WO1998014808A1 - Fiber bragg gratings in chalcogenide or chalcohalid based infrared optical fibers - Google Patents
Fiber bragg gratings in chalcogenide or chalcohalid based infrared optical fibers Download PDFInfo
- Publication number
- WO1998014808A1 WO1998014808A1 PCT/US1997/017146 US9717146W WO9814808A1 WO 1998014808 A1 WO1998014808 A1 WO 1998014808A1 US 9717146 W US9717146 W US 9717146W WO 9814808 A1 WO9814808 A1 WO 9814808A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- infrared transmitting
- glass fiber
- transmitting glass
- writing beams
- fiber
- Prior art date
Links
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
- G02B6/02057—Optical fibres with cladding with or without a coating comprising gratings
- G02B6/02076—Refractive index modulation gratings, e.g. Bragg gratings
- G02B6/02114—Refractive index modulation gratings, e.g. Bragg gratings characterised by enhanced photosensitivity characteristics of the fibre, e.g. hydrogen loading, heat treatment
-
- 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
- G02B6/02123—Refractive index modulation gratings, e.g. Bragg gratings characterised by the method of manufacture of the grating
- G02B6/02133—Refractive index modulation gratings, e.g. Bragg gratings characterised by the method of manufacture of the grating using beam interference
Definitions
- the present invention relates to fiber Bragg gratings and more particularly to a method of writing fiber Bragg gratings in infrared transmitting chalcogenide-based or chalcohalide-based fibers.
- Photodarkening is discussed in “Mechanisms of Photodarkening in Amorphous Chalcogenides” , K. Tanaka, Journal of Non-Crystalline Solids, Vol. 59-60, Part II, pp 925-928, (1983). Photoinduced birefringence and dichroism are discussed at greater length in "Photoinduced Optical
- the total refractive index change at 600 nm is about 0.01. (See “Photodarkening Profiles and Kinetics in Chalcogenide Glasses", S. Ducharme et al., Physical Review B, Vol. 41, No.17, pp. 12 250 - 12 259, 15 June 1990.) A simple Kramers-Kronig analysis predicts that this index change will decrease linearly with photon energy in the transparent region of the glass, thus allowing large amplitudes ( ⁇ n ⁇ 10 "3 ) to be induced in the infrared.
- the writing beams change an absorption line due to the germanium doping of the core, causing a change ⁇ n in the index of refraction n at lower photon energies.
- the index change amplitude is around ⁇ n ⁇ 10 ⁇ 5 -10 "6 for silica glass.
- the period of the standing wave sets the Bragg reflection condition, which gives a reflection maximum at the wavelength of the writing beam. Since the energy of the writing beam needs to be near the Tauc gap in order to photoinduce carriers, Hill- gratings will not be useful at infrared wavelengths which are not significantly absorbed in the material.
- Another object of the invention is to write reflective Bragg gratings into infrared transmitting fibers.
- Another object of the invention is to side write fiber Bragg gratings into infrared transmitting fibers.
- Another object of the invention is to provide fiber Bragg gratings in chalcogenide or chalcohalide-based infrared optical fibers with reflectances peaked at one or more wavelengths between 1.5 and 15 microns in the infrared.
- a further object of the invention is to side write highly-reflective, fiber Bragg gratings into sulfide-based chalcogenide infrared optical fibers.
- a further object of the invention is to provide fiber Bragg gratings in infrared transmitting sulfide-based fibers .
- reflective fiber Bragg gratings in the interior of an infrared transmitting glass fiber, such as a by side illuminating the fiber with two same-wavelength, laser writing beams which intersect at some angle in the fiber to form an intensity grating by way of interference along the length of the fiber, maintaining the infrared transmitting glass fiber at the intersection of the two writing beams to produce a reflective Bragg grating in the core and cladding of the glass fiber, and repeating this operation for each reflective fiber Bragg grating that is desired.
- Fig. 1 illustrates a simplified schematic diagram of a reflective fiber Bragg grating side-written into a sulfide- based chalcogenide infrared optical fiber and further indicates a method for side-writing the grating into the sulfide-based chalcogenide infrared optical fiber;
- Fig. 2 illustrates exemplary fiber material compositions of chalcogenide and chalcohalide based infrared optical fibers;
- Fig. 3 illustrates the Bragg reflection wavelength ⁇ B verses the writing angle ⁇ w for three typical writing wavelengths ⁇ w ; and Fig. 4 illustrates a schematic diagram of an experiment which demonstrated the side-writing of a fiber Bragg grating in an arsenic sulfide-based chalcogenide infrared optical fiber.
