WO1991013038A1 - A rare-earth doped fibre - Google Patents
A rare-earth doped fibre Download PDFInfo
- Publication number
- WO1991013038A1 WO1991013038A1 PCT/AU1991/000068 AU9100068W WO9113038A1 WO 1991013038 A1 WO1991013038 A1 WO 1991013038A1 AU 9100068 W AU9100068 W AU 9100068W WO 9113038 A1 WO9113038 A1 WO 9113038A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- fibre
- rare
- core
- doped
- inner core
- Prior art date
Links
Classifications
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
- C03C13/00—Fibre or filament compositions
- C03C13/04—Fibre optics, e.g. core and clad fibre compositions
- C03C13/045—Silica-containing oxide glass compositions
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06708—Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06708—Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
- H01S3/0672—Non-uniform radial doping
Definitions
- the present invention relates to rare-earth doped fibres for optical amplifiers and fibre lasers.
- Fused silica fibres form the basis of most single mode optical fibre applications.
- the effective operation of the fibre is dependant on the confinement of the light wave to the core of the fibre. This is achieved by different refractive Indexes, with a high refractive index being provided in the core as compared to that of the surrounding cladding.
- N.A. Aperture (N.A.). The extent of confinement is dependant upon the number of modes that operate within the core, the wavelength of the light and the N.A.
- these losses must be kept minimal by ensuring that the overlap of the intensity profiles of both fibres remain large for the signal wavelength.
- the fibre should also remain single moded at a single wavelength.
- a rare-earth metal doped fibre of small radius for use in an optical amplifier or fibre laser, said fibre having a rare-earth metal doped inner core of a high Numerical Aperture, and an outer core of larger radius than the inner core, said outer core having a
- the inner core is doped with Erbium, and the outer core is not doped.
- an optical fibre 1 which may be used in an optical amplifier or fibre laser.
- the fibre 1 has an Inner core 3 which is doped with a rare-earth metal, preferably Erbium.
- the inner core has a high Numerical Aperture and is preferably doped in Its central region.
- Surrounding the inner core is an outer core 4 which is not doped with a rare-earth metal, or has a low dopant concentration.
- the outer core has a larger radius relative to the inner core and has a low Numerical Aperture relative to the inner core 3.
- Surrounding the outer core 4 is a cladding 2.
- the inner core 3 allows a high intensity light to be obtained for both the pump and the signal wavelengths. This is done without affecting the coupling ability with a standard telecommunications fibre (the signal coupling efficiency). As the Erbium dopant is confined to a small area within the core, greater increases can be obtained in the gain in the amplifier.
- Numerical Aperture means the local Numerical Aperture relative to the cladding, which could, for example, be pure silica, with a refractive index of 1.46.
- the pump wavelength is considerably shorter than the signal.
- the signal wavelength is at about 1.536 ⁇ m, and two of the possible pumping bands are at 980 nm and 820 nm.
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Electromagnetism (AREA)
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- General Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Geochemistry & Mineralogy (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Life Sciences & Earth Sciences (AREA)
- Plasma & Fusion (AREA)
- Lasers (AREA)
Abstract
A rare-earth metal doped fibre (1) of small radius for use in an optical amplifier or fibre laser. The fibre (1) has its inner core (3) doped with a rare-earth metal so as to have a high Numerical Aperture. The outer core (4) has a low Numerical Aperture and surrounds the inner core (3). A cladding (2) surrounds the outer core (4).
Description
A Rare-Earth Doped Fibre
TECHNICAL FIELD
The present invention relates to rare-earth doped fibres for optical amplifiers and fibre lasers.
BACKGROUND ART
Fused silica fibres form the basis of most single mode optical fibre applications. The effective operation of the fibre is dependant on the confinement of the light wave to the core of the fibre. This is achieved by different refractive Indexes, with a high refractive index being provided in the core as compared to that of the surrounding cladding.
When the core radius is large and the refractive index difference is high, the vast majority of the light is confined to the core of the fibre.
This difference in refractive indexes is referred to as the Numerical
Aperture (N.A.). The extent of confinement is dependant upon the number of modes that operate within the core, the wavelength of the light and the N.A.
