Organic laser

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Liquid organic dye laser system excited by a copper vapor laser AVLIS laser.jpg
Liquid organic dye laser system excited by a copper vapor laser

An organic laser is a laser which uses an organic (carbon based) material as the gain medium. The first organic laser was the liquid dye laser. [1] [2] These lasers use laser dye solutions as their gain media.

Contents

Organic lasers are inherently tunable and when configured as optimized multiple-prism grating laser oscillators can yield efficient single-transverse mode, and single-longitudinal-mode, emission with laser linewidths as narrow as 350 MHz (approximately 0.0004 nm at a wavelength of 590 nm), in the high-power pulsed regime. [3]

Solid-state dye lasers

Organic solid-state narrow-linewidth tunable dye laser oscillator using a dye-doped polymer as gain medium Duarte's multiple-prism grating laser oscillator.png
Organic solid-state narrow-linewidth tunable dye laser oscillator using a dye-doped polymer as gain medium

Solid-state dye lasers are organic tunable lasers that use a variety of organic gain media, such as laser dye-doped polymers (DDP), [5] laser dye-doped ormosil (DDO), [6] and laser dye-doped polymer-nanoparticle (DDPN) matrices. [7]

DDO and DDPN gain media are subsets of a larger class of organic-inorganic hybrid materials used as laser matrices. [8] [9]

Organic semiconductor laser

Other types of solid-state organic lasers include the organic semiconductor lasers that use conjugated polymers as gain media. [10] [11] [12] [13] These semiconductor materials can also be configured as "neat films." [14]

Coherent emission, characterized via high-visibility double-slit interferograms (V ~ 0.9) and near diffraction-limited beam divergence, has been reported from electrically pumped coumarin dye-doped tandem OLED devices. [15]

Distributed feedback laser

Organic lasers are also available in distributed feedback configurations [16] [17] and distributed feedback waveguides. [18]

See also

Related Research Articles

<span class="mw-page-title-main">Dye laser</span> Equipment using an organic dye to emit coherent light

A dye laser is a laser that uses an organic dye as the lasing medium, usually as a liquid solution. Compared to gases and most solid state lasing media, a dye can usually be used for a much wider range of wavelengths, often spanning 50 to 100 nanometers or more. The wide bandwidth makes them particularly suitable for tunable lasers and pulsed lasers. The dye rhodamine 6G, for example, can be tuned from 635 nm (orangish-red) to 560 nm (greenish-yellow), and produce pulses as short as 16 femtoseconds. Moreover, the dye can be replaced by another type in order to generate an even broader range of wavelengths with the same laser, from the near-infrared to the near-ultraviolet, although this usually requires replacing other optical components in the laser as well, such as dielectric mirrors or pump lasers.

<span class="mw-page-title-main">Tunable laser</span>

A tunable laser is a laser whose wavelength of operation can be altered in a controlled manner. While all laser gain media allow small shifts in output wavelength, only a few types of lasers allow continuous tuning over a significant wavelength range.

<span class="mw-page-title-main">Theodor W. Hänsch</span> German physicist and nobel laureate

Theodor Wolfgang Hänsch is a German physicist. He received one-third of the 2005 Nobel Prize in Physics for "contributions to the development of laser-based precision spectroscopy, including the optical frequency comb technique", sharing the prize with John L. Hall and Roy J. Glauber.

<span class="mw-page-title-main">Solid-state laser</span> Laser which uses a solid gain medium

A solid-state laser is a laser that uses a gain medium that is a solid, rather than a liquid as in dye lasers or a gas as in gas lasers. Semiconductor-based lasers are also in the solid state, but are generally considered as a separate class from solid-state lasers, called laser diodes.

Amplified spontaneous emission (ASE) or superluminescence is light, produced by spontaneous emission, that has been optically amplified by the process of stimulated emission in a gain medium. It is inherent in the field of random lasers.

A fiber laser is a laser in which the active gain medium is an optical fiber doped with rare-earth elements such as erbium, ytterbium, neodymium, dysprosium, praseodymium, thulium and holmium. They are related to doped fiber amplifiers, which provide light amplification without lasing.

Ormosil is a shorthand phrase for organically modified silica or organically modified silicate. In general, ormosils are produced by adding silane to silica-derived gel during the sol-gel process. They are engineered materials that show great promise in a wide range of applications such as:

<span class="mw-page-title-main">F. J. Duarte</span>

Francisco Javier "Frank" Duarte is a laser physicist and author/editor of several books on tunable lasers.

Beam expanders are optical devices that take a collimated beam of light and expand its width.

