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NZ754419B2 - Weapons system having at least two hel effectors - Google Patents
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NZ754419B2 - Weapons system having at least two hel effectors - Google Patents

Weapons system having at least two hel effectors Download PDF

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Publication number
NZ754419B2
NZ754419B2 NZ754419A NZ75441918A NZ754419B2 NZ 754419 B2 NZ754419 B2 NZ 754419B2 NZ 754419 A NZ754419 A NZ 754419A NZ 75441918 A NZ75441918 A NZ 75441918A NZ 754419 B2 NZ754419 B2 NZ 754419B2
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NZ
New Zealand
Prior art keywords
switching unit
optical switching
hel
laser
optical
Prior art date
Application number
NZ754419A
Other versions
NZ754419A (en
Inventor
Markus Jung
Klaus Ludewigt
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
Priority claimed from DE102017104662.3A external-priority patent/DE102017104662B4/en
Application filed by Rheinmetall Waffe Munition Gmbh filed Critical Rheinmetall Waffe Munition Gmbh
Publication of NZ754419A publication Critical patent/NZ754419A/en
Publication of NZ754419B2 publication Critical patent/NZ754419B2/en

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Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41WEAPONS
    • F41HARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H13/00Means of attack or defence not otherwise provided for
    • F41H13/0043Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target
    • F41H13/005Directed 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
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F41WEAPONS
    • F41HARMOUR; ARMOURED TURRETS; ARMOURED OR ARMED VEHICLES; MEANS OF ATTACK OR DEFENCE, e.g. CAMOUFLAGE, IN GENERAL
    • F41H13/00Means of attack or defence not otherwise provided for
    • F41H13/0043Directed energy weapons, i.e. devices that direct a beam of high energy content toward a target for incapacitating or destroying the target
    • F41H13/005Directed 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
    • F41H13/0062Directed 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/02Constructional details
    • H01S3/04Arrangements for thermal management
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/08013Resonator comprising a fibre, e.g. for modifying dispersion or repetition rate
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/0912Electronics or drivers for the pump source, i.e. details of drivers or circuitry specific for laser pumping
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/094061Shared pump, i.e. pump light of a single pump source is used to pump plural gain media in parallel
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/091Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/0941Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/101Lasers provided with means to change the location from which, or the direction in which, laser radiation is emitted
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/23Arrangements of two or more lasers not provided for in groups H01S3/02 - H01S3/22, e.g. tandem arrangements of separate active media
    • H01S3/2308Amplifier arrangements, e.g. MOPA
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/23Arrangements of two or more lasers not provided for in groups H01S3/02 - H01S3/22, e.g. tandem arrangements of separate active media
    • H01S3/2383Parallel arrangements

Abstract

Conventional weapons systems using HEL effectors are often bulky and complex to integrate with conventional platforms. This invention relates to a weapons system with at least two HEL effectors, each with at least one beam guidance system, the at least two HEL effectors comprising at least one jointly useable power source comprising a light pump source, wherein the at least one laser source is connectable to each of the at least one beam guidance systems by means of at least one optical switching unit, wherein the at least one optical switching unit can adjust and/or vary the beam power of the laser light generated by the laser source, and wherein the at least one optical switching unit can divide the laser light between at least two outputs of the at least one optical switching unit at the same time. The present invention provides a weapons system optimised in terms of mass, space, and integration requirements, making it easier to set-up on a variety of different platforms. tly useable power source comprising a light pump source, wherein the at least one laser source is connectable to each of the at least one beam guidance systems by means of at least one optical switching unit, wherein the at least one optical switching unit can adjust and/or vary the beam power of the laser light generated by the laser source, and wherein the at least one optical switching unit can divide the laser light between at least two outputs of the at least one optical switching unit at the same time. The present invention provides a weapons system optimised in terms of mass, space, and integration requirements, making it easier to set-up on a variety of different platforms.

Description

WEAPONS SYSTEM HAVING AT LEAST TWO HEL EFFECTORS The invention concerns a weapons system consisting of at least two nergy laser (HEL) effectors (HEL = High Energy Laser). The invention ns the system structure of a weapons system with a plurality of, but at least two, HEL effectors on an object, in particular with regard to the aspects of system weight, volume, integration concept and installation effort.
