EP3870927A1 - Arme à énergie dirigée et procédé de représentation de la position d'un point d'impact de l'arme à énergie dirigée - Google Patents

Arme à énergie dirigée et procédé de représentation de la position d'un point d'impact de l'arme à énergie dirigée

Info

Publication number
EP3870927A1
EP3870927A1 EP19794537.1A EP19794537A EP3870927A1 EP 3870927 A1 EP3870927 A1 EP 3870927A1 EP 19794537 A EP19794537 A EP 19794537A EP 3870927 A1 EP3870927 A1 EP 3870927A1
Authority
EP
European Patent Office
Prior art keywords
weapon
radiation
optics
active
camera
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.)
Pending
Application number
EP19794537.1A
Other languages
German (de)
English (en)
Inventor
Klaus Ludewigt
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Rheinmetall Waffe Munition GmbH
Original Assignee
Rheinmetall Waffe Munition GmbH
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 Rheinmetall Waffe Munition GmbH filed Critical Rheinmetall Waffe Munition GmbH
Publication of EP3870927A1 publication Critical patent/EP3870927A1/fr
Pending legal-status Critical Current

Links

Classifications

    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41—WEAPONS
    • F41H—ARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H13/00—Means of attack or defence not otherwise provided for
    • F41H13/0043—Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target
    • F41H13/005—Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target the high-energy beam being a laser beam
    • F41H13/0062—Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target the high-energy beam being a laser beam causing structural damage to the target
    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41—WEAPONS
    • F41G—WEAPON SIGHTS; AIMING
    • F41G3/00—Aiming or laying means
    • F41G3/14—Indirect aiming means
    • F41G3/16—Sighting devices adapted for indirect laying of fire
    • F41G3/165—Sighting devices adapted for indirect laying of fire using a TV-monitor
    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41—WEAPONS
    • F41G—WEAPON SIGHTS; AIMING
    • F41G3/00—Aiming or laying means
    • F41G3/32—Devices for testing or checking
    • F41G3/323—Devices for testing or checking for checking the angle between the muzzle axis of the gun and a reference axis, e.g. the axis of the associated sighting device
    • F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41—WEAPONS
    • F41H—ARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H13/00—Means of attack or defence not otherwise provided for
    • F41H13/0043—Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target
    • F41H13/005—Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target the high-energy beam being a laser beam

