WO2002033460A1 - Dispositif de réseau à fibre optique - Google Patents
Dispositif de réseau à fibre optique Download PDFInfo
- Publication number
- WO2002033460A1 WO2002033460A1 PCT/JP2001/007547 JP0107547W WO0233460A1 WO 2002033460 A1 WO2002033460 A1 WO 2002033460A1 JP 0107547 W JP0107547 W JP 0107547W WO 0233460 A1 WO0233460 A1 WO 0233460A1
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- WO
- WIPO (PCT)
- Prior art keywords
- optical fiber
- region
- refractive index
- cladding region
- cutoff
- Prior art date
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02057—Optical fibres with cladding with or without a coating comprising gratings
- G02B6/02076—Refractive index modulation gratings, e.g. Bragg gratings
- G02B6/0208—Refractive index modulation gratings, e.g. Bragg gratings characterised by their structure, wavelength response
- G02B6/021—Refractive index modulation gratings, e.g. Bragg gratings characterised by their structure, wavelength response characterised by the core or cladding or coating, e.g. materials, radial refractive index profiles, cladding shape
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02057—Optical fibres with cladding with or without a coating comprising gratings
- G02B6/02076—Refractive index modulation gratings, e.g. Bragg gratings
- G02B6/0208—Refractive index modulation gratings, e.g. Bragg gratings characterised by their structure, wavelength response
- G02B6/02085—Refractive index modulation gratings, e.g. Bragg gratings characterised by their structure, wavelength response characterised by the grating profile, e.g. chirped, apodised, tilted, helical
- G02B6/02095—Long period gratings, i.e. transmission gratings coupling light between core and cladding modes
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03622—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only
- G02B6/03633—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only arranged - -
Definitions
- the present invention relates to an optical component suitably used in optical communication and the like, and more particularly to an optical fiber grating element having a long period grating formed in a core region of an optical fiber.
- the long-period grating is different from a short-period grating that reflects light of a specific wavelength, as disclosed in, for example, US Pat. Of these, those with specific wavelengths are converted into clad mode light, and the clad mode light is emitted outside the cladding region.
- An optical fiber grating in which a long-period grating is formed in the core region of the optical fiber is coupled between the core mode light of a predetermined wavelength and the cladding mode light through periodic perturbation of the grating.
- the optical fiber grating element selectively shifts the wavelength of the core mode light having the predetermined wavelength to the clad mode light.
- the core mode light is light of a mode that is confined and propagated in the core region of the optical fiber.
- the cladding mode light is a mode light radiated to the cladding region around the core region without being confined in the core region of the optical fiber.
- Such an optical fiber grating element is an optical fiber filter that selectively blocks core mode light of a predetermined wavelength (cutoff wavelength) among core mode lights of a certain wavelength band transmitted through an optical fiber in the field of optical communication and the like. It is used as a sunset.
- the cladding mode is a mode that takes into account the entire optical fiber defined by the boundary between the cladding region and the outer air layer or coating layer. Therefore, when the refractive index of the outer layer changes, the wavelength at which the coupling from the core mode light to the cladding mode light occurs, that is, the shielding, The cutoff wavelength also shifts, and the cutoff amount of core mode light at the cutoff wavelength also changes.
- the optical fiber is coated with a resin having a refractive index close to that of glass, the cladding mode is not formed, and the cutoff wavelength in the optical fiber grating element disappears. Therefore, the optical fiber grating element has a problem that it cannot be coated for the purpose of protection.
- An optical fiber grating device disclosed in Japanese Patent Application Laid-Open No. 11-326654 has been proposed to address such a problem, and has a refractive index of a silica-based dual shaved core (DSC) structure.
- DSC silica-based dual shaved core
- This is a single mode optical fiber having a profile, in which a long period grating is formed.
- the refractive index profile of the DSC structure but from the center of the optical axis of the structure including the first core area of the refractive index rii, the second core region and a cladding region of refractive index n 3 of the refractive index n 2 in order Yes (but! ⁇ >! ⁇ >! ⁇ ).
