The present disclosure generally relates to an optical fiber cable and in particular to an optical fiber cable having a high density of optical fiber cores and containing multicore optical fibers. Multicore optical fibers provide enhanced signal carrying capacity with a single transmission fiber or cable. Multicore optical fibers provide increased fiber density to overcome cable size limitations and duct congestion and are particularly useful for data center applications as well as high speed optical interconnects where there is a desire to increase the fiber density to achieve compact high fiber count connections. It may be desirable to provide for a multicore optical fiber having multiple core regions fit within a desired diameter size that provides low signal cross-talk, low tunneling loss and good bending performance.
In one aspect, embodiments of the present disclosure relate to an optical fiber cable. In one or more embodiments, the optical fiber cable includes a cable jacket having an inner surface and an outer surface. In embodiments, the inner surface defines a central cable bore, and the outer surface defines an outermost surface of the optical fiber cable. In one or more embodiments, the optical fiber cable also includes a cable core disposed in the central cable bore. In embodiments, the cable core includes a plurality of multicore optical fibers and a cross-sectional area. In exemplary embodiments, the plurality of multicore optical fibers fill at least 50% of the cross-sectional area of the cable core. Further, in embodiments, each multicore optical fiber of the plurality of multicore optical fibers has an inner glass region having a plurality of core regions surrounded by a common outer cladding. In one or more embodiments of the optical fiber cable, the cable core has a core region density that is at least 40 core regions/mm2
In another aspect, embodiments of the present disclosure relate to an optical fiber cable. In one or more embodiments, the optical fiber cable includes a cable jacket with an inner surface and an outer surface. In such embodiments, the inner surface may define a central cable bore, and the outer surface may define an outermost surface of the optical fiber cable. In one or more embodiments, the optical fiber cable also includes a buffer tube having an interior surface and an exterior surface. In such embodiments, the interior surface may define a cross-sectional area. In one or more embodiments, the optical fiber cable includes a plurality of multicore optical fibers that fill 50% to 90% of the cross-sectional area. In such embodiments, the multicore optical fiber of the plurality of multicore optical fibers may include from three to eight core regions surrounded by a common outer cladding. Further, in such embodiments, each multicore optical fiber of the plurality of multicore optical fibers may have a fiber diameter of 170 μm to 200 μm.
Additional features and advantages will be set forth in the detailed description which follows, and in part will be readily apparent to those skilled in the art from that description or recognized by practicing the embodiments as described herein, including the detailed description which follows, the claims, as well as the appended drawings.
It is to be understood that both the foregoing general description and the following detailed description are merely exemplary, and are intended to provide an overview or framework to understanding the nature and character of the claims. The accompanying drawings are included to provide a further understanding, and are incorporated in and constitute a part of this specification. The drawings illustrate one or more embodiments, and together with the description serve to explain principles and operation of the various embodiments.
Reference will now be made in detail to the present preferred embodiments, examples of which are illustrated in the accompanying drawings. Whenever possible, the same reference numerals will be used throughout the drawings to refer to the same or like parts.
The following detailed description represents embodiments that are intended to provide an overview or framework for understanding the nature and character of the claims. The accompanied drawings are included to provide a further understanding of the claims and constitute a part of the specification. The drawings illustrate various embodiments, and together with the descriptions serve to explain the principles and operations of these embodiments as claimed.
“Refractive index” refers to the refractive index at a wavelength of 1550 nm.
The “refractive index profile” is the relationship between refractive index or relative refractive index and waveguide fiber radius. The radius for each region of the refractive index profile is given by the abbreviations r1, r2, r3, r4, etc. and lower and upper case are used interchangeably herein (e.g., r1 is equivalent to R1).
The “relative refractive index percent” is defined as Δ%=100×(ni2−nc2)/2ni2, and as used herein ni is the refractive index of region i of the optical fiber and nc is the refractive index of undoped silica. As used herein, the relative refractive index is represented by Δ and its values are given in units of “%”, unless otherwise specified. The terms: delta, Δ, Δ%, % Δ, delta %, % delta, and percent delta may be used interchangeably herein. In cases where the refractive index of a region is less than the average refractive index of undoped silica, the relative index percent is negative and is referred to as having a depressed region or depressed index. In cases where the refractive index of a region is greater than the average refractive index of the cladding region, the relative index percent is positive.
An “updopant” is herein considered to be a dopant which has a propensity to raise the refractive index relative to pure undoped SiO2. Examples of updopants include GeO2 (germania), Al2O3, P2O5, TiO2, Cl, Br.
A “downdopant” is herein considered to be a dopant which has a propensity to lower the refractive index relative to pure undoped SiO2. Examples of down dopants include fluorine and boron.