Inter alia, HEL effectors are used to protect movable or stationary objects. A HEL effector is used to combat different targets. Multiple HEL effectors can be targeted at one target or multiple s at the same time. This can include static targets such as mines, IEDs (Improvised Explosive Devices), etc., but also dynamic targets, such as rockets, artillery shells or RAM projectiles, etc. These s are then shed and/or destroyed as part of the defense against the threat. Small targets (Low, Slow & Small = LSS targets) in ular can be more easily demolished or yed by such a weapons system. LSS targets also include socalled UAVs (Unmanned Air Vehicles), such as drones, which are often used improperly for transporting explosives.
Key components of a HEL effector include a laser source and a beam guidance system. The beam guidance system can house the sub-assemblies fine imaging system (FIS), fine tracking system (FTS), telescope and, if necessary, at least one adaptive optical system (AO). Well-known laser sources are gas lasers, such as C02 lasers, as well as solid state lasers, such as diode lasers, fiber lasers, etc.
Currently, fiber lasers, a special form of diode-pumped solid state laser, are red as laser sources for HEL effectors e of their advantages. The high- performance fiber laser includes one or more pump sources, such as one or more pump diodes. In the fiber laser, the pumping light is coupled into an active fiber and converted into laser light of very good beam quality.
High-performance fiber lasers are either constructed as pure oscillators (an active fiber with a resonator) or as multi-stage oscillator–amplifier systems so-called MOPA (MOPA = Master Oscillator and Power Amplifier). In a MOPA structure, the power of an oscillator is coupled into uent amplifier levels e fibers) and boosted to higher power. The laser light is then d via the beam guidance system to a target etc. to attack the target. All optical components are usually connected to optical fibers ve transport fibers). In addition, there are the power supply and cooling system, which supply and cool the pump source and the master oscillator power amplifier of the dual laser sources. The power supply and cooling system can be part of the laser source.
Due to non-linear processes that can occur in fibers at high power levels, the s of the ready-made fibers must be limited, for example between the MOPA or oscillator and the beam guidance system at high power levels in the multi-kW range. Depending on the power, fiber parameters, fiber structure, wavelength, etc., a maximum possible fiber length of a few meters can result.
The M2 beam y is also a decisive factor for the effect of HEL effectors. The beam quality value M2 should be as low as possible, preferably less than 2.
HEL effectors, like other weapons systems, can be supported on a fixed or movable platform. Weapons stations are also referred to as a platform. Said platforms, for their part, can be attached to stationary objects (e.g. houses, bunkers, containers, etc.) or moving objects (e.g. vehicles on land, in the air and at sea, containers, etc.). For larger objects, multiple platforms are often used. On a vehicle, ally on a maritime , such as a ship, the platforms are often disposed on the starboard and/or port side. Other platforms may additionally or atively be mounted on the bow and/or on the stern.
The advantage of a HEL effector over conventional effectors (conventional weapons) is, among other things, a high hit accuracy and a delay-free effect. There is no need to take any prediction into account. There are also no muzzle s and almost no firing signatures.
Similarly, there is no limit on the operational capability of the HEL effector due to a magazine capacity.
In order to achieve the required radiation quality of a HEL effector, the aim is also to accommodate the MOPA or the oscillator very close to the weapon station or platform.
The components of the HEL effector are housed in practice in a compartment (chamber). This leads to the restriction of deployment locations and the feasible maximum laser power. Such a restriction has a negative effect on maritime objects in particular.
A laser system for generating high or compact power densities on the object is known from DE 10 2010 051 097 A1. The power is divided between several lasers or laser s and geometrically mposed on the target, so that a total power density of all the individual power densities is achieved in total. As a weapon, the single lasers or laser weapons form a weapons system to combat an attacking object. Said laser weapons are aimed at the object by means of coarse tracking and fine ng. The laser weapons can be mounted on a moving or stationary platform. According to the document, such lasers can also be used as sing lasers for material processing, for example at greater distances.