- the optical fiber grating device both the first core region Contact Yopi second core region of the optical fiber was added GeO 2, which is irradiated with spatial intensity ultraviolet light modulation has been performed, these A refractive index modulation, that is, a grating is formed over two regions. Then, the optical fiber grating element couples the core mode light having a predetermined wavelength propagating in the first core region to the higher mode light propagating in both the first core region and the second core region, and Blocks core mode light of wavelength.
- a preferable refractive index profile in the optical fiber grating element disclosed in this publication is such that the relative refractive index difference of the first core region is in the range of 0.8% to 1.0%, and that of the second core region.
- the relative refractive index difference is in the range of 0.05% to 0.15%, and the radius of the first core region is 3.2 ⁇ ! ⁇ 3.8 m, and the radius of the second core area is 1! 22 O m. Disclosure of the invention
- the inventors have found the following problems as a result of studying the above-described conventional technology. That is, since the number of higher-order modes propagating in both the first core region and the second core region is small in this optical fiber grating element, the number of cut-off wavelength peaks is about one or two in the used wavelength band. Become. Therefore, the grating period is set when forming the grating so as to obtain a desired cutoff wavelength in the optical fiber grating, but the degree of freedom in setting the grating period is small.
- the coupling coefficient between the core mode light of a predetermined wavelength propagating in the first core region and the higher-order mode light propagating in both the first core region and the second core region is large, the ultraviolet light
- the change in the cutoff amount and the cutoff wavelength with respect to the increase in the refractive index due to the irradiation is large, and it is difficult to adjust the cutoff amount and the cutoff wavelength to be both compatible.
- the present invention has been made to solve the above problems, and has as its object to provide an optical fiber grating having a high degree of freedom in setting a grating period and capable of easily adjusting a cutoff amount and a cutoff wavelength.
- An optical fiber grating element comprises: a core region having a refractive index ri i and an outer diameter 2 a; a first cladding region surrounding the core region and having a refractive index n 2 and an outer diameter 2 b; a second cladding region having a refractive index n 3 and an outside diameter 2 c surrounding the first cladding region, an optical fiber grating device long period gray coating was formed in the core region of an optical fiber with a.
- the relative refractive index difference between the first cladding region and the second cladding region is 0.5% or more.
- the thickness (c ⁇ b) of the second cladding region is in the range of not less than 10 and not more than 10 to the cutoff peak wavelength.
- this optical fiber grating element the number of cutoff peaks in a predetermined wavelength band (for example, 1.2 / m to 1.8 / zm) is large, and the interval between cutoff peaks is small. Further, the coupling coefficient between the core mode light and the higher-order mode light propagating in the first cladding region is small, and the variation of the cutoff amount and the cutoff wavelength with respect to the change in the refractive index is reduced. In addition, the effect of the layer further outside the second cladding region is small, the blocking characteristics are stable, Excellent blocking effect in grating. Therefore, this optical fiber grating has a large degree of freedom in setting the grating period, easily adjusts the cutoff amount and the cutoff wavelength, and has excellent cutoff characteristics.
- a predetermined wavelength band for example, 1.2 / m to 1.8 / zm
- the relative refractive index difference between the first cladding region and the second cladding region is preferably 0.5% or more and 1.5% or less.
- Second Kuradzudo region The addition of F element, it is possible to reduce the refractive index n 3 of the refractive index n 2 yo Ri second cladding region of the first Kuradzudo region, first Kuradzudo against the second cladding region
- the relative refractive index difference of the region can be increased to 1.5%.
- the optical fiber grating element it is preferable that a resin coating having a refractive index of n 4 (where n 4 > n 2 ) is provided around the second cladding region.
- n 4 refractive index of n 4
- the higher-order mode light generated by the mode coupling at the cut-off wavelength is easily emitted to the outside of the optical fiber, which is preferable. It is also suitable for protecting the optical fiber grating element.