It is desirable to have a high intensity light transmission to thereby provide a strong signal. This is particularly Important in the case of optical amplifiers. A number of conclusions have been reached by researchers recently regarding the design of fibres to optimise their use as amplifiers. Fibre design has concentrated on increasing the N.A. and reducing the core size in an attempt to increase the intensity of both the signal wavelength and pump in the core.
However there are constraints on the N.A. that can be achieved in manufacturing processes. Further the compatability with existing telecommunications fibres is also a problem, which problem is exacerbated by the increase in refractive index of the core. This incompatability results in losses in coupling light from a standard fibre to a gain fibre.
Preferably these losses must be kept minimal by ensuring that the overlap of the intensity profiles of both fibres remain large for the signal wavelength. The fibre should also remain single moded at a single wavelength.
OBJECT OF THE INVENTION
It is the object of the present invention to overcome or substantially ameliorate the above disadvantages.
DISCLOSURE OF THE INVENTION
There is disclosed herein a rare-earth metal doped fibre of small radius for use in an optical amplifier or fibre laser, said fibre having a rare-earth metal doped inner core of a high Numerical Aperture, and an outer core of larger radius than the inner core, said outer core having a
SUBSTITUTE SHEET
low Numerical Aperture and surrounding the said inner core, and a cladding surrounding the said outer core.
Preferably the inner core is doped with Erbium, and the outer core is not doped.
BRIEF DESCRIPTION OF THE DRAWING
In the accompanying drawing there is schematically depicted in transverse cross-section an optical fibre which may be used in an optical amplifier or fibre laser.
BEST MODE FOR CARRYING OUT THE INVENTION
In the accompanying drawing, there is schematically depicted, in cross-section, an optical fibre 1 which may be used in an optical amplifier or fibre laser.
The fibre 1 has an Inner core 3 which is doped with a rare-earth metal, preferably Erbium. The inner core has a high Numerical Aperture and is preferably doped in Its central region. Surrounding the inner core is an outer core 4 which is not doped with a rare-earth metal, or has a low dopant concentration. The outer core has a larger radius relative to the inner core and has a low Numerical Aperture relative to the inner core 3. Surrounding the outer core 4 is a cladding 2.
Where the fibre 1 is provided with a two-step Numerical Aperture fibre design, the inner core 3 allows a high intensity light to be obtained for both the pump and the signal wavelengths. This is done without affecting the coupling ability with a standard telecommunications fibre (the signal coupling efficiency). As the Erbium dopant is confined to a small area within the core, greater increases can be obtained in the gain in the amplifier.
It should be appeciated that the definition of Numerical Aperture (N.A) means the local Numerical Aperture relative to the cladding, which could, for example, be pure silica, with a refractive index of 1.46.
2 2 N.A = (n(r) -nc_,la_d. ) where n is the local refractive index and nclad ^s tne re^ractive indeχ of the cladding.
This equation gives the local N.A at the radial distance r.
The main advantage of this preferred fibre design comes when the pump wavelength is considerably shorter than the signal. For example, for Erbium doping the signal wavelength is at about 1.536 μm, and two of the possible pumping bands are at 980 nm and 820 nm. In this case as well as the advantages already listed of high Intensity for pump and signal and good signal coupling to standard fibre, there is an additional advantage of low bending loss for the signal wavelength compared with standard fibres which are single-moded fibres at the pump wavelengths.
SUBSTITUTE SHE
Claims
1. A rare-earth metal doped fibre of small radius for use in an optical amplifier or fibre laser, said fibre having a rare-earth metal doped inner core of a high Numerical Aperture, and an outer core of larger radius than the inner core, said outer core having a low Numerical Aperture and surrounding the said inner core, and a cladding surrounding the said outer core.
2. The fibre of claim 1, wherein said inner core is doped with Erbium.
3. The fibre of claim 1 or 2, wherein said inner core is doped in its central region.
4. The fibre of claim 1, 2 or 3, wherein said outer core is not doped with a rare-earth metal.
5. The fibre of claim 1, 2 or 3, wherein said outer core has a low dopant concentration.
6. An optical fibre for use 1n an optical amplifier or fibre laser, substantially as hereinbefore described with reference to the accompanying drawings.