A2 describes a laser or laser weapon in which a laser generation unit is positionally separated from a telescope that is to be directed at the target.
While the telescope, together with a target detection or tracking arrangement, is located on a mobile platform of a mobile vehicle, the laser generation unit is fixedly integrated within the mobile vehicle or a separate unit.
The functional connection between the ope and the laser tion unit is made by means of an optical fiber.
DE 33 18 686 A1 discloses a device for aiming a laser beam. This device is designed to be able to pivot a highenergy laser beam in a fixed parallel orientation with the orientation of other s on a platform. The laser source is disposed away from the platform. The laser beam is transmitted to optical elements via deflection mirrors.
DE 10 2012 015 074 B3 publishes a beam directing unit for a laser weapons , wherein the beam directing unit comprises a stationary/partly movable component and a fully movable component. A target acquisition or target tracking device as well as a telescope and an output stage t are attached to the fully movable part. The beam directing unit includes at least one laser generation unit, which comprises at least one seed laser unit and at least one pump laser unit. The seed laser unit as well as the pump laser unit are ted to the output stage element (e.g. an amplifier) using an optical fiber. In the case of several pump laser units, the individual laser powers are merged in a beam coupler and also fed to the output stage element via an optical fiber.
This ensures that the mass on the fully movable part can be reduced. The total weight on the object, on the other hand, does not change.
It is the object of the ion to optimize the system design in terms of the required mass, space requirements and integration effort when using two or more HEL effectors. It is an additional or alternative object of the invention to at least provide the public with a useful alternative.
The object is achieved by the features of claim 1.
Advantageous ments are revealed in the sub-claims.
In a first aspect of the invention, there is provided a weapons system comprising at least two HEL effectors, each with at least one beam guidance system, the at least two HEL effectors comprising at least one jointly useable power source comprising a light pump source, n the at least one laser source is connectable to each of the at least one beam ce systems by means of at least one optical switching unit, wherein the at least one optical switching unit can adjust and/or vary the beam power of the laser light generated by the laser source, and wherein the at least one optical switching unit can divide the laser light between at least two outputs of the at least one optical switching unit at the same time.
In a second aspect of the ion, there is provided an object comprising the weapons system as outlined above in relation to the first aspect.
The embodiments described herein are based on the idea of not assigning all the key components of a HEL or to every HEL effector. For example, not every HEL or should have its own complete laser source, or parts thereof. Rather, it is envisaged that this key component, or parts thereof, will be jointly usable by several HEL effectors. This key component, or parts thereof, is/are defined as a shared component. In an optimal implementation, a HEL effector only needs its own key component, namely at least one beam guidance system as an individual component. The individual beam guidance systems may house the sub-assemblies of fine imaging systems (FIS), fine tracking systems (FTS), telescopes and, if necessary, at least one adaptive optical system (AO). The jointly usable key component, or parts thereof, is/are in turn connected to the individual key component(s) of the HEL effector in such a way that the operation of at least one HEL effector is guaranteed.
The embodiments described herein therefore propose to use only one laser source or pump source for at least two HEL effectors in a weapons system with at least two HEL ors, which have at least one beam ce system.
The beam guidance s of the HEL effectors access the common laser source or pump source. An optical tion of the common laser source or pumped source to the beam guides, directly or indirectly, is made by at least one optical ing unit, so that at least one functional, complete HEL effector is provided in the threat response weapons system.
As a consequence of this idea, individual key ents, or parts thereof, can be saved in the case of a plurality of HEL effectors on an object. By saving individual key components, or parts f, the total weight, space requirement and integration effort of the HEL effectors on the object can be d.
This idea is based on the knowledge that the accuracy, precision and fast alignment of today's HEL effectors make it possible to combat a target or even multiple targets by a single HEL effector. There is no need for all the HEL effectors attached to the object to be functional at the same time.
In an embodiment, a plurality of HEL effectors, at least two, consist of a jointly usable key component, the laser source, and an individual key component, the dedicated beam ce system. The laser source includes at least one pump source with at least one pump diode, preferably a plurality of pump diodes, as well as at least one MOPA, alternatively at least one oscillator. A power supply and cooling system can also be ed to the laser .