“Chromatic dispersion”, herein referred to as “dispersion” unless otherwise noted, of a waveguide fiber is the sum of the material dispersion, the waveguide dispersion, and the inter-modal dispersion. In the case of single mode waveguide fibers, the inter-modal dispersion is zero. Zero dispersion wavelength is a wavelength at which the dispersion has a value of zero. Dispersion slope is the rate of change of dispersion with respect to wavelength.
“Effective area” is defined as:
where f(r) is the transverse component of the electric field associated with light propagated in the waveguide. As used herein, “effective area” or “Aeff” refers to optical effective area at a wavelength of 1550 nm unless otherwise noted.
The trench volume V3 is defined for a depressed index region
where rTrench,inner is the inner radius of the trench cladding region, rTrench,outer is the outer radius of the trench cladding region, ΔTrench(r) is the relative refractive index of the trench cladding region, and Δc is the average relative refractive index of the common outer cladding region of the glass fiber. In embodiments in which a trench is directly adjacent to the core, rTrench,outer is r2=r1 (outer radius of the core), rTrench,outer is r3, and ΔTrench is Δ3(r). In embodiments in which a trench is directly adjacent to an inner cladding region, rTrench,inner is r2>r1, rTrench,outer is r3, and ΔTrench is Δ3(r). Trench volume is defined as an absolute value and has a positive value. Trench volume is expressed herein in units of %Δ-micron2, %Δ-μm2, or %-micron2, %-μm2, whereby these units can be used interchangeably.
The term “α-profile” refers to a relative refractive index profile, expressed in terms of Δ(r) which is in units of “%”, where r is radius, which follows the equation,
where ro is the point at which Δ(r) is maximum, r1 is the point at which Δ(r) % is zero, and r is in the range ri≤r≤rf, where Δ is defined above, r1 is the initial point of the α-profile, rf is the final point of the α-profile, and α is an exponent which is a real number.
The mode field diameter (MFD) is measured using the Peterman II method wherein,
Mode field diameter depends on the wavelength of the optical signal in the optical fiber. Specific indication of the wavelength will be made when referring to mode field diameter herein. Unless otherwise specified, mode field diameter refers to the LP01 mode at the specified wavelength.
The theoretical fiber cutoff wavelength, or “theoretical fiber cutoff,” or “theoretical cutoff,” for a given mode, is the wavelength above which guided light cannot propagate in that mode. A mathematical definition can be found in Single Mode Fiber Optics, Jeunhomme, pp. 39-44, Marcel Dekker, New York, 1990 wherein the theoretical fiber cutoff is described as the wavelength at which the mode propagation constant becomes equal to the plane wave propagation constant in the outer cladding. This theoretical wavelength is appropriate for an infinitely long, perfectly straight fiber that has no diameter variations.
Fiber cutoff is measured by the standard 2 m (2 meter) fiber cutoff test, FOTP-80 (EIA-TIA-455-80), to yield the “fiber cutoff wavelength,” also known as the “2 m fiber cutoff” or “measured cutoff.” The FOTP-80 standard test is performed to either strip out the higher order modes using a controlled amount of bending, or to normalize the spectral response of the fiber to that of a multimode fiber.
By cabled cutoff wavelength, or “cabled cutoff” as used herein, it is meant the 22 m (22 meter) cabled cutoff test described in the EIA-445 Fiber Optic Test Procedures, which are part of the EIA-TIA Fiber Optics Standards, that is, the Electronics Industry Alliance-Telecommunications Industry Association Fiber Optics Standards.
Unless otherwise noted herein, optical properties (such as dispersion, dispersion slope, etc.) are reported for the LP01 mode.
Referring to
Each core region 14 includes a core, an inner cladding surrounding the core and a trench. This allows the trench to be offset from the core and allows for a large trench volume. In some embodiments, the inner cladding may be omitted such that the trench is adjacent to the core. The common outer cladding 16 is shown having a generally circular end shape or cross-sectional shape in the embodiments illustrated. The plurality of core regions 14 each extend in a cylindrical shape through the length of the multicore optical fiber 10 and are illustrated spaced apart from one another and are surrounded and separated by the common outer cladding 16. The multicore optical fiber 10 contains at least two core regions 14, preferably at least three core regions 14, and more particularly at least four core regions 14, and therefore has a plurality of core regions 14. It should be appreciated that two or more core regions 14 may be included in the multicore optical fiber 10 in various numbers of core regions and various fiber arrangements.