- the outer diameter 2b of the first cladding region is 10 or more. This is preferable in that the number of cutoff peaks is increased, and is also preferable in that the cutoff effect is excellent.
- the mode field diameter of the fundamental mode light propagating in the core region is 1/10 or less of the outer diameter 2b of the first cladding region. This is preferable in that the number of cutoff peaks increases, and is also preferable in that the cutoff effect is excellent.
- FIG. 1 is a cross-sectional view of the optical fiber grating element according to the present embodiment. It shows a cross section when cut along a plane including an axis.
- FIG. 2 is a diagram showing a refractive index profile of the optical fiber grating element according to the present embodiment.
- FIG. 3 is a graph showing a transmission spectrum of the optical fiber grating element.
- FIG. 4 is a graph showing the relationship between the loss change amount ⁇ and the thickness (c ⁇ b) of the second cladding region in the optical fiber grating element.
- Figure 5 is a graph showing the relationship between the relative refractive index difference delta eta 2 of the number of cut-off peak in the optical fiber grating element and the first Kuradzu de area.
- FIG. 6 is a graph showing the relationship between the number of cutoff peaks in the optical fiber grating and the outer diameter 2b of the first cladding region.
- FIG. 7 is a graph showing the relationship between the shift amount of the cutoff peak wavelength and the irradiation time of ultraviolet light when forming the grating of the optical fiber grating element.
- FIG. 1 is a cross-sectional view of the optical fiber grating element 1 according to the present embodiment, and shows a cross section of the optical fiber 10 cut along a plane including the optical axis.
- FIG. 2 is a diagram showing a refractive index profile of the optical fiber grating element 1 according to the present embodiment.
- the optical fiber grating element 1 according to the present embodiment has a long-period grating 14 in an optical fin 10 having a core region 11, a first cladding region 12 and a second cladding region 13 in order from the optical axis center.
- the optical fins I0 are provided with a resin coating 20 around them.
- the core region 11 of the optical fiber 10 includes the center of the optical axis, has a refractive index of 2, has an outer diameter of 2a, and has a long-period grating 14 formed in a predetermined region.
- First Kuradzu de region 1 2 surrounds the core region 1 1, the refractive index is an n 2, an outer diameter of 2 b.
- the second cladding region 13 takes this first cladding region 12
- the box has a refractive index of n 3 and an outer diameter of 2 c (typically 125 zm). Resin to be covered 20 is provided around the second cladding region 13, a refractive index of n 4.
- the relationship between the refractive indices of the core region 11, the first cladding region 12, the second cladding region 13, and the resin coating 20 is as follows: ⁇ >! ⁇ >! ⁇ And n 4 > n 2 .
- the relative refractive index difference ⁇ 2 between the first cladding region 12 and the second cladding region 13 is 0.5% or more, preferably 1.5% or less.
- the relative refractive index difference ⁇ 2 (%) of the first cladding region 12 with respect to the second cladding region 13 is:
- ⁇ 2 100 X ( ⁇ 2 - ⁇ 3 ) / ⁇ 2 ... (1)
- the relative refractive index difference ⁇ ⁇ (%) of the core region 11 to the first cladding region 12 is
- the thickness (c ⁇ b) of the second cladding region 13 is in the range of not less than 10 mm to the cutoff peak wavelength, and more preferably, the thickness (c ⁇ b) is not less than 1.5 mm. It is in the following range.
- the outer diameter 2 b of the first cladding region 12 is 100 ⁇ m or more, and the mode field diameter of the base mode light propagating in the core region 11 is outside the first cladding region 12. It is 1Z10 or less of diameter 2b.
- the predetermined wavelength band e.g. 1. 2 zm ⁇ l. 8 ⁇ M
- the interval between the cutoff peaks is less than 0.2 zm. Since the thickness (c ⁇ b) of the second cladding region 13 is larger than the cutoff peak wavelength, the influence of the layer further outside the second cladding region 13 is small, and the blocking characteristics are stabilized. You.
