Patent Grant
6882789
The present invention relates generally to an optical transmission fiber that has improved dispersion characteristics across the low attenuation band of optical fibers, and specifically to an optical transmission fiber for use in a wavelength-division-multiplexing transmission system that has low attenuation and tailored dispersion characteristics across the bandwidth of 1450-1650 nm.
In optical communication systems, non-linear optical effects are known to degrade the quality of transmission along standard transmission optical fiber in certain circumstances. These non-linear effects, which include four-wave mixing, self-phase modulation, Brillouin scattering, Raman scattering, and cross-phase modulation, induce distortion into the transmitted signal in high-power systems, thereby degrading the quality of the transmission. In particular, the non-linear effects can hamper quality transmission using wavelength division multiplexing (WDM), which otherwise greatly enhances the signal carrying capability of optical transmission fibers by increasing the number of transmission channels through which signals may be sent.
These non-linear effects can be minimized or avoided by using single-mode transmission fibers that have a large effective area. In addition, the phenomenon of four-wave mixing can be minimized by fibers having an absolute value of dispersion that is greater than zero at or around the operating wavelengths. However, in advanced WDM systems, such as Dense Wavelength Division Multiplexing (DWDM) and Hyper-Dense Wavelength Division Multiplexing (HDWDM) systems, where the transmission channels are closely packed together (spacing≦0.4 nm), the value of dispersion must meet a minimum value to maintain the quality of the signals. On the other hand, if the dispersion value of the fiber becomes too large, the signals will become distorted during transmission unless dispersion correction devices are included in the transmission line. Thus, for an optical fiber to be effective in a WDM system, the fiber must have a minimum dispersion, but the value of dispersion must also be below a maximum value.
Optical fibers in general exhibit low attenuation across a wavelength range of about 1450-1650 nm. Indeed, the minimum spectral attenuation for standard optical fibers occurs at around 1580 nm, while intrinsic fiber attenuation remains typically below 0.27 dB/km for dispersion-shifted fibers up to around 1650 nm and even lower for dispersion unshifted fibers. However, conventional optical-fiber amplifiers doped with rare-earth materials such as erbium operate most effectively in a more limited wavelength window between around 1530-1565 nm. As a result, some research has focused on minimizing non-linear effects and attenuation for WDM systems across the wavelength range of 1530-1565 nm.
Due to recent technological advances in optical amplifiers, the transmission window of operating wavelengths for WDM systems is increasing from the traditional wavelength range of 1530-1565 nm to a much broader wavelength range of around 1450-1650 nm. Some publications have discussed working at lower wavelength regions down to 1470 nm. In this regard, Electronics Letters, vol. 34, no. 11, pp. 1118-1119 (May 28, 1998) discusses an eight-channel WDM system operating from 1467 nm to 1478 nm, based on Thulium-doped fiber amplifiers. Others have addressed extending the operating bandwidth toward higher wavelength regions up to about 1600 nm. See, e.g., Srivastava et al. '1 Tb/s Transmission of 100 WDM 10 Gb/s Channels Over 400 km of TrueWave™ Fiber' PD10, OFC'98. See also M. Jinno et al. 'First demonstration of 1580 nm wavelength band WDM transmission for doubling usable bandwidth and suppressing FWM in DSF' Electronics Letters, vol. 33 no. 10 pp. 882-883 (May 8, 1997). This extended range of available operating wavelengths is due to a use of gain-shifted erbium-doped amplifiers.
