CA2331424C

CA2331424C - Night viewer and laser range finder

Info

Publication number: CA2331424C
Application number: CA002331424A
Authority: CA
Inventors: Jerry Porter
Original assignee: Litton Systems Inc
Current assignee: L3 Technologies Inc
Priority date: 1998-05-18
Filing date: 1999-05-17
Publication date: 2004-03-23
Anticipated expiration: 2019-05-17
Also published as: CA2331424A1; IL158515A; EP1095516A1; WO1999060787A1; IL138684A0; IL138684A; EP1095516A4

Abstract

An integrated night vision device and laser range finder (l0) provides both night-time and day-time imaging of a scene by use ofan image intensifier tube (14), as well as providing laser range finding operations both day and night. In a laser range finder mode of operation the device (10) projects a pulse of laser light into a scene being viewed, and a power supply and laser range finder circuit (62) of the device (10) temporarily utilizes the image intensifier tube (14) as a sensor to detect reflected laser light. During laser range finding, imaging is cut off for a very short time interval, and a pre-amplifier circuit (66b) associated with the image intensifier tube (10) provides an electrical output signal in response to receipt of laser light reflected from an object in the scene.

Description

WO 991607$7 PCTIUS99I11093 NIGHT 'CIE WF:R
AND LASER RANGE FINDER
BACKGROUND OF THE I:~tVENTION
FIELD OF THE INVENTION
The present invention is in the field of night vision devices of the Iight amplification type. More particularly, the present: invention relates to an improved night vision device having an image intensifier tube (I2T). Also, the present invention is in the field of laser range finders. A method o~F operating the night vision device and a method of laser range finding (LRF) are disclosed also.
Related Technolony Laser range finders have been known for a considerable time. These devices are used, for example, by surveyors to calculate the distance from a point of observation to an object such as a geological forniation in the field of view (i.e., the device requires line of sight relationship between a user and the object to be ranged).
Generally, a laser range finder operates by projecting a pulse of laser light at an object.
The laser light illuminates the object, and a portion of the laser light is reflected back toward the laser range finder device. The reflected laser light is detected, and the time interval required for the laser light pulse to travel tto and from the object is measured.
Frorn this time interval measurement and the known speed of light, the distance between the laser range finder and the object is calculated.
A conventional laser range finder of the type described above generally includes a Iaser capable of producing laser light pulses of high peak power and very short duration (i.e., less than SOns duration). The detector for the reflected laser light may include a high speed photodetector (such as an InGaAs avalanche photodiode), which is coupled to a high gain, high speed amplifier. A high speed digital counter may be used as a timer to determine the time interval required for the laser Light to travel to the object and for laser light reflecting off' of the object to travel back to the device. From this time interval information an internal electronic calculator determines the range to the object, and this range is presented to the user of the device, usually on a visual display screen.
These conventional laser range finders have a disadvantage of a considerable cost and complexity. The laser pulses must be of considerable intensity as well, which requires a high power laser. The conventional laser range finders are subject to optical and electrical problems, such as vuinerabil:ity to electromagnetic interference, damage to electrical components and damage to optical components. Reliability of the devices is also adversely impacted by their complexity.
~n the other hand, conventional night vision devices of the image intensification type (i.e., light amplification) type have also been known for a considerable time. Generally, these night vision devices include an objective lens which focuses invisible infrared Light from the night time scene onto the transparent light-receiving face of an image intensifier tube. At its opposite image-face, the image intensifier tube provides an image in visible yellow-green phosphorescent light, which is then presented to a user of the device via an eye piece lens.
Even on a night which is too dark for diurnal vision, invisible infrared Light is richly provided by the stars. Human vision can not utilize this infrared Light from the stars because the so-called near-infrared portion. of the spectrum is invisible for humans. A night vision device of the light amplification type can provide a visible image replicating the night time scene.
A contemporary night vision device will generally use an image intensifier tube with a photocathode behind the light-receiving face of the tube. The photocathode is responsive to photons of infrared light to liberate photoelectrons.
These photoelectrons are moved by a prevailing electrostatic field to a microchannel plate (MCP) having a great multitude of dynodes, or microchannels with an interior surface substantially defined by a material having a high coefficient of secondary electron emissivity. The photoelectrons entering the microchannels cause a cascade of WO 99!60787 PCT/US99/11093 secondary emission electrons to move along the mic;rochannels so that a spatial output pattern of electrons which replicates an input pattern, and at a considerably higher electron density than the input pattern results. This pattern of electrons is moved from the microchannel plate to a phosphorescent screen to produce a visible image.
A
power supply for the image intensifier tube provides the electrostatic field potentials referred to above, and also provides a faeld and current flow to the microchannel plate.
Conventional night vision devices which .are usable to sight a weapon are found in United States patents No. 5,084,780; and 5,035,472. Neither of these patents is believed to suggest or disclose a night vision device which is combined with a laser range finder using the image intensifier tube of thE: night vision device as a detector for laser light in the laser range finder.
SUMMARY OF THE INVENTION
In view of the deficiencies of the conventional related technology, it would be desirable to provide a single device which provides both night vision imaging and Iaser range finding functions.
Additionally, it would be desirable to provide a laser range finder which uses an image intensifier tube as a detector for reflected laser light from an object.
Yet another advantage would be to providf; such a device which allows both night-time and day-time imaging and laser range Finding using the image intensifier tube of the imaging device as the detector for reflected laser light.
Still another advantage could be obtained b;y provision of such a device which utilizes the image intensif er tube as a detector for reflected laser light in the LRF
function, and which also includes electrical amplification of the electrical signal produced when this laser light is detected, therefore to provide an improved signal to noise ratio for the LRF function.
Accordingly it is an object for this invention to provide a method of laser range finding using an image intensifier tube as a detector for reflected laser light, and in which the image intensifier tube includes provision internally for amplifying an electrical signal indicative of the detection of reflected laser light during a LRF
function.
An advantage of the present combined night vision device and laser range finder is that a single device is provided of considerably less expense and of considerably improved durability in comparison to the conventional technology providing these functions in two separate devices. The laser pulses needed for laser range finding can be of remarkably lower power than those required by a conventional laser range finder. This further decreases the cost of the device because of the lower cost of a lower power Laser, and the energy use of the device is also decreased.
Other obj ects, features, and advantages ~of the present invention will be apparent to those skilled in the art from a consideration of the following detailed description of a preferred exemplary embodiment thereof taken in conjunction with the associated figures which will first be described ibriefly.
BRIEF DESCRIPTItJN OF THE DRAWINGS
Figure 1 is a schematic representation of an integrated night vision device and laser range finder embodying the present invention, and with a part of this device shown in alternative operative positions by use of solid and dashed lines;
Figure 2 shows an image intensifier tube embodying the present invention in longitudinal cross section;
Figure 3 is a schematic representation of a power supply and laser range finder operation circuit for an integrated night vision device and laser range finder embodying the present invention;
Figure 3a is a fragmentary schematic representation of an alternative embodiment of an image intensifier tube module for use in an integrated night vision device and Laser range finder according to the present invention; and Figures 4 and 5 respectively provide graphical illustrations of an automatic brightness control (ABC) function, and of a bright-source protection (BSP) function of the integrated night vision device and laser r~uige finder embodying the present invention.

