WO1994000784A1 - Photoinduced grating in b2o3 containing glass - Google Patents

Photoinduced grating in b2o3 containing glass Download PDF

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Publication number
WO1994000784A1
WO1994000784A1 PCT/GB1993/001321 GB9301321W WO9400784A1 WO 1994000784 A1 WO1994000784 A1 WO 1994000784A1 GB 9301321 W GB9301321 W GB 9301321W WO 9400784 A1 WO9400784 A1 WO 9400784A1
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WO
WIPO (PCT)
Prior art keywords
refractive index
modulation
optical device
fibre
radiation
Prior art date
Legal status (The legal status 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 status listed.)
Ceased
Application number
PCT/GB1993/001321
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French (fr)
Inventor
Benjamin James Ainslie
Douglas Lawrence Williams
Graeme Douglas Maxwell
Raman Kashyap
Jonathan Richard Armitage
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British Telecommunications PLC
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British Telecommunications PLC
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Filing date
Publication date
Application filed by British Telecommunications PLC filed Critical British Telecommunications PLC
Priority to JP50215594A priority Critical patent/JP3404040B2/en
Priority to CA002117682A priority patent/CA2117682C/en
Priority to EP93913418A priority patent/EP0647327B1/en
Priority to US08/302,931 priority patent/US6075625A/en
Priority to DE69317285T priority patent/DE69317285T2/en
Publication of WO1994000784A1 publication Critical patent/WO1994000784A1/en
Anticipated expiration legal-status Critical
Priority to US09/372,038 priority patent/US6229945B1/en
Ceased legal-status Critical Current

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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
    • 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
    • C—CHEMISTRY; METALLURGY
    • C03—GLASS; MINERAL OR SLAG WOOL
    • C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B19/00—Other methods of shaping glass
    • C03B19/14—Other methods of shaping glass by gas- or vapour- phase reaction processes
    • C03B19/1453—Thermal after-treatment of the shaped article, e.g. dehydrating, consolidating, sintering
    • C—CHEMISTRY; METALLURGY
    • C03—GLASS; MINERAL OR SLAG WOOL
    • C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B37/00—Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
    • C03B37/01—Manufacture of glass fibres or filaments
    • C03B37/012—Manufacture of preforms for drawing fibres or filaments
    • C03B37/014—Manufacture of preforms for drawing fibres or filaments made entirely or partially by chemical means, e.g. vapour phase deposition of bulk porous glass either by outside vapour deposition [OVD], or by outside vapour phase oxidation [OVPO] or by vapour axial deposition [VAD]
    • C03B37/018—Manufacture of preforms for drawing fibres or filaments made entirely or partially by chemical means, e.g. vapour phase deposition of bulk porous glass either by outside vapour deposition [OVD], or by outside vapour phase oxidation [OVPO] or by vapour axial deposition [VAD] by glass deposition on a glass substrate, e.g. by inside-, modified-, plasma- or plasma modified- chemical vapour deposition [ICVD, MCVD, PCVD, PMCVD], i.e. by thin layer coating on the inside or outside of a glass tube or on a glass rod
    • C03B37/01853—Thermal after-treatment of preforms, e.g. dehydrating, consolidating, sintering
    • 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
    • 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
    • C03C3/00—Glass compositions
    • C03C3/04—Glass compositions containing silica
    • C03C3/06—Glass compositions containing silica with more than 90% silica by weight, e.g. quartz
    • 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
    • C03C3/00—Glass compositions
    • C03C3/04—Glass compositions containing silica
    • C03C3/076—Glass compositions containing silica with 40% to 90% silica, by weight
    • 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
    • C03C4/00—Compositions for glass with special properties
    • C03C4/04—Compositions for glass with special properties for photosensitive glass
    • 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
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122—Basic optical elements, e.g. light-guiding paths
    • G02B6/124—Geodesic lenses or integrated gratings
    • C—CHEMISTRY; METALLURGY
    • C03—GLASS; MINERAL OR SLAG WOOL
    • C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B2201/00—Type of glass produced
    • C03B2201/06—Doped silica-based glasses
    • C03B2201/30—Doped silica-based glasses doped with metals, e.g. Ga, Sn, Sb, Pb or Bi
    • C03B2201/31—Doped silica-based glasses doped with metals, e.g. Ga, Sn, Sb, Pb or Bi doped with germanium
    • 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
    • C03C2201/00—Glass compositions
    • C03C2201/06—Doped silica-based glasses
    • C03C2201/30—Doped silica-based glasses containing metals
    • C03C2201/31—Doped silica-based glasses containing metals containing germanium
    • 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
    • C03C2203/00—Production processes
    • C03C2203/50—After-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
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S359/00—Optical: systems and elements
    • Y10S359/90—Methods

Definitions

  • This invention relates to optical devices which include refractive index modulation, e. g. reflection gratings.
