1978
DOI: 10.1364/ao.17.002224
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Spectrally narrow pulsed dye laser without beam expander

Abstract: We have developed a simplified version of the side-pumped pulsed dye laser which has a spectral halfwidth of 1.25 GHz and a peak power of 10 kW at 600 nm. The basic laser consists of only four components (output mirror, dye cell, diffraction grating, and tuning mirror) and is exceptionally easy to align. Since the beam expander has been eliminated, the laser cavity can be made quite compact. Under the condition of reduced gain, the laser has been operated in a single mode.

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Cited by 600 publications
(179 citation statements)
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“…The weaker, hom e bui l t pro b e dye l aser (Li ttm an-t yp e design [12], spectra l wi dth about 1 cm À 1 , pum p ed synchro no usly by the same exci mer l aser), was opera ted wi th a Rho da mi ne 6G / 110 mi xture, and was set at a Ùxed wa velength resona nt wi th a few ro vi bro ni c tra nsiti ons i n the B 1 Î ê X 1 Ï + system of KLi , kno wn f rom our previ ous hi gh resol uti on studi es [7,8], thus l ab ell i ng selected ro vi bra ti ona l levels i n the gro und sta te. For perm anent contro l of the pro b e l aser frequency duri ng the m easurem ents, we ha ve chosen eight Ùxed wavel engths coi nci di ng wi th stro ng opto gal vani c l ines o f arg on.…”
Section: Introductionmentioning
confidence: 99%
“…The weaker, hom e bui l t pro b e dye l aser (Li ttm an-t yp e design [12], spectra l wi dth about 1 cm À 1 , pum p ed synchro no usly by the same exci mer l aser), was opera ted wi th a Rho da mi ne 6G / 110 mi xture, and was set at a Ùxed wa velength resona nt wi th a few ro vi bro ni c tra nsiti ons i n the B 1 Î ê X 1 Ï + system of KLi , kno wn f rom our previ ous hi gh resol uti on studi es [7,8], thus l ab ell i ng selected ro vi bra ti ona l levels i n the gro und sta te. For perm anent contro l of the pro b e l aser frequency duri ng the m easurem ents, we ha ve chosen eight Ùxed wavel engths coi nci di ng wi th stro ng opto gal vani c l ines o f arg on.…”
Section: Introductionmentioning
confidence: 99%
“…5. They are named Littrow (due to the Littrow retro-diffraction geometry) and Littman or grazing-incidence configurations (sometimes referred to as Littman/Metcalf's [56,57]). The lasing wavelength in each of these designs is determined by the centre of the grating dispersion curve, which is given by the well-known grating equation…”
Section: Littrow and Littman Configurationsmentioning
confidence: 99%
“…This year we welcome the 50th anniversary of the laser technology, which has powered remarkable progress [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] in the past 50 years since the invention of the first laser in 1960 [19]. Fiber lasers are one kind of the most important lasers, which also include multi-wavelength fiber lasers (MWFLs) with a huge potential in applications such as WDM optical communication systems, optical fiber sensors, optical component testing, microwave photonics and spectroscopy [20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%