The present invention relates to a method for obscuring or marking objects, such as land, air or seafaring vessels.
Lasers are now commonly used for tactical designation, detection and ranging. Laser-based tactical systems can be used to detect many types of military vehicles, including submarines, ships, land vehicles and aircraft.
There are two types of laser-based systems. One type is “LIDAR,” which typically uses laser pulses and is fully analogous to RADAR. The other is “laser designation,” wherein the target is illuminated with a continuous beam or pulse train. LIDAR systems obtain range and bearing, while laser designating systems use reflected laser energy (possibly from a third platform) to home on the target.
In order to avoid detection or frustrate attempts at ranging by such systems, military vehicles often use “obscurants” to obscure their presence. But relatively few obscurants are effective against LIDAR or laser-designation systems. In fact, obscurants for these laser-based systems are typically limited to classical systems, such as smoke and water spray (for ships). And while somewhat effective for use by aircraft and land vehicles, smoke is generally not available for use as an obscurant for submarines.
Consequently, there is a need to develop new obscurants and a method to use them to bolster the limited arsenal of countermeasures available against LIDAR and laser-designation systems. And for obvious reasons, there is a continuing need to develop better “taggants” that tag vehicles to facilitate their detection and ranging.
The illustrative embodiment of the present invention is a method that avoids at least some of the drawbacks of the prior art. In accordance with the method, engineered particles are used as obscurants and taggants. In some embodiments, the method comprises:
Engineered particles suitable for use in conjunction with a method in accordance with the illustrative embodiment of the present invention include, without limitation, nanometer-scale crystals and micron-scale spheres. In some embodiments, the nanometer-scale crystals, and doped versions of the micron-scale spheres, are advantageously engineered to absorb photons having a first, predetermined wavelength λ1 and re-radiate (fluoresce) the absorbed energy as photons having a second wavelength λ2. In some other embodiments, the micron-scale spheres remain un-doped, and simply scatter the light that they receive without a change in wavelength. Particles that shift wavelength on re-radiation are advantageously (but not necessarily) used as obscurants. On the other hand, particles that do not shift the wavelength of re-emitted energy are advantageously (but not necessarily) used as taggants.
Consider a first vehicle that has deployed particles in accordance with the illustrative embodiment of the present invention, wherein the particles absorb light having wavelength λ1 and fluoresce at a second wavelength λ2. Assume that a LIDAR or laser designation system directs a beam of light having wavelength λ1 toward the first vehicle, wherein the light impinges upon the particles before it can reach the vehicle. The particles will absorb the light and re-radiate the energy at wavelength λ2. Since light having a wavelength other than λ1 will not be properly sensed and interpreted by the LIDAR or the laser-designation system, the particles, and the first vehicle that they shield, will remain undetected. In this fashion, the particles function as an obscurant.
Consider a first vehicle that has deployed particles in accordance with the illustrative embodiment of the present invention, wherein the particles receive and scatter light at the same wavelength λ1. Assume that a second vehicle passes through or near the released particles, and that the medium through which the vehicle travels (and in which the particles are suspended) is disturbed by the passage of the second vehicle. Assume further that an LIDAR system directs a beam of light having wavelength λ1 toward the second vehicle, wherein the light impinges upon the particles. Light having wavelength λ1 that is scattered by the particles is detected by the LIDAR system. The detected light reveals that the particles are moving in a characteristic fashion, indicative of the passage of a specific type of vehicle (e.g. submarine, aircraft, etc). In this fashion, the particles function as a taggant.
In some further variations of the illustrative embodiment, the particles are adhered to vehicle. In some of these variations, the particles are treated to become “sticky” on release from a first vehicle. When the particles come into contact with a second vehicle, the particles adhere to that vehicle, functioning as a taggant.
In yet some additional variations of the illustrative embodiment, the particles are incorporated into a paint, which is then adhered to a vehicle. In embodiments in which the particles absorb and fluoresce at different wavelengths, the particle-laden paint serves as an obscurant to prevent a painted vehicle from being detected.
These and other variations of the illustrative embodiment of the present invention are depicted in the Drawings and described further below in the Detailed Description.
The terms listed below are defined for use in this specification as follows:
Laser-based Detection and Ranging (LDR) Systems. As used herein, this phrase generically refers to both LIDAR systems and laser designation systems. That is, the illustrative embodiments of the invention can be used, as appropriate, in conjunction with either type of system. LIDAR and laser designation systems are well known to those skilled in the art and will not be described here in detail. It will suffice to note that LIDAR is capable of generating a beam of laser light having a specific wavelength, directing the beam toward a target, detecting a beam having the same wavelength that is reflected from the target, and ranging the target. Laser designation systems “illuminate” a target for a missile to home on. For clarity and simplicity, the illustrative embodiment of the present invention is described and illustrated in the context of LIDAR systems. Those skilled in the art will know how, and know when it's appropriate to use the illustrative embodiment of the invention with either type of system.