Definitions

  • the present invention relates to a method for
  • Such a method and such a radiation weapon are known per se.
  • the known method relates to a beam weapon which has an active beam optics and an imaging optics.
  • the active beam optics are used to focus and align primary radiation from the beam weapon is emitted in the form of an active beam or an auxiliary beam. Radiation emanating from an object irradiated with the active beam or auxiliary beam is detected by the imaging optics and directed at a camera on a screen that has a target point marking.
  • the imaging optics is an example of a target optic that is used for the optical representation of a target area.
  • Another example of such target optics is a
  • the target point of the weapon is usually marked by a crosshair in the optics of the telescopic sight or on a screen of the camera.
  • the target point marked as a crosshair indicates a target meeting point located in the target area when the target area is viewed through the telescopic sight or the target area shown on a screen.
  • the procedure for displaying an actual meeting point is also called
  • the weapon When carrying out a shot, the weapon is first aligned so that the crosshair of the
  • Target optics or the target point, matches the target meeting point. Then the shot is released. The
  • Accuracy of the weapon depends on how well the crosshair, or the target meeting point / target point, matches the actual target point of the weapon that was hit during a shot.
  • a good correspondence between the target point and the actual meeting point is of great importance, especially for radiation weapons, since radiation weapons generally have a very high level of precision.
  • this precision can only be used if the crosshairs of the target optics or the target point correspond to the precision of the beam weapon
  • An adjustment of the imaging optics that leads to the desired match requires a determination of the actual meeting point.
  • Such an actual meeting point is, for example, when a weapon is first assembled, after parts of the weapon have been replaced, or after the body has been misaligned due to environmental influences such as temperature and pressure fluctuations, vibrations, shock waves, etc.
  • the position of the actual meeting point is determined relative to the target meeting point with the aid of sharp shots of the weapon at a test target, on which the actual meeting point is represented, for example, as a bullet hole.
  • the resulting bullet is then sighted with the target optics of the weapon and the crosshairs of the
  • the aiming optics are set to the actual meeting point, which presents itself as a bullet hole, with the weapon still facing the same way. This procedure is used to increase the
  • Target distances can be a repetition of this procedure
  • High-power laser beam which is aimed at a test target and e.g. a branding in the material of the
  • Radiation weapon e.g. the cross point of a crosshair of an imaging optics
  • Radiation weapon is adjusted with the weapon orientation unchanged so that the target point at the
  • Radiation weapon triggered as active beam or auxiliary beam Radiation weapon triggered as active beam or auxiliary beam.
  • Object emits radiation which is used in the following
  • radiation Differentiation from the output radiation referred to as primary radiation of the radiation weapon is only referred to as radiation.
  • This radiation is, for example, a wide spectrum of visible light and / or
  • Irradiation is emitted with the primary radiation, but can also be reflected daylight, for example.
  • This radiation is captured by the imaging optics and directed at a camera on a screen.
  • the Burn-in point is shown on the screen as the actual meeting point.
  • the screen has one
  • Target point marking in the form of a crosshair so that the location of the meeting point is relative to the
  • Target mark is legible.
  • the method may be used in the area of application of the weapon. is not feasible if it is not a restricted area. Then e.g. after a
  • the object of the present invention is to provide a method and one
  • Auxiliary beam is captured by the imaging optics and aimed at a spot on the camera. This spot is shown on the screen as the determined actual meeting point.
  • the characterizing features of claim 2 correspond to these process features
  • Device features of the radiation weapon.
  • the housing When the method is carried out, the housing is closed in a light-tight manner. This ensures that no laser radiation can escape when the method is carried out, so that no safety measures are necessary.
  • the invention allows a determination and representation of the target point of the beam weapon without this
  • the determination and Representation of the target point can be carried out at any time with high accuracy, little time and without safety precautions relating to the environment of the radiation weapon, such as barriers, for example. Another advantage is that the target point of the beam weapon can be determined and displayed even when the beam weapon is in motion
  • a preferred embodiment of the beam weapon is characterized in that it has a primary radiation source and at least one radiation-guiding solid body having a first end and a second end, and a wavelength or beam splitter which has a
  • Active beam optics the first end being arranged relative to the primary radiation source such that primary radiation emitted by the primary radiation source can be coupled into the solid body via the first end and can be coupled out of the solid body via the second end, and that the wavelength or beam splitter in a beam path of the decouplable primary radiation is arranged such that it can be illuminated with the decouplable primary radiation.
