Some embodiments described herein relate generally to optical fiber assemblies and methods of making the same.
Known devices exist for coupling collimated free space beams. Such known devices can have strict mechanical tolerances, which can result in high loss and inefficient coupling. This can further result in undesirable variability in coupling. Known devices are particularly inefficient at coupling single mode optical fibers transmitting visible wavelength signals having small mode field diameters.
Accordingly, a need exists for an improved optical fiber assembly and method for making optical fiber assemblies.
In some embodiments, an optical fiber assembly apparatus includes a signal fiber having a substantially constant outer diameter, a proximal portion, and a distal portion. The proximal portion has a waveguide structure configured to propagate an optical signal having a first mode field diameter and the distal portion has an expanded waveguide structure configured to propagate the optical signal having the first mode field diameter at a proximal end of the distal portion and propagate the optical signal having a second mode field diameter at a distal end of the distal portion. The optical fiber assembly includes a lens fiber having a proximal end. The proximal end of the lens fiber is fused to the distal end of the distal portion of the signal fiber. The lens fiber is configured to propagate an optical signal through a nominally homogenous region.
In some embodiments, an optical fiber assembly apparatus includes a signal fiber having a substantially constant outer diameter, a proximal portion, and a distal portion. The proximal portion has a waveguide structure configured to propagate an optical signal having a first mode field diameter and the distal portion has an expanded waveguide structure configured to propagate the optical signal having the first mode field diameter at a proximal end of the distal portion and propagate the optical signal having a second mode field diameter at a distal end of the distal portion. The optical fiber assembly includes a lens fiber having a proximal end. The proximal end of the lens fiber is fused to the distal end of the distal portion of the signal fiber. The lens fiber is configured to propagate an optical signal through a nominally homogenous region.
In some embodiments, an apparatus includes an optical fiber assembly including a signal fiber having a substantially constant outer diameter. The signal fiber has a mode expansion region configured to expand a mode field diameter of a signal from a first mode field diameter to a second mode field diameter. The optical fiber assembly includes an intermediate optical fiber. A proximal end of the intermediate optical fiber has a first outer diameter and is fused to a distal end of the signal fiber. A distal end of the intermediate optical fiber has a second outer diameter. The optical fiber assembly includes a lens fiber having a substantially constant outer diameter, and the lens fiber is fused to the distal end of the intermediate optical fiber.
In some embodiments, a method includes heating a distal portion of a signal fiber to define a mode expansion region configured to expand a mode field diameter of an optical signal from a first mode field diameter to a second mode field diameter. The method includes fusing a proximal end of a lens fiber to a distal end of the signal fiber.
As used in this specification, the singular forms “a,” “an” and “the” include plural referents unless the context clearly dictates otherwise. Thus, for example, the term “a tapered fiber” is intended to mean a single tapered fiber or a combination of tapered fibers. As used in this specification, “monolithically formed” can mean that some or all of the optical components are formed from a common material. As used herein, “integrally formed” can mean some or all of the optical components are formed from different materials and are fixedly or permanently attached, coupled, fused or bonded together (e.g., spliced together).
In some embodiments described herein, an optical fiber assembly can be used to transmit power, data, sensor signals or any combinations of these signals. In some embodiments, the optical fiber assembly can be an “all-fiber” device, e.g., a device wherein all of the signal carrying components of the optical fiber assembly include glass, such as, for example, silica glass, phosphate glass, germanium glass, etc. In some embodiments, some or all of the optical components of the all-fiber device, such as the signal fiber, lens fiber, etc. can be monolithically formed or integrally formed. In some embodiments, the all-fiber device can be formed from a combination of one or more monolithically-formed optical components and one or more integrally formed optical components. The optical fiber assembly can be robust, inexpensive, reduce or eliminate mechanical misalignment, allow better control of mode field diameter size, accommodate a large free-space beam, and can have high coupling efficiency.
An optical fiber, such as, for example, a signal fiber, an intermediate fiber, a tapered fiber, a lens fiber, and/or portions thereof, can define a mode field diameter of a signal propagated through that optical fiber. In some embodiments, a waveguide structure, for example, an optical fiber having a core and cladding, can define the mode field diameter of the signal. In such embodiments, the optical fiber can substantially confine the signal to the core. Said another way, the waveguide structure can substantially prevent diffraction from expanding a mode field diameter of the signal. The mode field diameter of a signal can be characterized and/or represented by a mode profile. Said another way, an optical fiber can support a mode profile. A mode profile can be generally Gaussian and the characteristics of the Gaussian shape can depend on, for example, the mode field diameter of a signal propagating through the optical fiber. By way of example, a signal having a first mode field diameter can propagate through a first optical fiber having a first mode profile. The signal can pass into a second optical fiber supporting the first mode profile at a proximal end and supporting a second mode profile at a distal end. In this example, the mode field diameter of the signal can expand from the first mode field diameter to a second mode field diameter. In some such embodiments, the first optical fiber and the second optical fiber can be chosen such that the mode field diameter of the signal can expand from the first mode field diameter to the second mode field diameter adiabatically to reduce signal loss.