Micron-scale means greater than about 100 nanometers and less than about 10 microns.
Nanometer-scale means about 100 nanometers or smaller.
Obscurant is something that obscures the presence of a vehicle from a system that is trying to detect or range the vehicle.
Resonant Cross Section refers to the interaction cross section of a particle near a resonant frequency of the particle.
Taggant is something that enhances the ability of a system to detect or range a vehicle.
Vehicle means devices, typically military, which are capable of moving personnel, ordinance, supplies, etc. Vehicles include, without limitation, land vehicles (e.g., tanks, armored personal carriers, etc.), aircraft (e.g., helicopters, jets, prop-planes, drones, missiles, etc.), and seafaring vessels (e.g., submarines, surface ships, etc.).
The illustrative embodiment of the present invention is a method for using very small particles—particles having a size of about 10 microns or less—as obscurants and taggants for use in conjunction with LDR systems. When used as obscurants, the particles are capable of defeating LDR systems. When used as taggants, the particles are capable of enhancing the performance of these systems.
An important aspect of the present invention is the selection of particles for use as obscurants or taggants. Particles for use in conjunction with the illustrative embodiment of the present invention are advantageously:
It is recognized that, typically, the term “nano-crystal” refers to crystals having a size less than about 100 nm. As will become clear later in this specification, in some embodiments of the present invention, crystals that are larger than 100 nm or even 500 nm are advantageously used. It is immaterial whether these crystals are referred to as “over-sized nano-crystals,” “micro-crystals,” “nano-crystals,” or something else. For convenience and clarity, the term “nano-crystal” is used.
Nano-crystals are well known in the art, and have been manufactured from a variety of materials, typically metals. Nano-crystals have (photon) absorption and fluorescence properties that are size and material dependent. Those skilled in the art can produce such crystals in quantity with tailored absorption and fluorescence characteristics.
Nano-crystals for use in conjunction with the present invention are advantageously engineered to absorb photons having a particular wavelength, and re-radiate photons at another, typically longer wavelength. The absorption wavelength is selected to match the operating wavelength of a detection and ranging system. Typically, LDR systems operate in the infrared region of the electromagnetic spectrum. The infrared region extends from about 780 nm to 1.00 mm, and is often subdivided into four regions: the near IR (i.e., near visible) at 780–3000 nm, the intermediate IR at 3000–6000 nm, the far IR at 6000–15000 nm, and the extreme IR at 15000 nm–1.0 mm. Most atmospheric LDR systems operate in the near or intermediate range (i.e., 780–6000 nm).
For use underwater, LDR systems will operate at blue-green wavelengths (about 458 nm to 514 nm), since these wavelengths fall in a narrow transmission window for light through water. Light having a different wavelength is rapidly absorbed by water.
The ability of a suitably engineered nano-crystal to absorb a photon having a first wavelength λ1 and re-radiate a photon having a second wavelength λ2 is important for its use as an obscurant in accordance with the illustrative embodiment of the present invention. In particular, LDR systems are not typically capable of detecting light having a wavelength that is different from that of the interrogating beam. To the extent that an LDR system directs an interrogating light beam having a wavelength λ1 into a cloud of nano-crystals that is capable of absorbing those photons and re-radiating photons having a different wavelength λ2, the LDR will not be able to sense the returned light. Consequently, the LDR system will not be able to detect the cloud of nano-crystals. As described later in this specification and as illustrated in the appended Figures, to the extent that the cloud of nano-crystals is interposed between the LDR system and a vehicle, the vehicle will not be detectable by the LDR system (assuming that the nano-crystals absorb substantially all incoming light energy).
Due to their exceedingly small size, a very small amount of nano-crystals provide a large area of protection for a vehicle. In particular, the resonant cross section of a nano-crystal is about 1.2×10−10 square meters per particle. This provides a coverage area of about 5.5×1010 square meters per cubic meter or about 1×104 square meters per gram of nano-crystals. Many kilograms of smoke would be required to provide the same amount of coverage area as a gram of nano-crystals.