- the thickness (c-b) of the second cladding region 13 is 10 mm or less, higher-order mode light generated by mode coupling at the cutoff wavelength exits the optical fiber 10, and the cutoff effect at the grating 14 is excellent. . Also, by designing as described above, the coupling between the core mode light and the higher-order mode light propagating in the first cladding region is achieved. The coefficient becomes smaller, and the variation of the cutoff amount and cutoff wavelength with respect to the change in the refractive index is reduced. Therefore, the optical fiber grating element 1 has a large degree of freedom in setting the grating period, easily adjusts the cutoff rate and the cutoff wavelength, and has excellent cutoff characteristics.
- the thickness (c ⁇ b) of the second cladding region 13 is 1.5 mm or more, the wavelength dependence of the higher-order mode light exiting the optical fiber 10 is reduced, which is preferable. Suitable.
- the refractive index n 4 of the resin coating 2 0 provided around the second cladding region 1 3 is larger than the refractive index n 2 of the first Kuradzudo region 1 2, generated by our Keru mode coupling in cutoff wavelength This is preferable because high-order mode light easily exits outside the optical fiber 10.
- the outer diameter 2b of the first cladding region 12 is 100 m or more, it is preferable in that the number of cutoff peaks is increased, and it is also preferable in that the cutoff effect is excellent.
- the mode field diameter of the fundamental mode light propagating in the core region 11 is 1Z10 or less of the outer diameter 2b of the first cladding region 12 in that the number of cutoff peaks increases. Yes, and it is also preferable in that it has an excellent blocking effect.
- Such an optical fiber grating element 1 is manufactured, for example, as follows. First, an optical fiber 10 in which G e O 2 is added to a core region 11 and an F element is added to a second cladding region 13 is prepared based on silica glass. A long-period grating 14 is formed by irradiating the optical fiber 10 with an ultraviolet laser beam output from a KrF excimer laser light source via an intensity modulation mask having a constant pitch. Then, a resin coating 20 is provided around the fiber 10.
- FIG. 3 is a graph showing a transmission spectrum of the optical fiber grating element 1.
- the transmission spectrum of the optical fiber grating element 1 of the embodiment is shown by a solid line (A)
- the transmission spectrum of the conventional optical fiber grating element is shown by a broken line (B).
- the prepared optical fiber 10 has an outer diameter 2 a of the core region 11 of 3, an outer diameter 2 b of the first cladding region 12 of 105 ⁇ m, and a second cladding region of the optical fiber 10.
- the outer diameter 2 c of 13 is 125 mm, and the first cladding area 12 ⁇ relative refractive index of the core region 1 1 difference delta eta against the 1.
- the pitch of the intensity modulation mask was set at 410 zm
- the grating length was set at 3 Omm
- the grating 14 was formed in the core region 11 of the optical fin 10 to obtain the optical fiber grating device 1. Then, a light source was connected to one end of the optical fiber grating element 1, and a spectrum analyzer was connected to the other end of the optical fiber grating element 1, and the transmission spectrum of the optical fiber grating element 1 was measured. .
- FIG. 4 is a graph showing the relationship between the loss change ⁇ in the optical fiber grating element 1 and the thickness (c-b) of the second cladding region 13.
- the horizontal axis of this graph is a logarithmic scale.
- the change in loss ⁇ (%) is the wavelength of 1.55 m when the surroundings of the optical fiber; I 0 are air (refractive index: 1.0) without providing the resin coating 20 around the optical fiber 10.
- the outer diameter 2a of the core region 11 is 3.5 m
- the outer diameter 2c of the second cladding region 13 is 125 m
- the relative refractive index difference ⁇ ni of the core region 11 is 1 m. 1%
- the relative refractive index difference ⁇ 2 of the first cladding region 12 was 0.7%.
- the outer diameter 2b of the first cladding region 12 was manufactured with each value.