  • the method also works without any such solid when the laser beam is introduced into the optics as a free beam (adjustment to the optical axis of the optics). As a rule, the laser beam is then emitted as a collimated beam parallel light coupled into the optics. Coupling a divergent beam is also conceivable. Coupling in as a free jet has advantages at very high powers, since the powers that can be transmitted with fibers known today are capped.
  • optical elements that lie between the wavelengths or beam splitter and the active beam outlet opening of the beam weapon.
  • optical elements have a common optical axis.
  • the common optical elements ensure that the target plane is sharp on the camera and the screen
  • Another preferred embodiment of the beam weapon is characterized in that the further common optical elements include at least a first telescope optic and a second telescope optic.
  • the optical auxiliary element is a flat mirror, which is arranged perpendicular to the optical axis.
  • Auxiliary element has a retroreflector that does so is set up, incident primary radiation as reflected and in directions of the incident
  • a further preferred embodiment of the beam weapon is characterized in that the active beam optics and the imaging optics have, as a further common component, a deflection mirror which is arranged and aligned in such a way that it is incident primary radiation from the wavelength or beam splitter in the direction of
  • Active beam exit opening is reflected and reflected radiation from the direction of the optical auxiliary element is reflected to the wavelength or beam splitter.
  • the wavelength or beam splitter directs at least part of the reflected radiation incident from the deflection mirror onto at least one camera of the imaging optics.
  • the imaging optics have a first camera and a second camera and a second
  • Has wavelength or beam splitter the incident from the first wavelength or beam splitter
  • a single camera is sufficient to carry out the method. As a rule, this will be a so-called fine tracking camera.
  • the images of this camera are evaluated by software with regard to the target position for the beam position (crosshair), the position is calculated, and a control signal for the deflecting mirror is output.
  • a second (or further) camera (s) can be used independently of the first camera.
  • the method then delivers the target point (crosshair) for this camera at the same time as the first camera.
  • the second camera uses a different wavelength so that the optical paths in the optics are separated by a wavelength splitter mirror.
  • the software evaluation does not allow the images to be used by the observer
  • the second camera can be used
  • the second wavelength may provide better images than others
  • a second camera can have a higher resolution, optics with higher magnification for better resolution or with lower magnification for a larger image field.
  • Deflecting mirror is manually or automatically adjustable.
  • an optical element (lens or spherical mirror) between the wavelength or Beam splitter and a deflecting mirror is arranged and that another optical element (lens or spherical mirror) between the deflecting mirror and the second
  • Wavelength or beam splitter is arranged and that a second deflecting mirror between the second
  • Wavelength or beam splitter and the first camera is arranged.
  • imaging optics and the active beam optics are arranged in a housing which permits radiation to exit the housing and radiation to enter the housing
  • Active beam outlet opening is attachable.
  • a further preferred embodiment of the beam weapon is characterized in that the optical auxiliary element is fastened captively and can be folded away by means of a joint, the optical auxiliary element being in a first
  • Folding position leaves the active beam outlet opening and in a second folding position
  • the active beam outlet opening closes.
  • Figure 1 is a simplified representation of a radiation weapon as a technical environment of the invention with outgoing radiation;
  • FIG 2 shows the beam weapon from Figure 1 with more detail
  • Figure 3 shows an embodiment of an inventive
  • FIG. 4 shows a flow chart as an exemplary embodiment of a method according to the invention.
  • Figure 5 shows another embodiment of a
  • Figure 1 shows a simplified
  • the beam weapon 10 has a primary radiation source 12 and at least one having a first end 14 and a second end 16 radiation-conducting solid 18 and a first
  • Wavelength or beam splitter 20 The
  • Primary radiation source 12 preferably has one or more lasers.
  • the radiation-conducting solid 18 is, for example, a glass fiber or a glass fiber bundle.
  • the beam weapon 10 has an active beam optics 22 and an imaging optics 24 and is set up to represent the position of a meeting point 26 of the beam weapon 10.
  • the active beam optics 22 is set up to radiate primary radiation of the active beam 28 or auxiliary beam
  • Focus and align the beam weapon 10 in a target plane 30 takes place, for example, by means of a movable deflecting mirror 32.
  • the imaging optics 24 are set up to detect radiation emanating from an object irradiated with the active beam 28 or the auxiliary beam and to point it at a camera 34 of a screen 38 having a target point marking 36.
  • the beam weapon 10 has a screen 38. A is preferred
  • enlarged, high-resolution image 40 of the meeting point 26 is generated on the camera 34 and the screen 38.
  • Imaging optics 24 have in addition to the camera 34 and the
  • the first wavelength or beam splitter 20 is a common component of the imaging optics 24 and the active beam optics 22.
  • the wavelength or beam splitter 20 is based, for example, on an inversion of a wavelength coupling.
  • Reverse wavelength couplers are known.
  • Known wavelength splitters have a special mirror layer that has been evaporated onto a glass substrate. This layer reflects light with wavelengths from a certain wavelength range and transmits light with wavelengths from another wavelength range. Such mirrors are known to the person skilled in the art and are commercial
  • the wavelength or beam splitter 20 reflects the wavelength of the active laser and transmits the wavelength of the illumination laser (auxiliary laser).
