METHOD OF FORMING OPTICAL FIBRE GRATINGS

Abstract: An optical fibre (2) is fixed between a clamp (6) and a piezo-electric translation stage (10). An argon ion laser (12) emitting at 514.5 nm is used to write Bragg gratings in the fibre (2). A different longitudinal stress is applied to the fibre (2) before optically writing each Bragg grating. The fibre (2) when unstressed will have a Bragg grating of different peak reflectivity corresponding to the number of different applied stresses.

Description: ~ METHOD OF FORMI NG OPTI CAL FI BRE GRATI NGS This invention relates to a method of forming two or more Bragg gratings in an optical fibre waveguide. 5 In this specification the term "optical" is intended to refer to that part of the electromagnetic spectrum which is generally known as the visible region together with those parts of the infra-red and ultraviolet regions at each end of the visible region which are capable of being 10 transmitted by dielectric optical waveguides such as optical fibres. There is considerable interest in exploiting photosensitivity in germanosilicate optical fibres for application in the areas of optical communication and 15 sensors. The first reported permanent optically-induced changes of the refractive index of optical fibres was by K.0. Hill, Y. Fujii, D. C. Johnson and B. S. Kawasaki, "Photosensitivity in Optical Fibure Waveguides: Application to Reflection Filter Fabrication" Appl. Phys. Lett, 32. 647 20 (1978). In their experiment coherent radiation at 514.5nm, reflected from the fibre ends, generated a standing wave in the fibre which induced a periodic refractive index change along its length. This formed a high reflectivity Bragg grating in the fibre which peaked at the wavelength of the 25 incident beam. Since then numerous studies into the grating growth mechanism and photosensitive fibres have been carried out see for example D. K. W. Lam, B. K. Garside, "Characterisation of Single-Mode Optical Fibre Filters" Appl. Phys, Lett, 2 ___ 440 (1981) and J. Stone, J. Appl. i f ι 30 Phys., J2. 4371 (1987). However, .the mechanism which results in the perturbation to the refractive index of the fibre core is not fully understood. The spectral region where the fibre is photosensitive has been found to range from the UV to around 700nm. The potential applications of fibre gratings are numerous. For example, in telecommunication applications tunable integrated fibres gratings, externally written with a UV laser, may be used to spectrally control fibre lasers. B. S. Kawasaki, H.0. Hill, D. C. Johnson and Y. Fujii in an article entitled "Narrow-band Bragg reflectors in optical fibres", Optics Letters Vol 3 No.2 August 1978, pp 66-68 note that an important property of the grating formation process is the extent to which the filter response can be tailored. For example, one method of forming a complex filter is to superimpose two or more simple band-stop characteristics in the same fibre by illuminating or adjustment of the grating writing equipment the fibre with different wavelengths of light either simultaneously or consecutively. Another known method of forming the Bragg gratings is by side-writing the gratings by interfering two coherent radiation beams at an appropriate angle. The pitch of the grating is determined by the angle of intersection of the two beams so different grating pitches can be formed by adj sting this angle. According to the present invention a method of forming two Bragg gratings in an optical fibre is characterised in that a different longitudinal stress is applied to the fibre before optically writing each grating, all the gratings having the same Bragg condition at the time of writing. The present invention provides a method of writing two or more Bragg gratings without the need for multiple wavelength illumination. The method of the present invention exploits the fact that optical fibre can, theoretically, be linearly strained by up to 20%. If a photorefractive fibre, length 1, is illuminated by a light from a laser of wavelength λO, this will result in a grating of period of about λ 0 /2n ef( where ne,l,i is the fibre mode refractive index. If the fibre is now stretched by Δl, then when illuminated, a grating of the same pitch, i. e. same Bragg condition, as before will be 5 written. When the fibre as allowed to relax to its unstressed, normal length after writing the pitch of this second grating will now be slightly smaller than the first grating. For the case of a reflection filter the second grating has now a peak wavelength which is smaller than the 10 writing wavelength. This can be extended to providing several different pitch gratings in the same fibre. If, for example, there are two gratings of different period in the fibre then if it is assumed that they have some relative phase relationship the index modulation in 15 the fibre is now effectively given by the superposition of the two index modulations. This is given by n e(( (z)=A 1 COS ( (k 1 +k 2 )Z)COS( (k.