  • Reflection gratings are often implemented as waveguides which have a path region and/or a confining region with a modulated refracted index.
  • the waveguiding structure is often in the form of a fibre.
  • the modulation preferably takes the form of alternate regions of higher and lower refractive index. When radiation traverses the modulation, it is selectively reflected.
  • the period of the refractive index modulation is usually equal to the wavelength to be reflected or to a multiple or sub-multiple of said wavelength. Thus periods in the range 250 to 600 nm preferentially reflect selected wavelengths within the range 800 - 1650 n .
  • Reflection gratings have many applications in optical signalling.
  • a reflection grating can be associated with a fibre laser in order to narrow the lasing bandwidth.
  • the grating can be used for the selective removal of unwanted wavelengths.
  • refractive index modulation has other applications, e. g. to achieve phase matching in waveguides, to control spot size and/or shape in waveguides and for storing information.
  • Refractive index modulation is conveniently produced by an optical process in which a photosensitive glass is exposed to radiation which causes an adequate change in its refractive index.
  • the radiation has higher and lower intensities corresponding to the intended pattern of modulation of the refractive index of the glass.
  • the mutual interference of two beams of radiation produces the variation of intensity appropriate for reflection gratings.
  • the pattern of radiation relates to the data to be stored.
  • Silica/germania glasses are widely used in optical telecommunications and it has been noticed that these glasses have an optical absorption band extending approximately over the wavelength range 225 - 275 nm and exposure to radiation within this band increases the refractive index of the silica/germania composition.
  • the peak of the band occurs at a wavelength which is close to 240 nm. It has, therefore, been proposed to produce refractive index modulation, e. g. to make reflection gratings, by exposing silica/germania glass compositions to radiation within the wavelength band 225 - 275 nm. Radiation close to 240 nm is particularly suitable.
  • High powers of radiation e. g. above ImW continuous, are needed to produce adequate changes in the refractive index and writing times of a few minutes to a few hours are appropriate.
  • the sensitivity of the glass is important, and this invention is based upon the unexpected discovery that glasses which contain B 2 0 3 are particularly sensitive to radiation, e. g. radiation close to 240nm, and that these glasses are well adapted to carry the necessary refractive index modulation.
  • the glass contains at least one of Si0 2 and Ge0 2 as well as the B 2 0 3 .
  • compositions consisting essentially of Ge0 2 and B 2 0 3 preferably containing at least 2 mole % of each component, are suitable for thin film optical devices which are capable of storing data in the form of refractive index modulation.
  • compositions consisting essentially of Si0 2 and B 2 0 3 , preferably containing at least 2 mole % of each component, are particularly suitable for carrying the refractive index modulation wherein said modulation constitutes a reflection waveguide located in the confining region of an optical waveguide.
  • Glass consisting essentially of Si0 2 and Ge0 2 would be particularly suitable for use as the path region of said waveguide.
  • compositions consisting essentially of Si0 2 , Ge0 2 and B 2 0 3 are particularly suitable for use in optical devices according the invention.
  • Preferred ternary compositions contain: - 2-40 mole % of B 2 0 3 , 2-40 mole % of Ge0 2 , and at least 30 Mole % of Si0 2 .