In addition, the trend of expanding the amplification window is supported by the low attenuation of transmission fibers over the expanded transmission window between 1450 and 1650 nm. However, existing fibers are severely limited in their transmission capabilities outside of the traditional transmission window around 1550 nm. For example, currently available Non-Zero Negative Dispersion (NZD−) fibers have a zero-dispersion wavelength λ0 at approximately 1585 nm and are therefore not suited for WDM transmissions because of non-linear effects at this operating wavelength. Similarly, Non-Zero Positive Dispersion (NZD+) and Large Effective Area (LEA) fibers have zero-dispersion wavelengths λ0 in the area of 1500 nm and are therefore not suited for WDM transmissions at this operating wavelength. Thus, because of the associated non-linear effects, conventional fibers are not capable of supporting the newly broadened transmission window. Moreover, for NZD+ and LEA fibers, even if the transmission wavelengths were restricted to the band above 1530 nm, the dispersion at around 1600 nm and at higher wavelengths would be high, due to the steep slope of the dispersion curve, thus requiring dispersion compensation. Accordingly, Applicant has identified a need for an optical transmission fiber that is capable of supporting WDM transmissions across the transmission window from 1450 nm to 1650 nm that provides suitable dispersion characteristics, low attenuation, and resistance to non-linear effects.
Various patents and publications have discussed optical fibers for high performance communication systems. For example, U.S. Pat. No. 5,553,185 to Antos et al., discloses a NZD fiber that is characterized by a series of core regions each having a refractive-index profile and radius. The shape of the refractive-index profiles, in terms of the refractive-index difference and the radius, of each region may be adjusted to have properties tailored for a high performance telecommunication system. In particular, one of the regions has a depressed refractive-index difference. The dispersion slope of the disclosed fiber is less than 0.05 ps/nm2/km and the absolute value of the total dispersion is between 0.5 and 3.5 ps/nm/km over a pre-selected transmission range.
Another fiber for a high performance communication system is discussed in Y. Ak. et al., Enlargement of Effective Core Area on Dispersion-Flattened Fiber and Its Low Non-Linearity, OFC '98 Technical Digest, pp. 302-304. This fiber is also characterized by a series of core regions having varying refractive-index differences and radii. One of the core regions also has a depressed refractive-index difference. The disclosed fiber has a low dispersion slope over the transmission window.
Lucent Technologies provided a press release in June 1998 introducing its TrueWave® RS Fiber that has a reduced slope of dispersion. According to the release, the new fiber has a dispersion slope across a wavelength band of about 1530-1620 nm with a low value, such that the dispersion ranges from about 3.5-7.5 ps/nm-km. The press release does not disclose the refractive index profile of the TrueWave® RS Fiber.
U.S. Pat. No. 4,852,968 discloses a single mode optical fiber whose refractive index profile comprises a depressed-index or trench region in the cladding region. By suitable adjustment of the position, width and index of the trench region, one or more fiber characteristics can be improved, relative to a similar fiber that does not comprise an index trench, such as: the slope of the chromatic dispersion curve at the zero dispersion wavelength; the spectral value over which the absolute value of the chromatic dispersion is less than a predetermined value; the maximum absolute value of the chromatic dispersion in a given spectral range; the bending loss at a given bend radius; the ratio ad/a1; the optical quality of the tube-derived material; the integrated mode power at ad; the dopant concentration in the core; and the dependence of λ0 on the core radius.
U.S. Pat. No. 5,781,684 discloses a single mode optical waveguide having large effective area, achieved by using a segmented core profile which includes at least a segment, or a part of one segment, having a refractive index less than the minimum refractive index of the clad layer. Dispersion slope values above 0.085 ps/nm2/km are disclosed.
U.S. Pat. No. 5,684,909 discloses a single mode optical waveguide having a core refractive index profile of at least four segments. The main features of the core design are: at least two non-adjacent core profile segments have positive Δ%; and at least two non-adjacent segments have negative Δ%. The waveguide structure lends itself to the manufacture of dispersion managed waveguide fibers.
Throughout the present description reference is made to refractive index profiles of optical fibers. The refractive index profiles comprise various radially arranged sections. Reference is made in the present description to precise geometrical shapes for these sections, such as step, alpha-profile, parabola. It is evident that the refractive index profiles achieved in practice may differ from the above, idealized, profiles. It has been shown in the literature, however, that these differences do not change the fiber characteristics if they are kept under control. See, for example, U.S. Pat. No. 4,406,518 (Hitachi).
