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Excimer laser

From Wikipedia, the free encyclopedia
Type of ultraviolet laser important in chip manufacturing and eye surgery
An excimer laser

Anexcimer laser, sometimes more correctly called anexciplex laser,[1] is a form ofultravioletlaser which is commonly used in the production ofmicroelectronic devices,semiconductor basedintegrated circuits or "chips",eye surgery, andmicromachining.

Since the 1960s, excimer lasers have been widely used in high-resolutionphotolithography machines, one of the critical technologies required formicroelectronic chip manufacturing.

Terminology and history

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The Electra KrF laser demonstrates 90,000 shots over 10 hours

The termexcimer is short for 'exciteddimer', while 'exciplex' is short for 'excitedcomplex'. Most excimer lasers are of the noble gas halide type, for which the termexcimer is, strictly speaking, a misnomer.

Excimer laser was proposed in 1960 byFritz Houtermans.[2] The excimer laser development started with the observation of a nascent spectral line narrowing at 176nm  reported in 1971[3] byNikolai Basov, V. A. Danilychev and Yu. M. Popov, at theLebedev Physical Institute inMoscow, using liquidxenondimer (Xe2) excited by anelectron beam. Spurred by this report, H.A. Koehler et al. presented a better substantiation of stimulated emission in 1972,[4] using high pressure xenon gas. Definitive evidence of a xenon excimer laser action at 173 nm using a high pressure gas at 12 atmospheres, also pumped by an electron beam, was first presented in March 1973, byMani Lal Bhaumik of Northrop Corporation, Los Angeles. Strong stimulated emission was observed as the laser's spectral line narrowed from a continuum of 15 nm to just 0.25 nm, and the intensity increased a thousand-fold. The laser's estimated output of 1 joule was high enough to evaporate part of the mirror coatings, which imprinted its mode pattern. This presentation established the credible potential of developing high power lasers at short wavelengths.[5][6][7]

A later improvement was the use ofnoble gashalides (originallyXeBr) developed by many groups in 1975.[8] These groups include the Avco Everett Research Laboratory,[9] Sandia Laboratories,[10] theNorthrop Research and Technology Center,[11] the United States Government'sNaval Research Laboratory,[12] which also developed a XeCl Laser[13] that was excited using a microwave discharge,[14] and Los Alamos National Laboratory.[15]

Construction and operation

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Final amplifier of the Nike laser where laser beam energy is increased from 150 J to ~5 kJ by passing through a krypton/fluorine/argon gas mixture excited by irradiation with two opposing 670,000 volt electron beams.

An excimer lasertypically uses a combination of anoble gas (argon,krypton, orxenon) and areactive gas (fluorine orchlorine). Under the appropriate conditions of electrical stimulation and high pressure, a pseudo-molecule called anexcimer (or in the case of noble gas halides,exciplex) is created, which can only exist in an energized state and can give rise tolaser light in theultraviolet range.[16][17]

Laser action in an excimer molecule occurs because it has a bound (associative)excited state, but arepulsive (dissociative)ground state. Noble gases such as xenon andkrypton are highlyinert and do not usually formchemical compounds. However, when in an excited state (induced by electrical discharge or high-energy electron beams), they can form temporarily bound molecules with themselves (excimer) or with halogens (exciplex) such asfluorine andchlorine. The excited compound can release its excess energy by undergoingspontaneous or stimulated emission, resulting in a strongly repulsive ground state molecule which very quickly (on the order of apicosecond) dissociates back into two unbound atoms. This forms apopulation inversion.[citation needed]

Wavelength determination

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Thewavelength of an excimer laser depends on the molecules used, and is usually in the ultraviolet range ofelectromagnetic radiation:

ExcimerWavelengthRelative power
Ar2*126 nm
Kr2*146 nm
F2*157 nm
Xe2*172 & 175 nm
ArF193 nm60
KrCl222 nm25
KrF248 nm100
XeBr282 nm
XeCl308 nm50
XeF351 nm45

Excimer lasers, such as XeF and KrF, can also be made slightlytunable using a variety of prism and grating intracavity arrangements.[18]

Pulse repetition rate

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The electra laser at NRL is a KrF laser that demonstrated over 90,000 shots in 10 hours.
The electra laser at NRL is a KrF laser that demonstrated over 90,000 shots in 10 hours.