  • B 2 0 3 tends to decrease the refractive index of a silica glass whereas Ge0 2 tends to increase the refractive index of a silica glass.
  • the concentration of B 2 0 affects the refractive index as stated above, the refractive index will display a maxima at minima B 2 0 3 concentration and the refractive index will display a minima at maximum B 2 0 3 concentration.
  • glasses which contain B 2 0 3 are particularly sensitive to radiation and, as indicated above, the refractive index patterns produced in accordance with the invention are independent of the boron content of the glass.
  • the mole ratios B: Si and B: Ge are constant in the region where the refractive index modulation is applied. In most applications it is appropriate for both ratios to be constant, eg. the glass has a uniform composition. (Where one of the elements silicon or germanium is absent it is convenient to take the relevant ratio as 1: 0. )
  • the refractive index is one of the important properties because it is usually of major importance to match the refractive indices of the device according to the invention to the refractive index of adjacent optical components.
  • the device according to the invention is often required to perform a waveguiding function and proper adjustment of the refractive indices of the confining region and the path region are necessary to get good waveguiding properties.
  • the ternary compositions with B 2 0 3 in excess of the amount needed to balance the Ge0 2 will have refractive indices lower than that of pure silica whereas ternary compositions with an excess of Ge0 2 will have refractive indices greater than that of pure silica.
  • the ternary compositions can be used in either the confining region, or the path region or in both.
  • confining region and "path region” are used to designate the regions of lower and higher refractive index respectively. It will be appreciated that, especially in the case of single mode waveguides, substantial portions of energy will be transferred in that part of the confining region which is close to the path region. Thus the energy in the confining region will interact with a reflection grating located in the confining region whereby gratings in the confining region can be used either alone or to enhance the effect of gratings in the path region.
  • the waveguiding structures mentioned above maybe either planar waveguiding structures or fibres, especially single mode fibres.
  • the confining region corresponds to the cladding and the path region corresponds to the core.
  • the glasses used to make optical devices according to the invention may contain conventional additives, e. g. melting point depressants to facilitate processing during the manufacture of the articles.
  • melting point depressants for silica glasses include phosphorus, usually present as an oxide, and fluorine.
  • the preparation of optical devices according to the invention usually includes the preparation of the glasses by the oxidation of the appropriate chlorides using 0 2 at high temperature as the oxidizing agent.
  • the glass intended to carry the refracted index modulation may be subjected to mild reduction, e.g. by heating in the absence of oxygen. This is conveniently achieved by heating the glass in the presence of helium.
  • the refractive index modulation is applied to the glass which contains B 2 0 3 by exposing said glass to the appropriate pattern of radiation which accesses the absorption band having a peak close to 240nm. Radiation having wavelengths within the band 225 - 275 nm, e. g. a wavelength which is close to 240nm, is particularly suitable. Radiation which has double these wavelengths is also effective.
  • the gratings are located in the core of a fibre based on silica glasses and the preparation of the fibre will be described first.
  • the exposure of the fibre to radiation in order to produce the refractive index modulation will also be described with reference to accompanying drawing.
  • the fibre was prepared by a modification of the well-known inside deposition process for making optical fibre.
  • the appropriate number of layers are deposited on the inner surface of a tube which serves as a substrate.
  • the outermost layers are deposited first and the innermost layers are deposited last.
  • the tube is collapsed into a solid rod, and the solid rod is drawn into fibre.
  • the heating is carried out by causing a flame to traverse along the length of the tube.
  • the flame heats a short section of the tube so that a portion, about 20 mm long, is heated to the working temperature.
  • This technique of heating is used for all stages of the process, i. e. for the deposition, for consolidating porous layers to solid layers and for the collapse of the tube. Multiple passes are used at all stages of the process.
  • the starting tube was made of pure silica. It had an external diameter of 18 mm and an internal diameter of 15mm.
  • the deposited cladding took the form of Si0 2 with phosphorus and fluorine to reduce its melting point.
