Abstract:Chalcogenide glass fibers have attractive properties (e.g. wide transparent window, high optical non-linearity) and numerous potential applications in the mid-infrared (MIR) region. Low optical loss is desired and important in the development of these fibers. Ge-As-Se glass has a large glass-forming range to provide versatility of choice from continuously varying physical properties. Recently, broadband MIR supercontinuum generation has been achieved in chalcogenide fibers by using Ge-As-Se glass in the core/c… Show more
“…One should note, that compared with RFs made of silica glass, the solid-core non-silica fibers have lower optical losses in the mid-IR. For example, optical losses less than 0.1 dB/m were demonstrated in fluoroindate fibers in the 2.0-4.5 μm spectral range [36] and in chalcogenide fibers at a wavelength of up to 6.5 μm [37,38]. At an even longer wavelength (8-16 μm), the silver halides fibers with optical losses below 1 dB/m are available [39].…”
Section: Rf With Various Cladding Structuresmentioning
confidence: 99%
“…More details are given in the text [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. [36] and in chalcogenide fibers at a wavelength of up to 6.5 µm [37,38]. At an even longer wavelength (8-16 µm), the silver halides fibers with optical losses below 1 dB/m are available [39].…”
Section: Rfs With Touching and Non-touching Capillaries In A Claddingmentioning
Revolver optical fibers (RF) are special type of hollow-core optical fibers with negative curvature of the core-cladding boundary and with cladding that is formed by a one ring layer of capillaries. The physical mechanisms contributing to the waveguiding parameters of RFs are discussed. The optical properties and possible applications of RFs are reviewed. Special attention is paid to the mid-IR hydrogen Raman lasers that are based on RFs and generating in the wavelength region from 2.9 to 4.4 μm.
“…One should note, that compared with RFs made of silica glass, the solid-core non-silica fibers have lower optical losses in the mid-IR. For example, optical losses less than 0.1 dB/m were demonstrated in fluoroindate fibers in the 2.0-4.5 μm spectral range [36] and in chalcogenide fibers at a wavelength of up to 6.5 μm [37,38]. At an even longer wavelength (8-16 μm), the silver halides fibers with optical losses below 1 dB/m are available [39].…”
Section: Rf With Various Cladding Structuresmentioning
confidence: 99%
“…More details are given in the text [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. [36] and in chalcogenide fibers at a wavelength of up to 6.5 µm [37,38]. At an even longer wavelength (8-16 µm), the silver halides fibers with optical losses below 1 dB/m are available [39].…”
Section: Rfs With Touching and Non-touching Capillaries In A Claddingmentioning
Revolver optical fibers (RF) are special type of hollow-core optical fibers with negative curvature of the core-cladding boundary and with cladding that is formed by a one ring layer of capillaries. The physical mechanisms contributing to the waveguiding parameters of RFs are discussed. The optical properties and possible applications of RFs are reviewed. Special attention is paid to the mid-IR hydrogen Raman lasers that are based on RFs and generating in the wavelength region from 2.9 to 4.4 μm.
“…They have low phonon energy, transparency within the wavelength range 0.6-25 m [13,14] and are robust enough for development as MIR fiber-optics' and SNIM tips. For instance, we have recently reported ultra-low (83 dB/km [15]) loss GeAsSe based optical fibers, exhibiting loss of<10 dB/m across 1-12 m, which encompasses the region of interest for SNIM of human cells and tissue [11,12].…”
Section: B Mir-transmitting Glass Tapered-tips For Snimmentioning
“…The observed photoluminescence lifetimes are near to the radiative lifetimes predicted by the Judd-Ofelt theory. The fiber attenuation has been driven down to the dB/km level [14,15]. Lanthanide ion concentrations of up to 2000 ppm without crystallization have been achieved [6].…”
This paper presents the progress in the fields of the modelling and design of lanthanide ion-doped chalcogenide glass fiber lasers. It presents laser cavity designs that have been developed in order to optimize the performance of lanthanide ion-doped chalcogenide glass fiber lasers. Additionally, various numerical algorithms that have been applied for the optimization of chalcogenide glass lasers are reviewed and compared. The comparison shows that a combination of less accurate but more robust algorithms with more accurate ones gives the most promising performance.
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