In general, a refractive index profile has an associated effective refractive index profile which is different in shape. An effective refractive index profile may be substituted, for its associated refractive index profile without altering the waveguide performance. For example, see “Single Mode Fiber Optics”, Luc B. Jeunhomme, Marcel Dekker Inc., 1990, page 32, section 1.3.2.
It will be understood that disclosing and claiming a particular refractive index profile shape, includes the associated equivalents, in the disclosure and claims.
Applicant has discovered that transmission fibers that operate over an extended operating range with suitable dispersion values but have a region within the fiber core with exclusively a depressed refractive index are subject to several disadvantages. In particular, these fibers have a high attenuation, which is due, in part, to the region of depressed refractive index. In addition, the disclosed profiles that have an annular core region of exclusively a depressed refractive index between a central raised-index region and a raised-index ring often result in diffusion of dopants between layers during the manufacturing process, which degrades the quality of the refractive-index profile. In general, an optical transmission fiber consistent with the present invention involves a single-mode optical transmission fiber for use in a wavelength division multiplexing system that has carrier wavelengths ranging from 1450 nm to 1650 nm. The fiber has a glass core that includes an inner core having a first refractive-index difference, a first layer radially surrounding the inner core along the length of the fiber and having a second refractive-index difference of less than zero, a second layer radially surrounding the first layer along the length of the fiber and having a third refractive-index difference of substantially zero, a third layer radially surrounding the second layer along the length of the fiber and having a fourth refractive-index difference of greater than zero, and a fourth layer radially surrounding the third layer along the length of the fiber and having a fifth refractive-index difference of less than zero. A glass cladding surrounds the glass core and has a refractive-index difference substantially equal to zero. In addition, the slope of the dispersion curve is less than about 0.07 ps/nm2/km (and preferably less than about 0.05 ps/nm2/km) over the range of carrier wavelengths.
In another aspect, a fiber consistent with the present invention involves a single-mode optical transmission fiber for use in a wavelength division multiplexing system that has carrier wavelengths ranging from 1450 nm to 1650 nm. The fiber has a glass core that includes an inner core having a first refractive-index difference, a first layer radially surrounding the inner core along the length of the fiber and having a second refractive-index difference of less than zero, a second layer radially surrounding the first layer along the length of the fiber and having a third refractive-index difference of substantially zero, a third layer radially surrounding the second layer along the length of the fiber and having a fourth refractive-index difference of greater than zero. A glass cladding surrounds the glass core and has a refractive-index difference substantially equal to zero. In addition, the slope of the dispersion curve is less than about 0.07 ps/nm2/km (and preferably less than about 0.05 ps/nm2/km) over the range of carrier wavelengths.
In another aspect, a fiber consistent with the present invention involves a single-mode optical transmission fiber for use in a wavelength division multiplexing transmission system having carrier wavelengths ranging between about 1530 nm and 1650 nm. The fiber of this embodiment has a zero-dispersion wavelength of about 1480 nm.
In another aspect, the invention includes a single-mode optical transmission fiber that has a glass core having a central cross-sectional area with a first refractive-index peak, an outside ring with a second refractive-index peak, a first intermediate region between the two peaks having a low-dopant content, and a second intermediate region between the first peak and the first intermediate region, with a refractive-index depression lower than the first intermediate region. The fiber may also have a layer radially surrounding the second refractive-index peak and having a depressed refractive-index difference. The fiber also has a glass cladding surrounding the glass core, wherein the fiber has a dispersion value of at least 1.5 ps/nm/km and a dispersion slope of less than about 0.07 ps/nm2/km (and preferably less than about 0.05 ps/nm2/km) over a wavelength range of about 1450-1650 nm.