DETAILED DESCRIPTION OF AN EXEMPLAvRY
PREFERRED EMBODIMENT OF THE INVENTI N
While the present invention may be embodied in many different forms, disclosed herein is a specific exemplary embodiment that illustrates and explains the principles of the invention. It should be emphasized that the present invention is not limited to the specific embodiment illustrated.
NIGHT VISION
Refernng first to Fig. l, there is shown schematically the basic elements of one version of an integrated night vision device and laser range finder 10.
Particulars of the laser range finding (LRF) operation of the device are presented below. In order to provide night vision, the device 1d generally comprises a forward objective optical lens assembly 12 (illustrated schematically as a single lens, although those ordinarily skilled will understand that the objective lens assembly 12 may include plural lens elements). This objective lens 12 performs at least two functions in the device 10, lens I2 focuses incoming light from a distant scene through the front light-receiving end 14a of an image intensifier tube 14 (as will bE; seen, this surface is defined by a transparent window portion of the tube - to be further described below). As was generally explained above in the discussion of the related technology, the image intensifier tube 14 provides an image at light output end 14b in phosphorescent .
yellow-green visible light. This image replicates th,e scene being viewed by use of the device 10.
The scene being viewed by use of device 10 may be a dark night-time scene which is invisible, or is only poorly visible, to the user of the device 10 using natural human vision. On the other hand, as will be explained, the device 10 may be used to view a day-time scene, and to conduct laser range finding (LRF) in both daylight and at night. The visible image from tube 14 is presented by an eye piece lens illustrated schematically as a single lens 16 producing at the user's eye a virtual image of the rear light-output end 14b of the tube l 4.

