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WO1991013038A1 - A rare-earth doped fibre - Google Patents

A rare-earth doped fibre Download PDF

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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
Application number
PCT/AU1991/000068
Other languages
French (fr)
Inventor
Steven James Frisken
Original Assignee
Otc Limited
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Otc Limited filed Critical Otc Limited
Publication of WO1991013038A1 publication Critical patent/WO1991013038A1/en

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL 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
    • C03C13/00Fibre or filament compositions
    • C03C13/04Fibre optics, e.g. core and clad fibre compositions
    • C03C13/045Silica-containing oxide glass compositions
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06708Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/06Construction or shape of active medium
    • H01S3/063Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
    • H01S3/067Fibre lasers
    • H01S3/06708Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
    • H01S3/0672Non-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.

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  • 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

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
PCT/AU1991/000068 1990-02-28 1991-02-28 A rare-earth doped fibre WO1991013038A1 (en)

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
WO (1) WO1991013038A1 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
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)

* Cited by examiner, † Cited by third party
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

Patent Citations (5)

* Cited by examiner, † Cited by third party
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)

* Cited by examiner, † Cited by third party
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)

* Cited by examiner, † Cited by third party
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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