- the loss variation ⁇ suddenly decreases. If this is expressed in relation to the cut-off peak wavelength, if the thickness (c-b) of the second cladding region 13 is more than the thickness, the loss This is preferable because the loss change amount ⁇ ⁇ becomes small.
- the grating 14 formed in the core region 11 of the optical fiber grating element 1 has a long period, and high-order mode light generated by mode coupling at a cutoff wavelength needs to be emitted outside the optical fiber. There is.
- the thickness (c-b) of the second cladding region 13 is 10 mm or less.
- FIG. 5 is a graph showing the relationship between the number of cutoff peaks in the optical fiber grating element 1 and the relative refractive index difference ⁇ 2 of the first cladding region 12.
- the outer diameter 2a of the core region 11 is 3.5 ⁇ m
- the outer diameter 2b of the first cladding region 12 is 105 ⁇ m
- the second cladding region 13 Had an outer diameter 2c of 125 / m
- the relative refractive index difference ⁇ of the core region 11 was 1.1%.
- the amount of the F element added in the first cladding region 12 was variously changed, and the first cladding region 12 was manufactured in which the relative refractive index difference ⁇ 2 was each value.
- the number of cutoff peaks is the number of cutoff peaks in the wavelength band of 1.2 / m to 1.8 m.
- the relative refractive index difference delta n 2 is higher cutoff peak number larger first Kuradzudo region 12 increases. If the relative refractive index difference ⁇ n 2 of the first cladding region 12 is 0.5% or more, the number of cutoff peaks in the waveband 1.2 ⁇ m to 1.8 zm is 4 or more, and the interval between cutoff peaks is 0. 2 m or less is suitable.
- FIG. 6 is a graph showing the relationship between the number of cutoff peaks in the optical fiber grating element 1 and the outer diameter 2 b of the first cladding region 12.
- the outer diameter 2a of the core region 11 is 3.5 ⁇ m
- the outer diameter 2c of the second cladding region 13 is 125 ⁇ m
- the core region 11 the relative refractive index difference ⁇ n t is 1.
- the relative refractive index difference .DELTA..eta 2 of the first cladding region 12 was 7% 0.1.
- the outer diameter 2b of the first cladding region 12 was manufactured with each value.
- the number of cutoff peaks is the number of cutoff peaks in the wavelength band of 1.2 1.m to 1.8 zm. This graph As can be seen, the greater the outer diameter 2b of the first cladding region 12, the greater the number of cutoff peaks. If the outer diameter 2b of the first cladding region 12 is 6 or more, the number of cutoff peaks is 3 or more. If the outer diameter 2b of the first cladding region 12 is 72 m or more, the number of cutoff peaks is 4 or more. If the outer diameter 2b of the first cladding region 12 is 100 m or more, the number of cutoff peaks is 6 or more.
- the thickness (c ⁇ b) of the second cladding region 13 needs to be 10 mm or less, and the outer diameter 2 c of the second cladding region 13 is 125 ⁇ m.
- the outer diameter 2b of the first cladding region 12 is at least 100 zm.
- FIG. 7 is a graph showing the relationship between the shift amount of the cutoff peak wavelength when forming the grating 14 of the optical fiber grating element 1 and the ultraviolet light irradiation time.
- This figure also shows Comparative Example 1 (indicated by L2) and Comparative Example 2 (indicated by L3) in addition to the example (indicated by L1).
- the optical fiber 10 prepared in the embodiment has an outer diameter 2a of the core region 11 of 3.5 ⁇ m, an outer diameter 2b of the first cladding region 12 of 105 / m, and a second cladding region.
- the optical fiber prepared in Comparative Example 1 has the refractive index aperture file shown in FIG. 2, but the outer diameter 2a of the core-aged page area 11 is 3.5 zm and the first cladding area 12 has an outer diameter 2 b of 40 / m, the second cladding region 13 has an outer diameter 2 c of 125 zm, the core region 11 has a relative refractive index difference ⁇ n ⁇ of 1.1%, The relative refractive index difference ⁇ 2 of the cladding region 12 was 0.3%.