  • Six layers of cladding were deposited, and the conditions used for the deposition of each layer were as follows: -
  • the cladding layers could be considered to be part of the substrate tube upon which the core layers were deposited.
  • the deposition of cladding layers as described above could be omitted.
  • the main purpose of the cladding layers is to reduce the risk of contamination from the original tube affecting core layers.
  • the flow rates specify the rate of flow of 0 2 through a bubbler thermostated at 24°C.
  • the flow rate is that of the vapour itself at 300C and 1 atmosphere.
  • the working temperature was only 1450°C but this consolidated the core layers.
  • the tube was collapsed into a solid rod in the conventional manner using five traverses of the flame.
  • the solid rod ie the preform for fibre, had a core which contained approximately 57 mole % Si0 2 , 25 mole % B 2 0 3 and 18 mole % Ge0 2 giving an RI of 1. 462.
  • the composition of the glass in the core was substantially uniform, ie. the mole ratio B: Si was 1: 2.28 throughout and the mole ratio B: Ge was 1: 0.72 throughout.
  • the preform prepared as described above was drawn into fibre of 120 ⁇ m diameter at a temperature of 2,000°C.
  • the fibre was produced at a rate of 18 metres/min.
  • This fibre is the precursor of reflection gratings according to the invention.
  • Short lengths of the fibre described above were converted into reflection waveguides using the technique illustrated in the drawing.
  • the core had a uniform composition, ie. as specified for its preform. Before exposure as described below the refractive index of the core was uniform.
  • a short portion 14 of the fibre 15 was illuminated by a source 10.
  • This radiation was, in the first instance, produced by an Ar + laser, frequency doubled to give output at a wavelength of 244 nm.
  • the beam from the source 10 was directed onto a splitter 11 so that two beams were directed onto mirrors 12 and 13.
  • the mirrors 12 and 13 caused the beams to converge onto the target section, 14.
  • an interference pattern is produced with alternating regions of higher and lower intensity.
  • the region 14 (whereon the beams are focused) is affected by the beams and the refractive index is increased in the areas of high intensity.
  • a reflection grating is produced in the region 14.
  • the spacing of the interference pattern is affected by the angle at which the two beams intersect one another, and hence the spacing of the grating can be adjusted by adjusting the relative position of the splitter 11 and the mirrors 12 and 13.
  • the "RIC” is the relative index change and it is calculated as [(index modulation) / ⁇ n) ] x 100 (to convert to percentage) .
  • grating X can be compared directly with grating A because both gratings are 2mm long.
  • the most important property of the grating is reflectivity and in this key parameter grating A is very much better than grating X (99.5% as against 1.2%). It will be appreciated that the length of a grating has a strong effect upon its reflectivity and the longer a grating (other things being equal) the better its reflectivity. It is, therefore, important that both grating A and X have the same length.
  • Grating B has only half the length but its reflectivity is still 67% which is considerably better than grating X even though grating X is longer.
  • the index modulations of gratings A and B are similar (10 X 10 "4 as compared with 7 x 10 '4 ).
  • Grating X has a much lower modulation (0.34 x 10 " 4 ) which is a clear indication that the boron, containing the glasses are more photo sensitive.
  • Grating X has a slightly higher ⁇ n (0.005 against 0.004) so the RIC values emphasise the superiority of the gratings according to the invention.

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Organic Chemistry (AREA)
  • Chemical Kinetics & Catalysis (AREA)
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  • Glass Compositions (AREA)

Abstract

It has been demonstrated that B containing glasses are sensitive to radiation in the band 225-275 nm and, therefore, B2O3 glasses are particularly adapted to receive refractive index modulation, e.g., to make reflection gratings. Glasses containing SiO2 and B2O3 are particularly suitable when the grating is to be localised in the cladding of a fibre. Glasses containing SiO2, GeO2, and B2O3 are suitable when the grating is in the path region of a waveguide, e.g., in the core of a fibre.