More particularly, image intensifier tube 14 includes a photocathode 20 which is responsive to photons of light at the deep red endl of the visible spectrum and in the near-infrared portion of the spectrum to liberate photoelectrons in a pattern replicating the scene being viewed, a microchannel plate (MCP) 22 which receives the photoelectrons in the pattern replicating the scene, and which provides a greatly amplified pattern of electrons also replicating this scene, and a display electrode assembly 24 having an aluminized phosphor co<~ting or phosphor screen 26. A
transparent window portion 24a of the assembly 24 carries the electrode 24 and screen 26, and also conveys the image from screen 26 outwardly of the tube 14 so that it can be presented to the user 18. Window portion 24a defines surface 14b.
Still more particularly, MCP 22 is located ,just behind photocathode 20, with the MCP 22 having an electron-receiving face 28 and an opposite electron-discharge face 30. This MCP 22 further contains a plurality of angulated microchannels which open on an electron-receiving face 28 and on an opposite electron-discharge face 30. Microchannels 32 are separated by passage walls 34. At least a portion of the surfaces of the walls 34 bounding the microchannels 32 is formed by a material having a high coefficient of emissivity of secondary electrons. Thus, the channels 32 of the MCP 22 are each a dynode, emitting a shower of secondary electrons in response to receipt at face 28 of photoelectrons from photocathode 20.
The display electrode assembly 24, generally has a coated phosphor screen 26, and is located behind MCP 22 with phosphor screen 26 in electron line-of sight communication with the electron-discharge face 3(). This display electrode assembly 24 is typically formed of an aluminized phosphor screen 26 deposited on the vacuum-exposed surface of the optically transparent material of window portion 24a.
The eye piece lens 16 is located behind the display electrode assembly 24 and allows an observer 18 to view a correctly oriented image corresponding to the low level image (i.e., dim or invisible, perhaps) of the scene being viewed.
As will be generally appreciated by those skilled in the art (now also viewing Figure 2), the individual components of image intensifier tube 14 are all mounted and supported in a tube or chamber (to be further explained below) having forward and rear transparent plates cooperating to define a chamber (to be fuxther defined below) which has been evacuated to a low pressure. 'This evacuation allows electrons liberated into the free space within the tube (i.e., i;he photoelectrons and secondary-emission electrons) to be transferred by prevailing electrostatic fields between the various components without atmospheric interference that could possibly decrease the signal-to-noise ratio.
As indicated above, photocathode 20 is mounted immediately behind objective lens 12 on the inner vacuum exposed surface of th.e window portion of the tube and before MCP 22. It is upon this photocathode treat the objective lens 12 actually focuses the image of the distant scene, through tl~e window portion which defines surface 14a. Typically, this photocathode 20 i.s a circular disk-like structure having a predetermined construction of semiconductor materials, and is mounted on a substrate in a well known manner. Suitable photocatho~de materials are generally semi-conductors such as gallium arsenide; or alkali meW 1s, such as compounds of sodium, potassium, cesium, and antimony (commercially available as S-20). The photocathode is carried on a readily available substrate which is transparent to light in the wavelength band of interest (i.e., ordinarily i.n the deep-red and near infrared portion of the spectrum; extending in some cases to the blue portion of the visible spectrum - but which is not necessarily transparent to all visible light). A
variety of glass and fiber optic substrate materials are commercially available.
Still referring to Figure 2, and considering in somewhat greater detail the operation of the image intensif er tube 14 in its mode of operation providing a visible image it is seen that in response to photons 36 entering the forward end of night vision device 10 and passing thraugh objective lens 12, photocathode 20 has an active surface 38 from which are emitted photoelectrons in numbers proportionate to and at locations replicative of the received light from the scene being viewed. In general, at night the image received by the device 10 will be too dim to be viewed with human natural vision, and may be entirely or partially of infrared radiation which is invisible to the human eye. The device may also operate in daylight to provide an image, as will be explained. It is thus to be understood 'that the shower of photoelectrons emitted from the photocathode are representative of the image entering the forward end of image intensifier tube 14. The path of a typiical photoelectron emitted from the photon input point on the photocathode 20 is represented in Fig: 1 by dashed line 40.
Photoelectrons 40 emitted from photocathode 20 gain energy by passage through an applied electrostatic field between the 1>hotocathode 20 and the input face 28. The applied electric field is of a predetermined intensity gradient and is established between photocathode 20 and electrc'n-receiving face 28 by a power source diagrammatically depicted in Figure 1 and indicated by the numeral 42.
Typically, power source 42 will apply an electrostatic field voltage on the order of 200 l 0 to 800 volts to maintain an electrostatic field of the desired intensity.
This field is most negative at photocathode 20 and most positive at the face 28 of MCP 22.
Further, an electrostatic field most negative at photocathode 20 and most positive at output electrode 24 is maintained in the image intensifier tube 14, as will be seen.
After accelerating over a distance between the photocathode 20 and the input face 28 of the MCP 22, these photoelectrons 40 enter microchannels 32.
As will be discussed in greater detail below, the photoelectrons 40 are amplified by emission of secondary electrons in the microchannels 32 to produce a proportionately larger number of electrons upon passage through MCP 22. This amplified shower of secondary-emission electrons 44, also accelerated by a respective electrostatic field applied by power source 46, then exits from the microchannels 32 of MCP 22 at electron-discharge face 30.
Once in free space again (i.e., in the vacuum environment inside of tube 14), the amplified shower of photoelectrons and secondary emission electrons is again accelerated in an established electrostatic field provided by power source 48.
This electrostatic field is established between the electtron-discharge face 30 and display electrode assembly 24. Typically, the power source 48 produces a field on the order of 3,000 to 7,000 volts, and more preferably on the order of 6,000 volts in order to impart the desired energy to the multiplied electrons 44.
The shower of photoelectrons and secondary-emission electrons 44 (those ordinarily skilled in the art will know that considiered statistically, the shower 44 is WO 99!60787 PCT/US99/11093 almost or entirely devoid of photoelectrons and is made up entirely or almost entirely of secondary emission electrons. This is the case because the statistical probability of a photoelectron avoiding absorption in the microc~hannels 32 is low). However, the shower of electrons 44 is several orders of magniaude more intense than the initial shower of photoelectrons 40, but is still in a pattern replicating the image focused on photocathode 20. This amplified shower of electrons falls on the phosphor screen 26 of display electrode assembly 24 to produce an irna~;e in visible light.
Viewing Figure 2 in order to acquire a greater understanding of the detail of a typical image intensifier tube, the image intensifier tube 14 is seen to include a tubular body 50, which is closed at opposite ends by a front Light-receiving window 52, and by a rear fiber-optic image output window 54. The window 54 defines the light output surface 14b for the tube 14, and carries t:he coating 26, as will be fixrther described. As is illustrated in Figure 2, the rear window 54 may be an image-inverting type (i.e., with optical fibers bonded together and rotated 180° between the apposite faces of this window 54 in order to provide an erect image to the user 18.
The window member 54 is not necessarily of such inverting type. Both of the windows 52 and 54 are sealingly engaged with the body 50, so that an interior chamber 56 of the body 50 can be maintained at a vacuum relative to ambient.
The tubular body 50 is made up of plural conductive metal rings, each indicated with the general numeral S8 with an alphabetical suffix added thereto (i.e., 58a, 58b, 58c, and 58d) as is necessary to distinguish the individual rings from one another.
The tubular body sections S8 are spaced apart and are electrically insulated from one another by interposed insulator rings, each of which is indicated with the general numeral 60, again with an alphabetical suffix added thereto (i.e., 60a, 60b, and 60c). The sections 58 and insulators 60 are sealingly attached to one another.
End sections 58a and 58d are likewise sealingly attached to the respective windows 52 and 54.
The body sections 58 are individually connected electrically to a power supply and laser range finder circuit, generally indicated with numeral 62, and best seen in Figure 3, (and which includes the power sources diagrammatically illustrated in Figure l and indicated with reference numerals 42" 46, and 48, as described above).
This circuit 62 is effective during operation of the image intensifier tube 14 to maintain an electrostatic field most negative at the section 58a and most positive at the section 58d. As will be seen, the circuit 62 includes a section indicated with the numeral 62a, which is encapsulated with the images intensifier tube 14, and which is effective to provide the voltages necessary for operation of this tube. The image tube 14 and circuit section 62a will be recognized by those ordinarily skilled in the pertinent art as an image tube module. Another section 62b of the circuitry 62, seen together with section 62a in Figure 3, allows control of the operation of a laser to provide pulses of laser light, and to operate the image intensifier tube 14 as a detector for the reflected laser light in order to allow timing of the light pulses, and calculation of the range to a object illuminated by the laser light: pulses.
Further viewing Figure 2, it is seen that the :front window 52 carnes on its rear surface within the chamber 56 the photocathode 20. The section 58a is electrically continuous with the photocathode by use of a thin metallization (indicated with reference numeral 58a') extending between the secrtion 58a and the photocathode 20.
Thus, the photocathode by this electrical corn<;ction and because of its semi-conductive nature, has an electrostatic charge distributed across the areas of this disk-like photocathode structure. Also, a conductive coating or layer is provided at each of the opposite faces 28 and 30 of the MCP 22 (as is indicated by arrowed numerals 28a and 30a). Power supply 46 is conductive with these coatings by connection to housing sections 58b and 58c. Finally, the power supply 48 is conductive with a conductive layer or coating (possibly an aluminum :metallization, as mentioned above) at the display electrode assembly 24 by use of a nnetallization also extending across the vacuum-exposed surfaces of the window member 54, as is indicated by arrowed numeral 54a.
Still viewing Figure 2, it is seen that the circuit portion 62a is disposed within an encapsulating body 64, which is configured as an annulus extending about the body 50 of the tube 14. This power supply circuit portion 62a has electrical connection with each of the conductive ring sections 58a-d of the tube 14, as is indicated diagrammatically in Figure I. Additionally, as is indicated in Figure 3, this circuit portion includes a current transformer 66a and a preamplifier circuit portion 66b both disposed within the body 64 immediately adjacent to the tube 14.