While electron-beam pumped excimer lasers can produce high single energy pulses, they are generally separated by long time periods (many minutes).  An exception was the Electra system, designed for inertial fusion studies, which could produce a burst of 10 pulses each measuring 500 J over a span of 10 s.[19] In contrast, discharge-pumped excimer lasers, also first demonstrated at the Naval Research Laboratory, are able to output a steady stream of pulses.[20][21] Their significantly higher pulse repetition rates (of order 100 Hz) and smaller footprint made possible the bulk of the applications listed in the following section. A series of industrial lasers were developed at XMR, Inc[22] in Santa Clara, California between 1980 and 1988. Most of the lasers produced were XeCl, and a sustained energy of 1 J per pulse at repetition rates of 300 pulses per second was the standard rating. This laser used a high power thyratron and magnetic switching with corona pre-ionization and was rated for 100 million pulses without major maintenance. The operating gas was a mixture of xenon, HCl, and Neon at approximately 5 atmospheres. Extensive use of stainless steel, nickel plating and solid nickel electrodes was incorporated to reduce corrosion due to the HCl gas. One major problem encountered was degradation of the optical windows due to carbon build-up on the surface of the CaF window. This was due to hydro-chloro-carbons formed from small amounts of carbon in O-rings reacting with the HCl gas. The hydro-chloro-carbons would slowly increase over time and absorbed the laser light, causing a slow reduction in laser energy. In addition these compounds would decompose in the intense laser beam and collect on the window, causing a further reduction in energy. Periodic replacement of laser gas and windows was required at considerable expense. This was significantly improved by use of a gas purification system consisting of a cold trap operating slightly above liquid nitrogen temperature and a metal bellows pump to recirculate the laser gas through the cold trap. The cold trap consisted of a liquid nitrogen reservoir and a heater to raise the temperature slightly, since at 77 K (liquid nitrogen boiling point) the xenon vapor pressure was lower than the required operating pressure in the laser gas mixture. HCl was frozen out in the cold trap, and additional HCl was added to maintain the proper gas ratio. An interesting side effect of this was a slow increase in laser energy over time, attributed to increase in hydrogen partial pressure in the gas mixture caused by slow reaction of chlorine with various metals. As the chlorine reacted, hydrogen was released, increasing the partial pressure. The net result was the same as adding hydrogen to the mixture to increase laser efficiency as reported by T.J. McKee et al.[23]

Major applications

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Photolithography

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Main article:Semiconductor device fabrication

Since the 1960s the most widespread industrial application of excimer lasers has been in deep-ultravioletphotolithography,[24][25] a critical technology used in the manufacturing ofmicroelectronic devices. Historically, from the early 1960s through the mid-1980s, mercury-xenon lamps were used in lithography for their spectral lines at 436, 405 and 365 nm wavelengths. However, with the semiconductor industry's need for both higher resolution (to produce denser and faster chips) and higher throughput (for lower costs), the lamp-based lithography tools were no longer able to meet the industry's requirements. This challenge was overcome when in a pioneering development in 1982, deep-UV excimer laser lithography was proposed and demonstrated at IBM byKanti Jain.[24][26][25][27] From an even broader scientific and technological perspective, since the invention of the laser in 1960, the development of excimer laser lithography has been highlighted as one of the major milestones in the history of the laser.[28][29][30]

Current lithography tools (as of 2021) mostly use deep ultraviolet (DUV) light from the KrF and ArF excimer lasers with wavelengths of 248 and 193 nanometers (called "excimer laser lithography"[24][26][25][31]), which has enabled transistor feature sizes to shrink to 7 nanometers (see below). Excimer laser lithography has thus played a critical role in the continued advance of the so-calledMoore's law for the last 25 years.[32] By around 2020,extreme ultraviolet lithography (EUV) has started to replace excimer laser lithography to further improve the resolution of the semiconductor circuits lithography process.[33]