- Fig. 1 illustrates a simplified schematic diagram of a reflective fiber Bragg grating side-written into a sulfide-based chalcogenide infrared optical fiber and further indicates a method for infrared optical fiber.
- two exemplary laser beams at the same writing wavelength are used as input "writing" beams 11 and 13. These two writing beams 11 and 13 are crossed at some angle ⁇ _ in space.
- a chalcogenide- or chalcohalide- based glass (Fig. 2) infrared transmitting optical fiber, such as a sulfide-based fiber 15 having a core 17 and a cladding 19, is placed at the intersection point where the two writing beams 11 and 13 cross in space such that where the beams 11 and 13 cross coincides with the fiber 15 itself - the fiber core 17 and cladding 19.
- the writing wavelength ⁇ w is in the range of 0.5 ⁇ m to 1.5 ⁇ m.
- This wavelength is chosen to have an absorption length in the particular glass composition of the fiber 15 such that it is weakly absorbed in the glass. Weakly absorbed is defined as an absorption of between 0.1 and 10 cm -1 . For example, this would correspond to a wavelength in the range of 0.5 ⁇ m - 0.8 ⁇ m in the As 40 S 60 glass composition, and a wavelength range of 0.8 ⁇ m - 1.4 ⁇ m in the Ge 33 As 12 Se 55 composition.
- the interference pattern 21 in the fiber 15 produces an index change in the glass, causing a change ⁇ n in the index of refraction n at lower photon energies.
- the range of ⁇ n induced by the crossed beams 11 and 13 at ⁇ w is between 0 and 0.2. It should be noted at this time that the typical range of writing fluences at ⁇ w is between 0.1 and 100 W/cm 2 , and will be incident from 0 -1000 minutes.
- any writing fluence/temporal duration of writing sufficient to write a ⁇ n consistent with the above specified 0 to 0.2 range of an ⁇ n induced by the crossed beams 11 and 13 at ⁇ w is intended to be covered by the claimed invention.
- forms a Bragg reflector at the vacuum wavelength ⁇ B for light launched down the core of the fiber at ⁇ B 2n ⁇ .
- the wavelength at which the mirror reflects depends on the period of that grating which can be changed by changing the angle ⁇ _ between the beams 11 and 13. (To be discussed in regard to Fig. 3.)
- an infrared beam can be injected into the core 17 of the fiber 15 and the writing wavelength of the beams 11 and 13 can be changed until a wavelength is reflected from the fiber 15. That reflected wavelength is called the Bragg wavelength or the Bragg reflection wavelength ⁇ B .
- the Bragg reflection wavelength ⁇ B is in the infrared region from 1.5 ⁇ m - 15 ⁇ m.
- the necessary writing angles and wavelengths to achieve a desired Bragg reflection wavelength are shown and discussed in relation to Fig. 3.
- the mechanism for writing a photo- induced index change is based on rearranging the local bonding structure of the intrinsic atoms of the chalcogenide-based or chalcohalide- based glass used in the infrared optical fibers. No dopants are used or required for the photoinduced index change .
- the fiber materials covered by this application are all chalcogenide and chalcohalide glasses where an index change can be photoinduced with a writing wavelength ⁇ w using the mechanism described in the previous paragraph.
- Components of exemplary fiber material glass compositions of chalcogenide- based infrared optical fibers are shown in Fig. 2A, while components of exemplary fiber glass compositions of chalcohalide-based infrared optical fibers are shown in Fig. 2B.
- compositions include any glass composed of at least one of the anions sulfur (S) , selenium (Se) and tellurium (Te) and at least one suitable cation, including but not limited to barium (Ba) , germanium (Ge) , indium (In) , arsenic (As) , gallium (Ga) , or lanthanium (La) in binary, ternary, quaternary, etc. mixtures.
- Example chalcogenide glass compositions include As 40 S 60 , As 40 S 55 Se 5 , and Ge 33 As 12 Se 55 .
- the chalcohalide glass compositions include any glass composed of at least one of each of the aforementioned cations and anions, plus at least one of the halides (but less than a total of 50 weight percent) of chlorine (Cl) , fluorine (F) , bromine (Br) and iodine (I) .
- compositions of the chalcogenide and chalcohalide glasses that form a stable glass and exhibit photoinduced index changes are included in the claimed invention.
- Fig. 3 illustrates the Bragg reflection wavelength ⁇ B verses the writing angle ⁇ w for three typical writing wavelengths ⁇ w .