The optical behavior (absorption and fluorescence) of a nano-crystal is primarily a function of its size (for a given material). In other words, a nano-crystal can be “tuned” to absorb or fluoresce at a specific wavelength by varying crystallite size. As the size of a nano-crystal decreases, as controlled by its preparation method, its band gap shifts to higher energies due to the quantum size effect. Absorption and luminescence spectroscopy enables the shift in band gap to be determined. Consequently, with routine experimentation as to crystal size, nano-crystals can be engineered to provide a desired wavelength selectivity (i.e., absorb at a desired wavelength or fluoresce at a desired wavelength). There is a limited ability to independently control absorption and fluorescence wavelength. In particular, by varying crystallite size and material, a different set of characteristic absorption and fluorescence wavelengths are obtained.
In some embodiments, the nano-crystals are engineered to provide a relatively small shift in fluorescence wavelength. This can be done, for example, by producing the nano-crystals from a semiconductor material that has had its bandgap adjusted, in known fashion, to be near and slightly below the laser's photon energy.
For most applications, the nano-crystal is engineered to absorb at the operating wavelength of a LDR system (i.e., typically near infrared—the specific operating wavelength of most military systems is secret) without regard to fluorescence wavelength (since there is little ability to independently control the fluorescence wavelength).
Crystals having a size that is between about 10 to 100 percent of the wavelength of the laser light to be absorbed are advantageously used. A particularly strong absorption is often observed for crystals having a size that is about 50 percent of the wavelength of the interrogating laser beam. The term “size,” when used in the context of nano-crystals, refers to the largest dimension along the three crystal axes. Often, when dealing with light, the expression kd=2πd/λ, is used to provide a crystal diameter.
The preferred crystallite size will depend upon the physical shape and composition of the nano-crystal, and are determined by simple experimentation. Specifically, crystals are grown to a particular size, in known fashion, and then segregated by size. The different-size crystals are exposed to laser light at the wavelength of interest and the absorption and fluorescence wavelengths are determined in known fashion. The crystal having the most desirable absorption and/or fluorescence characteristics is then selected.
Nano-crystals have been prepared for most metals, both pure (e.g., platinum, palladium, gold, silver, nickel and copper etc.) and alloys (e.g., silver/palladium, silver/gold, silver/platinum, nickel/copper, nickel aluminum, etc.), diamond, carbon, and as a variety of oxides (e.g., ZnGa2O4, TiO2, Fe2O3, ZnO, GeO2), etc. A number of preparation methods are known to those skilled in the art. Nanoc-crystals are commercially available from a variety of sources, such as Cima NanoTech, Woodbury, Minn.
Nano-crystals for use in conjunction with the illustrative embodiment of the present invention are advantageously coated for protection from oxidation and chemical attack. The coating will enable use of the nano-crystals in harsh environments and provide a long shelf life. The coating can be suitably selected from polyethylene glycol, peptides, trioctylphosphine, dithiol, thiol, xylenedithiol and glass, among others.
As previously indicated, micron-scale spheres (“micro-spheres”) can be used as taggants and obscurants in conjunction with the illustrative embodiment of the present invention. The spheres are advantageously transparent and made of a dielectric material (e.g., glass, plastic, etc.). The micro-spheres capture light based on a difference in refractive index between the ambient environment and the micro-spheres. Glass micro-spheres will have a refractive index in the range of about 1.3 to 1.6, and plastic micro-spheres will have a refractive index that is somewhat less than 1.3.
In some embodiments, the micro spheres are doped with one or more materials (metals, rare-earth metals, etc.). The dopant is advantageously selected to provide a particular fluorescence behavior. For example, in some embodiments, the dopant is selected so that the micro-spheres radiate photons having a wavelength that is different from the wavelength of incoming photons, in the manner of appropriately-engineered nano-crystals, as previously described. In some other embodiments, the dopant system “traps” the fluorescent photon (i.e., produces a geometry-induced forbidden transition for the fluorescent photon), degrading it to much longer wavelengths (i.e., heat). In either case, the very high quality factor or “Q” of the micro-spheres provides an efficient transfer of energy to the dopant, wherein the character of the (re)-emitted electromagnetic energy is changed.
The optical behavior of micro-spheres can also be controlled by their size. For example, size can be chosen so that the micro-sphere is anti-resonant for the light that is produced by fluorescence (due to a dopant).
The high “Q” (quality factor) of micro-spheres indicates that they will be very efficient light scatters. Un-doped micro-spheres will return light at the same wavelength as it is received. Consequently, in some embodiments, un-doped micro-spheres are used as taggants. Also, un-doped micro-spheres are not wavelength selective in the sense that they will capture interrogating light having any of a variety of wavelengths.
Micro-spheres for use in conjunction with the present invention will typically have a diameter that is less than about 10 microns and greater than about 100 nanometers (0.1 microns). As for the nano-crystals, micro-sphere size is best determined by experimentation with regard to a specific wavelength of incoming light.