-k 2 ) Z) where j and k 2 are the wave numbers of the two gratings and z is the propagation direction and A j is the amplitude of 20 the refractive index perturbation. At present, it is the second modulation term that is of interest and it can be assumed that the first term, which is a high frequency term, is a constant at present. (This high frequency term can in principle be used as a short wavelength reflection 25 filter). The index modulation is therefore now given by n e(( (Z)=A 2 COS((k,-k 2 )Z) From this expression it can be seen that by choosing the periods of the two optically written gratings a resultant grating of any period can be generated. The frequency 30 difference grating written in the fibre is of particular interest in applications such as SHG, polarisation conversion and mode conversion as it allows the necessary I phase matching conditions to be met for. these processes. ' The actual operating wavelength depends only on the 35 difference in the values of k j and k 2 and not on the actual write wavelength itself. For example, a simple calculation shows that the fibre would have to be stretched by approximately 2% if it is to be used for phase matching in SHG. Even smaller changes in fibre length would be required for polarisation and mode convertors. These fibre length changes should be easily attainable in the fibre currently being used in experiments. It may also be possible to write reflection gratings for use at the telecommunications bandwidth of 1.3-1.5μm if the fibre can be stretched by approximately 10%. This is still within the theoretically predicted change but due to defects in the manufacture of the fibre it is not clear whether it is possible to do this. Assuming that it may be done this would allow highreflectivity small bandwidth gratings to be written in the fibre. It would also be possible to write several gratings in the fibres which would allow pulse generation and shaping of incident laser light. A convenient method of applying the different longitudinal stresses to the fibre to produce the different stains is to clamp one end of the fibre and apply the stress by means of a pizo-electric translation stage clamped to the other end of the fibre. Clearly, other stressing means may be used such as a clamped micrometer attached to the fibre end instead of the piezo-electric translation stage. Othe writing techniques can be used for example wrapping the fibre around a cylinder, the stress being applied to the fibre by varying the radius of the cylinder by a piezo-electric expander also the fibrecould be coated with a piezo-electric cladding, the strain can be changed by varying rhe applied voltage. The invention is applicable to external grating writing methods as well as to gratings written by launching an optical signal down the fibre. An embodiment of the present invention will now be described by way of example only, with reference to the accompanying drawings of which, Figure 1 is a schematic diagram of apparatus specifically designed for carrying out the method of the present invention; Figure 2 is a graph of the reflectance and transmittance of a fibre grating as a function of relative strain; and Figure 3 is a graph of the reflectance and transmittance of a fibre having two gratings as a function of applied strain. The experimental apparatus used to write gratings in single mode germanosilicate fibres at 514.5nm is shown in Figure 1. A fibre 2 with a radius of 0.9μm and a Δn of 0.012 is clamped at one end 4, which is enclosed in a glass ferrule 5 and clamped with a clamp 6, with the other end 8 being connected to a piezo-electric translation stage 10 which allows the length of the fibre, about equal to 50cm in this case, to be changed by up to by 20μm. The gratings are written by coupling an argon ion laser 12 lasing at 514.5nm into end 4 of the fibre 2 via a partial reflector 14 and lens 16. The signal exiting the end 8 of fibre 2 during writing of a grating is focussed onto a photodetector 18. The increasing signal reflected b^ the grating as it is written into the fibre 2 exits end 4 of the fibre 2 and is focussed by lens 16 and reflected to a photodetector 20 by the partial reflector 14. During the writing and reading of the grating, the polarisation of the input and monitor beams were carefully controlled. The reflectance profile of the fibre 2 after writing the gratings was obtained by launching . 0.5mW of 514.5nm light into the fibre and then stretching the fibre using the piezo-electric translation stage 10. Figure 2 shows the low power reflectance/transmittance of a typical grating formed in the fibre after 250mW, from the single mode argon ion laser 12 was launched into it for approximately two minutes. This gives the reflectance/transmittance profile of the grating as the Bragg condition of the grating linearly changes with strain. From this data the grating was found to have a peak relativity of 70% and a bandwidth of 482MHz. The profile of the grating shown in Figure 2 is similar to the sine 2 reflection profile normally associated with Bragg reflectors. By changing the strain applied to the fibre before writing a grating, a further three gratings were optically written in the same fibre each with a peak wavelength separated by 46GHz. By varying the strain applied to the fibre the four gratings written in the fibre can be scanned through. Figure 3 shows the transmittance and reflectance as a function of applied strain for a probe signal of 514.5 nm from the argon laser 12 for a strain range which scanned through two of the four gratings.

Claims: CLAIMS 1. A method of forming two or more Bragg gratings in an optical fibre waveguide characterised in that a different ■ V longitudinal stress is applied to the fibre before 5 optically writing each grating, all the gratings having the same Bragg condition at the time of writing. 2. A method as claimed in claim 1 in which all gratings are written by launching an optical signal of the same wavelength down the fibre. 10 3. A method as claimed in either one of claims 1 and 2 in which the strains are applied to the fibre by means of a piezo-electric stretcher.. 4. A method as claimed in any preceding claim in which the fibre is a single mode germanosilicate optical fibre. 15 5. A method as claimed in claim 4 in which the optical signal has a wavelength 514.5nm.

Inventors: CAMPBELL ROBERT JOHN, KASHYAP RAMAN, CAMPBELL, ROBERT, JOHN, KASHYAP, RAMAN
Applicants: BRITISH TELECOMM, BRITISH TELECOMMUNICATIONS PUBLIC LIMITED COMPANY
Application year: 1991
Main classification: G02B5
IPC codes: G02B5, G02B6