- the angle of 0 W on the X-axis of Fig. 3 corresponds to the angle ⁇ _ between the writing beams 11 and 13 that are incident upon the fiber 15 in Fig. 1.
- Fig. 3 indicates that upon choosing a given 0 W angle along the X-axis for one of the three typical writing wavelengths shown in Fig. 3, an associated Bragg reflection wavelength will be indicated on the Y-axis.
- Fig. 3 would indicate that a Bragg reflection wavelength of about 2.4 microns would result. So as indicated in the curve of Fig. 3, as the 0 W angle gets smaller as the left-hand side of the curve is approached down to 0o, the Bragg wavelength increases to longer and longer wavelengths ⁇ B . Thus, if it were desired to write a Bragg grating at, for example, 10 microns, it can be seen that the 10 on the Y-axis would correspond to a 0 W angle of Fig. 3 would correspond to Fig. 1.
- the three different curves correspond to three different writing wavelengths which would be crossed in Fig. 1. Pairs of beams would be derived from the same laser.
- the lowest curve 23 corresponds to a wavelength of 532 nm from an exemplary frequency doubled Nd:YAG.
- the center curve 25 corresponds to a 632 nm wavelength from a helium-neon laser.
- the upper curve 27 corresponds to a 1.064 ⁇ m wavelength from a Nd:YAG laser. From Fig. 3, it can be readily seen that the angle necessary to write a given reflectivity gets wider with longer wavelengths.
- a different writing wavelength may be required to write in infrared fibers having different compositions in order to make sure that the radiation from a laser is completely absorbed in the glass of the infrared transmitting fiber.
- the transmitted beam is sequentially reflected by two mirrors 33 and 35 so that the beam can be focused down to a small point by a lens 37.
- the focused beam from the lens 37 is passed through a spatial filter 39 which basically is just a pinhole (not shown) in a piece of metal to clean up the beam.
- the pinhole can be about an exemplary 100 microns in diameter, depending on the size of the lens 37 being used. Any irregularities in the shape of the beam or distortions caused by, for example, dust will not focus to a nice fine point of light that will readily pass through the pinhole in the spatial filter 39 but will be blocked by the spatial filter 39.
- the only light that comes through the pinhole in the spatial filter 39 is basically a perfect beam which starts to diverge as it exits the pinhole.
- the diverging beam that is exiting the pinhole in the spatial filter 39 is collimated by a lens 41.
- the lenses 37 and 41 and the output of the lens 41 round and clean-shaped.
- the collimated beam from the lens 41 is reflected by a mirror 43 to a beamsplitter 45 in the part of the experiment that actually writes the grating.
- the beam splitter 45 reflects half of the power or 20 mW to another mirror 47 which, in turn, reflects the light to a cylindrical lens 49.
- the beam splitter 45 passes the other half of the power or 20 mW therethrough to the cylindrical lens 49.
- the cylindrical lens 49 begins to focus each of the two beams in only one direction down to a relatively long and thin line.
- the beams are focusing, they are redirected toward each other by flat mirrors 51 and 53 to cross at an angle ⁇ .
- the beams look like lines at the point where they cross in space at the focus. It is at that point in space where an arsenic sulfide fiber 55 is placed and held in position by fiber holding clips 57 and 59 while at least one Bragg grating is being written into the fiber 55.
- a single mode fiber would preferably be used with the core size of the fiber being very small, such as an exemplary 10 microns in diameter.
- the two beams cross at an angle ⁇ along the core of the arsenic sulfide fiber 55 so that a Bragg grating can be written into into the fiber 55.
- the arsenic sulfide fiber transmits most of the 0.6471 ⁇ m light which is incident on the side of the fiber 55. This light emerges as from a very strong cylindrical lens in two opposing "arc" shaped patterns. Each beam also has a visible reflection from the surface of the fiber. To get the alignment correct, these directions of the "arc" shaped reflections off the fiber are matched with the complementary input beam to assure that the beams overlap in the fiber core.
- the first key new feature is that ⁇ B is now in the IR region of 1.5 - 15 ⁇ m.
- the second new key feature is that the mechanism of making ⁇ n does not depend on any dopant (s) to be present in the glass material. Also, when light is sent down the core of a single-mode sulfide fiber, it will be reflected by this Bragg grating. Unlike silica fiber Bragg gratings, however, the index-change amplitude of these gratings is larger by two orders of magnitude, allowing the possibility of constructing highly reflective, wide band structures.
- the writing wavelength is around 650 nm, the writing could be done in principle with commercially available pulsed or continuous-wave laser diodes, eliminating the need for an expensive and unwieldy excimer or krypton laser.
