List of laser types

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An immense slab of "continuous melt" processed neodymium-doped laser glass for use on the National Ignition Facility.

This is a list of laser types, their operational wavelengths, and their applications. Thousands of kinds of laser are known, but most of them are used only for specialized research.

Overview

Wavelengths of commercially available lasers. Laser types with distinct laser lines are shown above the wavelength bar, while below are shown lasers that can emit in a wavelength range. The height of the lines and bars gives an indication of the maximal power/pulse energy commercially available, while the color codifies the type of laser material (see the figure description for details). Most of the data comes from Weber's book Handbook of laser wavelengths,[1] with newer data in particular for the semiconductor lasers.

Gas lasers

Main article: Gas laser
Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Helium–neon laser 632.8 nm (543.5 nm, 593.9 nm, 611.8 nm, 1.1523 μm, 1.52 μm, 3.3913 μm) Electrical discharge Interferometry, holography, spectroscopy, barcode scanning, alignment, optical demonstrations.
Argon laser 454.6 nm, 488.0 nm, 514.5 nm (351 nm, 363.8, 457.9 nm, 465.8 nm, 476.5 nm, 472.7 nm, 528.7 nm, also frequency doubled to provide 244 nm, 227 nm) Electrical discharge Retinal phototherapy (for diabetes), lithography, confocal microscopy, spectroscopy pumping other lasers.
Krypton laser 416 nm, 530.9 nm, 568.2 nm, 647.1 nm, 676.4 nm, 752.5 nm, 799.3 nm Electrical discharge Scientific research, mixed with argon to create "white-light" lasers, light shows.
Xenon ion laser Many lines throughout visible spectrum extending into the UV and IR Electrical discharge Scientific research.
Nitrogen laser 337.1 nm Electrical discharge Pumping of dye lasers, measuring air pollution, scientific research. Nitrogen lasers can operate superradiantly (without a resonator cavity). Amateur laser construction. See TEA laser.
Carbon dioxide laser 10.6 μm, (9.4 μm) Transverse (high-power) or longitudinal (low-power) electrical discharge Material processing (laser cutting, laser beam welding, etc.), surgery, dental laser, military lasers.
Carbon monoxide laser 2.6 to 4 μm, 4.8 to 8.3 μm Electrical discharge Material processing (engraving, welding, etc.), photoacoustic spectroscopy.
Excimer laser 157 nm (F2), 193.3 nm (ArF), 248 nm (KrF), 308 nm (XeCl), 351 nm (XeF) Excimer recombination via electrical discharge Ultraviolet lithography for semiconductor manufacturing, laser surgery, LASIK, scientific research.

Chemical lasers

Main article: Chemical laser

Used as directed-energy weapons.

Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Hydrogen fluoride laser 2.7 to 2.9 μm for hydrogen fluoride (<80% atmospheric transmittance) Chemical reaction in a burning jet of ethylene and nitrogen trifluoride (NF3) Used in research for laser weaponry, operated in continuous-wave mode, can have power in the megawatt range.
Deuterium fluoride laser ~3800 nm (3.6 to 4.2 μm) (~90% atm. transmittance) chemical reaction US military laser prototypes.
COIL (chemical oxygen–iodine laser) 1.315 μm (<70% atmospheric transmittance) Chemical reaction in a jet of singlet delta oxygen and iodine Military lasers, scientific and materials research. Can operate in continuous wave mode, with power in the megawatt range.
Agil (All gas-phase iodine laser) 1.315 μm (<70% atmospheric transmittance) Chemical reaction of chlorine atoms with gaseous hydrazoic acid, resulting in excited molecules of nitrogen chloride, which then pass their energy to the iodine atoms. Scientific, weaponry, aerospace.

Dye lasers

Main article: Dye laser
Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Dye lasers 390-435 nm (stilbene), 460-515 nm (coumarin 102), 570-640 nm (rhodamine 6G), many others Other laser, flashlamp Research, laser medicine,[2] spectroscopy, birthmark removal, isotope separation. The tuning range of the laser depends on which dye is used.

Metal-vapor lasers

Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Helium–cadmium (HeCd) metal-vapor laser 325 nm, 441.563 nm Electrical discharge in metal vapor mixed with helium buffer gas. Printing and typesetting applications, fluorescence excitation examination (i.e. in U.S. paper currency printing), scientific research.
Helium–mercury (HeHg) metal-vapor laser 567 nm, 615 nm (Rare) Scientific research, amateur laser construction.
Helium–selenium (HeSe) metal-vapor laser up to 24 wavelengths between red and UV (Rare) Scientific research, amateur laser construction.
Helium–silver (HeAg) metal-vapor laser[3] 224.3 nm Scientific research
Strontium vapor laser 430.5 nm Scientific research
Neon–copper (NeCu) metal-vapor laser[3] 248.6 nm Electrical discharge in metal vapor mixed with neon buffer gas. Scientific research: Raman and fluorescence spectroscopy[4][5]
Copper vapor laser 510.6 nm, 578.2 nm Electrical discharge Dermatological uses, high speed photography, pump for dye lasers.
Gold vapor laser 627 nm (Rare) Dermatological uses, photodynamic therapy.[6]
Manganese (Mn/MnCl2) vapor laser 534.1 nm Pulsed electric discharge [citation needed]

