1980
DOI: 10.1109/tmtt.1980.1130115
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Transmission Characteristics of Dielectric Tube Leaky Waveguide

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Cited by 31 publications
(14 citation statements)
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“…It is possible to significantly reduce the optical losses of such a fiber by increasing the reflection coefficient from the core-cladding interface e.g., by reflection from two surfaces, using as a waveguide, a capillary with a thin glass wall (tube waveguide-TW) and constructive interference of radiation that is reflected from both surfaces of the capillary. Such a fiber was considered in [11], and it can be taken as a second approximation to RF (model TW). In this case, the capillary wall serves as a Fabry-Perot interferometer, the transmission spectrum of the optical fiber, respectively, acquires a band structure.…”
Section: Physical Demonstrative Approach To the Waveguiding Propertiementioning
confidence: 99%
See 1 more Smart Citation
“…It is possible to significantly reduce the optical losses of such a fiber by increasing the reflection coefficient from the core-cladding interface e.g., by reflection from two surfaces, using as a waveguide, a capillary with a thin glass wall (tube waveguide-TW) and constructive interference of radiation that is reflected from both surfaces of the capillary. Such a fiber was considered in [11], and it can be taken as a second approximation to RF (model TW). In this case, the capillary wall serves as a Fabry-Perot interferometer, the transmission spectrum of the optical fiber, respectively, acquires a band structure.…”
Section: Physical Demonstrative Approach To the Waveguiding Propertiementioning
confidence: 99%
“…(a) Cross-(1) and longitudinal (2) sections of the hollow waveguide [10]; (b) Cross-(1) and longitudinal (2) sections of the tube waveguide [11]; (c) Cross-section (1) of the RF [1], approximation of the part of the walls of the reflecting capillaries by the mirror sides of the angle α (2), a reflection scheme of a ray propagating along the RF, from a corner with mirror sides (a projection onto the cross section of the optical fiber) (3); and, (d) Calculated optical loss spectrum for silica fibers: hollow waveguide (HW), tube waveguide (TW) and RF. For all waveguides, the hollow core diameter is assumed to be 77 µm, and the thickness of the capillary wall (for TW and RF) is 1.15 µm.…”
Section: Physical Demonstrative Approach To the Waveguiding Propertiementioning
confidence: 99%
“…Nevertheless, their proposed solid plastic waveguide was rectangular which was not intended for the single-mode operation and was limited in link-distance due to the high dielectric loss of polyethylene at mm-Wave frequencies. To alleviate such disadvantages, we propose to 1) replace the solid rectangular waveguide with a hollow plastic cable to transmit energy mostly within the air-core; 2) maintain mm-Wave signal through a cylindrical cable under a circular HE11 single-mode operation [9], [10]. The proposed data link via a hollow plastic cable is explained in Fig.…”
Section: Proposed System Architecturementioning
confidence: 99%
“…The innermost thin glass wall supported by a glass microstructure optically functions and confines the light in the core [7,8]. However, Miyagi and Nishida proposed this type of waveguide with a circular core as a tubeleaky waveguide in 1980 [9], before ARROW waveguides were proposed. In that paper, they analytically explained In this paper, we designed and fabricated large-core tube-leaky waveguides for Er:YAG lasers that are commonly used in medical laser applications such as tissue cutting and dental drilling utilizing the high absorption coefficient for water contained in skin and tissue [10].…”
Section: Introductionmentioning
confidence: 99%