  • the illumination laser is an independent laser that is also moved so that it illuminates the target area with the target over a large area (like a spotlight). Alternatively, you can work without an illumination laser and at any wavelength for the camera image if there is enough daylight.
  • the camera could also be a thermal camera and one works with heat radiation in the near or far infrared.
  • the camera image in a wavelength range in which the active laser wavelength is also located.
  • the element 20 is then not a wavelength splitter but a beam splitter. This means that the element 20 reflects very light (99%) (namely the laser) and only lets a small part (1%) through to the camera.
  • wavelength splitters operating according to other principles can also be used.
  • the first end 14 of the radiation-conducting solid 18 is arranged relative to the primary radiation source 12 in such a way that the primary radiation source 12 emits
  • Primary radiation can be coupled into the solid 18 via the first end 14, and the second end 16 is arranged relative to the first wavelength or beam splitter 20 such that primary radiation propagating in the solid 18 can be coupled out of the solid 18 via the second end 16 and that the first wavelength or beam splitter 20 can be illuminated with the primary radiation that can be coupled out.
  • the collimation optics 42 is an optical element of the active beam optics 22, which is not also for
  • Imaging optics 24 belongs.
  • the imaging optics 24 and the active beam optics 22 are arranged in a housing 50.
  • the housing 50 has an active beam outlet opening 44, which allows radiation to exit from the housing 50 and to enter
  • the active beam optics 22 and the imaging optics 24 have further common optical elements on, which lie between the first wavelength or beam splitter 20 and the active beam outlet opening 44.
  • the further common optical elements are at least a first telescope optics 46 and a second telescope optics 48.
  • the common optical elements have one
  • common optical axis 51 Due to their common optical axis 51, the common optical elements ensure that the target plane 30 (laser focus plane) is imaged sharply on the camera 34.
  • Test target 52 which is at a large distance, e.g. at a distance of several hundred meters or a few kilometers from the radiation weapon 10.
  • FIG. 1 shows a beam weapon 10 with an active beam 28 or auxiliary beam, which is aimed at a distant test target 52 and generates a penetration point there.
  • This burn-in which marks the actual meeting point 26, is recorded by the camera 34 of the imaging optics 24 and displayed on the screen 38 as an image 40 of the meeting point 26.
  • FIG. 2 shows the beam weapon from FIG. 1 with a beam path of radiation 54, which emanates from the test target 52 in the direction opposite to the direction of the active beam 28 and through the active beam outlet opening 44 of the beam weapon 10 into the imaging optics 24 of FIG
  • This radiation 54 is, for example, visible light or Infrared radiation. This radiation can occur as a result of irradiation with the primary radiation, but it can also be emitted independently of the primary radiation, for example as temperature radiation or
  • FIG. 1 shows that the second end 16 of the
  • the radiation-conducting solid body which to a certain extent represents the source of the primary radiation for the radiation weapon 10, is imaged by a first image in the target plane 30.
  • the first illustration is by the
  • Active beam 28 mediates.
  • the image lying in the target plane 30 corresponds to the meeting point 26 on the test target 52.
  • FIG. 2 shows the same structure as FIG. 1 with a beam path in the opposite direction.
  • Figure 2 thus illustrates that this meeting point 26 in a second optical image through the imaging optics 24 sharp on the
  • Camera 34 is imaged and is shown as image 40 of the meeting point 26 on the screen 38. This double optical image can be seen as indirect
  • Illustration of the second end 16 of the radiation-conducting solid 18 can be considered.
  • FIG. 3 shows an exemplary embodiment of a beam weapon 10.
  • This beam weapon 10 has all the elements of the beam weapon 10 explained with reference to FIGS. 1 and 2 and differs from it by one
  • optical auxiliary element 56 is distinguished by the fact that its shape, dimensions and arrangement enable it to cover a beam cross-section of an active beam 28 or auxiliary beam emerging from the beam weapon 10 and primary radiation directed out of the beam weapon 10 into the imaging optics 24 of the beam weapon 10 to reflect.
  • the imaging optics 24 are set up to detect primary radiation from the reflecting optical auxiliary element 56
  • Detect active beam 28 or the auxiliary beam direct it as an image of the second end 16 onto the camera 34 and display this image as a meeting point 40 on the screen 38.
  • the optical auxiliary element 56 is a flat mirror 58, which is arranged perpendicular to the optical axis 51. To do this, the mirror must reflect the beam exactly in itself. For that, the mirror in the
  • the retroreflector reflects the beam in itself without angular adjustment.
  • a retroreflector is a device that largely detects incident electromagnetic radiation regardless of its direction of incidence and the direction of incidence
  • Alignment of the retroreflector is reflected in the direction from which the radiation is incident.
  • An incident beam is reflected laterally offset by 180 °.
  • Such a retroreflector 60 is therefore set up to absorb incident primary radiation reflected and reflected in directions opposite to directions of the incident primary radiation.
  • the retroreflector can have a much smaller diameter than the beam diameter.
  • the retroreflector does not necessarily have to be positioned in the center of the beam; a small retroreflector in the outer beam area is also possible.