Description

PHOTOINDUCED GRATING IN B2O3 CONTAINING GLASS
This invention relates to optical devices which include refractive index modulation, e. g. reflection gratings.
Reflection gratings are often implemented as waveguides which have a path region and/or a confining region with a modulated refracted index. The waveguiding structure is often in the form of a fibre. The modulation preferably takes the form of alternate regions of higher and lower refractive index. When radiation traverses the modulation, it is selectively reflected. The period of the refractive index modulation is usually equal to the wavelength to be reflected or to a multiple or sub-multiple of said wavelength. Thus periods in the range 250 to 600 nm preferentially reflect selected wavelengths within the range 800 - 1650 n .
Reflection gratings have many applications in optical signalling. For example, a reflection grating can be associated with a fibre laser in order to narrow the lasing bandwidth. When the refractive index bands are not perpendicular to the fibre axis, the grating can be used for the selective removal of unwanted wavelengths. In addition to reflection gratings, refractive index modulation has other applications, e. g. to achieve phase matching in waveguides, to control spot size and/or shape in waveguides and for storing information.
Refractive index modulation is conveniently produced by an optical process in which a photosensitive glass is exposed to radiation which causes an adequate change in its refractive index. The radiation has higher and lower intensities corresponding to the intended pattern of modulation of the refractive index of the glass. In many commonly used embodiments, the mutual interference of two beams of radiation produces the variation of intensity appropriate for reflection gratings. In the case of information storage, the pattern of radiation relates to the data to be stored.
Silica/germania glasses are widely used in optical telecommunications and it has been noticed that these glasses have an optical absorption band extending approximately over the wavelength range 225 - 275 nm and exposure to radiation within this band increases the refractive index of the silica/germania composition. The peak of the band occurs at a wavelength which is close to 240 nm. It has, therefore, been proposed to produce refractive index modulation, e. g. to make reflection gratings, by exposing silica/germania glass compositions to radiation within the wavelength band 225 - 275 nm. Radiation close to 240 nm is particularly suitable. High powers of radiation, e. g. above ImW continuous, are needed to produce adequate changes in the refractive index and writing times of a few minutes to a few hours are appropriate.
The sensitivity of the glass is important, and this invention is based upon the unexpected discovery that glasses which contain B203 are particularly sensitive to radiation, e. g. radiation close to 240nm, and that these glasses are well adapted to carry the necessary refractive index modulation. Preferably the glass contains at least one of Si02 and Ge02 as well as the B203.
Compositions consisting essentially of Ge02 and B203 preferably containing at least 2 mole % of each component, are suitable for thin film optical devices which are capable of storing data in the form of refractive index modulation.
Compositions consisting essentially of Si02 and B203, preferably containing at least 2 mole % of each component, are particularly suitable for carrying the refractive index modulation wherein said modulation constitutes a reflection waveguide located in the confining region of an optical waveguide. Glass consisting essentially of Si02 and Ge02 would be particularly suitable for use as the path region of said waveguide.
Compositions (herein after called ternary compositions) consisting essentially of Si02, Ge02 and B203 are particularly suitable for use in optical devices according the invention. Preferred ternary compositions contain: - 2-40 mole % of B203, 2-40 mole % of Ge02, and at least 30 Mole % of Si02. It should be noted that B203 tends to decrease the refractive index of a silica glass whereas Ge02 tends to increase the refractive index of a silica glass.
Since the concentration of B20, affects the refractive index as stated above, the refractive index will display a maxima at minima B203 concentration and the refractive index will display a minima at maximum B203 concentration. It is standard practice in the preparation of optical waveguides to vary the concentration of a dopant radially through the core region, eg to fabricate a graded index multimode fibre. However, it is less convenient (and even impractical) to produce fine detail longitudinal variation, eg a reflection grating, by varying the concentrations of relevant components.