The central laser source is the key component of all HEL effectors. The optical connections are realized using optical fibers or free space. The laser source, which can be used by several HEL effectors, can in turn be placed centrally on the object. It should be noted that a necessary beam quality is maintained during beam transport.
An optical connection of the central laser source to the individual beam guidance systems is carried out via at least one optical switching unit. The optical switching unit can be an optical switch or an optical switching point. An optical switching point is characterized in that it switches quickly, with angular precision and always reliably. The optical ing unit should also be designed to be able to divide the laser light between at least two outputs of the l switching unit, even at the same time. The distribution should be achievable continuously or in l stages. There are at least two stages to be provided, for example via end stops. The laser light should be able to be divided from 0 to 100%.
The single HEL effector thus consists in a first embodiment of a jointly usable laser source and at least one dedicated beam guidance system. This creates the ility that only the dual beam guidance system of the respective HEL effector needs to be supported on a platform as already defined. This le embodiment is not favored, but it is technically feasible.
In a further, preferred ment the entire laser source, i.e. with all components, such as pump source, MOPA or oscillator, is disposed centrally. It can be sufficient if only the pump source(s) of the laser source is/are centralized. In addition to the dedicated beam guidance system, a ted master oscillator + ier (MOPA) or oscillator is assigned to each HEL effector. Said MOPA or oscillator can then be disposed in the vicinity of, even in close proximity to, the respective platform, but can even be mounted on the respective platform. Each amplifier of the MOPA or oscillator can be optically connected to the pump source.
The master oscillator (MO) can be accommodated in the vicinity of the pump source or the amplifier depending on the length of the fiber. Other iers may also be integrated am of the individual beam guidance systems of the HEL effectors.
The optical switching unit, for its part, serves to apportion the pumping power of the pump source to at least two outputs of the optical switching unit. For a plurality of pump sources, these can also be distributed via the optical switching unit to at least two outputs of the optical switching unit. The outputs of the optical switching unit(s) for g power are in turn associated with at least one input of the iers (PA) of the HEL effectors, preferably by means of l fibers. The division of pumping power should be carried out uously or in multiple stages. In this case, at least two stages are to be provided, for example via end stops. The pump power should be able to be split from 0 to 100%. It is also provided that the division is possible at the same time for a plurality of outputs of the optical switching unit. A simultaneous division of pump power between the amplifiers (PA) of the HEL effectors allows several HEL effectors to be able to function at the same time.
Alternatively, each pump source can be fed to the dedicated optical ing unit thereof and apportioned thereby to at least two outputs. Furthermore, a cascaded arrangement of 2n outputs can be realized with the help of a plurality of optical switching units comprising at least two outputs.
In this embodiment, the individual HEL effector consists of a y usable central pump source, as well as at least one dedicated MOPA or at least one dedicated oscillator and at least one dedicated beam guidance system. The respective MOPA or oscillator of the HEL effectors can be accommodated near the beam guidance system of the HEL effector. A direct connection to the platform together with the beam guidance system is also conceivable.
The optical connection between the pump source and the amplifiers of the MOPA or the oscillators is preferably established via optical fibers. A free space version is also possible.
The l connection of the central pump source to the ators or the amplifiers of the MOPA is established here too via at least one optical switching unit. The optical switching unit can also be an l switch or an optical switching point. By means of the optical switching unit, a working line can result in this embodiment: pumping unit - fiber (optical path) al switching unit - fiber (optical path) - oscillator or amplifier. When using a plurality of oscillators, the outputs of the optical switching s) are connected to a pump input (active medium) of the ator, preferably by means of optical fibers. Even with a low beam quality of the pump diodes, despite the high power, an optical connection (fiber, free space) with a significantly greater distance than a few meters can be established between the at least one optical switch and the amplifiers or oscillators. However, variations that lack an optical path are also conceivable in this embodiment.
Another option is to provide a commonly usable master oscillator (MO) separately from the pump source instead of the many individual master oscillators. The optical connections between the pump source and the amplifiers of the HEL effectors are implemented ing to the above bed embodiment. The central master ator provided can be located near the pump source, which simplifies the power supply and cooling of the master oscillator. The output of the master oscillator can be switched to at least one input of the iers (PA) of the HEL effectors by means of at least one further optical switching unit.
