1972
DOI: 10.1364/ao.11.002729
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History of Optics at Itek

Abstract: Itek Corporation was founded in 1957. A major business quickly developed in the manufacture of large precision optical systems principally for aerospace photography. While the company is now highly diversified, this work continues as a major activity. This article discusses the work of the group especially in the field of image formation as it has been described in the scientific literature. An outline is given of the historical roots in earlier laboratory programs beginning at Boston University in 1946 and at… Show more

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Cited by 4 publications
(4 citation statements)
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“…SBS is one of the highest gain material-level nonlinearities in optics [15] making it one of Department of Mechanical Science and Engineering, University of Illinois at Urbana-Champaign, 1206 W. Green St., Urbana, Illinois, USA 61801 * Corresponding author: e-mail: bahl@illinois.edu the first nonlinear effects to appear in high energy density systems such as high power fiber lasers and high quality factor resonators. The suppression of SBS is thus particularly important in laser systems as it represents a parasitic loss effect and prevents further power scaling of the source [24,25].…”
Section: Introductionmentioning
confidence: 99%
“…SBS is one of the highest gain material-level nonlinearities in optics [15] making it one of Department of Mechanical Science and Engineering, University of Illinois at Urbana-Champaign, 1206 W. Green St., Urbana, Illinois, USA 61801 * Corresponding author: e-mail: bahl@illinois.edu the first nonlinear effects to appear in high energy density systems such as high power fiber lasers and high quality factor resonators. The suppression of SBS is thus particularly important in laser systems as it represents a parasitic loss effect and prevents further power scaling of the source [24,25].…”
Section: Introductionmentioning
confidence: 99%
“…For the fiber used here, A eff is 5.0 · 10~1 1 m 2 and L eff is 17 km. The g B is given by [3], where n is core index, p 12 the elastic optical constant, c the light velocity, ρ the density, and v a the acoustic velocity. As well, k is the polarization factor, which is unity for a polarization-maintaining fiber and 1/2 otherwise.…”
Section: Discussionmentioning
confidence: 99%
“…The amplifier using Raman scattering is well known as a broadband light amplifier for high-bit-rate signals such as optical soliton [1,2]. On the other hand, backward Brillouin scattering is very attractive for a narrowband amplifier since the threshold level of Brillouin scattering, which is typically a few milliwatts, is much lower than that of Raman scattering [3][4][5]. Therefore, the Brillouin amplifier, although with a narrow gain width, has large potential for systems at a bit-rate of less than a few hundred Mbit/s employed with laser diodes and single-mode fibers.…”
Section: Introductionmentioning
confidence: 99%
“…However, when an ultimately low-loss optical fiber is used, the transmission power is limited by the stimulated Brillouin scattering (SBS) below several milliwatts [1,2]. When the bit rate is very high and an appropriate modulation scheme is employed, the SBS limitation can be relaxed to some extent [3,4].…”
Section: Introductionmentioning
confidence: 99%