Solid-state lasers

Main article: Solid-state laser
Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Ruby laser 694.3 nm Flashlamp Holography, tattoo removal. The first laser, invented by Theodore Maiman in May 1960.
Nd:YAG laser 1.064 μm, (1.32 μm) Flashlamp, laser diode Material processing, rangefinding, laser target designation, surgery, tattoo removal, hair removal, research, pumping other lasers (combined with frequency doubling to produce a green 532 nm beam). One of the most common high-power lasers. Usually pulsed (down to fractions of a nanosecond), dental laser
Nd:YAP laser (yttrium aluminium perovskite) 1.0646 μm[7] Flashlamp, laser diode Surgery, tattoo removal, hair removal, research, pumping other lasers (combined with frequency doubling to produce a green 532 nm beam)
Nd:Cr:YAG laser 1.064 μm, (1.32 μm) solar radiation Experimental production of nanopowders.[8]
Er:YAG laser 2.94 μm Flashlamp, laser diode Periodontal scaling, dental laser, skin resurfacing
Neodymium YLF (Nd:YLF) solid-state laser 1.047 and 1.053 μm Flashlamp, laser diode Mostly used for pulsed pumping of certain types of pulsed Ti:sapphire lasers, combined with frequency doubling.
Neodymium-doped yttrium orthovanadate (Nd:YVO4) laser 1.064 μm laser diode Mostly used for continuous pumping of mode-locked Ti:sapphire or dye lasers, in combination with frequency doubling. Also used pulsed for marking and micromachining. A frequency doubled nd:YVO4 laser is also the normal way of making a green laser pointer.
Neodymium-doped yttrium calcium oxoborate Nd:YCa4O(BO3)3 or simply Nd:YCOB ~1.060 μm (~530 nm at second harmonic) laser diode Nd:YCOB is a so-called "self-frequency doubling" or SFD laser material which is both capable of lasing and which has nonlinear characteristics suitable for second harmonic generation. Such materials have the potential to simplify the design of high brightness green lasers.
Neodymium glass (Nd:Glass) laser ~1.062 μm (silicate glasses), ~1.054 μm (phosphate glasses) Flashlamp, laser diode Used in extremely high-power (terawatt scale), high-energy (megajoules) multiple beam systems for inertial confinement fusion. Nd:Glass lasers are usually frequency tripled to the third harmonic at 351 nm in laser fusion devices.
Titanium sapphire (Ti:sapphire) laser 650-1100 nm Other laser Spectroscopy, LIDAR, research. This material is often used in highly-tunable mode-locked infrared lasers to produce ultrashort pulses and in amplifier lasers to produce ultrashort and ultra-intense pulses.
Thulium YAG (Tm:YAG) laser 2.0 μm Laser diode LIDAR.
Ytterbium YAG (Yb:YAG) laser 1.03 μm Laser diode, flashlamp Laser cooling, materials processing, ultrashort pulse research, multiphoton microscopy, LIDAR.
Ytterbium:2O3 (glass or ceramics) laser 1.03 μm Laser diode Ultrashort pulse research, [9]
Ytterbium-doped glass laser (rod, plate/chip, and fiber) 1. μm Laser diode. Fiber version is capable of producing several-kilowatt continuous power, having ~70-80% optical-to-optical and ~25% electrical-to-optical efficiency. Material processing: cutting, welding, marking; nonlinear fiber optics: broadband fiber-nonlinearity based sources, pump for fiber Raman lasers; distributed Raman amplification pump for telecommunications.
Holmium YAG (Ho:YAG) laser 2.1 μm Flashlamp, laser diode Tissue ablation, kidney stone removal, dentistry.
Chromium ZnSe (Cr:ZnSe) laser 2.2 - 2.8 μm Other laser (Tm fiber) MWIR laser radar, countermeasure against heat-seeking missiles etc.
Cerium-doped lithium strontium (or calcium) aluminum fluoride (Ce:LiSAF, Ce:LiCAF) ~280 to 316 nm Frequency quadrupled Nd:YAG laser pumped, excimer laser pumped, copper vapor laser pumped. Remote atmospheric sensing, LIDAR, optics research.
Promethium-147-doped phosphate glass (147Pm+3:Glass) solid-state laser 933 nm, 1098 nm ?? Laser material is radioactive. Once demonstrated in use at LLNL in 1987, room temperature 4 level lasing in 147Pm doped into a lead-indium-phosphate glass étalon.
Chromium-doped chrysoberyl (alexandrite) laser Typically tuned in the range of 700 to 820 nm Flashlamp, laser diode, mercury arc (for CW mode operation) Dermatological uses, LIDAR, laser machining.
Erbium-doped and erbium–ytterbium codoped glass lasers 1.53-1.56 μm Laser diode These are made in rod, plate/chip, and optical fiber form. Erbium doped fibers are commonly used as optical amplifiers for telecommunications.
Trivalent uranium-doped calcium fluoride (U:CaF2) solid-state laser 2.5 μm Flashlamp First 4-level solid state laser (November 1960) developed by Peter Sorokin and Mirek Stevenson at IBM research labs, second laser invented overall (after Maiman's ruby laser), liquid helium cooled, unused today. [1]
Divalent samarium-doped calcium fluoride (Sm:CaF2) laser 708.5 nm Flashlamp Also invented by Peter Sorokin and Mirek Stevenson at IBM research labs, early 1961. Liquid helium-cooled, unused today. [2]
F-center laser 2.3-3.3 μm Ion laser Spectroscopy
Optically pumped semiconductor laser 920 nm-1.35 μm Laser diode Projection, life sciences, forensic analysis, spectroscopy, eye surgery, laser light shows.