Due to the low weight of the individual amplifier, it can be supported directly on the platform with the beam guidance system. This allows the good beam quality of the amplifier to be coupled into the beam guidance system at high power. ing on the output power of the master oscillator, different permissible fiber lengths result for the optical connection, e.g. optical fiber, between the master oscillator and the amplifiers.
The individual HEL effector ts in this third, also favored embodiment of a jointly usable central pump source, a shared master oscillator (MO), dedicated amplifiers (PA) as well as ted beam guidance systems.
An additional controller can also be used to determine which of the MOPA, amplifier (PA) or oscillator(s) to be added should be ed with what percentage of laser or pumping power. Thus, for each HEL effector, the beam power of the laser or pump source can be adjusted and/or varied. Said percentage n can be controlled by means of the optical switching unit(s).
The l switching units, for their part, can be spaced apart from the central laser source or the l pump source and, if necessary, from the central master oscillator (MO). Due to the low beam quality of the pump , an optical connection (fiber, free space) with a significantly longer distance than a few meters can be implemented here, ally between the optical switching units and the amplifiers or ators. With poorer beam quality, the beam transport takes place in fibers with a larger core diameter at a reduced intensity, so that non-linear processes are used to a reduced extent.
The optical switching unit also allows the laser source or pump source to be separated from the other components of the HEL effectors. The HEL effectors can be changed to a safety state by means of the optical switching unit(s).
Of course, other central laser sources, pump sources and other central master oscillators, etc. can also be provided as jointly usable key components. This makes it possible to create a redundant system. Also, multiple HEL effectors can be grouped together into groups that can then be operated in el.
The use of a laser source, alternatively a pump source, etc., for a ity of HEL effectors allows the total weight on the object to be reduced. The decentralized arrangement of the common central laser source or pump source etc. for the plurality of HEL effectors also creates the possibility of placing them on or in the object and protected from environmental influences.
In addition to the weight saving, the present invention gives a further advantage. The laser source, pump source, possibly the central master ator power amplifier (MOPA) or the central master ator (MO) or central oscillator can now preferably be accommodated within the object, e.g. in the hull of a ship or vehicle. These components are no longer t to the environmental requirements on the object. A positional separation also gives another age. In this way, the individual components can be led in smaller spaces on the object, for example in recesses.
Especially on a ship, saving components is a huge win.
Such scaling down of components makes the use of HEL effectors on such s possible and also financially practicable. The HEL effectors can be offered more costeffectively.
Existing platforms, such as conventional effectors, can also be used. For example, the platform of a naval light gun, etc., can be used to accommodate individual components of the HEL effectors. However, these advantages also arise for other vehicles on land, sea and in the air and can be transferred to other objects.
The mode of operation is generalized as follows: If a target or threat is detected, for example by means of a weapon delivery system, it is determined which of the beam guidance system(s) of the HEL effectors on the object can provide the best possible defense against or lization of the threat as quickly as possible. Such procedures are known to the person skilled in the art.
The weapon delivery system then s which beam guidance system(s) to use. Alternatively, this can be carried out by an operator. As a result of this decision, an optical linking of the ed beam guidance system(s) is carried out as described above. The switching of the optical switching unit(s) can be carried out pneumatically, hydraulically as well as electrically or electro-optically, although other possibilities are not excluded. The switching is controlled by the central control unit.
In this specification where nce has been made to patent specifications, other external documents, or other sources of information, this is generally for the purpose of providing a context for discussing the features of the invention. Unless specifically stated otherwise, reference to such external documents or such sources of ation is not to be construed as an admission that such documents or such sources of ation, in any jurisdiction, are prior art or form part of the common general knowledge in the art.