Fusion

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TheNaval Research Laboratory built two systems, theKrypton fluoride laser (248 nm) and theArgon fluoride laser (193 nm) to test approaches to prove outInertial Confinement Fusion approaches. These were the Electra andNike laser systems. Because the excimer laser is a gas-based system, the laser does not heat up like solid-state systems such asNational Ignition Facility and theOmega Laser. Electra demonstrated 90,000 shots in 10 hours; ideal for aInertial fusion power plant.[34]

Medical uses

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The ultraviolet light from an excimer laser is well absorbed bybiological matter andorganic compounds. Rather than burning or cutting material, the excimer laser adds enough energy to disrupt the molecular bonds of the surface tissue, which effectivelydisintegrates into the air in a tightly controlled manner throughablation rather than burning. Thus excimer lasers have the useful property that they can remove exceptionally fine layers of surface material with almost no heating or change to the remainder of the material which is left intact. These properties make excimer lasers well suited to precision micromachining organic material (including certainpolymers and plastics), or delicatesurgeries such asLASIK eye surgery. In 1980–1983,Rangaswamy Srinivasan,Samuel Blum andJames J. Wynne atIBM'sT. J. Watson Research Center observed the effect of the ultraviolet excimer laser on biological materials. Intrigued, they investigated further, finding that the laser made clean, precise cuts that would be ideal for delicate surgeries. This resulted in a fundamental patent[35] and Srinivasan, Blum and Wynne were elected to theNational Inventors Hall of Fame in 2002. In 2012, the team members were honored withNational Medal of Technology and Innovation byUS PresidentBarack Obama for their work related to the excimer laser.[36] Subsequent work introduced the excimer laser for use inangioplasty.[37] Xenon chloride (308 nm) excimer lasers are also used to treat a variety of dermatological conditions includingpsoriasis,vitiligo,atopic dermatitis,alopecia areata and leukoderma.[38]

As light sources, excimer lasers are generally large in size, which is a disadvantage in their medical applications, although their sizes are rapidly decreasing with ongoing development.[citation needed]

Research is being conducted to compare differences in safety and effectiveness outcomes between conventional excimer laserrefractive surgery and wavefront-guided or wavefront-optimized refractive surgery, as wavefront methods may better correct forhigher-order aberrations.[39]

Scientific research

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Excimer lasers are also widely used in numerous fields of scientific research, both as primary sources and, particularly the XeCl laser, as pump sources for tunabledye lasers, mainly to excite laser dyes emitting in the blue-green region of the spectrum.[40][41] These lasers are also commonly used inpulsed laser deposition systems, where their largefluence, short wavelength and non-continuous beam properties make them ideal for the ablation of a wide range of materials.[42]