- fiber Bragg gratings can be written via the same method and using the same physical process in other fiber compositions.
- This photodarkening effect occurrs in any chalcogenide or chalcohalide based fibers, including fiber compositions containing the chalcogens sulfur, tellurium, and selenium, and mixtures of the aforementioned chalcogens with halides such as fluorine and chlorine.
- chalcogenide fibers which are doped with rare-earths such as erbium and praesodymium, which will allow mirror integration in laser and laser amplifier devices based on these materials.
- an infrared transmitting glass fiber such as a chalcogenide or chalcohalide-based infrared optical fiber
- a chalcogenide or chalcohalide-based infrared optical fiber by side illuminating the fiber with two same- wavelength, laser writing beams which intersect at some angle in the fiber to form an intensity grating by way of interference along the length of the fiber, maintaining the infrared transmitting glass fiber at the intersection of the two writing beams to produce a reflective Bragg grating in the core and cladding of the glass fiber, and repeating this operation for each reflective fiber Bragg grating that is desired.
- the laser 31 could be replaced with a different laser to develop a different writing wavelength, such as a Nd:YAG laser which emits at 1064 nm, a doubled Nd:YAG laser which emits at 532 nm, or preferably with a helium neon laser which emits at 632 nm.
- the output power of the laser such be limited to, for example about 40 mW to avoid burning the fiber 55 that a Bragg grating is being written into.
- the fiber 55 could be replaced with any chalcogenide or chalcohalide infrared transmitting fiber having a composition selected according to the discussion in relation Figs.
- Fig. 4 which is shown being comprised of the exemplary combination of mirrors 33, 35 and 43, lenses 37 and 41 and the spatial filter 39, could be simplified and/or replaced with any other combination of optical components to direct and split the output of the laser 31 into two substantially equal power beams before example, the laser beam from the laser 31 could be directly applied to the beam splitter 45. It is therefore to be understood that, within the scope of the appended claims, the invention may be practiced otherwise than as specifically described.
Abstract
Description
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Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA002271127A CA2271127C (en) | 1996-09-30 | 1997-09-25 | Fiber bragg gratings in chalcogenide or chalcohalid based infrared optical fibers |
EP97945273A EP0929831A4 (en) | 1996-09-30 | 1997-09-25 | Fiber bragg gratings in chalcogenide or chalcohalid based infrared optical fibers |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US08/721,846 US6195483B1 (en) | 1996-09-30 | 1996-09-30 | Fiber Bragg gratings in chalcogenide or chalcohalide based infrared optical fibers |
US08/721,846 | 1996-09-30 |
Publications (1)
Publication Number | Publication Date |
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WO1998014808A1 true WO1998014808A1 (en) | 1998-04-09 |
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ID=24899551
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/US1997/017146 WO1998014808A1 (en) | 1996-09-30 | 1997-09-25 | Fiber bragg gratings in chalcogenide or chalcohalid based infrared optical fibers |
Country Status (4)
Country | Link |
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US (1) | US6195483B1 (en) |
EP (1) | EP0929831A4 (en) |
CA (1) | CA2271127C (en) |
WO (1) | WO1998014808A1 (en) |
Families Citing this family (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CA2443129A1 (en) * | 2001-04-12 | 2002-10-24 | Emilia Anderson | High index-contrast fiber waveguides and applications |
US6904201B1 (en) * | 2001-05-09 | 2005-06-07 | Intel Corporation | Phase-controlled fiber Bragg gratings and manufacturing methods |
FR2845833A1 (en) * | 2002-10-15 | 2004-04-16 | Cit Alcatel | Clamped gain semiconductor optical amplifier having active waveguide with three dimension surround coupled laser oscillator with resonant cavities following first/second longitudinal active waveguide directions providing frequencies |
US20040141702A1 (en) * | 2002-11-22 | 2004-07-22 | Vladimir Fuflyigin | Dielectric waveguide and method of making the same |
US20040198582A1 (en) * | 2003-04-01 | 2004-10-07 | Borrelli Nicholas F. | Optical elements and methods of making optical elements |
US7366378B2 (en) * | 2004-10-29 | 2008-04-29 | Matsushita Electric Industrial Co., Ltd. | Ultrafast laser machining system and method for forming diffractive structures in optical fibers |