Considering now Figure 3, it is seen that the circuit 62 includes a power source, which in this case is illustrated as a battery 68. It will be appreciated that a battery 68 is generally used as the power source for portable apparatus, such as night vision devices. However, the invention is not limilted to any particular power source.
For example, a regulated line-power source could b~e used to provide input power to a power supply implementing and embodying the principles of the present invention.
Considered generally, the circuit 62 includes three voltage multipliers, respectively indicated with the numerals 70, 72, and 74. 'I"he voltage multiplier 70 for the photocathode 20 includes two multipliers of differing voltage level, indicated with the numerals 70a and 70b. A tri-stable switching :network 76 switches controllably between alternative conditions either conducting the photocathode 20 to voltage I S multiplier 70a, to voltage multiplier 70b, or to are open circuit position, all via the conductive connection 76a. In other words, the switching network 76 alternatingly connects the photocathode 20 of the tube I4 to a voltage source at about -800 volts, or to a source at about +30 volts relative to the front face of the microchannel plate, as will be further seen. The open circuit interval of time employed in the present embodiment between connections of the photocathode 20 to the two voltage sources 70a and 70b is used for purposes of energy efficiency, and is optional. A duty cycle control 78 controls the switching position of the switching network 76, and receives as inputs a square wave gating trigger signal from an. oscillator 80, and a control signal via a conductor 82 from an ABC/BSP control circuit 84. Once again, the use of a square wave duty cycle trigger signal is optional. Other forms of duty cycle trigger waves can be employed.
Power supply to the MCP 22 (that is, to the conductive layers or metallizations 28a and 30a) is effected from the voltage multiplier 72 via connections 72a and 72b.
Interposed in connection 72a is a series element 86, which in effect is a variable resistor. A high-voltage MOSFET may be used fc~r element 86, and the resistance of Il this element is controlled over a connection 86a by a regulator circuit 88.
Regulator circuit 88 receives a feed back control signal from a surnrning junction 90, which receives an input from conductor 92 via a level-adjusting resistor 94, and also receives an input via conductor 96 from the ABCBSP control circuit 84. Conductor 92 also provides a reference voltage signal of the voltage level applied to the input face 28 (i.e., at metallization 28a) of the MCP 22 into the voltage multiplier circuit 70.
The voltage multiplier 74 has connection t:o the screen 26 via a connection 74a, and provides a feed back of screen current level into ABCBSP control circuit via conductor 98. It will be noted that the conductor 74a passes through the current transformer 66a, so that current flow in this conductor 74a is electromagnetically {i.e., inductively) linked to the pre-amplifier 66b. Energy flow in the circuit 62 is provided by an oscillator 100 and coupled transformer :102, with output windings 102a providing energy input to voltage multipliers 70 and 74, and a conductor 104 providing energy to voltage multiplier 72. The oscillator 100 receives a control feed back via a regulator 106 and a feed back circuit 108, having an input from a feedback winding 102b of transformer 102.
Having generally considered the structure o:f the circuit 62, attention may now be given to its operation, and the cooperation of this circuit operation with the operation of the image intensifier tube 14 to provide; imaging. It will be noted that this imaging of a scene for a user of the device 10 may take place at night in conditions of viewing a scene under dark-field conditions, or during the day with the scene illuminated by sun light. It will be noted also tlhat the voltage level produced by voltage multiplier 70a is a substantially constant voltage level. Preferably, this voltage is about negative 800 volts. ~n the other hand, the voltage multiplier section 70b provides a substantially constant voltage level referenced to the voltage provided by voltage multiplier 72 to the front face 28a of thf; MCP 22. Preferably, this voltage level is positive 30 volts relative to the front face 2!3 of the MCP 22.
By operation of the switching network 76, the photocathode 20 is controllably and cyclically changed between connection to the constant voltage source 70a, to an open circuit (i.e., voltage off), and to the lower voltage provided by source 70b WO 99160787 PCTlUS99/11093 (simulating darkness for the photocathode). This gating function is carried on at a constant frequency (preferably at about 50 Hz), with a constant cycle interval, while varying the duty cycle of the applied constant voltal;e from voltage multiplier 70a as a function of current level sensed at screen 26 (i.e., by feed back over conductor 104).
The frequency of the duty cycle for the photocathade is sufficiently fast {i.e., somewhat above about 30Hz} so that no flicker is perceived in the viewed image.
Automatic Brightness ControlBright Source Protection Viewing Figure 4, it is seen that over a first selected range of screen current the duty cycle of the applied constant voltage from multiplier 70a to the photocathode is fixed at 100%. However, at screen current levels above a selected level of screen current, the duty cycle progressively ramps down substantially linearly to a low level of essentially 10-4% as a function of increasing screen current. For screen current levels above that at which the duty cycle for gating of the constant voltage 15 from source 70a to the photocathode 20 drops to its low level, an additional function of BSP is provided by decreasing the voltage applied to the MCP 22. As Figure shows, for all screen current levels lower than those necessary to initiate this BSP
protection function, the voltage applied across the MCP 22 is a constant. The reduction of voltage level applied across the MCP :22 for BSP is effected by action of 20 the series element 86 increasing its resistance under control of MCP
regulator 88.
As noted this regulator 88 receives a .summed input from the voltage multipliers 70, and from the ABCBSP control circuit 84, which is responsive to screen current level sensed by conductor 98. An understanding of the voltage level experienced as a function of time within duty cycle intervals at the photocathode 20 can be obtained by noting that a virtual capacitor exists between the photocathode 20 and the front face 28 of MCP 22. This capacitor exists electrically, but not as a conventional capacitor structure. On Figure 3, this virtual capacitor is diagrammatically indicated, and indicated by the arrowed reference character "C".
When the duty cycle for the application of the constant voltage supplied by voltage multiplier 70a is 100%, or close to this level, then :following the opening of the circuit WO 99/60'78' PCT/US99/11093 through switching network 77, the voltage across the virtual capacitor "C"
decays over a time interval at a natural open-circuit, capacitor-discharge rate. This voltage decay is actually a very small voltage because of the short time interval (i.e., 1/SOth second at a SOHz frequency for the gating operation of switching network 76).
Next in each duty cycle, the network 76 conducts the photocathode to voltage multiplier 70b, which effectively replicates darl~;ness for the photocathode 20 by dropping the voltage on the photocathode to +30 volts relative to the face 28 of MCP
22. As noted above, this voltage cutoff is provided by having voltage multiplier 72b provide a voltage which is about 30 volts positive with respect to the voltage provided at coating 28a an the front face of the MCP 22 by voltage multiplier 72.
In essence, when the photocathode 20 operates, it always operates at the high constant voltage provided by voltage multiplier 70;3. When the photocathode 20 is not operating, it is switched to a voltage which replicates a dark field for the photocathode (i.e., the +30 volts from voltage multiplier 70b). T'he photocathode 20 operated by the 1 S circuit 62 of the present invention is switched between operation at its designed voltage level and dark-field condition at a duty cycle which varies dependent upon the Light intensity of the scene being viewed, as indicated by current flow at the screen 26.
This function is carried out in accord with the duty cycle function in order to provide ABC. The result of this ABC operation is a substantially constant brightness for the image presented to a user of the night vision device 10 is achieved, until the scene becomes too dim to produce an image even with image intensification technology. In other words, over the entire operating range of the image intensifier tube 14, its operation by circuit 62 provides substantially constant brightness for the image presented to the user of the device.
Further considering the operation of circuit; 62 to provide an image for the user of the device 10, is seen that once the duty cycle is reduced to its low level of 10-4%, in the event that screen current increases further, then as a function of increasing screen current the voltage across the MCP 22 is reduced slightly, viewing now Figure 5. This reduction of MCP voltage has the effect of providing BSP. That is, after the ABC function has reached its lowest level of duty cycle to the photocathode 20, if WO 99160787 PCTlUS99/11093 ..
Light level of the viewed scene continues to increase (indicative of a bright source in the scene), then the duty cycle maintains its low 10-4% level, while the bright-source protection function explained above is effected.
LASER RANGE FINI?ING
Further considering now Figures 1 and 3, the operation of the device and circuit 62 to provide a laser range finder function will be explained. The device 10 further includes a laser I LO capable of projecting; a short-duration laser light pulse 106a into the scene being viewed by the operator of the night vision and laser range finder device I0. This pulse of lasex light is diagrammatically illustrated on Figure 3 with the arrow 110a. Laser range finding operations are conducted by the device 10 temporarily using the image intensifier tube 14 as a sensor for the reflected laser light returned from the scene being viewed.
Laser 110 is powered by a laser driver circuit, indicated with numeral 112. A
laser range finder (LRF) control logic circuit 114 (the operation of which will be further explained below) provides a control input to the driver circuit 112 to effect operation of the laser 110, and also provides a control input to the oscillator 100 via a conductor 116.
Conductor 116 at a branch 116a thereof also provides a control input to an actuator 1 I $, which in response to this control input moves a spatial f lter 120 (to be further described below) first into, and then after' a short interval, out of the optical pathway between lens I2 and the image intensifier tube I4, as is indicated by dashed lines on Figure 1. The spatial filter 120 is essentially a shutter with a central aperture, which blocks returning laser light from portions of the viewed scene other than in the central area where the object of interest is located. During a LRF operation, the actuator I 18 pauses the spatial filter 120 in the opitical pathway of the device 10. That is, there is a controlled momentary pause between the movement of the spatial filter into and out of the optical pathway. During the laause of the filter 120 in the optical pathway, laser light is projected to an object in t:he viewed field, and reflected laser light returned from the object for a LRF operation is received at the device 10.