It has been noticed that some glasses are photo-sensitive whereby exposure to suitable light causes changes in the refractive index and exposure to fine patterns is adapted to produce the desired fine detail. It is doubtful that the optical exposure changes the chemical composition of the glass and it is more appropriate to postulate that structural changes, possibly including defect centres, play a substantial role in the overall effect. Even though the mechanism is not fully understood, the production of refractive index patterns by exposure to radiation has been demonstrated experimentally.
It has already been stated that glasses which contain B203 are particularly sensitive to radiation and, as indicated above, the refractive index patterns produced in accordance with the invention are independent of the boron content of the glass. Conveniently the mole ratios B: Si and B: Ge are constant in the region where the refractive index modulation is applied. In most applications it is appropriate for both ratios to be constant, eg. the glass has a uniform composition. (Where one of the elements silicon or germanium is absent it is convenient to take the relevant ratio as 1: 0. )
Ternary compositions as defined above have great potential for adjusting the important properties of the glass as required. The refractive index is one of the important properties because it is usually of major importance to match the refractive indices of the device according to the invention to the refractive index of adjacent optical components. The device according to the invention is often required to perform a waveguiding function and proper adjustment of the refractive indices of the confining region and the path region are necessary to get good waveguiding properties. In particular it is important to adjust the refractive index difference between the path region and the confining region to a predetermined value. This difference is usually called Δn.
It is possible to adjust the ratio of B203: G203 so that the decrease in refractive index caused by the B203 is balanced (approximately or exactly) by the increase caused by the
B203. Thus the ternary compositions with B203 in excess of the amount needed to balance the Ge02 will have refractive indices lower than that of pure silica whereas ternary compositions with an excess of Ge02 will have refractive indices greater than that of pure silica. The ternary compositions can be used in either the confining region, or the path region or in both.
The terms "confining region" and "path region" are used to designate the regions of lower and higher refractive index respectively. It will be appreciated that, especially in the case of single mode waveguides, substantial portions of energy will be transferred in that part of the confining region which is close to the path region. Thus the energy in the confining region will interact with a reflection grating located in the confining region whereby gratings in the confining region can be used either alone or to enhance the effect of gratings in the path region.
It will be appreciated that the waveguiding structures mentioned above maybe either planar waveguiding structures or fibres, especially single mode fibres. In the case of a fibre the confining region corresponds to the cladding and the path region corresponds to the core.
In addition to the essential ingredients as specified above the glasses used to make optical devices according to the invention may contain conventional additives, e. g. melting point depressants to facilitate processing during the manufacture of the articles. Melting point depressants for silica glasses include phosphorus, usually present as an oxide, and fluorine.
The preparation of optical devices according to the invention usually includes the preparation of the glasses by the oxidation of the appropriate chlorides using 02 at high temperature as the oxidizing agent. If desired, the glass intended to carry the refracted index modulation may be subjected to mild reduction, e.g. by heating in the absence of oxygen. This is conveniently achieved by heating the glass in the presence of helium.
The refractive index modulation is applied to the glass which contains B203 by exposing said glass to the appropriate pattern of radiation which accesses the absorption band having a peak close to 240nm. Radiation having wavelengths within the band 225 - 275 nm, e. g. a wavelength which is close to 240nm, is particularly suitable. Radiation which has double these wavelengths is also effective.
Two reflection gratings according to the invention will now be described by way of example. The gratings are located in the core of a fibre based on silica glasses and the preparation of the fibre will be described first. The exposure of the fibre to radiation in order to produce the refractive index modulation will also be described with reference to accompanying drawing.
The fibre was prepared by a modification of the well-known inside deposition process for making optical fibre. In this process, the appropriate number of layers are deposited on the inner surface of a tube which serves as a substrate. Thus the outermost layers are deposited first and the innermost layers are deposited last. After all the layers have been deposited, the tube is collapsed into a solid rod, and the solid rod is drawn into fibre.