The lasing medium is a semiconductor chip. Frequency doubling or tripling is typically done to produce visible or ultraviolet radiation. Power levels of several watts are possible. Beam quality can be extremely high- often rivaling that of an ion laser.

Semiconductor lasers

Main article: Laser diode
Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Semiconductor laser diode (general information) 0.4-20 μm, depending on active region material. Electrical current Telecommunications, holography, printing, weapons, machining, welding, pump sources for other lasers, high-beam headlights for automobiles.[10]
GaN 0.4 μm Optical discs. 405 nm is used in Blu-ray Discs reading/recording.
InGaN 0.4 - 0.5 μm Home projector, primary light source for some recent small projectors
AlGaInP, AlGaAs 0.63-0.9 μm Optical discs, laser pointers, data communications. 780 nm compact disc, 650 nm general DVD player and 635 nm DVD for Authoring recorder laser are the most common lasers type in the world. Solid-state laser pumping, machining, medical.
InGaAsP 1.0-2.1 μm Telecommunications, solid-state laser pumping, machining, medical..
lead salt 3-20 μm
Vertical-cavity surface-emitting laser (VCSEL) 850–1500 nm, depending on material Telecommunications
Quantum cascade laser Mid-infrared to far-infrared. Research, Future applications may include collision-avoidance radar, industrial-process control and medical diagnostics such as breath analyzers.
Quantum dot laser wide range. Medicine (laser scalpel, optical coherence tomography), display technologies (projection, laser TV), spectroscopy and telecommunications.
Quantum well laser 0.4-20 μm, depending on active region material. Telecommunications
Hybrid silicon laser Mid-infrared Low cost silicon integrated optical communications

Other types of lasers

Laser gain medium and type Operation wavelength(s) Pump source Applications and notes
Free-electron laser A broad wavelength range (0.1 nm - several mm); a single FEL may be tunable over a wavelength range Relativistic electron beam Atmospheric research, material science, medical applications.
CO₂ gas dynamic laser Several lines around 10.5 μm; other frequencies may be possible with different gas mixtures Spin state population inversion in carbon dioxide molecules caused by supersonic adiabatic expansion of mixture of nitrogen and carbon dioxide Military applications; can operate in CW mode at several megawatts optical power. Manufacturing and Heavy Industry.
"Nickel-like" samarium laser[11] X-rays at 7.3 nm wavelength Lasing in ultra-hot samarium plasma formed by double pulse terawatt scale irradiation fluences. Sub–10 nm X-ray laser, possible applications in high-resolution microscopy and holography.
Raman lasers, use inelastic stimulated Raman scattering in a nonlinear media, mostly fiber, for amplification 1-2 μm for fiber version Other laser, mostly Yb-glass fiber lasers Complete 1-2 μm wavelength coverage; distributed optical signal amplification for telecommunications; optical solitons generation and amplification
Nuclear pumped laser See gas lasers, soft x-ray Nuclear fission: reactor, nuclear bomb Research, weapons program.
Polariton laser Near infrared optically and electrically pumped[12] spin switches and terahertz lasers[13]
Plasmonic laser Near infrared and ultraviolet optically pumped[14] Nanoscale lithography, fabrication of ultra-fast photonic nano circuits, single-molecule biochemical sensing, and microscopy
Phonon laser microwave to Far-infrared electrically pumped Investigation of terahertz-frequency ultrasound and optoelectronics
Gamma-ray laser Gamma rays Unknown Hypothetical