- the optical fiber prepared in Comparative Example 2 has a simple refractive index profile consisting of a core region and a cladding region.
- the outer diameter of the core region is 3.
- the outer diameter of the cladding region is 125. It was 111, and the relative refractive index difference in the core region was 1.1%.
- the pitch of the intensity modulation mask was set to 410 m, and the ultraviolet light irradiation intensity was the same.
- the optical fiber grating element of the present invention the number of cutoff peaks in a predetermined wavelength band (eg, 1.2 / zm to 1.8 m) is large, and the interval between cutoff peaks is small. Further, the coupling coefficient between the core mode light and the higher-order mode light propagating in the first cladding region is small, and the variation in the cutoff amount and the cutoff wavelength with respect to the refractive index change is reduced. Further, the influence of the layer further outside the second cladding region is small, the blocking characteristics are stable, and the blocking effect in the grating is excellent. Therefore, this optical fiber grating element has a large degree of freedom in setting the grating period, easily adjusts the cutoff amount and cutoff wavelength, and has excellent cutoff characteristics.
- a predetermined wavelength band eg, 1.2 / zm to 1.8 m
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
- Diffracting Gratings Or Hologram Optical Elements (AREA)
Description
Claims
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AU82584/01A AU8258401A (en) | 2000-09-04 | 2001-08-31 | Optical fiber grating device |
EP01961262A EP1316822A4 (en) | 2000-09-04 | 2001-08-31 | FIBER OPTIC NETWORK DEVICE |
US10/129,276 US6785444B2 (en) | 2000-09-04 | 2001-08-31 | Optical fiber grating device |
KR1020027005730A KR20020062737A (ko) | 2000-09-04 | 2001-08-31 | 광파이버 그레이팅 소자 |
CA002390210A CA2390210A1 (en) | 2000-09-04 | 2001-08-31 | Optical fiber grating device |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2000267303A JP2002071975A (ja) | 2000-09-04 | 2000-09-04 | 光ファイバグレーティング素子 |
JP2000-267303 | 2000-09-04 |
Publications (1)
Publication Number | Publication Date |
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WO2002033460A1 true WO2002033460A1 (fr) | 2002-04-25 |
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Application Number | Title | Priority Date | Filing Date |
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PCT/JP2001/007547 WO2002033460A1 (fr) | 2000-09-04 | 2001-08-31 | Dispositif de réseau à fibre optique |
Country Status (7)
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US (1) | US6785444B2 (ja) |
EP (1) | EP1316822A4 (ja) |
JP (1) | JP2002071975A (ja) |
KR (1) | KR20020062737A (ja) |
AU (1) | AU8258401A (ja) |
CA (1) | CA2390210A1 (ja) |
WO (1) | WO2002033460A1 (ja) |
Families Citing this family (3)
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JP4660543B2 (ja) * | 2004-06-04 | 2011-03-30 | クィーンズ ユニバーシティー アット キングストン | 長周期格子センサ方法および装置 |
US7437046B2 (en) * | 2007-02-12 | 2008-10-14 | Furukawa Electric North America, Inc. | Optical fiber configuration for dissipating stray light |
JP6277115B2 (ja) * | 2014-12-05 | 2018-02-07 | 日本電信電話株式会社 | 試験光遮断フィルタおよびそれを適用したインサービス試験方法 |
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JPH07261048A (ja) * | 1994-03-23 | 1995-10-13 | Sumitomo Electric Ind Ltd | 分散補償ファイバ |