Individual layers are produced by passing a mixture of oxygen and SiCl4 with reagents such as B2C13 and GeCl4 through the tube and heating a small section thereof to temperatures in the range 1200°C - 2000-C, Under these conditions the chlorides are converted into the corresponding oxides which initially deposit on the wall of the tube in the form of a fine "soot" which is immediately fused to give a consolidated glass. As an alternative the deposition is carried out at a temperature such that the deposit remains in a porus state and, at a later stage in the process, the "soot" is fused at a higher temperature to give the consolidated glass. This alternative is appropriate when it is desired to submit the deposit to chemical treatments wherein the porus state facilitates the desired reaction, e. g. reduction. Melting point depressants such as phosphorus and fluorine may be incorporated in the mixture to facilitate processing by 10 causing fusing at lower temperatures.
The heating is carried out by causing a flame to traverse along the length of the tube. The flame heats a short section of the tube so that a portion, about 20 mm long, is heated to the working temperature. This technique of heating is used for all stages of the process, i. e. for the deposition, for consolidating porous layers to solid layers and for the collapse of the tube. Multiple passes are used at all stages of the process.
The starting tube was made of pure silica. It had an external diameter of 18 mm and an internal diameter of 15mm.
Cladding Deposition
The deposited cladding took the form of Si02 with phosphorus and fluorine to reduce its melting point. Six layers of cladding were deposited, and the conditions used for the deposition of each layer were as follows: -
Figure imgf000010_0001
In the case of SiCl2 and P0C13 the flow rates specify the rate of flow of 02 through a bubbler thermostated at 24°C. The working temperature was approximately 1525°C. It is emphasised, that after each traverse, each cladding layer was in the form of a clear glassy layer before the next layer was deposited.
The cladding layers could be considered to be part of the substrate tube upon which the core layers were deposited. The deposition of cladding layers as described above could be omitted. The main purpose of the cladding layers is to reduce the risk of contamination from the original tube affecting core layers.
Core Deposition
Core was deposited in two layers and the conditions for the deposition of each of the two layers were as follows:
Figure imgf000011_0001
In the case of SiCl4 and the GeCl4 the flow rates specify the rate of flow of 02 through a bubbler thermostated at 24°C. In the case of BC13 the flow rate is that of the vapour itself at 300C and 1 atmosphere.
The working temperature was only 1450°C but this consolidated the core layers.
After the preparation described above, the tube was collapsed into a solid rod in the conventional manner using five traverses of the flame.
The solid rod, ie the preform for fibre, had a core which contained approximately 57 mole % Si02, 25 mole % B203 and 18 mole % Ge02 giving an RI of 1. 462. The cladding, essentially Si02, had an RI of 1.458 so that Δn = 0.006. The composition of the glass in the core was substantially uniform, ie. the mole ratio B: Si was 1: 2.28 throughout and the mole ratio B: Ge was 1: 0.72 throughout.
The procedure described above, apart from the use of BC13 in the core, constitutes an essentially conventional preparation of a fibre preform.
The preform prepared as described above was drawn into fibre of 120μm diameter at a temperature of 2,000°C. The fibre was produced at a rate of 18 metres/min. This fibre is the precursor of reflection gratings according to the invention. Short lengths of the fibre described above were converted into reflection waveguides using the technique illustrated in the drawing. In each short length of fibre the core had a uniform composition, ie. as specified for its preform. Before exposure as described below the refractive index of the core was uniform.
A short portion 14 of the fibre 15 was illuminated by a source 10. This radiation was, in the first instance, produced by an Ar+ laser, frequency doubled to give output at a wavelength of 244 nm. The beam from the source 10 was directed onto a splitter 11 so that two beams were directed onto mirrors 12 and 13. The mirrors 12 and 13 caused the beams to converge onto the target section, 14. Thus an interference pattern is produced with alternating regions of higher and lower intensity. Because the fibre 15 is photosensitive, the region 14 (whereon the beams are focused) is affected by the beams and the refractive index is increased in the areas of high intensity. Thus a reflection grating is produced in the region 14.
It will be appreciated that the spacing of the interference pattern is affected by the angle at which the two beams intersect one another, and hence the spacing of the grating can be adjusted by adjusting the relative position of the splitter 11 and the mirrors 12 and 13.