WO 99/6078'1 PCTIUS99/11093 The LRF control Logic circuit 114 also has a control output 122a to a gating control circuit 122. This circuit has connection to switching network 76, as is illustrated. An operator-input command device 1:24 (which may take the form of a push button switch, far example) is provided by which the operator of the device .i0 can indicate a command that a LRF operation be earned out be the device 10.
The remainder of the elements of the device 10 will be described in connection with a LRF
operation.
A LASER RANGE FINDTNG OPERATION
Considering Figure 3 still, when the operator of the device 10 wishes to obtain range information to an object in the viewed field, the operator centers the object in the viewed scene, possibly by using a reticule provided by the device 10, and makes a LRF input command at device 124. To repeate, this input command may be effected by use of a simple push-button switch, for example. In response to this input command, the LRF control logic circuit 124 effects the following sequential activities:
First, the oscillator 100 is shut down by a command over conductor 116. This command also has the effect of causing actuator 118 to move the spatial filter 120 into the optical pathway. The shutdown command for the oscillator 100 also is used to cause the voltage multiplier 72 to drive the MCP 22 to a high-gain differential voltage level. Preferably, this high-gain voltage Level is a. differential voltage of about i 200 volts across the MCP 22.
Second, the LRF control logic circuit com~:nands the switching netwoxk 76 to perform a timed switching operation (as is further described below), first switching photocathode 20 to the voltage from multiplier 7C)b (i.e., to +30 volts relative to the front face of MCP 22 - effecting a hard turn off for the photocathode 20 of the tube 14); and then later in timed relation connecting this. photocathode to source 70a.
Third, after a time interval of about 3 ms (which is required to allow the oscillator 80 to stop its operation), the laser light pulse is fired. The photocathode 20 is then effectively switched to the voltage source of multiplier 70a (i.e., to about -800 volts). Actually, the photocathode 20 is switched to voltage source 70a in timed relation before the laser light pulse is fired. The: photocathode needs to settle for about 200 p.s before the laser is fired. If the device 10 is configured to project the laser light pulse from the same lenses used to receive ambient light, then in order to provide a non-responsiveness of the device 10 to the back scatter of laser light which may occur in the optics of the device the pre-amplifier circuit 62 is caused to have a time-dependent gain. One way in which thiis time-dependent gain may be implemented is to provide a high and time-variant threshold value which the electron pulse which will be caused within image intensifier tube 14 by reflected laser light must exceed before the signal is provided to stop timer 130. This threshold value IO would be high immediately after laser pulse 22 is fired, and would decrease as a function of time after the pulse is fired. Another al'''ternative is to have a step-function change in the threshold value at a certain time after the laser light pulse is fired. In this way, the timer 130 will respond to the electron pulse resulting from reflection of laser light from the object of interest in the field of view of the device 10, rather than I5 to any back scatter of laser light from surfaces of lenses in the device 10.
Fourth, shortly after the time the LRF cont~~ol logic commands the Laser I 10 to fire a pulse of laser light into the scene which was being viewed by the user of the device 10, this pulse will actually be fired. A time-zero (to) detector I26 detects the moment of actual firing of this laser light pulse, and provides a signal on conductor 20 128 which starts the high-speed digital timer 130.. Prior to the moment of firing of this laser light pulse, the photocathode is connected to voltage source 70b (i.e.' to the +30 volts relative source) for a purpose to be further explained below.
Fifth, when the laser light reflects from an object in the scene, returning laser light passes through a central aperture 120a of spatial filter 120, so that reflections of 25 laser light from other objects in the scene are lblocked (i.e.' having the effect of increasing the signal to noise ratio of the returning light pulse).
During day time LRF operations an optical filter 144 may also be used along with spatial filter 120 and has the beneficial effect of improving signal-to-noise level This is the case because the spectral filter removes some of the background light from the 30 day-time scene which is present at frequencies close to that of the laser I10. The WO 99/60787 PCTNS99/11093 _.
operator of the device 10 may select to include optical filter 144 along with spatial filter 120 by manipulation of a control 144x The reflected laser light (still in the form of a pulse) passing to image intensifier tube 14 causing a pulse of photoelectrons to be released by photocathode 20, as is graphically depicted on Figure 1 and indicated with the character "P1". The pulse Pl of photoelectrons passes to MCP 22, and causes a corresponding pulse of secondary-emission electrons "P2" (produced under "high gain" conditions for the microchannel plate 22), which electrons pass to the output electrode assembly 24. A
corresponding pulse in the current from screen 26 is detected by amplifier circuit 66b because of its inductive relationship with the lead 74a, and the preamplifier then provides an amplified output signal. This amplifiied output signal is provided via a conductor 132, which preferably is a shielded conductor including a shield electrode 132a, to provide a timer-stop command to the high.-speed timer 130. Also, if desired, another level of amplification (indicated on Figure 3 by numeral 132b and a dashed line amplif er symbol) may be interposed in tlhe electrical connection provided between the pre-amplif er circuit 66b and the high speed timer 130.
Next, spatial filter 120 is withdrawn from the optical pathway, the oscillator 80 is restarted, and the gating operation of the switching network 76 is resumed (if it was operating before the LRF operation as a result of the light conditions in the field being viewed. In other words, the explanation below concerning daytime operations of the device 10 may be consulted at this time. The image of the scene being viewed is thus restored for the user of the device 10. During the LRF operation, the operator of the device 10 may detect a flicker in the viewed image along with a very brief flash of Iight (i.e., from the pulse of electrons P2 impacting the screen 26). The LRF
operation takes only about 5ms to complete (although the physical movements of filter 120 will be somewhat slower than this) so the; user's view of the scene in not significantly interrupted. The time interval betwE:en the to signal and the timer-stop command is provided by the timer 130 to a range calculator 134, which then supplies an output (indicated with arrowed numeral 136) of range information to the object for the operator of the device 10.