<span class="mw-page-title-main">Multiple-prism dispersion theory</span> Theory in optics

The first description of multiple-prism arrays, and multiple-prism dispersion, was given by Newton in his book Opticks. Prism pair expanders were introduced by Brewster in 1813. A modern mathematical description of the single-prism dispersion was given by Born and Wolf in 1959. The generalized multiple-prism dispersion theory was introduced by Duarte and Piper in 1982.

<span class="mw-page-title-main">Laser medicine</span>

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Fritz Peter Schäfer was a German physicist, born in Hersfeld, Hesse-Nassau. He is the co-inventor of the organic dye laser. His book, Dye Lasers, is considered a classic in the field of tunable lasers. In this book the chapter written by Schäfer gives an ample and insightful exposition on organic laser dye molecules in addition to a description on the physics of telescopic, and multiple-prism, tunable narrow-linewidth laser oscillators.

<span class="mw-page-title-main">Solid-state dye laser</span>

A solid-state dye laser (SSDL) is a solid-state lasers in which the gain medium is a laser dye-doped organic matrix such as poly(methyl methacrylate) (PMMA), rather than a liquid solution of the dye. These lasers are also referred to as solid-state organic lasers and solid-state dye-doped polymer lasers.

Gas in scattering media absorption spectroscopy (GASMAS) is an optical technique for sensing and analysis of gas located within porous and highly scattering solids, e.g. powders, ceramics, wood, fruit, translucent packages, pharmaceutical tablets, foams, human paranasal sinuses etc. It was introduced in 2001 by Prof. Sune Svanberg and co-workers at Lund University (Sweden). The technique is related to conventional high-resolution laser spectroscopy for sensing and spectroscopy of gas, but the fact that the gas here is "hidden" inside solid materials give rise to important differences.

<span class="mw-page-title-main">Multiple-prism grating laser oscillator</span>

Multiple-prism grating laser oscillators, or MPG laser oscillators, use multiple-prism beam expansion to illuminate a diffraction grating mounted either in Littrow configuration or grazing-incidence configuration. Originally, these narrow-linewidth tunable dispersive oscillators were introduced as multiple-prism Littrow (MPL) grating oscillators, or hybrid multiple-prism near-grazing-incidence (HMPGI) grating cavities, in organic dye lasers. However, these designs were quickly adopted for other types of lasers such as gas lasers, diode lasers, and more recently fiber lasers.

Laser linewidth is the spectral linewidth of a laser beam.

A liquid-crystal laser is a laser that uses a liquid crystal as the resonator cavity, allowing selection of emission wavelength and polarization from the active laser medium. The lasing medium is usually a dye doped into the liquid crystal. Liquid-crystal lasers are comparable in size to diode lasers, but provide the continuous wide spectrum tunability of dye lasers while maintaining a large coherence area. The tuning range is typically several tens of nanometers. Self-organization at micrometer scales reduces manufacturing complexity compared to using layered photonic metamaterials. Operation may be either in continuous wave mode or in pulsed mode.

Organic photorefractive materials are materials that exhibit a temporary change in refractive index when exposed to light. The changing refractive index causes light to change speed throughout the material and produce light and dark regions in the crystal. The buildup can be controlled to produce holographic images for use in biomedical scans and optical computing. The ease with which the chemical composition can be changed in organic materials makes the photorefractive effect more controllable.

<span class="mw-page-title-main">International Conference of Laser Applications</span>

The International Conference on Lasers and Applications, Lasers 'XX was an annual conference organized by the former Society for Optical and Quantum Electronics. The conference, known in short by Lasers 'XX, was held at various locations in The United States from 1978 to 2000.

<span class="mw-page-title-main">Organic photonics</span>

Organic photonics includes the generation, emission, transmission, modulation, signal processing, switching, amplification, and detection/sensing of light, using organic optical materials.