In a further aspect the invention includes a method for producing a single-mode optical fiber for use in a wavelength-division-multiplexing transmission system having carrier wavelengths ranging between about 1450-1650 nm, comprising the steps of: producing a preform having an inner core region with a first refractive-index difference; a first layer radially surrounding the inner core region along the length of the preform and having a second refractive-index difference of less than zero, a second layer radially surrounding the first layer along the length of the preform and having a third refractive-index difference that, in absolute value, is less than 40% of said second refractive-index difference, a third layer radially surrounding the second layer along the length of the preform and having a fourth refractive-index difference of greater than zero; and a glass cladding layer surrounding the core region and having a refractive-index difference substantially equal to zero; and drawing said preform.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory only, and are not restrictive of the invention as claimed.
The accompanying drawings, which are incorporated and constitute a part of this specification, illustrate several embodiments of the invention, and together with the description, serve to explain the principles of the invention.
Reference will now be made in detail to the present preferred embodiments of the invention, examples of which are illustrated in the accompanying drawings. Wherever possible, the same reference numbers will be used throughout the drawings to refer to the same or like parts.
Optical fibers consistent with the present invention have a refractive-index profile that includes an area of depressed refractive-index difference adjacent an area having a refractive-index difference of substantially zero. Applicant has discovered that optical transmission fibers having refractive-index profiles of this nature can produce optical transmission characteristics in an operating wavelength range of between about 1450 nm and 1650 nm that include a moderate dispersion value at the lowest operating wavelength, a low dispersion slope, and a low attenuation.
Applicant has further discovered that optical transmission fibers including this refractive-index profile can effectively support Wavelength Division Multiplexing (WDM) and Hyper-Dense WDM optical transmissions over the operating wavelength transmission window between 1450 nm and 1650 nm.
As shown in
The profile of
Applicant has found that optical transmission fibers having refractive-index profiles according to the present invention are better suited for use with WDM transmissions that range from about 1450 nm to 1650 nm than conventional fibers such as the fiber of FIG. 5. In particular, Applicant has discovered that by including in the cross-sectional outer part of the annular depression, a second glass layer having a refractive-index difference of substantially less, in absolute value, than the depressed refractive index difference, the depressed profile volume of the fiber according to Equation (1) above is reduced when compared to prior art fibers, while a desirably low dispersion slope can be achieved across the transmission window. The lower depressed profile volume results in lower amount of negative dopant and thus ease of manufacture of the fiber and lower attenuation. In addition, the fibers have a moderate value of dispersion at the lower end of the transmission window.
An optical fiber according to a preferred embodiment of the present invention is schematically illustrated in FIG. 1 and is generally designated by the reference number 10. In accordance with the present invention, an optical transmission fiber for use in a WDM transmission system includes a glass core with an inner core having a first refractive-index difference Δn1, a first layer radially surrounding the inner core along the length of the fiber and having a second refractive-index difference Δn2 of less than zero, a second layer radially surrounding the first layer along the length of the fiber and having a third refractive-index difference Δn3 of substantially zero, a third layer radially surrounding the second layer along the length of the fiber and having a fourth refractive-index difference Δn4 of greater than zero. A glass cladding surrounds the glass core and has a refractive-index difference substantially equal to zero. Preferably the core comprises a fourth layer radially surrounding the third layer along the length of the fiber and having a fifth refractive-index difference Δn5 of less than zero.
The fiber has a dispersion value of at least 1.5 ps/nm/km over the carrier wavelength range (preferably over 2.5 ps/nm/km for dense WDM transmission) and a dispersion slope less than about 0.07 ps/nm2/km (preferably less than about 0.05 ps/nm2/km) over the carrier wavelength range.