WO 99/bU787 PCT/US99111093 It will be noted that prior to the firing of the: Laser light pulse, the photocathode is connected to voltage source 70b, which is abou~~t +30 volts positive relative to the face 28 of microchannel plate 22. This positive voltage level on the photocathode 20 has the effect of a "hard turn ofd' on the photocalhode, preparing it to be somewhat insensitive to photons of laser Light which may be back scattered from surfaces of the lenses between laser 110 and the projection outvnardly of the beam 110a. That is, laser light may be reflected within the device 10 during the firing of this laser light pulse, but the image intensifier tube is momentarily somewhat blinded to this Light after the hard turn off effected on photocathode 20, even though voltage source 70a is connected before the actual moment of firing of this laser light pulse in order to provide charge settling on the photocathode.
DAYTIME IMAGING AND LRF OPERATION
It will be noted that far daytime operation o~f the device 10, the BSP
function is disabled, and the ABC function of the device 10 allows imaging to be accomplished in daylight. Accordingly, the ABC function may be operating the photocathode at less than 100% duty cycle. Under these conditions, a LRF operation additionally momentarily interrupts the duty cycle gating operation carried out by switching network 76, and effects the switching of the photocathode 20 to the voltages provided by sources 70b and 70a (in sequence as described above) in order to effect the hard turn off of the photocathode during laser firing, anal then to allow the photocathode to be highly responsive to photons of reflected laser Light in order to provide the LRF
pulses Pl, as described above.
Figure 3a provides a fragmentary view of an alternative embodiment of the present invention. In order to obtain reference numerals for use in describing this alternative embodiment, features which are the same as, or which are analogous in structure or function to, featured depicted and described above are indicated on Figure 3a using the same numeral used above, and with a prime (') added. Viewing Figure 3a, it is seen that the image intensifier tube 14' also has a current transformer 66a and a pre-amplifier circuit 66b which are also carried on the housing SO' within the annular circuit portion 62a'. However, in this em,bodirnent, the current transformer 66a is electromagnetically (i.e., inductively) associated with the lead 72b.
This preamplifier circuit 66b' similarly responds to the current pulse produced by electron pulse P2, recalling Figure 1, to provide an output signal via a shielded conductor 132' extending to the timer 126 (recalling Figure 3). The pre-amplifier circuit 66b' is powered from power supply 96 via transformer 98, as was explained above Those skilled in the art will appreciate that the embodiment of the present invention depicted and described herein and above is not exhaustive of the invention.
Those skilled in the art will further appreciate that the present invention may be embodied in other specific forms without departing from the spirit or central attributes of the invention. For example, it is clear from the description above that a viewing device using an image intensifier tube may also perform laser range finding functions using the image intensifier tube as a sensor for the; reflected laser light pulse without using the "hard turn off' technique described herein. Such a device would project the laser light pulse for laser range finding using a separate projection optical system. The image intensifier tube would still be used as a sensor by insuring that the photo cathode and microchannel plate of the tube are i.n high gain conditions during the interval in which the laser light pulse returns. In this way, the electrical response of the image intensifier tube can be used to initiate the "timer stop" command necessary for measuring the transit time for the laser light pulse to and from the scene and object of to which a range is desired.
However, in view of the above it will also be apparent that the present invention provides a night vision device with a laser range finder having an improved ratio of signal to noise in a laser range finder signal. This is the case in part because the pre-amplifier 62 is located within the image intensifier tube 14, close to the source of the LRF return signal, and amplifies this signal before any ambient or environmental influences can appear as noise in tine signal. Further, the shielding of the amplified signal by shield 132a of conductor 132 assists in seeing that a "clean"
signal of low noise content is supplied to timer 130. Thus, the present night vision device with laser range finder can provide a finer degree of range resolution than was previously possible by such devices using a low power laser (as is the present case).
Because the foregoing description of the present invention discloses only an exemplary embodiment, it is to be understood that other variations are recognized as being within the scope of the present invention. Accordingly, the present invention is not limited to the particular embodiment which has been depicted and described in detail herein. Rather, reference should be made to the appended claims to define the scope and content of the present invention.

