High-power lasers and their applications on the battlefield

Gas lasers, as well as various types of solid-state, fiber, and free-electron lasers, enable successful development of a high-power ‘space-age’ weapon.
17 February 2011
Yehoshua Kalisky and Ofra Kalisky

The dream of a weapon that can instantaneously destroy targets from a remote distance is becoming true. Development of a high-energy laser weapon is currently considered tactical as well as strategic. It is as a part of a general layered defense system against ballistic missiles and short-range rockets (the ‘space-age’ weapon). Why are laser beams so attractive? Unlike regular light bulbs, laser beams have unique characteristics, such as narrow bandwidth, as well as high brightness and coherence, so that they can be concentrated onto a small area and generate catastrophic failures of incoming missiles.1

Gas or solid-state lasers, including fiber lasers, are candidates for powerful laser sources. Gas lasers—such as hydrogen or deuterium fluoride (HF/DF) light sources—or chemical oxygen-iodine lasers (COILs) achieve lasing through chemical reactions. COILs are strategic airborne weapons (Megawatt-class lasers) that emit at a wavelength of 1.315μm. The COIL system is also referred to as an airborne laser, since it is carried on a Boeing 747-400F freighter aircraft (see Figure 1). It already achieved destruction of Scud missiles. An advanced tactical (kW-class) laser version, mounted on an aircraft, was recently tested successfully.

Figure 1. Boeing 747-400F equipped with an airborne chemical oxygen-iodine laser that is capable of destroying ballistic missiles in their boost phase. The nose-mounted turret is the laser-beam exit. (Courtesy: Northrop-Grumman.)

A second type of gas laser is the HF/DF chemical laser, with emission in the 2.6–3.3μm and 3.5–4.2μm wavelength ranges, respectively. In recent years, DF lasers managed to produce 1MW output power at 3.8μm. Other DF versions of ≈100kW output power are ground-based, mobile, or airborne, all for targeting short-range rockets. Operation of chemical lasers is limited by the available reactants that serve as its ‘ammunition.’ They are also corrosive, hazardous, and have a large footprint. Our team obtained atmospheric-pressure operation of chemical lasers (such as HF) by using various preionization technologies. In our research, we found that using a novel design of plasma-cathode preionized HF laser yielded, for the first time, an efficient room temperature atmospheric pressure chemical laser. Solid-state lasers (SSLs) seem to overcome the limitations of HF/DF lasers and are presently considered as a future tactical antimissile, antirocket, and antimortar laser weapon. Instead of using chemical reactants that are mixed together, SSLs are based on solids (crystals or crystalline ceramics) doped with rare-earth ions—such as neodymium (Nd3+) or ytterbium ions (Yb3+)—and pumped by powerful diode lasers. They are compact, mobile, modular, and capable of generating multiwavelength emission, with simple logistics owing to the absence of toxic gases. However, like COIL, they are limited by atmospheric transmission.

A solid-state laser system developed by Northrop Grumman (see Figure 2) recently produced 105kW with a good beam quality. Another approach involves use of a 50kW total-internal-reflection laser (ThinZag of Textron), with Nd-doped yttrium aluminum garnet (Nd:YAG) ceramic slabs placed between pieces of quartz. Other types of SSLs developed recently include heat-capacity Nd:YAG ceramic lasers (see Figure 3). Its unique method of operation reduces the thermal load on the laser crystal during lasing.2

Figure 2. Gain-module slab, part of the amplifying chain, with a total amplified output power of 15kW. Nd:YAG: Neodymium-doped yttrium aluminum garnet. (Courtesy: Northrop-Grumman.)

Figure 3. Cross-sectional view of the 10×10cm2diode-pumped, heat-capacity neodymium-doped yttrium aluminum garnet ceramic-slab laser developed at Lawrence Livermore National Laboratory (LLNL). (Courtesy: LLNL.)

The disk laser developed by Boeing3 features a multipass pump configuration using several high-reflection parabolic mirrors (it is based on a laser developed by Trumpf Inc. for the automotive industry4), with output power >25kW, reduced thermal gradients, and reduced thermal-lensing effects.

Figure 4. Schematic layout of a commercial disk laser produced by Trumpf Inc.4HR: High reflection. λpump: Pump wavelength. λlas: Lasing wavelength. T: Transmission. No.: Number.

Fiber lasers represent another type of efficient source, because they are compact, modular, and exhibit reduced thermally induced effects. Companies such as IPG Photonics5 have reported operation of a 10kW single-mode output-power Yb3+-doped silicate fiber laser at a wavelength of ≈1μm, with excellent beam quality. Using a beam combiner, up to ≈50kW multimode output power can be obtained. At present, approximately 3kW power can be delivered to a target at ∼1.2km by the Naval Research Laboratory.6 Our future efforts include development of a tunable 100kW free-electron laser, multi-kW laser-diode stacks, and ultrafast SSLs aimed at creating nonlethal alternatives in various scenarios using dynamic-pulse detonation.

Yehoshua Kalisky
Nuclear Research Center NEGEV (NRCN)
Beer-Sheva, Israel

Yehoshua Kalisky is a senior laser scientist with expertise in electro-optics and laser physics. He has been a SPIE Fellow since 2007. He wrote the book The Physics and Engineering of Solid State Lasers.

Ofra Kalisky
Jerusalem College of Technology
Jerusalem, Israel

Ofra Kalisky has been active in a large number of scientific and technological business initiatives, as well as management positions in various chemical and electro-optical industries in Israel and the USA. She also holds several academic positions in Israel. She has authored or co-authored more than 40 publications, internal reports, patents, and conference presentations.

1. Y. Kalisky, O. Kalisky, The status of high power lasers and their applications in the battlefield, Opt. Eng. 49, no. 9, pp. 091003, 2010.
2. K. N. Lafortune, R. L. Hurd, E. M. Joansson, C. B. Dane, S. N. Fochs, J. M. Brase, Intracavity adaptive correction of a 10 kW, solid state, heat capacity lasers, Proc. SPIE 5333, pp. 53-61, 2004. doi:10.1117/12.549480
3. P. V. Avizonis, D. J. Bossert, M. S. Curtin, A. Killi, Physics of high performance Yb:YAG thin disk lasers, Conf. Lasers Electro-Opt. (CLEO)/Int'l Quant. Electron. Conf. (IQEC), 2009. Paper CThA2.
4. J. Deile, R. Brockmann, D. Havrilla, Current status and most recent developments of industrial high power disk lasers, Conf. Lasers Electro-Opt. (CLEO)/Int'l Quant. Electron. Conf. (IQEC), pp. 1-2, 2009.
5. B. Shiner, Recent progress in high power fiber lasers, Laser Appl. Wrksh., 2009. Conf. presentation
6. P. Sprangle, A. Ting, J. Peñano, R. Fischer, B. Hafizi, Beam combining: high-power fiber-laser beams are combined incoherently, Laser Focus World 45, 2009.
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