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JP3500041B2 (ja) * | 1996-07-02 | 2004-02-23 | 古河電気工業株式会社 | 光ファイバとその製造方法 |
JPH1082918A (ja) * | 1996-09-09 | 1998-03-31 | Sumitomo Electric Ind Ltd | 光ファイバグレーティング |
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JPH11183718A (ja) * | 1997-12-24 | 1999-07-09 | Sumitomo Electric Ind Ltd | 光導波路型回折格子 |
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TW419607B (en) * | 1999-01-13 | 2001-01-21 | Sumitomo Electric Industries | Optical fiber grating element, manufacture method of the same and optical filter |
JP3138731B2 (ja) * | 1999-01-18 | 2001-02-26 | 工業技術院長 | 光ファイバーフィルター |
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KR100318918B1 (ko) * | 2000-01-10 | 2002-01-04 | 윤종용 | 다중 클래딩 구조를 이용하여 온도 보상된 장주기 광섬유격자 필터 |
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TWI226464B (en) * | 2000-11-13 | 2005-01-11 | Sumitomo Electric Industries | Optical fiber, non-linear optical fiber, optical amplifier using the same optical fiber, wavelength converter and optical fiber manufacture method |
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-
2000
- 2000-09-04 JP JP2000267303A patent/JP2002071975A/ja active Pending
-
2001
- 2001-08-31 CA CA002390210A patent/CA2390210A1/en not_active Abandoned
- 2001-08-31 US US10/129,276 patent/US6785444B2/en not_active Expired - Fee Related
- 2001-08-31 KR KR1020027005730A patent/KR20020062737A/ko not_active Application Discontinuation
- 2001-08-31 EP EP01961262A patent/EP1316822A4/en not_active Withdrawn
- 2001-08-31 WO PCT/JP2001/007547 patent/WO2002033460A1/ja not_active Application Discontinuation
- 2001-08-31 AU AU82584/01A patent/AU8258401A/en not_active Abandoned
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JPS63121807A (ja) * | 1986-11-11 | 1988-05-25 | Sumitomo Electric Ind Ltd | 光フアイバ |
WO1997026571A2 (en) * | 1996-01-18 | 1997-07-24 | British Telecommunications Public Limited Company | Optical waveguide with photosensitive refractive index cladding |
JPH09205239A (ja) * | 1996-01-26 | 1997-08-05 | Mitsubishi Cable Ind Ltd | 増幅用光ファイバ |
JPH09203816A (ja) * | 1996-01-29 | 1997-08-05 | Sumitomo Electric Ind Ltd | 光ファイバ母材の製造方法 |
EP0905834A2 (en) * | 1997-09-11 | 1999-03-31 | Lucent Technologies Inc. | Silica-based optical fiber comprising low refractive index intermediate cladding |
JPH11202139A (ja) * | 1998-01-20 | 1999-07-30 | Shin Etsu Chem Co Ltd | グレーティング用光ファイバ、グレーティング用光ファイバ母材およびその光ファイバ母材の製造方法 |
JP2000009956A (ja) * | 1998-06-02 | 2000-01-14 | Alcatel Alsthom Co General Electricite | 変更された感光性プロフィルを有するろ波光ファイバ |
Non-Patent Citations (3)
Title |
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See also references of EP1316822A4 * |
SEIICHI SHIGEHARA ET AL.: "Hifukujou shousha fiber grating", DENSHI JOHO TSUUSHIN GAKKAI GIJUTSU KENKYUU HOUKOKU, vol. 100, no. 85, 26 May 2000 (2000-05-26), JAPAN, pages 1 - 6, XP002949591 * |
YAHEI KOYAMADA: "Numerical analysis of core-mode to radiation-mode coupling in long-period fiber gratings", IEEE PHOTONICS TECHNOLOGY LETTERS, vol. 13, no. 4, April 2000 (2000-04-01), US, pages 308 - 310, XP002949592 * |
Also Published As
Publication number | Publication date |
---|---|
KR20020062737A (ko) | 2002-07-29 |
CA2390210A1 (en) | 2002-04-25 |
US6785444B2 (en) | 2004-08-31 |
EP1316822A1 (en) | 2003-06-04 |
JP2002071975A (ja) | 2002-03-12 |
EP1316822A4 (en) | 2005-11-02 |
AU8258401A (en) | 2002-04-29 |
US20030103727A1 (en) | 2003-06-05 |
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