The invention will be explained in more detail on the basis of an exemplary embodiment with a drawing. In the figures Fig. 1 shows a first embodiment of the inventive idea in a tic block image representation, wherein a laser source can be used for at least two or more HEL effectors, Fig. 2 shows a second embodiment of the inventive idea in a schematic block image representation, wherein at least one pump source is used for at least two or more HEL effectors, Fig. 3 shows a third embodiment r to Fig.2, Fig. 4 shows another embodiment of the inventive idea in a schematic block image representation Fig. 5 shows a sketched entation of a e structure for a division of laser power.
In Fig. 1 a laser source 1 as well as at least two beam guidance systems 2.1, 2.2, 2.3 are represented as key components of several, at least two, HEL effectors 5.1, .2, 5.3.
An imaging system is defined as the beam guidance system 2.1, 2.2, 2.3. This can be built according to DE 10 2010 051 097 A1. Beam ce systems with a different structure are also conceivable. The laser source 1 contains at least one pump source 10, which is formed by at least one pump diode. The pump source 10 can be supplied with electricity and cooled by a power supply and g system 11. Said power supply and cooling system 11 can be a component of the laser source 1.
Associated with the laser source 1 is a master oscillator power amplifier (MOPA) 12 (e.g. a seed laser + ier), which can be placed therein. Alternatively, an oscillator (single resonator) 13 can be used.
The individual beam guidance systems 2.1, 2.2, 2.3 of the HEL ors 5.1, 5.2, 5.3 can be connected by means of an optical ing unit 4 to the laser source 1. HEL effectors 5.1, 5.2, 5.3 thus have a common laser source 1 and individual beam guidance systems 2.1, 2.2, 2.3 as their key components.
The optical switching unit 4 can be an optical switch or an l switching point. The optical switching unit comprises at least one input and at least two outputs.
The optical switching unit 4 should be designed to be able to split the laser power (optical power) generated in the laser source 1 for the beam guides 2.1, 2.2, 2.3 of the HEL ors 5.1, 5.2, 5.3. The division can be carried out continuously or in multiple stages. The optical power can be divided between 0% and 100%. It is also provided that it is possible to split the optical power at the same time, so that a plurality of beam guides 2.1, 2.2, 2.3 of the optical switching unit 4 can be supplied with optical power at the same time. For example, if the optical switching unit 4 comprises only two outputs, several optical switching units 4 can be used to build a cascade, by means of which a division of the laser power between the beam guides 2.1, 2.2, 2.3 can be realized (fig. 5).
The output of the laser source 1 is optically (15) connected to an input of the optical switching unit 4, ideally by an optical fiber. A free space link is also possible.
The multiple outputs of the optical switching unit 4 are fed to the inputs of the beam ce systems 2.1, 2.2, 2.3 by means of optical connections 15. The switching of the l switching unit 4 is controlled by an additional controller 6.
The beam guidance systems 2.1, 2.2, 2.3 can in turn be ted on a platform 7, 8, 9. The platforms 7, 8, 9, for their part, are preferably movable, so that the beam guidance s 2.1, 2.2, 2.3 of the HEL effectors 5.1, .2, 5.3 can be pivoted in azimuth and/or elevation. This allows the HEL effectors 5.1, 5.2, 5.3 to be aimed at the threat(s).
The HEL effectors 5.1, 5.2, 5.3 are formed in a first embodiment by the common l laser source 1, the optical switching unit 4, the ted beam guidance systems 2.1, 2.2, 2.3 as well as the optical connections , ideally optical fibers.
A plurality of HEL effectors 5.1, 5.2, 5.3 can be combined into a weapons system 100.
The manner of operation is as follows: After a threat or threats has/have been detected in a conventional way, it is determined by a weapon delivery system, e.g. a fire control system (not shown in more detail), which beam guidance system 2.1, 2.2, 2.3 would achieve a good e against the threat. In the event that the beam guidance system 2.1 of the HEL effector 5.1 is determined, this information is given to the controller 6. The controller 6 in turn switches the optical switching unit 4 so that the optical power of the laser source 1 is transmitted via the switched output of the optical ing unit 4 and the input of the selected beam guidance system 2.1. said beam guidance system 2.1 radiates the optical power against the threat.
The l power of the laser source 1 can also be output to the beam guidance system 2.1 to a d extent by the optical switching unit 4 ed to less than 100%).