  • Figure 3 shows a large retroreflector (area corresponds to the inside width of the housing opening), which is centered on the beam. This solution may provide the greatest accuracy. It also works with a small retroreflector that is not centered. For example, it is sufficient to stick a small retroreflector on the inside of the lid. For the process, the lid was then closed light-tight. Since there are no angles or position requirements for the retroreflector, the process can be carried out immediately without adjustments.
  • the optical auxiliary element 56 is preferably in the form of a cover which closes the active beam outlet opening 44 at an edge of the active beam outlet opening 44
  • this is optical
  • Auxiliary element 56 captively and hinged to the housing 50 by means of a joint 62.
  • the optical auxiliary element 56 leaves the active beam outlet opening 44 free in a first folding position, and closes the active beam outlet opening 44 in a second folding position.
  • the first folding position is represented in FIG. 3 by the broken line representation of the optical auxiliary element 56.
  • the second folding position is shown in Figure 3 by the solid representation of the optical
  • Auxiliary elements 56 represents.
  • the reflective side of the optical auxiliary element 56 is arranged on the side of the optical auxiliary element 56 which, in the closed state, faces the interior of the housing 50.
  • the closure is preferably constructed in such a way that the housing is closed in a light-tight manner when the method is carried out.
  • the closure of a cover closing the housing is preferably monitored in a safety-relevant manner. It is thereby achieved that no laser radiation can escape when the method is carried out, so that none
  • FIG. 3 shows a direct optical image of the beam exit of the second end 16 (or the beam exit of an auxiliary beam that is collinear with the active beam) Camera 34.
  • the optical auxiliary element 56 is for this purpose directly in front of the
  • Active beam exit opening 44 active beam 28 exiting along the optical axis 51 into the common part of the imaging optics 24 and the active beam optics 22.
  • the direction of the rays incident on the optical auxiliary element 56 is reversed upon reflection on the optical auxiliary element 56, so that the reflected radiation in the imaging optics 24 propagates to the camera 34 as if this radiation originated from a distant test target that is in a remote test target side
  • Focus of the active beam 28 is located.
  • the direct imaging takes place in such a way that the direct optical image of the beam exit of the active beam or auxiliary beam (ie of the second end 16) corresponds to the image of the
  • Impact point 26 of the active beam 28 corresponds to a distant test target 52.
  • the image of the second end 16 thus generated can therefore be used to determine and display the actual meeting point.
  • This optical method can be carried out in such a way that the active beam 28 does not leave the housing 50, so that no test station is required for execution and no safety precautions need to be taken.
  • the active beam of one or more lasers is guided to the active beam optics with a glass fiber or a bundle of glass fibers.
  • the optical image is synonymous with the
  • a laser beam of a different wavelength can also be used for direct imaging on the camera.
  • the laser beam source for optics is made without fiber.
  • the laser beam is then introduced into the optics as a free beam.
  • the adjustment is then made to the optical axis of the optics.
  • the laser beam is then coupled into the optics as a collimated beam of parallel light. Then that is not applicable
  • Collimation optics (42).
  • the coupling of a divergent beam is also conceivable.
  • FIG. 4 shows a flow diagram as an exemplary embodiment of a method according to the invention for representing the position of a meeting point of a beam weapon 10 having an active beam optics 22 and an imaging optics 24.
  • Beam cross section of an active beam 28 or auxiliary beam emerging from the beam weapon 10 is covered with an optical auxiliary element 56 reflecting the incident active beam 28 or auxiliary beam.
  • a second step 102 the active beam 28 or the auxiliary beam is triggered when the beam is covered
  • the outgoing radiation is captured by the imaging optics 24 and directed onto a camera 34 of a screen 38 which has a target point marking 36.
  • the irradiated object is a distant test target 26.
  • the object is the optical one
  • a fourth step 106 the radiation spot generated by the camera 34 is displayed on the screen 38 as the actual meeting point 40.
  • the active beam optics 22 and the imaging optics 24 have the deflection mirror 32 as a common component, which is arranged and aligned such that it is from the first Wavelength or beam splitter 20 incident here
  • Wavelength or beam splitter 20 reflected.
  • the first wavelength or beam splitter 20 directs at least a portion of those from the deflecting mirror 32
  • the imaging optics have a first camera 34 and a second camera 34 ′ and a second wavelength or beam splitter 64, which separates reflected radiation incident from the first wavelength or beam splitter 20 into a reflected portion and a transmitted portion.
  • the first camera 34 is arranged so that it can be illuminated with the reflected portion, and the second camera 34 'is arranged so that it can be illuminated with the transmitted portion.
  • the orientation of the deflection mirror 32 is in one
  • An optical element 66 is between the first wavelength or beam splitter 20 and a deflection mirror 68
  • optical element 70 is arranged between the deflection mirror 68 and the second wavelength or beam splitter 64.
  • a second deflecting mirror 72 is arranged between the second wavelength or beam splitter 64 and the first camera.
  • the optical elements can each be implemented as a lens or as a spherical mirror.
  • the telescope optics, collimation optics and imaging optics can also each be implemented as lenses or spherical mirrors.