Claims

The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:

1. A range finder apparatus, said range finder apparatus being usable in conjunction with a source of energy providing an energy pulse projecting toward an object the range to which is to be determined so that a portion of the energy pulse reflects from the object back to the apparatus, said apparatus comprising:

an image intensifier tube receiving energy reflected from the object and responsively providing an electrical output;

a detection circuit receiving said electrical output and responsively providing a timer-stop signal upon detection of a phase change in a magnetic circuit, said detection circuit including an oscillator driving oscillation in the magnetic circuit, and means for detecting the phase change in said magnetic circuit;

a timer device for measuring a time interval from projection of said energy pulse until provision of said timer-stop signal; and .
a calculator determining the range from the apparatus to the object using said time interval and the speed of said energy pulse as a measuring standard.

2. The range finder apparatus of claim 1 wherein said source of energy includes a laser, and said energy pulse includes a pulse of laser light.

3. The range finder apparatus of claim 1 wherein said timer circuit includes a detector responding to projection of said energy pulse to provide a timer-start signal, and a timer responding to said timer start signal to begin timing said time interval.

4. A laser range finder apparatus, said apparatus comprising:
a laser light source projecting a pulse of laser light toward an object the range to which is to be determined so that a portion of the projected laser light illuminates the object and is reflected back toward the apparatus;
an image intensifier tube receiving reflected laser light and responsively providing an electrical output;

a detection circuit receiving said electrical output and responsively providing a timer-stop signal upon detection of a phase change in a magnetic circuit, said detection circuit including an oscillator driving oscillation in the magnetic circuit, and means for detecting the phase change in said magnetic circuit;

a timer device for measuring a time interval from projection of said pulse of laser light until provision of said timer-stop signal; and a calculator determining the range from the apparatus to the object using said time interval and the speed of light as a measuring standard.

5. The laser range finder of claim 4 further including a phase detector responding to said change in oscillation phase to provide said timer-stop signal.