Should the fire control system stipulate that more than one beam guidance system 2.1, 2.2, 2.3 is used for e, the optical power of the laser source 1 will be split and this optical power will be divided between the inputs of the beam guidance systems 2.1, 2.2, 2.3 ated or defined for the defense. From these, the optical power can then be radiated to avert the threat against it. In doing so, beam guidance systems 2.1, 2.2, 2.3 can be jointly aimed at one threat, as well as at different threats.
Fig. 2 and fig. 3 show a variant of the solution according to fig. 1 as a second exemplary embodiment. Unlike the solution according to fig. 1, in the second exemplary embodiment the MOPA 12 or oscillator 13 is removed from laser source 1. A central pump source 10 is provided that generates the required pumping power for all the HEL effectors 5.1, 5.2, 5.3.
According to fig. 2 instead of a central oscillator 13 a plurality of oscillators 21.1, 21.2, 21.3 are ed for the HEL effectors 5.1, 5.2, 5.3. An output of the respective oscillator 21.1, 21.2, 21.3 is fed to the associated beam guidance system 2.1, 2.2, 2.3. The optical switching unit 4 provides the oscillators 21.1, 21.2, 21.3 with pumping power of the pump source 10. The optical switching unit 4 is switched as described for fig. 1.
The MOPA 12 can also be d into le MOPAs 22.1, 22.2, 22.3 (fig. 3). Said MOPAs 22.1, 22.2, 22.3 can be arranged near rms 7, 8, 9. An output of the amplifier of the MOPA 22.1, 22.2, 22.3 is directed to the associated beam guidance system 2.1, 2.2, 2.3. The supply of pumping power of the pump source 10 to the amplifiers of the MOPAs 22.1, 22.2, 22.3 is carried out by means of the optical switching unit 4. The manner of operation and the switching of the optical switching unit 4 are carried out as described for fig. 1.
The HEL effectors 5.1, 5.2, 5.3 are formed in these embodiments by a common pump source 10 (plus a power supply and cooling device 11), an l switching unit 4, oscillators 21.1, 21.2, 21.3 and MOPAs 22.1, 22.2, 22.3 and their dedicated beam guides 2.1, 2.2, 2.3 as well as the optical connections 15, y optical fibers.
Fig. 4 shows another solution variant of the inventive idea, based on fig. 3. The exemplary embodiment according to fig. 3 shows the variant according to which the entire MOPA 22.2, 22.3 can be mounted separately from the pump source 10 close to the pump source 10 or the beam guidance systems 2.1, 2.2, 2.3. ingly Fig. 4 is now a further step in the implementation of the idea in that said MOPAs 22.1, 22.2, 22.3 are implemented in such a way that a common master oscillator (MO) 22 can be provided for the remaining amplifiers .1, .2, .3. This in particular minimizes the weight to be supported, since only the respective amplifier .1, .2, .3 would have to be supported.
For this embodiment, another optical switching unit 14 is used, which, like the optical switching unit 4 for pumping power, can also connect the central master oscillator 22 to the dual amplifiers 1, .2, .3 at the same time. Said optical switching unit 14 should be able to meet the same requirements as the optical switching unit 4. The optical switching unit 14 is located between the output of the master oscillator 22 and an input of the amplifiers .1, .2, .3 for this and switches the output of the master oscillator 22 to the respective input of the amplifiers .1, .2, .3. r input of the amplifiers .1, .2, .3 is reserved for ing the pumping power of the pump source 10.
The HEL effectors 5.1, 5.2, 5.3 in this fourth version are provided by a central pump source 10, a central master oscillator (MO) 22, the individual dedicated amplifier(s) .1, .2, .3, which are aligned with the dedicated beam guidance system 2.1, 2.2, 2.3, as well as the optical connections 15, ideally optical fibers.
It is understood that within the scope of the inventive idea, more than one s system 100 will also be ed to the object, e.g. a port weapons system or a starboard weapons system, etc.
The term ‘comprising’ as used in this specification and claims means ‘consisting at least in part of’. When interpreting statements in this specification and claims which include the term ising’, other features besides the features prefaced by this term in each statement can also be present. Related terms such as ise’ and ‘comprised’ are to be interpreted in a similar manner.

