIGS. 1, 2. This is shown in FIG. 6 which duplicates the system of FIGS. 1, 2 but using some visible light components. Components common to FIGS. 1, 2 and 6 are given like reference numerals. The rotor 5' is extended along its axis and carries a second bundle 6' of visible light transmitting fibres arranged diametrically in the rotor 5'. A visible light modulated light source 10', e.g., one or more light emitting diodes (LED's), is modulated by the electrical signal from the detector 10. Light from the LED's 10' passes along the fibre bundle 6' and onto a visible fibre optic plate 2' where it may be observed as a visible image of the infra red scene.