References

  1. Sorokin, P. P.; Lankard, J. R. (1966). "Stimulated Emission Observed from an Organic Dye, Chloro-aluminum Phthalocyanine". IBM Journal of Research and Development. IBM. 10 (2): 162–163. doi:10.1147/rd.102.0162. ISSN   0018-8646.
  2. Schäfer, Fritz P.; Schmidt, Werner; Volze, Jürgen (1966-10-15). "Organic dye solution laser". Applied Physics Letters. AIP Publishing. 9 (8): 306–309. doi: 10.1063/1.1754762 . ISSN   0003-6951.
  3. Duarte, Francisco J. (1999-10-20). "Multiple-prism grating solid-state dye laser oscillator: optimized architecture". Applied Optics. The Optical Society. 38 (30): 6347–6349. doi:10.1364/ao.38.006347. ISSN   0003-6935. PMID   18324163.
  4. Duarte, Francisco J.; Taylor, Travis S.; Costela, Angel; Garcia-Moreno, Inmaculada; Sastre, Roberto (1998-06-20). "Long-pulse narrow-linewidth dispersive solid-state dye-laser oscillator". Applied Optics. The Optical Society. 37 (18): 3987–3989. doi:10.1364/ao.37.003987. ISSN   0003-6935. PMID   18273368.
  5. Soffer, B. H.; McFarland, B. B. (1967-05-15). "Continuously tunable narrow-band organic dye lasers". Applied Physics Letters. AIP Publishing. 10 (10): 266–267. doi:10.1063/1.1754804. ISSN   0003-6951.
  6. B. S. Dunn, J. D. Mackenzie, J. I. Zink, and O. M. Stafsudd, Solid-state tunable lasers based on dye-doped sol-gel materials, Proc. SPIE1328, 174-182 (1990). doi : 10.1117/12.22557
  7. Duarte, F. J.; James, R. O. (2003-11-01). "Tunable solid-state lasers incorporating dye-doped, polymer– nanoparticle gain media". Optics Letters. The Optical Society. 28 (21): 2088–2090. doi:10.1364/ol.28.002088. ISSN   0146-9592. PMID   14587824.
  8. A. Costela, I. Garcia-Moreno, R. Sastre, Solid-state dye lasers, in Tunable Laser Applications, 2nd Edition, F. J. Duarte, Ed. (CRC, New York, 2009) Chapter 3.
  9. Costela, A.; Cerdán, L.; García-Moreno, I. (2013). "Solid state dye lasers with scattering feedback". Progress in Quantum Electronics. Elsevier BV. 37 (6): 348–382. doi:10.1016/j.pquantelec.2013.10.001. ISSN   0079-6727.
  10. Samuel, I. D. W.; Turnbull, G. A. (2007). "Organic Semiconductor Lasers". Chemical Reviews. American Chemical Society (ACS). 107 (4): 1272–1295. doi:10.1021/cr050152i. ISSN   0009-2665. PMID   17385928. S2CID   46525744.
  11. C. Karnutsch, Low Threshold Organic Thin Film Laser Devices (Cuvillier, Göttingen, 2007).
  12. Kuehne, Alexander J. C.; Gather, Malte C. (2016-08-08). "Organic Lasers: Recent Developments on Materials, Device Geometries, and Fabrication Techniques". Chemical Reviews. American Chemical Society (ACS). 116 (21): 12823–12864. doi:10.1021/acs.chemrev.6b00172. hdl: 10023/11411 . ISSN   0009-2665. PMID   27501192.
  13. Patil, N. (2006). "Optical Pumping in Polymer Lasers: Advances and Challenges". Optics and Photonics News. Optical Society of America (OSA). 17 (5): 37–41. doi:10.1364/OPN.17.5.000037. ISSN   1047-6938.
  14. Bansal, A.K.; Penzkofer, A. (2008). "Linear and nonlinear optical spectroscopic characterisation of triphenylamine and 1,2,3-tris(3-methylphenylphenylamino)benzene". Chemical Physics. Elsevier BV. 352 (1–3): 48–56. doi:10.1016/j.chemphys.2008.05.006. ISSN   0301-0104.
  15. Duarte, F. J.; Liao, L. S.; Vaeth, K. M. (2005-11-15). "Coherence characteristics of electrically excited tandem organic light-emitting diodes". Optics Letters. The Optical Society. 30 (22): 3072–3074. doi:10.1364/ol.30.003072. ISSN   0146-9592. PMID   16315725.
  16. Wadsworth, W.J.; McKinnie, I.T.; Woolhouse, A.D.; Haskell, T.G. (1999-08-01). "Efficient distributed feedback solid state dye laser with a dynamic grating". Applied Physics B: Lasers and Optics. Springer Science and Business Media LLC. 69 (2): 163–165. doi:10.1007/s003400050791. ISSN   0946-2171. S2CID   122330477.
  17. Zhu, Xiao-Lei; Lam, Sio-Kuan; Lo, Dennis (2000-06-20). "Distributed-feedback dye-doped solgel silica lasers". Applied Optics. The Optical Society. 39 (18): 3104–3107. doi:10.1364/ao.39.003104. ISSN   0003-6935. PMID   18345240.
  18. Oki, Yuji; Miyamoto, Shinichi; Tanaka, Masamitsu; Zuo, Duluo; Maeda, Mitsuo (2002). "Long lifetime and high repetition rate operation from distributed feedback plastic waveguided dye lasers". Optics Communications. Elsevier BV. 214 (1–6): 277–283. doi:10.1016/s0030-4018(02)02125-9. ISSN   0030-4018.