The multicore optical fiber 10 employs a plurality of glass core regions 14 spaced from one another and surrounded by the common outer cladding 16. The core regions 14 and common outer cladding 16 may be made of glass or other optical fiber material and may be doped suitable for optical fiber. In one embodiment, each core region 14 is comprised of germania-doped silica core, an inner cladding and a fluorine-doped silica trench. In one embodiment, the shape of the multicore optical fiber 10 may be a circular end shape or circular cross-sectional shape as shown in
The multicore optical fiber 10 illustrated in
In the embodiments shown in
The multicore optical fiber 10 includes an outer coating layer 20 which surrounds and encapsulates the inner glass region 12. The outer coating layer 20 is shown in
The coating layer 20 has a ratio of the thickness of the secondary coating layer 24 to the thickness of the primary coating layer in the range of 0.65 to 1.0, according to one embodiment. According to other embodiments, the ratio of the secondary coating layer thickness to the primary coating layer thickness may be in the range of 0.70 to 0.95, more particularly in the range of 0.75 to 0.90, and more particularly in the range of 0.75 to 0.85. The ratio of the secondary coating layer thickness to the primary coating layer thickness within the range of 0.65 to 1.0 and the reduced thickness coating layer 20 advantageously aids in a desirable goal in reducing signal cross-talk between core regions 14 in the multicore optical fiber 10 and leakage of signal from the fiber cores to the outside of the multicore optical fiber 10.
The primary coating layer 22 may be made of a known primary coating composition. For example, the primary coating composition may have a formulation listed below in Table 1 which is typical of commercially available primary coating composition.
where the oligomeric material may be prepared from H12MDI, HEA, and PPG4000 using a molar ratio n:m:p=3.5:3.0:2.0, H12MDI is 4,4′-methylenebis(cyclohexyl isocyanate) (available from Millipore Sigma), HEA is 2-hydroxyethylacrylate (available from Millipore Sigma), PPG4000 is polypropylene glycol with a number average molecular weight of about 4000 g/mol (available from Covestro), SR504 is ethoxylated(4)nonylphenol acrylate (available from Sartomer), NVC is N-vinylcaprolactam (available from Aldrich), TPO (a photoinitiator) is (2,4,6-trimethylbenzoyl)-diphenyl phosphine oxide (available from BASF), Irganox 1035 (an antioxidant) is benzenepropanoic acid, 3,5-bis(1,1-dimethylethyl)-4-hydroxythiodi-2,1-ethanediyl ester (available from BASF), 3-acryloxypropyl trimethoxysilane is an adhesion promoter (available from Gelest), and pentaerythritol tetrakis(3-mercaptopropionate) (also known as tetrathiol, available from Aldrich) is a chain transfer agent. The concentration unit “pph” refers to an amount relative to a base composition that includes all monomers, oligomers, and photoinitiators. For example, a concentration of 1.0 pph for Irganox 1035 corresponds to 1 g Irganox 1035 per 100 g combined of oligomeric material, SR504, NVC, and TPO.
The secondary coating layer 24 may be made of a known secondary coating composition. The secondary coating may be prepared from a composition that exhibits high Young's modulus (also referred to as “elastic modulus”). Higher values of Young's modulus may represent improvements that make the secondary coating prepared for the coating composition better suited for small diameter optical fibers. More specifically, the higher values of Young's modulus enable use of thinner secondary coatings on optical fibers without sacrificing performance. Thinner secondary coatings reduce the overall diameter of the optical fiber and provide higher fiber counts in cables of a given cross-sectional area. The Young's modulus of secondary coatings prepared as the secondary coating composition may be equal to or greater than 1500 MPa, more particularly about 1800 MPa or greater, or about 2100 MPa or greater and about 2800 MPa or less or about 2600 MPa or less. The results of tensile property measurements prepared from various curable secondary compositions are listed below in Table 2.
A representative curable secondary coating composition is listed below in Table 3.
SR601 is ethoxylated (4) bisphenol A diacrylate (a monomer). SR602 is ethoxylated (10) bisphenol A diacrylate (a monomer). SR349 is ethoxylated (2) bisphenol A diacrylate (a monomer). Irgacure 1850 is bis(2,6-dimethoxybenzoyl)-2,4,4-trimethylpentylphosphine oxide (a photoinitiator).
Two additional curable secondary coating compositions (A and SB) are listed in Table 4.