It is contemplated that other very small, engineered particles can be used as obscurant or taggant. For example, if it were possible to create a nano-sphere (i.e., nanometer-scale sphere), which at present it is not, they could be used.
Having described two types of particles (i.e., nano-crystals and micro-spheres) that are suitable for use in conjunction with the present invention, a method for obscuring or tagging a vehicle using these particles is now described.
With regard to task 202, particles are stored (e.g., in a container, compartment, etc.) within a vehicle. The term “vehicle” has been defined above to include, without limitation, land vehicles, aircraft, and seafaring vessels. Typically, the vehicle will be in use in military service.
It will be appreciated that the manner in which the particles are deployed is somewhat application specific. For example, when used as an obscurant, the particles will typically be ejected from the vehicle via a puff of air or explosively. For deployment from a submarine, the particles will typically be released upstream of the screw (i.e., the propellers) to take advantage of the turbulence that is provided by the screw to disperse the particles in the water. When the particles are being deployed by a surface ship for use as taggant (e.g., for a submarine, etc.), they are, in some embodiments, released underwater from a canister. The particles can be dispersed in the form of a column (vertically) by lowering/raising the canister from a stationary ship, or in the form of a layer (horizontally) by dragging the canister from a moving ship.
In some embodiments, method 200 includes an additional task—task 206, which is to adhere the released particles to a second vehicle. Task 206 is described in more detail later in this specification.
It is noted that the inability to detect light at wavelength λ2 is not a technical limitation per se; rather, it is due to an inability to predict the wavelength of the back-scattered light. In other words, detection is problematic because it is not known where (i.e., at what wavelength) to look.
In further detail,
An LDR system (not shown) directs a beam of light 126 having wavelength λ1 towards vehicle 122. Light beam 126 is intercepted and absorbed by particles 330, and the absorbed energy is re-radiated as photons having wavelength λ2. Since the LDR system cannot reliably detect light having wavelength λ2, the vehicle (i.e., aircraft 122, land vehicle 122, and submarine 122) is neither detected nor ranged.
LDR system 120 interrogates particles 330 with light beam 126 having wavelength λ1. Particles 330 receive light beam 126 and scatter it, returning light 128 at the same wavelength λ1. The returned light, once suitably analyzed, will indicate the presence of vehicle 122 and, in some cases, provide an identifying signature, as described further below.
More particularly,
Particles 330 are advantageously dispersed in a layer. Movement of submarine 122 through the water creates disturbance 814, which is known to cause large-amplitude submerged waves 816. An LDR system (not depicted) that operates at blue-green wavelengths can readily detect movement of particles 330, as caused by waves 816.
Like
In subtask 1108, particles are released from a first vehicle. In subtask 1110, a material is applied (e.g., sprayed, etc.) to the particles on release, wherein the material causes the particles to adhere to a second vehicle. In other words, the material functions as an adhesive to render the particles “sticky.” The sticky particles are dispersed into the environment and, on contact with a second vehicle, adhere to it. (It is noted that subtask 1110 is also a subtask of task 206.)
The material functioning as the adhesive is application specific. In other words, the material is selected to react with the exterior of the target vehicle. For example, in some embodiments in which the particles are to be adhered to a submarine, the particles are coated with antibodies. This can cause the particles to adhere to the bio-film on the hull of the submarine. Dithiol-coated particles will adhere to bare metal. Those skilled in the art can suitably select an adhesive material as a function of the target.
The variation of task 1002 depicted in
In subtask 1404, particles are mixed with paint that is advantageously transparent at the interrogation wavelength. The more likely application for this variation is to obscure the vehicle; consequently, the particles are engineered to absorb light having wavelength λ2 and radiate photons at wavelength λ2. Once the paint is prepared, it is applied to the vehicle.
The variation of the illustrative embodiment that is depicted in
It is to be understood that the above-described embodiments are merely illustrative of the present invention and that many variations of the above-described embodiments can be devised by those skilled in the art without departing from the scope of the invention. It is therefore intended that such variations be included within the scope of the following claims and their equivalents.
Number | Name | Date | Kind |
---|---|---|---|
4053433 | Lee | Oct 1977 | A |
4448106 | Knapp | May 1984 | A |
5324567 | Bratchley et al. | Jun 1994 | A |
5401976 | Bannasch | Mar 1995 | A |
6380547 | Gonzalez et al. | Apr 2002 | B1 |
6388246 | Fry et al. | May 2002 | B1 |
6432715 | Nelson et al. | Aug 2002 | B1 |
6484640 | Schneider et al. | Nov 2002 | B1 |
Number | Date | Country | |
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20040227112 A1 | Nov 2004 | US |