Claims (21)

Claims
1. A weapons system comprising at least two HEL effectors, each with at least one beam guidance system, the at least two HEL effectors comprising at least one jointly useable laser source comprising a light pump source, wherein the at least one laser source is table to each of the at least one beam guidance s by means of at least one l switching unit, wherein the at least one optical switching unit can adjust and/or vary the beam power of the laser light generated by the laser source, and wherein the at least one optical switching unit can divide the laser light between at least two outputs of the at least one optical switching unit at the same time.
2. The s system as claimed in claim 1, n the at least one optical ing unit is installed between an output of the laser source and an input of the beam guidance systems to form the HEL effectors.
3. The weapons system as claimed in claim 1, wherein the at least one optical switching unit is disposed between an output of the light pump source and an input of an oscillator of the respective HEL effectors to form the HEL effectors.
4. The weapons system as claimed in claim 1, wherein the at least one optical switching unit is ed between an output of the light pump source and an input of an amplifier of a MOPA of the respective HEL effectors to form the HEL effectors.
5. The weapons system as claimed in claim 1, wherein the at least one optical switching unit is disposed between an output of the light pump source and an input of an amplifier of the respective HEL effector and wherein at least one master oscillator is conenctable by means of another at least one optical switching unit disposed n an output of the master oscillator and another input of the amplifier of the respective HEL effector, to form the HEL effectors.
6. The weapons system as claimed in any one of claims 1 through 5, comprising an additional controller.
7. The s system as claimed in any one of claims 1 through 6, wherein the at least one optical switching unit is an optical switch or an optical switching point.
8. The weapons system as d in any one of claims 1 through 7, wherein the laser light is divisible by n 0 to 100%.
9. The weapons system as claimed in any one of claims 1 through 8, wherein the laser light is divisible continuously or in at least two stages.
10. The weapons system as claimed in any one of claims 1 through 9, wherein the at least one optical switching unit can change the HEL effectors to a safety state.
11. An object comprising a weapons system as claimed in any one of claims 1 through 10, wherein the at least one laser source is disposable in or on the object in a position proximate both of the at least one beam guidance systems.
12. An object comprising a s system as claimed in any one of claims 1 through 10, wherein the at least one laser source is disposable in or on the object in a position away from both of the at least one beam guidance systems.
13. An object sing a weapons system as claimed in any one of claims 6 through 10 when dependent on claim 5, wherein the at least one laser source and the master oscillator are disposable in or on the object in a position proximate both of the at least one beam guidance
14. An object comprising a weapons system as claimed in any one of claims 6 through 10 when dependent on claim 5, wherein the at least one laser source and the master oscillator are disposable in or on the object in a position away from both of the at least one beam guidance systems.
15. The object as claimed in in any one of claims 11 through 14, wherein at least the beam guidance systems of the HEL effectors are supportable on platforms.
16. The object as claimed in any one of claims 11 through 15, wherein the object is a stationary object.
17. The object of claim 16, wherein the stationary object comprises a house, a bunker or a container.
18. The object as claimed in any one of claims 11 through 15, wherein the object is a movable object.
19. The object as claimed in claim 18, wherein the movable object comprises a e on land, a vehicle in the air or a vehicle at sea.
20. The weapons system as claimed in any one of claims 1 through 10, substantially as herein bed with nce to any embodiment sed.
21. The object as d in any one of claims 11 through 19, substantially as herein described with reference to any embodiment disclosed. WO 62148
NZ754419A 2017-03-06 2018-01-31 Weapons system having at least two hel effectors NZ754419B2 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
DE102017104662.3 2017-03-06
DE102017104662.3A DE102017104662B4 (en) 2017-03-06 2017-03-06 Weapon system with at least two HEL effectors
PCT/EP2018/052400 WO2018162148A1 (en) 2017-03-06 2018-01-31 Weapons system having at least two hel effectors

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Publication Number Publication Date
NZ754419A NZ754419A (en) 2021-01-29
NZ754419B2 true NZ754419B2 (en) 2021-04-30

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