PE210 is bisphenol-A epoxy diacrylate (available from Miwon Specialty Chemical, Korea), M240 is ethoxylated (4) bisphenol-A diacrylate (available from Miwon Specialty Chemical, Korea), M2300 is ethoxylated (30) bisphenol-A diacrylate (available from Miwon Specialty Chemical, Korea), M3130 is ethoxylated (3) trimethylolpropane triacrylate (available from Miwon Specialty Chemical, Korea), TPO (a photoinitiator) is (2,4,6-trimethylbenzoyl)diphenyl phosphine oxide (available from BASF), Irgacure 184 (a photoinitiator) is 1-hydroxycyclohexyl-phenyl ketone (available from BASF), Irganox 1035 (an antioxidant) is benzenepropanoic acid, 3,5-bis(1,1-dimethylethyl)-4-hydroxythiodi-2,1-ethanediyl ester (available from BASF). DC190 (a slip agent) is silicone-ethylene oxide/propylene oxide copolymer (available from Dow Chemical). The concentration unit “pph” refers to an amount relative to a base composition that includes all monomers and photoinitiators. For example, for secondary coating composition A, a concentration of 1.0 pph for DC-190 corresponds to 1 g DC-190 per 100 g combined of PE210, M240, M2300, TPO, and Irgacure 184.
The curable secondary coating compositions were cured and configured in the form of cured rod samples for measurement of Young's modulus. The cured rods were prepared by injecting the curable secondary composition into Teflon® tubing having an inner diameter of about 0.025″. The rod samples were cured using a Fusion D bulb at a dose of about 2.4 J/cm2 (measured over a wavelength range of 225-424 nm by a Light Bug model IL390 from International Light). After curing, the Teflon® tubing was stripped away to provide a cured rod sample of the secondary coating composition. The cured rods were allowed to condition for 18-24 hours at 23° C. and 50% relative humidity before testing. Young's modulus was measured using a Sintech MTS Tensile Tester on defect-free rod samples with a gauge length of 51 mm, and a test speed of 250 mm/min. The Young's modulus was measured according to ASTM Standard D882-97. The Young's modulus was determined as an average of at least five samples, with defective samples being excluded from the average.
Secondary coatings with high Young's modulus as disclosed herein may be better suited for small diameter optical fibers. More specifically, a higher Young's modulus enables use of thinner secondary coatings on optical fibers, thereby enabling smaller fiber diameters without sacrificing performance. Thinner secondary coatings reduce the overall diameter of the optical fiber and provide higher fiber counts in cables of a given cross-sectional area.
The primary coating layer 22 may have a Young's modulus of less than 1 MPa and a Tg (glass transition temperature) of less than −20° C., and the secondary coating layer 24 may have a Young's modulus of greater than 1500 MPa and a Tg of greater than 65° C.
The inner glass region 12 has an overall cross-sectional diameter Dg which may be in the range of 120-130 microns, according to one example. The outer coating layer 20 may have a thickness in the range of 22-45 microns, or in the range of 22-40 microns, or in the range from 22-35 microns. The primary coating layer 22 may have a thickness in the range of 12-25 microns, or in the range from 12-22 microns, or in the range from 12-19 microns. The secondary coating layer 24 may have a thickness in the range of 10-20 microns, or in the range from 10-18 microns, or in the range from 10-16 microns. The optional tertiary coating layer 25 may have a thickness equal to or less than 10 microns, more particularly equal to or less than 5 microns, and more particularly in the range of 2-5 microns. The coated multicore optical fiber 10 has an overall fiber diameter Df equal to or less than 200 microns. More specifically, the overall diameter Df may be in the range of 170-200 microns, or in the range of 170-190 microns, or in the range of 180-200 microns.
Each core region 14 may be formed of germania-doped silica or other suitable glass and may have a fluorine-doped silica trench, wherein the trench volume of the fluorine-doped silica trench is greater than 50%Δ-μm2. The common outer cladding 16 may be made of silica or fluorine-doped silica or other suitable glass. It should be appreciated that the inner glass region 12 may be formed from a preform drawn at an elevated temperature (e.g., temperature of about 2000° C.) in a furnace. The outer coating layer 20, including one or more of the primary coating layer 22, secondary coating layer 24 and tertiary coating layer 25, may be applied after the uncoated optical fiber exits the furnace and is cooled.
The multicore optical fiber 10 shown in
Each core region 14 has a trench-assisted refractive index design profile having a mode field diameter of greater than 8.2 microns at a wavelength of 1310 nm, a cable or fiber cut-off wavelength of less than 1260 nm, and zero dispersion wavelength of less than 1340 nm. The trench volume of the trench in each core region 14 is at least 30%Δ-μm2 and up to 90%Δ-μm2. The signal cross-talk at 1310 nm per 100 km is less than −30 dB, and more preferably less than −40 dB, and even more preferably less than −50 dB.
