SU1254336A1 - Method of measuring losses in optical waveguides - Google Patents
Method of measuring losses in optical waveguides Download PDFInfo
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- SU1254336A1 SU1254336A1 SU843808494A SU3808494A SU1254336A1 SU 1254336 A1 SU1254336 A1 SU 1254336A1 SU 843808494 A SU843808494 A SU 843808494A SU 3808494 A SU3808494 A SU 3808494A SU 1254336 A1 SU1254336 A1 SU 1254336A1
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- waveguide
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Abstract
Изобретение относитс к интегральной оптике и позвол ет увеличить точность и упростить способ измерени . Оптическое излучение, расщепленное на два пучка, через крайние неподвижные призмы ввод т в измер емый волновод. Измер ют интенсивности выходного излучени при двух положени х вдоль волновода третьей средней призмы, вьтолненной симметричной с двусторонней св зью, и определ ют потери волновода. 1 ил.The invention relates to integrated optics and permits an increase in the accuracy and simplicity of the measurement method. Optical radiation, split into two beams, through the extreme fixed prisms is introduced into the measured waveguide. The intensities of the output radiation are measured at two positions along the waveguide of the third middle prism, a symmetrical, two-way, symmetrical connection, and the waveguide losses are determined. 1 il.
Description
II
Изобретение относитс к интегралной оптике, к разделу измерени параметров оптических волноводов.The invention relates to integrated optics, to a section for measuring parameters of optical waveguides.
Целью изобретени вл етс увеличение точности и упрощение способа измерени .The aim of the invention is to increase the accuracy and simplify the measurement method.
Способ осуществл етс следующим образом.The method is carried out as follows.
Оптическое излучение расщепл ют на два пучка, которые через крайние неподвижные призмы ввод т в измер емый , волновод. Дл вьшода излучени из волновода используетс треть средн призма, выполненна симметричной с двухсторонней св зью с рав ной эффективностью вывода, В положении I средней призмы выполн ютс , услови Optical radiation is split into two beams, which are inserted into the measured waveguide through the extreme fixed prisms. For the radiation output from the waveguide, a third middle prism is used, made symmetrically with a two-way connection with equal output efficiency. In position I, the middle prism is fulfilled, the conditions
I, , ;I,,;
I I
: :
1 о I,1 o I,
(О(ABOUT
е I, и I, - интенсивности выходных излучений из волновода , осун ествл емых с помощью средней призмы; I и I - интенсивности вводнмос e I and I, are the intensities of the output radiation from the waveguide, which are carried out with the help of an average prism; I and I - the intensity of input
ТО излучени на крайних входных призмах; Ч и h - эффективность вводаTHAT radiation at the extreme input prisms; H and h - input efficiency
о flo fl
излучени на входных призмах; - эффективность выводаradiation at the input prisms; - output efficiency
излучени средней призмы дл двухсторонней св зи в положении I; X и X, - рассто ние точки св зи средней призмы от крайних призм; , d- коэффициент затухани radiation of the middle prism for two-way communication in position I; X and X are the distance between the middle prism and the extreme prisms; d is the attenuation coefficient
света в волноводе. После перемещени средней призмы рассто ние лХ .выполн ютс услови light in the waveguide. After moving the middle prism, the distance lH is fulfilled.
к . -о1{Х,-ЛХ)to -o1 {X, -LH)
5 five
i; i;
))
(2)(2)
где I j и I,., - интенсивности вых:од- ных излучений.из волновода , осуществл емых с помощью средней призмы; - эффективность выводаwhere I j and I,., are the intensities of the outputs: of one radiation. From the waveguide, carried out with the help of an average prism; - output efficiency
излучени средней призмы дл двусторонней св зи в положении II; m - коэффициент флюктуации лазерного излучени за промежуток времени меж- ДУ двум измерени ми. Из системы уравнений (1) и (2) ледует выражение дл потерь в оптиеском волноводеradiation of an average prism for two-way communication in position II; m is the fluctuation coefficient of the laser radiation for the time interval between two measurements. From the system of equations (1) and (2), the expression for the loss in an optical waveguide is investigated
51g 51g
е e
Р лхR lh
2020
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SU843808494A SU1254336A1 (en) | 1984-11-02 | 1984-11-02 | Method of measuring losses in optical waveguides |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SU843808494A SU1254336A1 (en) | 1984-11-02 | 1984-11-02 | Method of measuring losses in optical waveguides |
Publications (1)
Publication Number | Publication Date |
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SU1254336A1 true SU1254336A1 (en) | 1986-08-30 |
Family
ID=21145266
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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SU843808494A SU1254336A1 (en) | 1984-11-02 | 1984-11-02 | Method of measuring losses in optical waveguides |
Country Status (1)
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SU (1) | SU1254336A1 (en) |
-
1984
- 1984-11-02 SU SU843808494A patent/SU1254336A1/en active
Non-Patent Citations (1)
Title |
---|
Интегральна оптика / Под ред. Т.Тамира. М.: Мир, 1978, с.238-242, Аникин В.И, и Горобец А.П. Квантова электроника 2. 1975, с. 1465. * |
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