SUBSTITUTESHEET
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AUPJ887290 | 1990-02-28 | ||
AUPJ8872 | 1990-02-28 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1991013038A1 true WO1991013038A1 (en) | 1991-09-05 |
Family
ID=3774523
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/AU1991/000068 WO1991013038A1 (en) | 1990-02-28 | 1991-02-28 | A rare-earth doped fibre |
Country Status (1)
Country | Link |
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WO (1) | WO1991013038A1 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2273389A (en) * | 1992-12-14 | 1994-06-15 | Pirelli Cavi Spa | Rare earth doped optical fibre amplifier |
CN1038029C (en) * | 1993-07-22 | 1998-04-15 | 中国建筑材料科学研究院 | Modified quartz optical fiber |
CN111129927A (en) * | 2019-12-30 | 2020-05-08 | 大族激光科技产业集团股份有限公司 | Fiber laser and laser emitting device |
RU2740005C1 (en) * | 2019-05-07 | 2020-12-30 | Тойота Дзидося Кабусики Кайся | Optical fibre laser device |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61262708A (en) * | 1985-05-17 | 1986-11-20 | Sumitomo Electric Ind Ltd | Single mode optical fiber for 1.5 micron band |
JPS6252508A (en) * | 1985-09-02 | 1987-03-07 | Nippon Telegr & Teleph Corp <Ntt> | Optical fiber |
EP0313209A1 (en) * | 1987-10-22 | 1989-04-26 | BRITISH TELECOMMUNICATIONS public limited company | Optical fibre with fluorescent additive |
EP0320990A2 (en) * | 1987-12-17 | 1989-06-21 | Polaroid Corporation | Optical fiber lasers and amplifiers |
JPH01224706A (en) * | 1988-03-04 | 1989-09-07 | Sumitomo Electric Ind Ltd | Optical fiber |
-
1991
- 1991-02-28 WO PCT/AU1991/000068 patent/WO1991013038A1/en unknown
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61262708A (en) * | 1985-05-17 | 1986-11-20 | Sumitomo Electric Ind Ltd | Single mode optical fiber for 1.5 micron band |
JPS6252508A (en) * | 1985-09-02 | 1987-03-07 | Nippon Telegr & Teleph Corp <Ntt> | Optical fiber |
EP0313209A1 (en) * | 1987-10-22 | 1989-04-26 | BRITISH TELECOMMUNICATIONS public limited company | Optical fibre with fluorescent additive |
EP0320990A2 (en) * | 1987-12-17 | 1989-06-21 | Polaroid Corporation | Optical fiber lasers and amplifiers |
JPH01224706A (en) * | 1988-03-04 | 1989-09-07 | Sumitomo Electric Ind Ltd | Optical fiber |
Non-Patent Citations (3)
Title |
---|
DERWENT ABSTRACT, Accession No. 87-003182/01, Class V07; & JP,A,61 262 708, (SUMITOMO ELECTRIC INDUSTRIES KK), 20 November 1986. * |
PATENT ABSTRACTS OF JAPAN, P-603, page 61; & JP,A,62 052 508, (NIPPON TELEGRAPH AND TELEPHONE CORPORATION), 7 March 1987. * |
PATENT ABSTRACTS OF JAPAN, P-970, page 55; & JP,A,1 224 706, (SUMITOMO ELECTRIC INDUSTRIES LIMITED), 7 September 1989. * |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2273389A (en) * | 1992-12-14 | 1994-06-15 | Pirelli Cavi Spa | Rare earth doped optical fibre amplifier |
US5491581A (en) * | 1992-12-14 | 1996-02-13 | Pirelli Cavi S.P.A. | Rare earth doped optical fibre amplifiers |
GB2273389B (en) * | 1992-12-14 | 1996-07-17 | Pirelli Cavi Spa | Rare earth doped optical fibre amplifiers |
CN1038029C (en) * | 1993-07-22 | 1998-04-15 | 中国建筑材料科学研究院 | Modified quartz optical fiber |
RU2740005C1 (en) * | 2019-05-07 | 2020-12-30 | Тойота Дзидося Кабусики Кайся | Optical fibre laser device |
US11424589B2 (en) | 2019-05-07 | 2022-08-23 | Toyota Jidosha Kabushiki Kaisha | Optical fiber laser device |
CN111129927A (en) * | 2019-12-30 | 2020-05-08 | 大族激光科技产业集团股份有限公司 | Fiber laser and laser emitting device |
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