In one aspect, the trench of the core region 14 can be characterized by a trench volume of greater than about 30%Δ-μm2. In one aspect, the trench of the core region 14 can have a trench volume of greater than about 30%Δ-μm2, greater than about 40%Δ-μm2, greater than about 50%Δ-μm2, or greater than about 60%Δ-μm2. In some aspects, the trench of the core region 14 has a trench volume of less than about 90%Δ-μm2, less than about 85%Δ-μm2, less than about 80%Δ-μm2, less than about 75%Δ-μm2, less than about 70%Δ-μm2, less than about 65%Δ-μm2, or less than about 60%Δ-μm2. In some aspects, the trench of the core region 14 has a trench volume of from about 30%Δ-μm2 to about 90%Δ-μm2, about 40%Δ-μm2 to about 90%Δ-μm2, about 50%Δ-μm2 to about 90%Δ-μm2, about 60%Δ-μm2 to about 90%Δ-μm2, about 30%Δ-μm2 to about 85%Δ-μm2, about 40%Δ-μm2 to about 85%Δ-μm2, about 50%Δ-μm2 to about 85%Δ-μm2, about 30%Δ-μm2 to about 80%Δ-μm2, or about 40%Δ-μm2 to about 80%Δ-μm2. For example, the trench of the core region 14 has a trench volume of about 30%Δ-μm2, about 35%Δ-μm2, about 40%Δ-μm2, about 45%Δ-μm2, about 46%Δ-μm2, about 47%Δ-μm2, about 48%Δ-μm2, about 49%Δ-μm2, about 50%Δ-μm2, about 55%Δ-μm2, about 60%Δ-μm2, about 61%Δ-μm2, about 62%Δ-μm2, about 68%Δ-μm2, about 69%Δ-μm2, about 70%Δ-μm2, about 75%Δ-μm2, about 80%Δ-μm2, about 85%Δ-μm2, about 90%Δ-μm2, or any trench volume between these values. Each trench of the core regions 14 can have the same or different trench volume. The trench volume of the trench can be determined as described above.
The multicore optical fiber 10 can be characterized by crosstalk between adjacent regions 14 of equal to or less than −20 dB, as measured for a 100 km length of the multicore optical fiber 10 operating at 1550 nm. In some aspects, the multicore optical fiber 10 can be characterized by crosstalk between adjacent core regions 14 of equal to or less than −30 dB, as measured for a 100 km length of the multicore optical fiber 10. In some aspects, crosstalk between adjacent cores Ci is ≤−20 dB, ≤−30 dB, ≤−40 dB, ≤−50 dB, or ≤−60 dB, as measured for a 100 km length of the multicore optical fiber 10 operating at 1550 nm. The crosstalk can be determined based on the coupling coefficient, which depends on the design of the core and a distance between two adjacent cores, and Δβ, which depends on a difference in β values between the two adjacent cores. For two cores placed next to each other, assuming the power launched into the first core is P1, using coupled mode theory and considering the perturbations along the fiber, the power coupled to the second core, P2, can be determined using the following equation:
where denotes the average, L is fiber length, κ is the coupling coefficient, ΔL is the length of the fiber segment over which the fiber is uniform, Lc is the correlation length, and g is given by the following equation:
where Δβ is the mismatch in propagation constant between the modes in two cores when they are isolated. The crosstalk (in dB) can be determined using the following equation:
The crosstalk between the two core regions grows linearly in the linear scale, but does not grow linearly in the dB scale. As used herein, crosstalk performance is reported for a 100 km length of optical fiber. However, crosstalk performance can also be represented with respect to alternative optical fiber lengths, with appropriate scaling. For optical fiber lengths other than 100 km, the crosstalk between cores can be determined using the following equation:
For example, for a 10 km length of optical fiber, the crosstalk can be determined by adding “−10 dB” to the crosstalk value for a 100 km length optical fiber. For a 1 km length of optical fiber, the crosstalk can be determined by adding “−20 dB” to the crosstalk value for a 100 km length of optical fiber.
In some embodiments, the core-to-core separation distance S is greater than 35 microns. In other embodiments, the core-to-core separation distance S is greater than 40 microns. In still further embodiments, the core-to-core separation distance S is greater than 45 microns.
In some embodiments, the minimum core region edge to fiber edge distance E (
In some embodiments, the outer trench radius is between 11 microns and 20 microns. In other embodiments, the outer trench radius is between 12 microns and 18 microns. The fiber 10 has an overall diameter Df measured across the fiber coating of less than 200 microns. In some embodiments, the coating layer outer diameter Df is less than 190 microns. In yet other embodiments, the coating layer outer diameter Df is less than 180 microns.
The coating layer 20 which is comprised of the primary coating layer 22, secondary coating layer 24 and an optional tertiary layer 25 provides a puncture resistant coating for the multicore optical fiber 10. The primary coating layer 22 may have an elastic modulus of less than 1 MPa and Tg (glass transition temperature) of less than −40° C. The secondary coating layer 24 may have an elastic modulus of greater 1500 MPa and Tg of greater than 65° C. In some embodiments, the puncture resistance of the fiber 10 is greater than 20 g, and in other embodiment, the puncture resistance of the fiber 10 is greater than 25 g.
