The present invention relates to an optical fiber suitable for fiber Bragg grating.
International Publication No. 2003/093887 (Patent Document 1) discloses an optical fiber Bragg grating having a refractive-index modulation in a predetermined range along the optical axis of an optical fiber, and an optical fiber suitable for forming such refractive-index modulation. The optical fiber Bragg grating disclosed in Patent Document 1 is a slanted fiber grating (SFG), in which the periodic length of refractive-index modulation is several hundred nanometers, and the lattice plane of the grating is inclined relative to a section perpendicular to the optical axis of the optical fiber. Such SFG is applied as a gain equalization filter for flattening the gain spectrum of an erbium-doped fiber amplifier (EDFA), for example.
The optical fiber disclosed in Patent Document 1 is made of silica-based glass and comprises a core region including the center of an optical axis and a cladding region formed around the core region, whereas the core region does not contain GeO2, and the cladding region contains GeO2 at least at its part. The silica glass doped with GeO2 has photosensitivity to light having a predetermined wavelength (for example, ultraviolet light having a wavelength of 270 nm or less), and the refractive index thereof increases when it is irradiated with such light. Utilizing such phenomenon makes it possible to form a refractive-index modulation in the silica glass doped with GeO2. The composition of an optical fiber which is the most suitable from the viewpoint of both process time for filter formation and filter properties (base loss, peak wavelength shift, and change of width at half maximum in a transmission spectrum due to refractive-index modulation) is unknown, since Patent Document 1 does not disclose it. Here, the “base loss” means a transmission loss that is not influenced by refractive-index modulation, and the “peak wavelength” means a wavelength at which the transmittance becomes minimum with the refractive-index modulation.
An object of the present invention is to provide an optical fiber having a composition that is optimal from the viewpoint of filter properties of SFG and filter formation time.
An optical fiber of the first embodiment of the present invention, which is made of silica-based glass, comprises a core region including an optical axis of the fiber and a cladding region formed around the core region, whereas the cladding region has a refractive index smaller than a refractive index of the core region and contains GeO2 having a concentration of 6.8 wt % or more at least at a part of the cladding.
In the optical fiber of the first embodiment, the concentration may be 7.4% or less or 8.7% or less. The part of the cladding region may have an outer diameter that is 1.5 to 4.0 times larger than a mode field diameter at a wavelength in the C-band. Here, the “C-Band” spreads from 1530 nm to 1565 nm.
The optical fiber of the second embodiment of the present invention is an optical fiber made of silica-based glass and comprises a core region including an optical axis of the fiber and a cladding region formed around the core region, whereas the cladding region has a refractive index smaller than a refractive index of the core region and contains GeO2 having a concentration of 7.4 wt % or more and 7.9 wt % or less, or not less than 7.4 wt % and not more than 8.7 wt % at least at a part thereof, the part of the cladding region has an outer diameter that is 1.5 to 4.0 times larger than a mode field diameter at a wavelength in the C-band.
In the optical fiber of both embodiments, the part of the cladding region may include an inner circumference and an outer circumference around the inner circumference. The concentration of GeO2 at the inner circumference is larger than the concentration of GeO2 at the outer circumference, and the difference between the GeO2 concentration at the inner circumference and the GeO2 concentration at the outer circumference is 0.2 wt % or more. The above-mentioned core region does not need to contain GeO2.
According to the present invention, it is possible to offer an optical fiber which has an optimal composition from the viewpoint of filter formation time and filter properties of SFG.
Hereafter, with reference to accompanying drawings, detailed explanation of preferred embodiments for carrying out the present invention will be given. In the explanation of drawings, the same mark is given to identical elements and the overlapping explanation is omitted. The present invention is not limited to these embodiments, and it is intended that the scope of the invention be understood by the claims and equivalents, including all modifications thereto.
In the optical fiber 1, the optical cladding region 12 is a photosensitive region which has photosensitivity to light having a predetermined wavelength in the ultraviolet region, and the refractive index of the optical cladding region is made larger by irradiation of the ultraviolet light. The core region 11 and the jacket region 13 do not have photosensitivity. By irradiating the optical fiber 1 with light which has a predetermined wavelength in the ultraviolet region and in which the intensity is spatially modulated, a refractive-index can be modulated in a predetermined range in the optical cladding region 12 along the direction of the optical axis of the optical fiber 1, whereby SFG can be formed. Of light guided through the core region 11, light having a specific wavelength in the operating window which satisfies Bragg condition can be leaked to the optical cladding region 12, so that a SFG can function as a filter having a specific loss as a function of wavelength. By changing the periodic length of refractive index modulation, the filtering properties of SFG can be changed. It is possible to obtain arbitrary filter properties by changing the periodic length of refractive index modulation in the direction of the optical axis of an optical fiber.
The photosensitive region may include an inner circumference and an outer circumference around the inner circumference. The concentration of GeO2 at the inner circumference is larger than that at the outer circumference. In such case, it is possible to obtain satisfactory characteristics for the base loss, the peak wavelength shift, and the change of width at half maximum in a transmission spectrum. Also, by decreasing the GeO2 concentration of the outermost layer in the photosensitive region, the generation of voids at the interface between the cladding region and the jacket region can be suppressed, whereby the yield can be improved.
To secure the long-term reliability of SFG, it is preferable to carry out an annealing treatment upon manufactured SFG. However, filter properties may be changed by the annealing treatment.
The annealing treatment will degrade the filtering function. Therefore, the filter spectrum should be made as one having the higher loss beforehand. As the residual ratio increases, the control of filter properties which change as the time of annealing becomes easier. Also, the initial loss in filter spectrum can be made lower. As a result, the manufacturing time can be shortened. The residual ratio is preferably 36% or more. However, even if the GeO2 concentration is increased, the residual ratio tends to gradually approach to about 34%. If the GeO2 concentration is 8.7 wt % or less, writing properties and yield will be superior to the case of 7.85 wt % of GeO2 concentration as well as the residual ratio of 34% or more can be maintained. Thus, the GeO2 concentration of 8.7 wt % or less also is suitable.
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The following is an explanation about the outer diameter 2b of an optical cladding region (photosensitive region). When the outer diameter 2b of an optical cladding region is too small, the overlap of the optical cladding region and the electromagnetic field of propagating lightwave guided through the core becomes smaller, resulting in degradation of filter properties. When the outer diameter 2b of an optical cladding region is too large, the silica glass doped with Ge and fluorine tends to generate voids by heating. Therefore, the larger the outer diameter 2b, the less the yield of a fiber becomes, although it does not affect filter properties. The lower limit of the outer diameter 2b of the optical cladding region is preferably 1.5 or more times larger than the MFD at a wavelength in the operating wavelength in view of the electromagnetic field of the propagation lightwave guided through the core. The upper limit of the outer diameter 2b of the optical cladding region is preferably 4.0 or less times larger than the MFD. By forming the outer diameter of an optical cladding region so as to be 1.5 to 4.0 times larger than the mode field diameter in an operating wavelength band, it is made possible to manufacture an optical fiber Bragg grating at high yield, while the degradation of filter properties can be small.
Number | Date | Country | Kind |
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2014-211378 | Oct 2014 | JP | national |
2015-142847 | Jul 2015 | JP | national |