Two specimens of this fibre were subjected, to an interference pattern to produce reflection gratings A and B. For comparison, a reflection grating was prepared from a conventional fibre, i. e. without the boron. This comparative grating is identified as grating X. Important measurements on these gratings and their fibre waveguides are given in the following table.
Figure imgf000013_0001
The "RIC" is the relative index change and it is calculated as [(index modulation) /Δn) ] x 100 (to convert to percentage) .
(In optical technology, refractive index matching of components is often important to avoid unwanted reflections from component interfaces. Thus reflection gratings need to be refractive index-matched to adjacent components and this limits the freedom to adjust the composition to maximise the photo sensitivity and the grating properties. It is usually easier to obtain index modulation in fibre which has high Δn and the RIC takes this circumstance into account) .
The properties of grating X can be compared directly with grating A because both gratings are 2mm long. The most important property of the grating is reflectivity and in this key parameter grating A is very much better than grating X (99.5% as against 1.2%). It will be appreciated that the length of a grating has a strong effect upon its reflectivity and the longer a grating (other things being equal) the better its reflectivity. It is, therefore, important that both grating A and X have the same length.
Grating B has only half the length but its reflectivity is still 67% which is considerably better than grating X even though grating X is longer. The index modulations of gratings A and B are similar (10 X 10"4 as compared with 7 x 10'4). Grating X has a much lower modulation (0.34 x 10" 4) which is a clear indication that the boron, containing the glasses are more photo sensitive. Grating X has a slightly higher Δn (0.005 against 0.004) so the RIC values emphasise the superiority of the gratings according to the invention.

Claims

£I LM& β 1. An optical device comprising refractive modulation wherein said modulation is applied to glass composition 5 which contains B203 and at least one of Si02 and Ge02 wherein the pattern of refractive index variations is independent of the boron content of the glass composition to which the refractive index modulation is applied.
10 2. An optical device according to claim.1, wherein the modulation constitutes a reflection grating which takes the form of alternate regions of higher and lower refractive index whereby said modulation is adapted for use as a reflection grating.
15
3. An optical device according to claim 2, wherein the period of said refractive index modulation is within the range 0.25 to 0.6 μm whereby said modulation selectively reflects radiation within the wavelength band 800 - 1650
20 nm.
4. An optical device according to either claim 2 or claim 3, wherein said modulation is located in the confining region of a waveguide.
25
5. An optical device according to claim 4, wherein the confining region is formed of a silica glass doped with B203 and the path region is formed of a silica glass doped with Ge02.
30
6. An optical device according to either claim 2 or claim 3, wherein said modulation is located in the path region of a waveguide.
35 7. An optical device according to claim 6, wherein the confining region is formed of a silica glass and the path region is formed of a silica glass doped with B203 and Ge02.
8. An optical device according to any one of claims 4-7, wherein the waveguide is in the form of a fibre.
9. An optical device according to claim 8, wherein the fibre is single mode at the signal wavelength.
10. A method of producing an optical device according any one of the preceding claims, which method-comprises exposing a portion of said article to a modulated intensity of radiation which accesses the absorption band having a peak close to 240nm whereby the refractive index of said portion is modulated to reproduce the intensity pattern of said radiation, said portion being formed of a glass composition which contains B203, and at least one of Si02 and Ge02.
11. A method according to claim 10, wherein the wavelength of said radiation is within the band 225 -
275nm.
PCT/GB1993/001321 1992-06-24 1993-06-24 Photoinduced grating in b2o3 containing glass Ceased WO1994000784A1 (en)

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EP93913418A EP0647327B1 (en) 1992-06-24 1993-06-24 Photoinduced grating in b2o3 containing glass
US08/302,931 US6075625A (en) 1992-06-24 1993-06-24 Photoinduced grating in B2 O3 containing glass
DE69317285T DE69317285T2 (en) 1992-06-24 1993-06-24 LIGHT INDUCED GRATING IN GLASS CONTAINING B2O3
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