The puncture resistance of secondary coatings suitable for the multicore optical fiber 10 for different combinations of secondary coating cross-section area and elastic modulus is shown in
Puncture resistance measurements were made on samples that included a glass fiber, a primary coating, and a secondary coating. The glass fiber had a diameter of 125 μm. The primary coating was formed from the reference primary coating composition listed in Table 8 below. Samples with various secondary coatings were prepared as described below. The thicknesses of the primary coating and secondary coating were adjusted to vary the cross-sectional area of the secondary coating as described below. The ratio of the thickness of the secondary coating to the thickness of the primary coating was maintained at about 0.8 for all samples.
The puncture resistance was measured using the technique described in the article entitled “Quantifying the Puncture Resistance of Optical Fiber Coatings”, by G. Scott Glaesemann and Donald A. Clark, published in the Proceedings of the 52nd International Wire & Cable Symposium, pp. 237-245 (2003). A summary of the method is provided here. The method is an indentation method. A 4-centimeter length of optical fiber was placed on a 3 mm-thick glass slide. One end of the optical fiber was attached to a device that permitted rotation of the optical fiber in a controlled fashion. The optical fiber was examined in transmission under 100× magnification and rotated until the secondary coating thickness was equivalent on both sides of the glass fiber in a direction parallel to the glass slide. In this position, the thickness of the secondary coating was equal on both sides of the optical fiber in a direction parallel to the glass slide. The thickness of the secondary coating in the directions normal to the glass slide and above or below the glass fiber differed from the thickness of the secondary coating in the direction parallel to the glass slide. One of the thicknesses in the direction normal to the glass slide was greater and the other of the thicknesses in the direction normal to the glass slide was less than the thickness in the direction parallel to the glass slide. This position of the optical fiber was fixed by taping the optical fiber to the glass slide at both ends and is the position of the optical fiber used for the indentation test.
Indentation was carried out using a universal testing machine (Instron model 5500R or equivalent). An inverted microscope was placed beneath the crosshead of the testing machine. The objective of the microscope was positioned directly beneath a 75° diamond wedge indenter that was installed in the testing machine. The glass slide with taped fiber was placed on the microscope stage and positioned directly beneath the indenter such that the width of the indenter wedge was orthogonal to the direction of the optical fiber. With the optical fiber in place, the diamond wedge was lowered until it contacted the surface of the secondary coating. The diamond wedge was then driven into the secondary coating at a rate of 0.1 mm/min and the load on the secondary coating was measured. The load on the secondary coating increased as the diamond wedge was driven deeper into the secondary coating until puncture occurred, at which point a precipitous decrease in load was observed. The indentation load at which puncture was observed was recorded and is reported herein as grams of force. The experiment was repeated with the optical fiber in the same orientation to obtain ten measurement points, which were averaged to determine a puncture resistance for the orientation. A second set of ten measurement points was taken by rotating the orientation of the optical fiber by 180°.
Several fiber samples with each of the three secondary coating layers are shown. Each fiber sample included a glass fiber with a diameter of 125 μm, a primary coating layer formed from the example primary coating composition disclosed herein, and one of three secondary coating layers with different cross-section areas and elastic modulus. The thicknesses of the primary coating layer and secondary coating layer were adjusted to vary the cross-sectional area of the secondary coating layer as shown in
Fiber samples with a range of thicknesses were prepared for each of the secondary coating layers to determine the dependence of puncture load on the thickness of the secondary coating. One strategy for achieving higher fiber count in cables is to reduce the thickness of the secondary coating layer. As the thickness of the secondary coating layer is decreased, however, its performance diminishes and its protective function is compromised. Puncture resistance is a measure of the protective function of a secondary coating layer. A secondary coating layer with a high puncture resistance withstands greater impact without failing and provides better protection for the inner glass region 12 of the multicore optical fiber 10.
The puncture load as a function of cross-sectional area for the three coatings is shown in
The higher modulus traces show an improvement in puncture load for high cross-sectional areas. The improvement, however, diminishes as the cross-sectional area decreases. At a cross-sectional area of 7000 μm2, for example, the puncture load of the secondary coating layer obtained from secondary coating layer having a modulus of 1800 MPa becomes approximately equal to the puncture load of the secondary coating layer having a modulus of 1500 MPa and the increase in puncture load of the secondary coating layer with a modulus of 2100 MPa relative to the secondary coating layers having moduli of 1800 MPa and 1500 MPa becomes smaller than the increase observed at higher cross-sectional areas.