As schematically illustrated in
A first glass layer 14 radially surrounds inner core 12 along the length of fiber 10. First glass layer 14 extends from the outer radius r1 of the inner core to a radius r2 and has a depressed index of refraction Δn2 across its width. As is well known in the art, a depressed index of refraction exists when the index of refraction of a given glass layer is less than the refractive index of the cladding layer, i.e. Δn2, as given by the above equation, is less than 0. As also known in the art, the dispersion slope of a fiber may, in general, be reduced by including a layer of glass having an area of depressed refractive index. Δn2 can be chosen in the range −0.006-0.001, while a preferred range for Δn2 is −0.003 to −0.002. Preferably, first glass layer 14 is made of SiO2 doped with a substance that decreases the refractive index of pure SiO2, such as fluorine. The width of first glass layer 14 can be chosen in the range 1-6 μm, a preferred range being 2-4 μm.
A second glass layer 16 radially surrounds first glass layer 14 along the length of fiber 10. Second glass layer 16 extends from the outer radius r2 of the first glass layer to a radius r3 and has an index of refraction Δn3 within its width. The index of refraction Δn3 of second glass layer 16 is, in absolute value, less than about 40% of Δn2, preferably less than about 20% of Δn2. Preferably, second glass layer is made of SiO2, although the second glass layer may be made of any material or combination of materials having a refractive-index difference substantially equal to the refractive index of the cladding layer, described below. The width of second glass layer 16 can be chosen in the range 1-5 μm, a preferred range being 2-4 μm.
A third glass layer 18 radially surrounds second glass layer 16 along the length of fiber 10. Third glass layer extends from the outer radius r3 of second glass layer 16 to an outer radius r4. The third glass layer has a maximum refractive index Δn4. Δn4 can be chosen in the range 0.003-0.010, while a preferred range for Δn4 is 0.004-0.008. The width of third glass layer 18 can be chosen in the range 1-4 μm, a preferred range being 2-3 μm
A fourth glass layer 15 radially surrounds third glass layer 18 along the length of fiber 10. Fourth glass layer extends from the outer radius r4 of third glass layer 18 to an outer radius r5. The fourth glass layer has a refractive index difference Δn5 that is less than zero. Δn5 can be chosen in the range −0.003 to 0.0, while a preferred range for Δn5 is −0.002 to 0.0. The width of fourth glass layer 15 can be chosen in the range 1-6 μm, a preferred range being 3-5 μm.
Finally, a light conducting cladding 19 surrounds the third glass layer 18 in a conventional manner to help guide light propagating along the axis of fiber 10. Cladding 19 may comprise pure SiO2 glass with a refractive-index difference substantially equal to zero or include a refractive-index modifying dopant.
In an alternative embodiment, showed by dashed line, a fifth glass layer 17 having a refractive index difference Δn6 that is substantially zero is comprised between third glass layer 18 and fourth glass layer 15.
A particular embodiment, as shown in
As also shown in 40, the dispersion at 1450 nm of a fiber 10 according to a first embodiment is about 1.5 ps/nm/km. The slope of the dispersion curve is less than 0.06 ps/nm2/km across the bandwidth of 1450 nm to 1650 nm. Fiber 10 has a dispersion value less than about 12 ps/nm/km at 1650 nm. Curve 42 depicts a second embodiment of the present invention where the zero-dispersion wavelength occurs at around 1480 nm. A fiber 10 according to this second embodiment has a dispersion value of less than about 9 ps/nm/km at 1650 nm.
In addition, the effective area of fiber 10 at 1550 nm is greater than about 50 μm2. As is readily known in the art, a large effective area will help limit the impact of non-linear effects. However, the dispersion slope of the fiber increases as the effective area of the fiber increases. The fiber of the present invention has an effective area that is large enough to limit the impact of non-linear effects while being small enough to achieve an optimal trade off between effective area and dispersion slope.
The transmission characteristics of a first embodiment of a fiber 10 having a refractive-index profile according to the present invention are provided in Table 1.
As shown in
First glass layer 74 has a depressed refractive-index difference Δn2 of about −0.0010 and extends for a radial distance of about 2.8 μm. Depressed profile volume is about −0.013 μm2. The refractive-index difference of first glass layer 74 may be decreased by doping the width of the first core layer with fluorine or any other well-known refractive-index-decreasing dopant. Second glass layer 76 has a refractive-index difference Δn3 of about 0 and extends for a radial distance of about 2.0 μm.
