This application claims priority to an application entitled “Dispersion-controlled optical fiber” filed with the Korean Intellectual Property Office on Apr. 3, 2002 and assigned Serial No. 2002-18162, the contents of which are hereby incorporated by reference.
1. Field of the Invention
The present invention relates to an optical fiber and, more particularly, to a broad band dispersion-controlled optical fiber.
2. Description of the Related Art
As one skilled in the art can readily appreciate, an optical fiber consists of a core and a cladding, wherein the refractive index of the core is higher than that of the cladding. Common known methods for manufacturing the base material of an optical fiber includes the Modified-Chemical-Vapor Deposition (MCVD) method, Vapor-phase Axial Deposition (VAD) method, Outside Vapor-phase Deposition(OVD) method, Plasma-Chemical-Vapor Deposition(PCVD) method and the like.
For achieving ultra-high speed and high capacity communication, dispersion-controlled optical fibers (for example, dispersion-shifted fiber (DSF), non-zero DSF (NZDSF), dispersion-compensated fiber (DSF)) have been deployed which are superior to the existing single-mode optical fiber in terms of transmission capability. As such, the demand for the dispersion-controlled fibers has been increasing. If a region with a depressed refractive index is interposed between the core and cladding to form an optical fiber, it is possible to effectively control the dispersion characteristics of the optical fiber. An example of such an optical fiber is disclosed in U.S. Pat. No. 4,715,679 to Venkata A. Bhagavatula, entitled “Low Dispersion, Low-loss Single-mode Optical Waveguide.”
However, the dispersion-controlled optical fiber of this type has drawbacks in that its bending loss tends to be high as it has a region with a highly depressed refractive index in its cladding. In addition, a non-linear effect occurs due to its small effective cross-sectional area as it has a small mode-field diameter (MFD) when compared to common single-mode optical fibers. Furthermore, it is inappropriate for broad-band transmission, and the loss and dispersion characteristics are poor in higher and lower wavelength ranges.
A dispersion-controlled optical fiber has a very small core diameter and high refractive index when compared to a single-mode optical fiber. As such, if the dimension of its base material forms a large aperture, a problem will arise as relatively large stresses are applied to the core part at the time of drawing it. Namely, the distribution of wavelengths will be changed. This means that it is difficult for various optical characteristics to have constant values in accordance with drawing temperatures. Also, it is not easy to manufacture a dispersion-controlled optical fiber if it has relatively sensitive characteristics when compared to a common single-mode optical fiber.
In addition, the existing dispersion-controlled optical fibers are adapted to be used in the wavelength range of about 1530˜1565 nm by setting the zero dispersion wavelength around 1530 nm, wherein the optical fibers have a dispersion characteristic of not more than 5 ps/nm·km at 1550 nm and their diameters range between 8˜9 μm, thus being problematic in that they are inappropriate for communication exceeding the 10 Gbps level.
As explained above, dispersion-controlled optical fibers in the prior art have the following problems:
Accordingly, the present invention has been made to solve the above-mentioned problems occurring in the prior art and provides a dispersion-controlled optical fiber, in which a desired dispersion characteristic and a dispersion slope characteristic can be obtained, and further has a low-loss characteristic.
Another aspect of the present invention is to provide a dispersion-controlled optical fiber, in which a large effective cross-sectional area can be obtained to reduce a non-linear effect with a large mode-field diameter through a large core diameter.
Another aspect of the present invention is to provide a dispersion-controlled optical fiber, which can secure a broad range of usable wavelengths (1400˜1625 nm) by positioning a zero-dispersion wavelength range on or below 1400 nm, and which can have a dispersion characteristic in the range of about 5˜13 ps/nm·km at 1550 nm, thus reducing the non-linear effect.
Accordingly, there is provided an optical fiber comprising a center core which forms a passageway for transmitting optical signals and has a refractive index N1, and a cladding that encloses the center core and has a refractive index N0, wherein the optical fiber further comprises an upper core that has a distribution of refractive indices, which increase starting from a refractive index N2 (>N0) at its outer circumference to the refractive index N1 at its internal circumference, and a minutely-depressed, refractive-index region, which is interposed between the upper core and the cladding and has a refractive index N3, wherein the refractive index N3 is lower than the refractive index N0.