The puncture load of a secondary coating layer having a Young's modulus of at least 1500 MPa at a cross-sectional area of about 7000 μm2 is greater than 20 g. The puncture load of a secondary coating layer having a Young's modulus of at least 1500 MPa at a cross-sectional area of about 10,000 μm2 is greater than 25 g. The puncture load of a secondary coating layer having a Young's modulus of at least 1500 MPa at a cross-sectional area of 15,000 μm2 is greater than 35 g. The puncture load of a secondary coating layer having a Young's modulus of at least 1500 MPa at a cross-sectional area of 20,000 μm2 is greater than 45 g. The puncture load of a secondary coating layer having a Young's modulus of 2100 MPa is greater than 35 g for a cross-sectional area of 7000 μm2 and greater. Embodiments of the multicore optical fiber include secondary coatings having any combination of the foregoing puncture loads.
One example of a multicore optical fiber 10 having four core regions 14 arranged in a 2×2 array, as shown in
In Table 5, the optical properties of the 2×2 (four) arrangement of core regions of an exemplary multicore optical fiber 10, with each core region having the refractive index design profile as seen in
As seen in Table 6, the cross-talk measurements on the four core regions at 1310 nm and 1550 nm for the multicore optical fiber with each core-portion having the refractive index design profile shown in sample 2 in Table 5 and
Relative refractive index design profiles of three examples 2-4 of the multicore optical fiber having exemplary trench assisted core regions, an MFD at a wavelength of 1310 nm of greater than 8.5 microns and trench volumes greater than 60%Δ microns2 are shown in
As can be seen in Table 7 above, the trench assisted core region designs of the multicore optical fibers having an MFD at 1310 nm of greater than 8.5 microns and a trench volume greater than 60%Δ-μm2 are illustrated.
Referring to
As can be seen in Table 8, the examples 5 and 6 trench assisted core region designs and multicore optical fiber has an MFD at 1310 nm greater than 8.5 microns and trench volumes greater than 60%Δ-μm2 are shown.
Referring to
The optical fiber design and optical properties of the multicore optical fiber disclosed in examples 7-10 are shown in Table 9.
Having described a multicore optical fiber design, the following discussion pertains to an optical fiber cable having a high density of cores using the described multicore optical fibers.
In one or more embodiments, the cable core 110 defines a cross-sectional area, and the multicore optical fibers 112 occupy a percentage of the cross-sectional area (also referred to as a “fill fraction”). In embodiments, the multicore optical fibers 112 occupy from 50% to 90% (i.e., fill fraction of 0.5 to 0.9) of the cross-sectional area defined by the cable core 110. In embodiments, the cable core 110 is defined by the inner surface 116 of the buffer tube 114. For example, the inner surface 116 of the buffer tube 114 may define an inner diameter of the buffer tube 114 (i.e., a maximum interior cross-sectional dimension of the buffer tube 114). In such embodiments, the buffer tube 114 inner diameter may be used to calculate the cross-sectional area of the cable core 110. In other embodiments, the cable core 110 can be described as any of the cable structures disposed within the central cable bore 108. For example, the central cable bore 108 may contain multiple buffer tubes 114, each containing a plurality of multicore optical fibers 112.
As mentioned, the multicore optical fibers 112 are depicted in the loose tube configuration, but in other embodiments, the multicore optical fibers 112 may be arranged in ribbons comprising a plurality of multicore optical fibers 112 held together by a ribbon matrix material. In one or more embodiments, each multicore optical fiber 112 is bound to an adjacent multicore optical fiber 112 along its length by a ribbon matrix material. In one or more embodiments, each multicore optical fiber 112 is bound to an adjacent multicore optical fiber only intermittently along its length by a ribbon matrix material. In embodiments, the ribbons are arranged into stacks within the buffer tube 114. Such stacks may have a rectangular or a cross-shaped cross section when viewed from the endfaces of the multicore optical fibers 112. In other embodiments, such as depicted in
In one or more embodiments, water blocking yarns 122 are provided in the buffer tube 114 along with the plurality of multicore optical fibers 112. The water blocking yarns 122 may be yarns impregnated with superabsorbent polymer powder or resin and are configured to absorb water that enters the buffer tube 114.
Disposed around the exterior surface 118 of the buffer tube 114 are a plurality of strengthening yarns 124. In one or more embodiments, the optical fiber cable 100 includes from two to twelve strengthening yarns 124. In the embodiment depicted in
In one or more embodiments, the optical fiber cable 100 includes a water blocking tape 126 wrapped around the strengthening yarns 122. The water-blocking tape 126 is configured to prevent water from penetrating the cable core 110.