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optical Radar Systems And Details Thereof (AREA)
  • Aiming, Guidance, Guns With A Light Source, Armor, Camouflage, And Targets (AREA)

Abstract

L'invention concerne un procédé de représentation de la position d'un point d'impact (26) d'une arme à énergie dirigée (10), qui comporte une optique (22) de rayon actif et une optique de reproduction (24). Le procédé consiste à déclencher une émission d'un rayonnement primaire à concentrer par l'optique (22) de rayon actif et à diriger de l'arme à énergie dirigée (10) en tant que rayon actif (28) et à détecter par l'optique de reproduction (24) un rayonnement partant d'un objet irradié et à le diriger sur une caméra (34) d'un écran (38). Le procédé est caractérisé en ce qu'une section transversale de faisceau de rayons d'un rayon actif (28) est recouvert d'un élément auxiliaire (56) optique réfléchissant, le déclenchement du rayon actif (28) ou du rayon auxiliaire est effectué lorsque la section transversale de faisceau de rayons est recouverte, et qu'un rayonnement primaire, réfléchi par l'élément auxiliaire (56) optique réfléchissant, du rayon actif (28) ou du rayon auxiliaire est détecté par l'optique de reproduction (24) et est dirigé sur une tache de la caméra (34), laquelle tache est représentée sur l'écran (38) comme un point d'impact (40). Une revendication indépendante concerne une arme à énergie dirigée (10).
EP19794537.1A 2018-10-26 2019-10-25 Arme à énergie dirigée et procédé de représentation de la position d'un point d'impact de l'arme à énergie dirigée Pending EP3870927A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE102018126833.5A DE102018126833A1 (de) 2018-10-26 2018-10-26 Strahlenwaffe und Verfahren zur Darstellung der Lage eines Treffpunkts der Strahlenwaffe
PCT/EP2019/079143 WO2020084107A1 (fr) 2018-10-26 2019-10-25 Arme à énergie dirigée et procédé de représentation de la position d'un point d'impact de l'arme à énergie dirigée

Publications (1)

Publication Number Publication Date
EP3870927A1 true EP3870927A1 (fr) 2021-09-01

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
EP19794537.1A Pending EP3870927A1 (fr) 2018-10-26 2019-10-25 Arme à énergie dirigée et procédé de représentation de la position d'un point d'impact de l'arme à énergie dirigée

Country Status (7)

Country Link
US (1) US11867482B2 (fr)
EP (1) EP3870927A1 (fr)
JP (1) JP7416777B2 (fr)
AU (1) AU2019366763A1 (fr)
DE (1) DE102018126833A1 (fr)
IL (1) IL282543A (fr)
WO (1) WO2020084107A1 (fr)

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US3752587A (en) * 1971-09-09 1973-08-14 Philco Ford Corp Apparatus for boresighting a laser beam emitter device
US4155096A (en) * 1977-03-22 1979-05-15 Martin Marietta Corporation Automatic laser boresighting
GB2165957B (en) * 1984-10-18 1988-05-25 Ferranti Plc Checking aiming apparatus alignment
US5410815A (en) * 1994-04-29 1995-05-02 Cubic Defense Systems, Inc. Automatic player identification small arms laser alignment system
JP4718832B2 (ja) 2004-12-28 2011-07-06 株式会社東芝 光伝送システムおよび光伝送方法
US8203109B2 (en) 2009-05-08 2012-06-19 Raytheon Company High energy laser beam director system and method
DE102011015779B4 (de) * 2011-04-01 2022-03-24 Mbda Deutschland Gmbh Strahler für gerichtete Energie
DE102012022039B4 (de) * 2012-11-09 2020-03-26 Mbda Deutschland Gmbh Modulare Laserbestrahlungseinheit
IL234036B (en) * 2014-08-10 2018-11-29 Rafael Advanced Defense Systems Ltd A directed energy based weapon
DE102015016274B4 (de) 2015-12-16 2023-10-19 Mbda Deutschland Gmbh Optisches System und Verfahren zum Justieren eines Signalstrahls

Also Published As

Publication number Publication date
US20220307803A1 (en) 2022-09-29
JP7416777B2 (ja) 2024-01-17
DE102018126833A1 (de) 2020-04-30
AU2019366763A1 (en) 2021-05-13
JP2022514174A (ja) 2022-02-10
US11867482B2 (en) 2024-01-09
WO2020084107A1 (fr) 2020-04-30
IL282543A (en) 2021-06-30

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