Device for producing apodized gratings

Information

  • Patent Grant
  • 6313473
  • Patent Number
    6,313,473
  • Date Filed
    Friday, May 14, 1999
    25 years ago
  • Date Issued
    Tuesday, November 6, 2001
    22 years ago
Abstract
A device for producing apodized gratings on a stationary optical fiber. The device includes a slit-generating means, a stationary phase mask and a stationary writing-beam-generating means. A slit is generated by the slit-generating means. A writing beam is generated by the stationary writing-beam-generating means to pass through the slit and the stationary phase mask and then focus on the stationary optical fiber for a plurality of exposure time periods. The slit is adjustable in width so that the slit has a plurality of widths during the plurality of exposure time periods, respectively.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates in general to a device for producing apodized gratings.




2. Description of the Related Art




Apodized gratings are particularly important for telecommunications applications, such as dense wavelength division multiplexing and dispersion compensation, because well-designed apodization profiles can considerably suppress the sidelobes in the grating reflection spectra. J. Martin et al. disclosed a method of producing apodized gratings (ELECTRONICS LETTERS, May 12, 1994, Vol.30, No.10, pp.811-812). Referring to

FIG. 1

, an optical fiber


11


and a phase mask


12


are movably mounted on a translation stage


13


, wherein the optical fiber


11


is placed behind the phase mask


12


. Then, a UV beam


14


is projected through the phase mask


12


to write gratings on the optical fiber


11


. In this method, however, any offset of the beam position relative to the optical fiber center during the translation results in a corresponding variation of the average refractive index of the optical fiber. The variation of the average refractive index imparts an often undesired chirp to the gratings. To resolve such a problem, W. H. Loh et al. disclosed a moving fiber-scanning beam technique (OPTICS LETTERS, Oct. 15, 1995, Vol.20, No.20, pp.2051-2053). Referring to

FIG. 2

, an optical fiber


21


is mounted on a computer-controlled stage


23


which slowly moves with respect to a phase mask


22


. A UV beam


24


is reflected by a moving mirror


25


to pass through the phase mask


22


so as to write gratings on the optical fiber


21


. By the movement of the UV beam, variation of the average refractive index of the optical fiber is totally avoided because the average UV fluence along the length of the grating is the same. However, simultaneously control of the movement of the stage


23


and the mirror


25


is required in this system. Such a system is very complex.




SUMMARY OF THE INVENTION




An object of the present invention is to provide a device that solves the above-mentioned problems.




In accordance with the object of the present invention, a device for producing apodized gratings on a stationary optical fiber is provided. The device includes a slit-generating means, a stationary phase mask and a stationary writing-beam-generating means. A slit is generated by the slit-generating means. A writing beam is generated by the stationary writing-beam-generating means to pass through the slit and the stationary phase mask and then focus on the stationary optical fiber for a plurality of exposure time periods. The slit is adjustable in width so that the slit has a plurality of widths during the plurality of exposure time periods, respectively.




In the present invention, neither the UV-generating means nor the optical fiber is moved. Therefore, controlling the device of the present invention is much simpler than controlling the device of the prior art. In addition, the problem of chirps does not arise because the UV-generating means does not move with respect to the optical fiber.











BRIEF DESCRIPTION OF THE DRAWINGS




The present invention can be more fully understood by reading the subsequent detailed description and examples with references made to the accompanying drawings, wherein:





FIG. 1

is a schematic diagram of a device for producing apodized gratings in accordance with a first example of the prior art;





FIG. 2

is a schematic diagram of a device for producing apodized gratings in accordance with a second example of the prior art;





FIG. 3

is a schematic diagram of a device for producing apodized gratings in accordance with the present invention;





FIG. 4A

shows the exposure time periods in accordance with a first example of the present invention; and





FIG. 4B

shows the exposure time periods in accordance with a second example of the present invention.











DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT




Referring to

FIG. 3

, a device for producing apodized gratings of the present invention includes a phase mask


32


, a slit-generating means


35


and a UV-generating means


36


. The slit-generating means


35


can generate a slit


33


of adjustable width “W”. In operation, a UV beam


34


emitted from the UV-generating means


36


passes through the slit


33


and the phase mask


32


to focus on an optical fiber


31


. That is, gratings are written on the optical fiber


31


. It is noted that in the operation the UV beam


34


, the phase mask


32


and the optical fiber


31


are stationary. On the other hand, the slit-generating means


35


operates to change the width “W” of the slit


33


through which the UV beam


34


passes. The change of the slit width can be accomplished in two different ways:




(1) Referring to

FIG. 4A

, the original time is t


o


. The optical fiber


31


is exposed to the UV beam


34


through a slit width “W


1


” in the time interval t


o


≦T≦t


1


, wherein the exposure time is Δt (=t


1


−t


o


). Then, the slit width is changed from W


1


to W


2


, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W


2


” in the time interval t


1


≦T≦t


2


, wherein the exposure time is also Δt. Then, the slit width is changed from W


2


to W


3


, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W


3


” in the time interval t


2


≦T≦t


3


, wherein the exposure time is still Δt. By analogy, the slit width is changed from W


n−1


to W


n


, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W


n


” in the time interval t


n−1


≦T≦t


n


, wherein the exposure time is still Δt. In this example, every exposure time for every slit width is the same (=Δt) while the slit widths are mutually different (W


1


≠W


2


≠W


3


≠. . . ≠W


n


).




(2) Referring to

FIG. 4B

, the original time is T=T


o


. The optical fiber


31


is exposed to the UV beam


34


through a slit width “W” in the time interval t


o


≦T≦t


1


, wherein the exposure time is Δt


1


. Then, the slit width is changed from “W” to “W+ΔW”, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W+ΔW” in the time interval t


1


≦T≦t


2


, wherein the exposure time is Δt


2


and Δt


2


≠Δt


1


. Then, the slit width is changed from “W+ΔW” to “W+2ΔW”, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W+2ΔW” in the time interval t


2


≦T≦t


3


, wherein the exposure time is Δt


3


and Δt


3


≠Δt


2


. By analogy, the slit width is changed from “W+(n−1) ΔW” to “W+nΔW”, and the optical fiber


31


is exposed to the UV beam


34


through the slit width “W+nΔW” in the time interval t


n−1


≦T≦t


n


, wherein the exposure time is Δt


n


and Δt


n


≠Δt


n−1


. In this example, the differences among the slit widths are the same (=ΔW) while the exposure time is adjustable (Δt


1


≠Δt


2


≠Δt


3


. . . ≠ΔT


n


).




By changing the exposure time and slit width, we can produce apodized gratings of any mathematical functions on the optical fibers. Furthermore, in the present invention, neither the UV-generating means nor the optical fiber is moved. Therefore, controlling the device of the present invention is much simpler than controlling the device of the prior art. The problem of chirps does not arise because the UV-generating means does not move with respect to the optical fiber.




While the invention has been described by way of example and in terms of the preferred embodiment, it is to be understood that the invention is not limited to the disclosed embodiments. To the contrary, it is intended to cover various modifications and similar arrangements (as would be apparent to those skilled in the art). Therefore, the scope of the appended claims should be accorded with the broadest interpretation so as to encompass all such modifications and similar arrangements.



Claims
  • 1. A device for producing apodized gratings on a stationary optical fiber, comprising:a slit-generating means for generating a slit; a stationary phase mask; and a stationary writing-beam-generating means for generating a writing beam which passes through the slit and the stationary phase mask and then focuses on the stationary optical fiber for a plurality of exposure time periods; wherein the slit is adjustable in width so that the slit has a plurality of widths during the plurality of exposure time periods, respectively.
  • 2. A device for producing apodized gratings on a stationary optical fiber as claimed in claim 1, wherein the writing beam is an ultraviolet beam.
  • 3. A device for producing apodized gratings on a stationary optical fiber as claimed in claim 1, wherein the plurality of exposure time periods are the same while the plurality of widths are mutually different.
  • 4. A device for producing apodized gratings on a stationary optical fiber as claimed in claim 1, wherein differences between the plurality of widths are the same while the plurality of exposure time periods are mutually different.
US Referenced Citations (4)
Number Name Date Kind
5104209 Hill et al. Apr 1992
5953471 Espindola et al. Sep 1999
6043497 Quetel et al. Mar 2000
6160261 Hoshino Dec 2000
Non-Patent Literature Citations (2)
Entry
Article entitled “Novel Writing Technique of Long and Highly Reflective In-Fibre Gratings” by J. Martin et al., (Electronics Letters, 12th May 1994, vol. 30, No. 10, pp. 811-812).
Article entitled “Complex Grating Structures With Uniform Phase Masks Based On The Moving Fiber-Scanning Beam Technique” by W.H. Loh et al. (Optics Letters, Oct. 15, 1995, vol. 20 No. 20, pp. 2051-2053).