US7376307B2 (en) * | 2004-10-29 | 2008-05-20 | Matsushita Electric Industrial Co., Ltd | Multimode long period fiber bragg grating machined by ultrafast laser direct writing |
US7587110B2 (en) * | 2005-03-22 | 2009-09-08 | Panasonic Corporation | Multicore optical fiber with integral diffractive elements machined by ultrafast laser direct writing |
CN101622556B (en) * | 2006-09-28 | 2012-07-18 | 拉瓦勒大学 | System and method for permanently writing a diffraction grating in a low phonon energy glass medium |
US20110038587A1 (en) * | 2009-08-11 | 2011-02-17 | Leslie Brandon Shaw | Multi-clad optical fiber |
Citations (5)
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US5066133A (en) * | 1990-10-18 | 1991-11-19 | United Technologies Corporation | Extended length embedded Bragg grating manufacturing method and arrangement |
US5218651A (en) * | 1991-03-25 | 1993-06-08 | Gaz De France | Optical fibre incorporating a variable internal bragg grating and its applications |
US5388173A (en) * | 1993-12-20 | 1995-02-07 | United Technologies Corporation | Method and apparatus for forming aperiodic gratings in optical fibers |
US5400422A (en) * | 1993-01-21 | 1995-03-21 | The United States Of America As Represented By The Secretary Of The Navy | Technique to prepare high-reflectance optical fiber bragg gratings with single exposure in-line or fiber draw tower |
US5636304A (en) * | 1992-12-23 | 1997-06-03 | Lucent Technologies Inc. | Article comprising a spatially varying Bragg grating in an optical fiber |
Family Cites Families (9)
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JPH0734069B2 (en) * | 1987-07-08 | 1995-04-12 | 富士写真フイルム株式会社 | Phase-locked semiconductor laser optical system |
US5136677A (en) * | 1989-12-21 | 1992-08-04 | Galileo Electro-Optics Corporation | Photorefractive effect in bulk chalcogenide glass and devices made therefrom |
US5309452B1 (en) * | 1992-01-31 | 1998-01-20 | Univ Rutgers | Praseodymium laser system |
US5364434A (en) * | 1992-09-30 | 1994-11-15 | The United States Of America As Represented By The Secretary Of The Navy | Plasma treatment of glass surfaces to remove carbon |
US5397891A (en) * | 1992-10-20 | 1995-03-14 | Mcdonnell Douglas Corporation | Sensor systems employing optical fiber gratings |
GB2275347A (en) * | 1993-02-19 | 1994-08-24 | Univ Southampton | Optical waveguide grating formed by transverse optical exposure |
US5627933A (en) * | 1994-02-17 | 1997-05-06 | Sumitomo Electric Industries, Ltd. | Optical waveguide and process for producing it |
US5559907A (en) * | 1994-02-17 | 1996-09-24 | Lucent Technologies Inc. | Method of controlling polarization properties of a photo-induced device in an optical waveguide and method of investigating structure of an optical waveguide |
US5629953A (en) * | 1995-05-05 | 1997-05-13 | The Board Of Trustees Of The University Of Illinois | Chalcogenide optical pumping system driven by broad absorption band |
-
1996
- 1996-09-30 US US08/721,846 patent/US6195483B1/en not_active Expired - Lifetime
-
1997
- 1997-09-25 EP EP97945273A patent/EP0929831A4/en not_active Ceased
- 1997-09-25 CA CA002271127A patent/CA2271127C/en not_active Expired - Fee Related
- 1997-09-25 WO PCT/US1997/017146 patent/WO1998014808A1/en not_active Application Discontinuation
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5066133A (en) * | 1990-10-18 | 1991-11-19 | United Technologies Corporation | Extended length embedded Bragg grating manufacturing method and arrangement |
US5218651A (en) * | 1991-03-25 | 1993-06-08 | Gaz De France | Optical fibre incorporating a variable internal bragg grating and its applications |
US5636304A (en) * | 1992-12-23 | 1997-06-03 | Lucent Technologies Inc. | Article comprising a spatially varying Bragg grating in an optical fiber |
US5400422A (en) * | 1993-01-21 | 1995-03-21 | The United States Of America As Represented By The Secretary Of The Navy | Technique to prepare high-reflectance optical fiber bragg gratings with single exposure in-line or fiber draw tower |
US5388173A (en) * | 1993-12-20 | 1995-02-07 | United Technologies Corporation | Method and apparatus for forming aperiodic gratings in optical fibers |
Non-Patent Citations (1)
Title |
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See also references of EP0929831A4 * |
Also Published As
Publication number | Publication date |
---|---|
EP0929831A1 (en) | 1999-07-21 |
US6195483B1 (en) | 2001-02-27 |
CA2271127C (en) | 2004-12-07 |
EP0929831A4 (en) | 2000-04-19 |
CA2271127A1 (en) | 1998-04-09 |
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