Third glass layer 78 has a substantially parabolic profile and reaches a maximum refractive index Δn4 of about 0.0032 at a midpoint within its width of about 2.9 μm. The refractive-index difference of the third glass layer may be formed by doping the glass layer with increasing amounts of GeO2, or other well-known refractive-index-increasing dopant.
Third glass layer 78 is surrounded by cladding 80 that has a refractive-index difference of about 0.
The specific embodiment of fiber 10 illustrated in
Cable cut off≦1400 nm
Dispersion at 1450 nm=1.9 ps/nm/km
Dispersion Slope at 1450 nm=0.050 ps/nm2/km
Dispersion at 1550 nm=6.5 ps/nm/km
Dispersion Slope at 1550 nm=0.046 ps/nm2/km
Mode Field Diameter at 1550 nm=9.1 μm
Effective Area at 1550 nm=63 μm2
Non Linearity Coefficient γ=1.4 W−1 km−1
Macrobending attenuation<0.5 dB for 100 turns on a 60 mm diameter mandrel
Microbending sensitivity=2.9 (dB/km)/(g/mm) as determined by the expandable bobbin method, as described for example in G. Grasso and F. Meli “Microbending losses of cabled single-mode fibers”, ECOC '88, page 526-ff., or in G. Grasso et al. “Microbending effects in single-mode optical cables”, International Wire and Cable Symposium, 1988, page 722-ff.
In another embodiment and as shown in
First glass layer 74 has a depressed refractive-index difference Δn2 of about −0.0015 and extends for a radial distance of about 3.4 μm. Depressed profile volume is about −0.025 μm2. The refractive-index difference of first glass layer 74 may be decreased by doping the width of the first core layer with fluorine or any other well-known refractive-index-decreasing dopant. Second glass layer 76 has a refractive-index difference Δn3 of about 0 and extends for a radial distance of about 2.2 μm.
Third glass layer 78 has a substantially parabolic profile and reaches a maximum refractive index Δn4 of about 0.0090 at a midpoint within its width of about 1.1 μm. The refractive-index difference of the third glass layer may be formed by doping the glass layer with increasing amounts of GeO2, or any other well-known refractive-index-increasing dopant.
As can be seen, this embodiment of
The specific embodiment of fiber 10 illustrated in
Cable cut off≦1400 nm
Dispersion at 1450 nm=1.6 ps/nm/km
Dispersion Slope at 1450 nm=0.042 ps/nm2/km
Dispersion at 1550 nm=5.0 ps/nm/km
Dispersion Slope at 1550 nm=0.036 ps/nm2/km
Mode Field Diameter at 1550 nm=8.6 μm
Effective Area at 1550 nm=57 μm2
Non Linearity Coefficient γ=1.6 W−1 km−1
Macrobending attenuation<0.5 dB for 100 turns on a 60 mm diameter mandrel Microbending sensitivity=2.1 (dB/km)/(g/mm) as determined by the expandable bobbin method.
In another preferred embodiment and as shown in
First glass layer 74 has a depressed refractive-index difference Δn2 of about −0.0014 and extends for a radial distance of about 3.1 μm. Depressed profile volume is about −0.021 μm2. The refractive-index difference of first glass layer 74 may be decreased by doping the width of the first core layer with fluorine or any other well-known refractive-index-decreasing dopant. Second glass layer 76 has a refractive-index difference Δn3 of about 0 and extends for a radial distance of about 3.0 μm.
Third glass layer 78 has a substantially parabolic profile and reaches a maximum refractive index Δn4 of about 0.0040 at a midpoint within its width of about 3.2 μm. The refractive-index difference of the third glass layer may be formed by doping the glass layer with increasing amounts of GeO2, or any other well-known refractive-index-increasing dopant.
