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Solid-state laser

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(Redirected fromSolid state laser)
Laser which uses a solid gain medium

Laser rods (from left to right):Ruby,alexandrite,Er:YAG,Nd:YAG

Asolid-state laser is alaser that uses again medium that is asolid, rather than aliquid as indye lasers or agas as ingas lasers.[1]Semiconductor-based lasers are also in the solid state, but are generally considered as a separate class from solid-state lasers, calledlaser diodes.

Solid-state media

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Further information:List of laser types § Solid-state lasers

Generally, the active medium of a solid-state laser consists of aglass orcrystalline "host" material, to which is added a "dopant" such asneodymium,chromium,erbium,[2]thulium[3] orytterbium.[4] Many of the common dopants arerare-earth elements, because the excited states of such ions are not strongly coupled with the thermal vibrations of their crystal lattices (phonons), and theiroperational thresholds can be reached at relatively low intensities oflaser pumping.

There are many hundreds of solid-state media in which laser action has been achieved, but relatively few types are in widespread use. Of these, probably the most common isneodymium-doped yttrium aluminum garnet (Nd:YAG). Neodymium-doped glass (Nd:glass) and ytterbium-doped glasses orceramics are used at very high power levels (terawatts) and high energies (megajoules), for multiple-beaminertial confinement fusion.

The first material used for lasers wassynthetic ruby crystals.Ruby lasers are still used for a few applications, but they are no longer common because of their low power efficiencies. At room temperature, ruby lasers emit only short pulses of light, but atcryogenic temperatures they can be made to emit a continuous train of pulses.[5]

The second solid-state gain medium wasuranium-dopedcalcium fluoride. Peter Sorokin and Mirek Stevenson atIBM's laboratories inYorktown Heights (US) experimented with this material in the 1960s and achieved lasing at 2.5 μm shortly afterMaiman'sruby laser.

Some solid-state lasers can be madetunable by using intracavityetalons,prisms,gratings, or a combination of these.[6]Titanium-doped sapphire is widely used for its broad tuning range, 660 to 1080nanometers.Alexandrite lasers are tunable from 700 to 820 nm and yield higher-energy pulses than titanium-sapphire lasers because of the gain medium's longer energy storage time and higherdamage threshold.

Pumping

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Further information:Laser pumping

Solid statelasing media are typicallyoptically pumped, using either aflashlamp orarc lamp, or bylaser diodes.[1]Diode-pumped solid-state lasers tend to be much more efficient and have become much more common as the cost of high-powersemiconductor lasers has decreased.[7]

Mode locking

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Mode locking of solid-state lasers andfiber lasers has wide applications as large-energy ultra-short pulses can be obtained.[1] There are two types of saturable absorbers that are widely used as mode lockers: SESAM,[8][9][10] and SWCNT.Graphene has also been used.[11][12][13] These materials use a nonlinear optical behavior calledsaturable absorption to make a laser create short pulses.

Applications

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This sectionneeds expansion. You can help byadding to it.(June 2008)

Solid state lasers are used in research, medical treatment, and military applications, among others.

See also

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References

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  1. ^abcHeller, Jörg (1 March 2022)."A Primer on Solid-State Lasers".www.techbriefs.com. SAE Media Group. Retrieved7 August 2022.
  2. ^Singh, G.; Purnawirman; Bradley, J. D. B.; Li, N.; Magden, E. S.; Moresco, M.; Adam, T. N.; Leake, G.; Coolbaugh, D.; Watts, M. R. (2016)."Resonant pumped erbium-doped waveguide lasers using distributed Bragg reflector cavities".Optics Letters.41 (6):1189–1192.Bibcode:2016OptL...41.1189S.doi:10.1364/OL.41.001189.PMID 26977666.
  3. ^Su, Z.; Li, N.; Magden, E. S.; Byrd, M.; Purnawirman; Adam, T. N.; Leake, G.; Coolbaugh, D.; Bradley, J. D.; Watts, M. R. (2016)."Ultra-compact and low-threshold thulium microcavity laser monolithically integrated on silicon".Optics Letters.41 (24):5708–5711.Bibcode:2016OptL...41.5708S.doi:10.1364/OL.41.005708.PMID 27973495.
  4. ^Z. Su, J. D. Bradley, N. Li, E. S. Magden, Purnawirman, D. Coleman, N. Fahrenkopf, C. Baiocco, T. Adam, G. Leake, D. Coolbaugh, D. Vermeulen, and M. R. Watts (2016)"Ultra-Compact CMOS-Compatible Ytterbium Microlaser",Integrated Photonics Research, Silicon and Nanophotonics 2016, IW1A.3.
  5. ^"Continuous solid-state laser operation revealed by BTL"(PDF).Astronautics: 74. March 1962.
  6. ^N. P. Barnes, Transition metal solid-state lasers, inTunable Lasers Handbook,F. J. Duarte (Ed.) (Academic, New York, 1995).
  7. ^"Diode-Pumped Lasers: Performance, Reliability Enhance Applications".photonics.com.
  8. ^H. Zhang et al.,"Induced solitons formed by cross polarization coupling in a birefringent cavity fiber laser"Archived 7 July 2011 at theWayback Machine, Opt. Lett., 33, 2317–2319.(2008).
  9. ^D. Y. Tang et al.,"Observation of high-order polarization-locked vector solitons in a fiber laser"Archived 20 January 2010 at theWayback Machine,Physical Review Letters, 101, 153904 (2008).
  10. ^L. M. Zhao et al.,"Polarization rotation locking of vector solitons in a fiber ring laser"Archived 7 July 2011 at theWayback Machine,Optics Express, 16,10053–10058 (2008).
  11. ^H. Zhang; D. Y. Tang; L. M. Zhao; Q. L. Bao; K. P. Loh (2009)."Large energy mode locking of an erbium-doped fiber laser with atomic layer graphene"(PDF).Optics Express.17 (20):17630–5.arXiv:0909.5536.Bibcode:2009OExpr..1717630Z.doi:10.1364/OE.17.017630.PMID 19907547.S2CID 207313024. Archived fromthe original(PDF) on 17 July 2011.
  12. ^Han Zhang; Qiaoliang Bao; Dingyuan Tang; Luming Zhao & Kianping Loh (2009)."Large energy soliton erbium-doped fiber laser with a graphene-polymer composite mode locker"(PDF).Applied Physics Letters.95 (14): 141103.arXiv:0909.5540.Bibcode:2009ApPhL..95n1103Z.doi:10.1063/1.3244206.S2CID 119284608. Archived fromthe original(PDF) on 17 July 2011.
  13. ^"Graphene: Mode-locked lasers".NPG Asia Materials. 21 December 2009.doi:10.1038/asiamat.2009.52.
Distinct subtypes
Yttrium aluminium garnet
Glass
Othergain media
Structures
Specific lasers
Types of lasers
Laser physics
Laser optics
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