See also

Notes

  1. ^ Weber, Marvin J. (1999). Handbook of laser wavelengths. CRC Press. ISBN 978-0-8493-3508-2.
  2. ^ Costela, A.; et al. (2009). "Medical applications of dye lasers". In Duarte, F. J. (ed.). Tunable Laser Applications (2nd ed.). CRC Press.
  3. ^ a b Storrie-Lombardia, M. C.; et al. (2001). "Hollow cathode ion lasers for deep ultraviolet Raman spectroscopy and fluorescence imaging". Review of Scientific Instruments. 72 (12): 4452. Bibcode:2001RScI...72.4452S. CiteSeerX 10.1.1.527.8836. doi:10.1063/1.1369627.
  4. ^ Beegle, L.; Bhartia, R.; White, M.; DeFlores, L.; Abbey, W.; Wu, Yen-Hung; Cameron, B.; Moore, J.; Fries, M. (2015-03-01). "SHERLOC: Scanning habitable environments with Raman & luminescence for organics & chemicals". 2015 IEEE Aerospace Conference. pp. 1–11. doi:10.1109/AERO.2015.7119105. ISBN 978-1-4799-5379-0. S2CID 28838479.
  5. ^ Overton, Gail (11 Aug 2014). "Photon Systems Deep-UV NeCu laser to power Mars 2020 Raman fluorescence instrument". www.laserfocusworld.com. Retrieved 2020-03-17.
  6. ^ Goldman, L. (1990). "Dye lasers in medicine". In Duarte, F. J.; Hillman, L. W. (eds.). Dye Laser Principles. Academic Press. ISBN 978-0-12-222700-4.
  7. ^ Sulc, Jan; Jelinkova, Helena; Jabczynski, Jan K.; Zendzian, Waldemar; Kwiatkowski, Jacek; Nejezchleb, Karel; Skoda, Vaclav (27 April 2005). "Comparison of diode-side-pumped triangular Nd:YAG and Nd:YAP laser" (PDF). In Hoffman, Hanna J; Shori, Ramesh K (eds.). Solid State Lasers XIV: Technology and Devices. Vol. 5707. p. 325. doi:10.1117/12.588233. S2CID 121802212. Retrieved 16 February 2022.
  8. ^ Sh. D. Payziyeva; S. A. Bakhramov; A. K. Kasimov (2011). "Transformation of concentrated sunlight into laser radiation on small parabolic concentrators". Journal of Renewable and Sustainable Energy. 3 (5): 053102. doi:10.1063/1.3643267.
  9. ^ M. Tokurakawa; K. Takaichi; A. Shirakawa; K. Ueda; H. Yagi; T. Yanagitani; A. A. Kaminskii (2007). "Diode-pumped 188 fs mode-locked Yb3+:Y2O3 ceramic laser". Applied Physics Letters. 90 (7): 071101. Bibcode:2007ApPhL..90g1101T. doi:10.1063/1.2476385.
  10. ^ BMW, Audi will introduce laser headlamps this year, Automotive News Europe, 7 January 2014, David Sedgwick
  11. ^ J. Zhang*, A. G. MacPhee, J. Lin; et al. (16 May 1997). "A Saturated X-ray Laser Beam at 7 Nanometers". Science. 276 (5315): 1097–1100. doi:10.1126/science.276.5315.1097. Retrieved 31 October 2013.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  12. ^ Schneider, Christian; Rahimi-Iman, Arash; Kim, Na Young; Fischer, Julian; Savenko, Ivan G.; Amthor, Matthias; Lermer, Matthias; Wolf, Adriana; Worschech, Lukas; Kulakovskii, Vladimir D.; Shelykh, Ivan A. (2013). "An electrically pumped polariton laser". Nature. 497 (7449): 348–352. Bibcode:2013Natur.497..348S. doi:10.1038/nature12036. ISSN 1476-4687. PMID 23676752. S2CID 126376454.
  13. ^ "Why do we need polariton lasers?". spie.org. Retrieved 2022-06-11.
  14. ^ Kristanz, Gerold V.; Arnold, Nikita; Kildishev, Alexander V.; Klar, Thomas A. (2018-09-19). "Power Balance and Temperature in Optically Pumped Spasers and Nanolasers". ACS Photonics. 5 (9): 3695–3703. doi:10.1021/acsphotonics.8b00705. ISSN 2330-4022. PMC 6156092. PMID 30271813.

Further references

  • Silfvast, William T. Laser fundamentals, Cambridge University Press, 2004. ISBN 0-521-83345-0
  • Weber, Marvin J. Handbook of laser wavelengths, CRC Press, 1999. ISBN 0-8493-3508-6
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