6. The laser range finder of claim 4 wherein said image intensifier tube includes a photocathode, a microchannel plate, and a screen electrode, said screen electrode providing said electrical output in response to receipt by said image intensifier tube of reflected laser light.

7. A night vision device comprising:
an objective lens receiving light from a scene;
an image intensifier tube receiving light from the scene via the objective lens and responsively providing a visible image of the scene, an eyepiece lens providing the visible image to a user of the night vision device;
a laser projecting a pulse of laser light into the scene, a portion of this pulse of laser light reflecting from an object in the scene to provide a reflected laser light pulse;
circuit means causing said image intensifier tube to provide an electrical output in response to receipt of said reflected laser light pulse and responsively providing a timer-stop signal upon detection of a phase change in a magnetic circuit, said circuit means including an oscillator driving oscillation in the magnetic circuit, and means for detecting the phase change in said magnetic circuit;
a timer measuring an interval from the time of projection of said pulse of laser light until the time of provision of said electrical output by said image intensifier tube;
a calculator determining range information indicative of the distance from the night vision device to the object using said time interval and the speed of light as a measuring standard; and means for providing said range information to a user of the device.

8. An integrated night vision device and laser range finder apparatus, said apparatus including an image intensifier tube and providing in one mode of operation a visible image of a scene, and another mode of operation providing range information indicative of distance from the apparatus to a selected object in the scene, said apparatus comprising:
an image tube power supply section, said image tube power supply section providing respective operating voltage levels for each of: a photocathode, to respective first and a second facial electrodes of a microchannel plate, and to an output electrode of the image intensifier tube;
an operator-input device for receiving an LRF operator input command selecting laser range finding mode of operation;

a laser in response to said LRF command providing a laser light pulse projecting into the scene to illuminate the selected object;
a time-zero detector responsive to projection of said laser light pulse to provide a time-zero output signal;
an interval timer starting in response to the time-zero output signal;
a laser range finding control logic unit for providing operating control commands to said image tube power supply section to in response to a LRF command momentarily suspend imaging operation, and charging the microchannel plate of said image intensifier tube to a high-gain voltage differential between said first and second facial electrodes;
an electrical connection to said output electrode to detect an impulse current indicative of reflected laser light returning to said image intensifier tube from an object in the scene, said electrical connection providing said impulse current to a magnetic circuit;
means for detecting application of said impulse current to said magnetic circuit and responsively providing a timer-stop signal measuring a time interval upon detection of a phase change in a magnetic circuit; and a calculator using said time interval and the speed of light as a measuring standard to determine range from said apparatus to the selected object.

9. A combined night vision and laser range finder device, said device comprising:
an objective lens through which light from a scene being viewed is received, said objective lens directing light from the scene to an image intensifier tube providing a visible image of the scene and an electrical output in response to receipt of reflected laser light;
a laser light source projecting a pulse of laser light outwardly through said objective lens in to the scene being viewed;
said image intensifier tube receiving reflected laser light from the object and responsively providing an electrical output; and means for measuring a time interval from projection of said pulse of laser light until provision of said electrical output by said image intensifier tube, said time interval measuring means including a magnetic circuit, means for driving oscillation in said magnetic circuit, means for applying said electrical output to said magnetic circuit to effect an oscillation change therein, and means for detecting said oscillation change;
means for calculating the range from the device to the object using said time interval and the speed of light as a measuring standard.

10. A method of operating a night vision device in order to provide both a visible image and range finding, said method comprising steps of;
providing the device with an image intensifier tube, and directing light from a scene to the image intensifier tube;
causing the image intensifier tube to responsively provide a visible image;

projecting a pulse of light into the scene, and causing a portion of this pulse of light to be reflected from an object in the scene to the image intensifier tube;
in response to the reflected portion of the pulse of light causing said image intensifier tube to provide an electrical response;
providing a magnetic circuit, and driving oscillation therein; applying said electrical response to said magnetic circuit to effect a change in said oscillation;
detecting said change in oscillation of said magnetic circuit; and measuring a time interval between projection of said pulse of fight and detection of said change in oscillation of said magnetic circuit, and responsively providing range information indicative of a range from the device to the object using said time interval and the speed of light as a measuring standard.

11. A method of using an image intensifier tube to measure a range to an object, said method comprising steps of;
projecting a pulse of light to the object and causing a portion of this pulse of light to be reflected from the object to the image intensifier tube;
utilizing said image intensifier tube to provide an electrical response to receipt of the reflected light;
providing an oscillating magnetic circuit receiving said electrical response to provide a timer-stop signal in response to said electrical response;
measuring a time interval from projection of said pulse of light until provision of said timer-stop signal; and from said time interval determining the range to the object using the speed of light as a measuring standard.

12. The method of claim 11 further including the steps of preparing said image intensifier tube to provide the electrical output signal by applying a determined high-gain voltage across a microchannel plate of the image intensifier tube preparatory to provision of said electrical response.

13. The method of claim 11 further including the steps of preparing said image intensifier tube to provide the electrical output by first applying a relative positive voltage to a photocathode of the image intensifier tube during projection of said pulse of light, and thereafter applying a constant negative voltage to the photocathode during receipt of reflected light at the image intensifier tube.

14. A method of determining a range from a location to an object comprising steps of;
projecting a pulse of light from the location to the object via an objective lens and causing a portion of this pulse of light to be reflected from the object back to the location and through the objective lens;

providing an image intensifier tube at the location;
utilizing said image intensifier tube both to provide a visible image from light received via said objective lens and to provide an electrical response to receipt of the reflected light pulse portion;
electrically connecting said image intensifier tube with a magnetic circuit having an oscillator so as to apply said electrical response thereto to modify oscillation of said magnetic circuit;
measuring a time interval from projection of said pulse of light until said modification of oscillation in said magnetic circuit; and from said time interval determining the range from the location to the object using the speed of light as a measuring standard.