Third glass layer 78 is surrounded by a fourth glass layer 79 that has a refractive-index difference of about −0.0011 along its width of 4.0 μm.
Fourth glass layer 79 is surrounded by cladding 80 that has a refractive-index difference of about 0.
The specific embodiment of fiber 10 illustrated in
Cable cut off≦1400 nm
Dispersion at 1450 nm=1.6 ps/nm/km
Dispersion Slope at 1450 nm=0.038 ps/nm2/km
Dispersion at 1550 nm=5.1 ps/nm/km
Dispersion Slope at 1550 nm=0.034 ps/nm2/km
Mode Field Diameter at 1550 nm=8.6 μm
Effective Area at 1550 nm=56 μm2
Non Linearity Coefficient γ=1.6 W−1 km−1
Macrobending attenuation<0.5 dB for 100 turns on a 60 mm diameter mandrel
Microbending sensitivity=2.0 (dB/km)/(g/mm) as determined by the expandable bobbin method.
In accordance with the present invention, the optical transmission fiber having a refractive-index profile as described herein may be used with a WDM transmission system that operates at larger wavelengths. In particular, a second embodiment of the invention fiber may be used with WDM transmission systems that have carrier wavelengths in the range of about 1530 nm to 1650 nm.
As shown in
First glass layer 74 has a depressed refractive-index difference Δn2 of about −0.0013 and extends for a radial distance of about 3.3 μm. Depressed profile volume is about −0.021 μm2. The refractive-index difference of first glass layer 74 may be decreased by doping the width of the first core layer with fluorine or any other well-known refractive-index-decreasing dopant. Second glass layer 76 has a refractive-index difference Δn3 of about 0 and extends for a radial distance of about 2.4 μm.
Third glass layer 78 has a substantially parabolic profile and reaches a maximum refractive index Δn4 of about 0.0058 at a midpoint within its width of about 2.1 μm. The refractive-index difference of the third glass layer may be formed by doping the glass layer with increasing amounts of GeO2, or any other well-known refractive-index-increasing dopant.
Third glass layer 78 is surrounded by a fourth glass layer 79 that has a refractive-index difference of about −0.0008 along the width of 4.3 μm.
Fourth glass layer 79 is surrounded by cladding 80 that has a refractive-index difference of about 0.
The specific embodiment of fiber 10 illustrated in
Cable cut off≦1500 nm
Dispersion at 1550 nm=3.3 ps/nm/km
Dispersion Slope at 1550 nm=0.038 ps/nm2/km
Mode Field Diameter at 1550 nm=8.7 μm
Effective Area at 1550 nm=59 μm2
Non Linearity Coefficient γ=1.5 W−1 km−1
Macrobending attenuation <0.5 dB for 100 turns on a 60 mm diameter mandrel
Microbending sensitivity=3.0 (dB/km)/(g/mm) as determined by the expandable bobbin method.
First glass layer 74 has a substantially parabolic depressed profile and reaches a minimum refractive-index difference Δn2 of about −0.0024 at a midpoint within its width of about 2.4 μm. The refractive-index difference of first glass layer 74 may be decreased by doping the width of the first core layer with fluorine or any other well-known refractive-index-decreasing dopant. Second glass layer 76 has a refractive-index difference Δn3 of about 0 and extends for a radial distance of about 2.6 μm.
Third glass layer 78 has a substantially parabolic profile and reaches a maximum refractive index Δn4 of about 0.0063 at a midpoint within its width of about 2.1 μm. The refractive-index difference of the third glass layer may be formed by doping the glass layer with increasing amounts of GeO2, or any other well-known refractive-index-increasing dopant.
Third glass layer 78 is surrounded by a depressed fourth glass layer 79 that has a minimum refractive-index difference of about −0.001 across its width of 2.9 μm.
Fourth glass layer 79 is surrounded by cladding 80 that has a refractive-index difference of about 0.