See also

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References

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  1. ^Atkins, P. W.; De Paula, Julio (2014). "13".Atkins' Physical chemistry (Tenth ed.). Oxford ; New York: Oxford University Press. p. 354.ISBN 978-0-19-969740-3.
  2. ^F.G. Houtermans (1960). "Über Massen-Wirkung im optischen Spektralgebiet un die Möglichkeit absolut negativer Absorption für einige Fälle von Molekülspektren (Licht-Lawine)".Helvetica Physica Acta.33: 939.
  3. ^Basov, N G; Danilychev, V A; Popov, Yurii M (1971-01-31). "Stimulated emission in the vacuum ultraviolet region".Soviet Journal of Quantum Electronics.1 (1):18–22.Bibcode:1971QuEle...1...18B.doi:10.1070/qe1971v001n01abeh003011.ISSN 0049-1748.
  4. ^Koehler, H.A.; Ferderber, L.J.; Redhead, D.L.; Ebert, P.J. (September 1972). "Stimulated VUV emission in high-pressure xenon excited by high-current relativistic electron beams".Applied Physics Letters.21 (5):198–200.Bibcode:1972ApPhL..21..198K.doi:10.1063/1.1654342.ISSN 0003-6951.
  5. ^Ault, E.; Bhaumik, M.; Hughes, W.; Jensen, R.; Robinson, C.; Kolb, A.; Shannon, J. (March 1973). "Xe Laser Operation at 1730 Ǻ".Journal of the Optical Society of America.63 (7): 907.doi:10.1364/JOSA.63.000907.
  6. ^"The News in Focus".Laser Focus.9 (5):10–14. May 1973.
  7. ^Ault, E.; Bhaumik, M.; Hughes, W.; Jensen, R.; Robinson, C.; Kolb, A.; Shannon, J. (March 1973). "Xenon molecular laser in the vacuum ultraviolet".IEEE Journal of Quantum Electronics.9 (10):1031–1032.Bibcode:1973IJQE....9.1031A.doi:10.1109/jqe.1973.1077396.ISSN 0018-9197.
  8. ^Basting, Dirk; Pippert, Klaus D.; Stamm, Uwe (2002). "History and future prospects of excimer lasers". In Miyamoto, Isamu; Lu, Yong Feng; Sugioka, Koji; Dubowski, Jan J. (eds.).Second International Symposium on Laser Precision Microfabrication. Vol. 4426. p. 25.doi:10.1117/12.456812.
  9. ^Ewing, J. J.; Brau, C. A. (1975). "Laser action on the2Σ+1/22Σ+1/2 bands of KRF and XeCl".Applied Physics Letters.27 (6):350–352.Bibcode:1975ApPhL..27..350E.doi:10.1063/1.88473.
  10. ^Tisone, G.C.; Hays, A.K.; Hoffman, J.M. (1975). "100 MW, 248.4 nm, KRF laser excited by an electron beam".Optics Communications.15 (2):188–189.Bibcode:1975OptCo..15..188T.doi:10.1016/0030-4018(75)90281-3.
  11. ^Ault, E. R.; Bradford, R. S.; Bhaumik, M. L. (1975). "High-power xenon fluoride laser".Applied Physics Letters.27 (7):413–415.Bibcode:1975ApPhL..27..413A.doi:10.1063/1.88496.
  12. ^Searles, S. K.; Hart, G. A. (1975). "Stimulated emission at 281.8 nm from XeBr".Applied Physics Letters.27 (4):243–245.Bibcode:1975ApPhL..27..243S.doi:10.1063/1.88409.
  13. ^Christensen, C. P.; Waynant, R. W.; Feldman, B. J. (1985). "High efficiency microwave discharge XeCl laser".Applied Physics Letters.46 (4):321–323.Bibcode:1985ApPhL..46..321C.doi:10.1063/1.95617.
  14. ^Microwave discharge resulted in much smaller footprint, very high pulse repetition rate excimer laser, commercialized under U. S. Patent 4,796,271 by Potomac Photonics, Inc,
  15. ^Butcher, Rober R. (1975).A Comprehensive Study of Excimer Lasers, Robert R. Butcher (MSc Thesis). University of New Mexico.
  16. ^IUPAC,Compendium of Chemical Terminology, 5th ed. (the "Gold Book") (2025). Online version: (2006–) "excimer laser".doi:10.1351/goldbook.E02243
  17. ^Basting, D. and Marowsky, G., Eds., Excimer Laser Technology, Springer, 2005.
  18. ^F. J. Duarte (Ed.),Tunable Lasers Handbook (Academic, New York, 1995) Chapter 3.
  19. ^Wolford, M. F.; Hegeler, F.; Myers, M. C.; Giuliani, J. L.; Sethian, J. D. (2004). "Electra: Repetitively pulsed, 500 J, 100 ns, KRF oscillator".Applied Physics Letters.84 (3):326–328.Bibcode:2004ApPhL..84..326W.doi:10.1063/1.1641513.