In the embodiment depicted, the cable jacket 102 is disposed around the water-blocking tape 126. In embodiments, the inner surface 104 and the outer surface 106 define a thickness of the cable jacket 102. In embodiments, the cable jacket 102 has a thickness of 0.75 mm to 2 mm, in particular 1 mm to 1.75 mm, and most particularly 1.25 mm to 1.5 mm, for example about 1.3 mm. In embodiments, the outer surface 106 defines an outermost surface of the optical fiber cable 100. Further, in embodiments, the outer surface 106 defines an outer diameter OD of the optical fiber cable 100. In embodiments, the outer diameter OD of the optical fiber 100 is from 5 mm to 10 mm, in particular 7 mm to 9 mm, and particularly about 9 mm.
In one or more embodiments, the cable jacket 102 includes one or more structures, such as strength members 128 and/or ripcords 130, embedded between the inner surface 104 and the outer surface 106. In the embodiment depicted, the optical fiber cable 100 includes a plurality of strength members 128 positioned within the cable jacket 102. In particular, the cable jacket 102 includes eight strength members 128 arranged in pairs at diametrically opposed positions (i.e., in each quadrant) around the circumference of the cable jacket 102. In one or more embodiments, the strength members 128 comprise glass-reinforced plastic rods, fiber-reinforced plastic rods, or metal strands, among others. Further, in embodiments, the strength members 128 comprise a diameter of 0.25 mm to 1 mm, in particular 0.5 mm to 0.75 mm, more particularly about 0.6 mm.
Further, in one or more embodiments, the optical fiber cable 100 includes access features, such as ripcords 130. In the embodiment depicted, the ripcords 130 are arranged diametrically between pairs of strength members 128. In embodiments, the ripcords 130 are, for example, aramid strands used to tear through the cable jacket 102 to access the cable core 110.
In one or more embodiments, each of the multicore optical fibers 112 comprises a glass diameter from 120 microns to 130 microns. In one or more embodiments, the multicore optical fibers 112 comprises an overall fiber diameter Df of 200 microns or less, 190 microns or less, or 180 microns or less. In one or more embodiments, the multicore optical fibers 112 comprise an overall fiber diameter Df of 170 microns or more.
In one or more embodiments, the number of cores in each multicore optical fiber 112 is at least 3 cores, at least 4 cores, at least 5 cores, at least 6 cores, or at least 7 cores. In one or more embodiments, the number of cores in each multicore optical fiber 112 is up to 8 cores.
In one or more embodiments, the optical fiber cable 100 is sized and contains a number of multicore optical fibers 112 such that the core density in the cable core 110 is at least 40 cores/mm2, at least 60 cores/mm2, at least 80 cores/mm2, at least 100 cores/mm2, or at least 200 cores/mm2. In one or more embodiments, the core density in the cable core is up to 350 cores/mm2.
In one or more embodiments, the fill fraction of multicore optical fibers 112 in the cable core 110 is at least 50%, at least 55%, at least 60%, at least 65%, at least 70%, at least 75%, at least 80%, or at least 85%. In one or more embodiments, the fiber fill fraction in the cable core 110 is up to 90%. Table 10, below, provides examples of core densities that can be achieved for optical fiber cables 100 including multicore optical fibers 112 as described herein.
Advantageously, the multicore optical fibers allow for an increasing core density for optical fiber cables to overcome cable size limitations and duct congestion issues in passive optical network systems. In particular, optical fiber cables as disclosed herein may be particularly suitable for use in data center applications, as well as in high speed optical interconnects, where a need exists to increase the core density to achieve compact high fiber count connections. In such applications, the installation method typically involves air blowing or jetting. To increase the jetting distance and have still have high core densities in ducts, smaller diameter cables with high fiber counts are desirable. Embodiments of the high core density optical fiber cables disclosed herein allow for increased core density without requiring an increased cable size, which allows for the disclosed cables to be routed through existing ducts using conventional jetting or air blowing technology.
Various modifications and alterations may be made to the examples within the scope of the claims, and aspects of the different examples may be combined in different ways to achieve further examples. Accordingly, the true scope of the claims is to be understood from the entirety of the present disclosure in view of, but not limited to, the embodiments described herein.
It will be apparent to those skilled in the art that various modifications and variations can be made without departing from the spirit or scope of the claims.
This application is a continuation of International Patent Application No. PCT/US2022/031515 filed May 31, 2022, which claims the benefit of priority under 35 U.S.C. § 119 of U.S. Provisional Application No. 63/195,846, filed on Jun. 2, 2021, the content of which is relied upon and incorporated herein by reference in its entirety.
Number | Date | Country | |
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63195846 | Jun 2021 | US |
Number | Date | Country | |
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Parent | PCT/US2022/031515 | May 2022 | US |
Child | 18515915 | US |