The specific embodiment of fiber 10 illustrated in
Cable cut off≦1500 nm
Dispersion at 1550 nm=3.5 ps/nm/km
Dispersion Slope at 1550 nm=0.043 ps/nm2/km
Mode Field Diameter at 1550 nm=8.9 μm
Effective Area at 1550 nm=61 μm2
Non Linearity Coefficient γ=1.4 W−1 km−1
Macrobending attenuation<0.5 dB for 100 turns on a 60 mm diameter mandrel
Microbending sensitivity=3.9 (dB/km)/(g/mm) as determined by the expandable bobbin method.
Each cross in
Theoretical cut-off <1800 nm
Dispersion at 1550 nm 2-8 ps/nm/km
Effective area 53-57 μm2
Macrobending attenuation<0.5 dB for 100 turns on 60 mm diameter mandrel
Microbending sensitivity<5 (dB/km)/(g/mm) by the expandable bobbin test method,
while parameter sets giving refractive-index profiles having optical transmission characteristics outside the above ranges have not been represented on FIG. 12.
A comparative example for a set of invention refractive-index profiles according to
On both graphs a line 90 has been drawn corresponding to the relationship
S=0.07+V (2)
between the dispersion slope S (in units of ps/nm2/km) and the depressed profile volume V (in units of μm2).
As it is shown by above exemplary embodiments, there is a trade off between low dispersion slope and depressed profile volume. For corresponding fiber performances, the lower the dispersion slope, the higher the depressed profile volume, thus increasing manufacturing complexity and dopant content.
The above graphs in
A refractive index profile of a fiber preform made by Applicant with the MCVD technique is shown in FIG. 14. The preform comprises inner core region 72, first glass layer 74, second glass layer 76, third glass layer 78, depressed fourth glass layer 79 and cladding 80.
The preform layers correspond to those of the invention fiber according to the embodiment described with reference to FIG. 3.
During the drawing process, in particular due to dopant diffusion, the refractive-index profile for the drawn fiber may in general undergo some changes from the preform refractive-index profile. In particular, second glass layer 76 is doped so as to achieve a refractive index difference value that is more negative than the desired refractive index value of the drawn fiber, to account for a corresponding small increase in the refractive index of this layer during the drawing process. The amount of this increase can be determined by the skilled in the art, based on the preform characteristics and on the fiber drawing process parameters.
Applicant has determined that a preform having a refractive-index profile corresponding to that described in general with reference to
Although the MCVD technique has been used to produce the preform shown in
It will be apparent to one skilled in the art that various modifications and variations may be made to the fiber of the present invention without departing from the scope of the invention. For example, the refractive-index profiles depicted in the figures are intended to be exemplary of preferred embodiments. The precise shape, radial distance, and refractive-index differences may readily be fluctuated by one of ordinary skill in the art to obtain equivalent fibers to those disclosed herein without departing from the scope of this invention. The present invention covers the modifications and variations of this invention provided they come within the scope of the appended claims and their equivalents.
| Number | Date | Country | Kind |
|---|---|---|---|
| 98117828 | Sep 1998 | EP | regional |
This is a continuation of application Ser. No. 09/812,019, filed Mar. 20, 2001, now U.S. Pat. No. 6,751,389 which is a continuation application of PCT/EP99/06958, filed on Sep. 21, 1999, which claimed priority of European Patent Application No. 98117828.8, filed on Sep. 21, 1998 and the benefit of U.S. provisional application No. 60/104,636, filed Oct. 16, 1998, all of which are incorporated herein by reference.
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| WO 8604689 | Aug 1986 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20050002627 A1 | Jan 2005 | US |
| Number | Date | Country | |
|---|---|---|---|
| 60104636 | Oct 1998 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 09812019 | Mar 2001 | US |
| Child | 10825101 | US | |
| Parent | PCTEP99/06958 | Sep 1999 | US |
| Child | 09812019 | US |