The above and other features and advantages of the present invention will be more apparent from the following detailed description taken in conjunction with the accompanying drawings, in which:
Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings. For the purposes of clarity and simplicity, a detailed description of known functions and configurations incorporated herein will be omitted as it may make the subject matter of the present invention unclear.
The center core 110 consists of silica and has a radius, a. In the embodiment, the center core 110 is doped with a predetermined amount of germanium for tuning its refractive index to N1.
The upper core 120 has an internal radius of a and an external radius of b, and a refractive index of N1 at its internal circumference and a refractive index of N2 at its external circumference. As shown in
The minutely-depressed, refractive-index region 130 is formed from a silica material with an internal radius of b and an external radius of c. Furthermore, the minutely depressed refractive index region 130 is doped with germanium, phosphorus, and fluorine in a predetermined ratio for tuning its refractive index to N3.
The cladding 140 is formed of silica and has an internal radius of a and an external radius of b, and further has a refractive index of N0, which is higher than N3 and lower than N2.
As constructed above, the zero-dispersion characteristic exists in the dispersion-controlled optical fiber 100 at the region of wavelengths below 1400 nm, and the dispersion-controlled optical fiber 100 has a predetermined range of dispersion values (0.1˜4 ps/nm·km at 1400 nm, 5˜13 ps/nm·km at 1550 nm, and 8˜16 ps/nm·km at 1625 nm) and a large MFD or effective cross-sectional area (8.5˜10.0 μm at 1550 nm), thereby reducing the non-linear effect. For this purpose, the dispersion-controlled optical fiber 100 conforms to the relationships of 0.06≦a/c≦0.9, 0.06≦a/b≦0.8, 0.02≦a/c≦0.9, 1.2≦N1/N2≦2.67 and −8≦N1/N3≦1.6. In this case, the refractive index of referenced glass exhibits 1.45709 when measured with a He—Ne laser at 632.8 nm.
The upper core 120, which has the predetermined refractive index slope, permits a large mode field diameter and can be tuned to have the desired dispersion value and dispersion-slope characteristics, together with the minutely-depressed, refractive-index region 130. As the minutely-depressed, refractive-index region 130 has a refractive index that is minutely different from that of the cladding 140, a minute bending may be induced which is small when compared to the prior art, thereby reducing the bending loss.
In the optical characteristics, if the dispersion is too high, the transmission length of the optical fiber will be restricted and the transmission characteristics will be deteriorated by a self-phase modulation due to phase shifting caused by the non-linear effect. In addition, the dispersion value at a wavelength near zero-dispersion and the small dispersion-value characteristic readily cause phase matching, whereby the transmission characteristic will be deteriorated by four-wave mixing process in the case of multiple-channel transmission, which is typically employed to extend the transmission capacity. Accordingly, it is necessary to have a proper dispersion value to allow a super-high speed and broad-band transmission and to have a large mode-field diameter in order to reduce the non-linear effect.
As such, the dispersion-controlled optical fiber in accordance with the present invention can obtain a dispersion value and dispersion slope suitable for super-high speed and broad-band transmission through the tuning of the minutely-depressed, refractive-index region and upper core.
Furthermore, the dispersion-controlled optical fiber in accordance with the present invention has a loss not exceeding 0.25 dB/km, a cutoff wavelength not exceeding 1400 nm, and a dispersion slope not exceeding 0.08 ps/nm2·km, at the wavelength of 1550 nm, has a dispersion value not less than 0.1 ps/nm·km at the wavelength of 1400 nm and a dispersion value not exceeding 16 ps/nm·km at the wavelength of 1625 nm, and further has a mode-field diameter not less than 8.2 μm at the wavelength of 1550 nm, thus it has suitable optical characteristics for wavelength-division multiplexing transmission using a wavelength band of 1400˜1625 nm.
In summary, as explained above, the dispersion-controlled optical fiber has the following advantages:
a) it has a large effective cross-sectional area, whereby it can reduce the non-linear effect;
b) it can easily provide a dispersion value and a dispersion slope that are suitable for super-high speed and broad band-transmission through the tuning of the minutely depressed refractive index region and upper core; and,
c) due to the fine difference in refractive indices between the minutely depressed refractive index region and upper core, the bending loss can be reduced.
While the invention has been shown and described with reference to certain preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims.
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2002-18162 | Apr 2002 | KR | national |
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Number | Date | Country | |
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20030190128 A1 | Oct 2003 | US |