  20. ^Burnham, R.; Djeu, N. (1976). "Ultraviolet-preionized discharge-pumped lasers in XeF, KRF, and ArF".Applied Physics Letters.29 (11):707–709.Bibcode:1976ApPhL..29..707B.doi:10.1063/1.88934.
  21. ^Original device acquired by the National Museum of American History's Division of Information Technology and Society for the Electricity and Modern Physics Collection (Acquisition #1996.0343).
  22. ^Personal notes of Robert Butcher, Laser Engineer at XMR, Inc.
  23. ^McKee, T. J.; James, D. J.; Nip, W. S.; Weeks, R. W.; Willis, C. (1980). "Lifetime extension of XeCl and KRCL lasers with additives".Applied Physics Letters.36 (12):943–945.Bibcode:1980ApPhL..36..943M.doi:10.1063/1.91658.
  24. ^abcJain, K.; Willson, C. G.; Lin, B. J. (1982). "Ultrafast deep UV Lithography with excimer lasers".IEEE Electron Device Letters.3 (3): 53.Bibcode:1982IEDL....3...53J.doi:10.1109/EDL.1982.25476.
  25. ^abcJain, K."Excimer Laser Lithography", SPIE Press, Bellingham, WA, 1990.
  26. ^abPolasko, K. J.; Ehrlich, D. J.; Tsao, J. Y.; Pease, R. F. W.; Marinero, E. E. (1984). "Deep UV exposure of Ag2Se/GeSe2utilizing an excimer laser".IEEE Electron Device Letters.5 (1): 24.Bibcode:1984IEDL....5...24P.doi:10.1109/EDL.1984.25818.
  27. ^Basting, D.; Djeu, N.; Jain, K. (2005). "Historical Review of Excimer Laser Development".Excimer Laser Technology. pp. 8–21.doi:10.1007/3-540-26667-4_2.ISBN 3-540-20056-8.
  28. ^American Physical Society / Lasers / History / Timeline:http://www.laserfest.org/lasers/history/timeline.cfm
  29. ^SPIE / Advancing the Laser / 50 Years and into the Future(PDF) (Report). Jan 6, 2010.
  30. ^U.K. Engineering & Physical Sciences Research Council / Lasers in Our Lives / 50 Years of Impact:"Archived copy"(PDF). Archived fromthe original(PDF) on 2011-09-13. Retrieved2011-08-22.{{cite web}}: CS1 maint: archived copy as title (link)
  31. ^Lin, B. J.,"Optical Lithography", SPIE Press, Bellingham, WA, 2009, p. 136.
  32. ^La Fontaine, B., "Lasers and Moore's Law", SPIE Professional, Oct. 2010, p. 20.http://spie.org/x42152.xml
  33. ^"Samsung 5 nm and 4 nm Update". WikiChip Fuse. 19 October 2019. Retrieved29 October 2021.
  34. ^Obenschain, Stephen; Lehmberg, Robert; Kehne, David; Hegeler, Frank; Wolford, Matthew; Sethian, John; Weaver, James; Karasik, Max (2015). "High-energy krypton fluoride lasers for inertial fusion".Applied Optics.54 (31): F103-22.Bibcode:2015ApOpt..54F.103O.doi:10.1364/AO.54.00F103.OSTI 1222231.PMID 26560597.
  35. ^US 4784135, "Far ultraviolet surgical and dental procedures", issued 1988-10-15 
  36. ^"IBM News Release". IBM. 2012-12-21. Archived fromthe original on December 31, 2012. Retrieved21 December 2012.
  37. ^R. Linsker; R. Srinivasan; J. J. Wynne; D. R. Alonso (1984). "Far-ultraviolet laser ablation of atherosclerotic lesions".Lasers Surg. Med.4 (1):201–206.doi:10.1002/lsm.1900040212.PMID 6472033.S2CID 12827770.
  38. ^Hartmann Schatloff D, Retamal Altbir C, Valenzuela F (2024)."The role of excimer light in dermatology: a review".Brazilian Annals of Dermatology.99 (6):887–894.doi:10.1016/j.abd.2023.12.007.PMC 11551234.PMID 39107199.
  39. ^Li SM, Kang MT, Zhou Y, Wang NL, Lindsley K (2017)."Wavefront excimer laser refractive surgery for adults with refractive errors".Cochrane Database Syst Rev.6 (6) CD012687.doi:10.1002/14651858.CD012687.PMC 6481747.
  40. ^Duarte, F. J. and Hillman, L. W. (Eds.),Dye Laser Principles (Academic, New York, 1990) Chapter 6.
  41. ^Tallman, C. and Tennant, R., Large-scale excimer-laser-pumped dye lasers, inHigh Power Dye Lasers, Duarte, F. J. (Ed.) (Springer, Berlin, 1991) Chapter 4.
  42. ^Chrisey, D.B. and Hubler, G.K.,Pulsed Laser Deposition of Thin Films (Wiley, 1994),ISBN 9780471592181, Chapter 2.
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