Signal fiber 110 can include a waveguide structure (not shown) defining a core (not shown), and can include a proximal portion (not shown in
When a monolithically formed signal fiber 110 having a constant outer diameter supports a second mode profile for the distal portion, different from a first mode profile supported by the proximal portion, the distal portion of the signal fiber 110 can be referred to as a mode expansion region. The length of the mode expansion region can vary. In some embodiments, the length of the mode expansion region can be about one millimeter. In other embodiments, the length of the mode expansion region can be between about 100 microns and about ten millimeters. The mode expansion region can expand the mode field diameter of the signal for an amount between about ten percent expansion and about 400 percent expansion. The amount of expansion of the mode field diameter of the signal through the mode expansion region can be based on, for example, the length of the mode expansion region, characteristics of the waveguide structure of the signal fiber 110, how the distal portion of the signal fiber 110 was altered, the outer diameter of the signal fiber, and/or combinations of the above.
Lens fiber 130 can include a coreless structure, e.g., may not have a waveguide structure to reduce or prevent diffraction. In this manner, lens fiber 130 can include a nominally homogenous refractive index. Lens fiber 130 supports mode profile 132 at a distal end and includes lens 134. In some embodiments, the coreless structure of lens fiber 130 can allow the mode field diameter of a signal to expand by diffraction. In this manner, the mode field diameter of the signal can increase along a length of lens fiber 130. Lens 134 of lens fiber 130 can be curved to collimate the signal light exiting lens fiber 130. In some embodiments, lens 134 can be curved such that the signal mode field diameter increases, decreases, or is collimated as it propagates away from the lens fiber, e.g., to expand or to reduce the signal mode field diameter. In such embodiments, increasing the radius of curvature of the lens can increase the mode field diameter of the signal as it propagates away from the lens fiber, and decreasing the radius of curvature can reduce the mode field diameter of the signal as it propagates away from the lens fiber.
Lens fiber 130 can have a substantially constant outer diameter. In some embodiments, the substantially constant outer diameter of lens fiber 130 can be larger than the substantially constant outer diameter of signal fiber 110. In such embodiments, the substantially constant outer diameter of the lens fibers can be, for example, less than about three times as large as the substantially constant outer diameter of signal fiber 110. In this manner, lens fibers 130 can be more easily spliced/fused to signal fiber 110, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments, the substantially constant outer diameter of lens fiber 130 can be larger or smaller than three times the substantially constant outer diameter of signal fiber 110. In some embodiments, the outer diameter of lens fiber 130 can be at least twice the size of the mode field diameter. In such embodiments, the outer diameter of the lens fiber 130 can be at least three times the size of the mode field diameter. Lens fiber 130 can include a waveguide structure (not shown) defining a core (not shown). A diameter of the core can be, for example, larger than the mode field diameter of the signal at any point within lens fiber 130. In such embodiments, the core of lens fiber 130 may not prevent the expansion of the mode field diameter of a signal passing through lens fiber 130.
In one example, a single mode signal can have about a four micron mode field diameter for the visible range centered around 630 nanometers. The signal can enter the distal portion of signal fiber 110 and can propagate through the mode expansion region; the mode field diameter of the signal can expand from about four microns to about five microns. The signal can enter lens fiber 130, which has a length of about two millimeters, and the mode field diameter of the signal can expand from about five microns to about 0.22 millimeters. The signal can exit lens fiber 130 via lens 134 as a collimated beam with a substantially constant outer diameter of about 0.22 millimeters. In some other embodiments, lens fiber 130 can be about one millimeter long and the signal can exit lens fiber 130 via lens 134 as a collimated beam with a substantially constant outer diameter of about 0.11 millimeters. In yet other embodiments, lens fiber 130 can be about four millimeters long and the signal can exit lens fiber 130 via lens 134 as a collimated beam with a substantially constant outer diameter of about 0.44 millimeters.
Signal fiber 210 can include a waveguide structure (not shown) defining a core (not shown). Signal fiber 210 can be configured to propagate a single mode signal. In some embodiments, the single mode signal can be transmitted about a center wavelength in the visible spectrum, such as, for example, between about 400 nanometers and about 700 nanometers. In some embodiments, signal fiber 210 can have a substantially constant outer diameter D1. In some embodiments, the substantially constant outer diameter D1 can be about 125 microns. In other embodiments, the substantially constant outer diameter D1 can be larger or smaller. The substantially constant outer diameter can be larger than a mode field diameter of a signal passing through signal fiber 210. The waveguide structure of distal portion 218 of signal fiber 210 is altered, for example, by applying heat to distal portion 218 of the signal fiber 200, such that the waveguide structure of distal portion 218 of signal fiber 210 is altered. Altering can include, for example, causing diffusion of dopants in signal fiber 210. In such embodiments, first mode profile 212 can be different from second mode profile 214. The first mode profile 212 can be such that the mode field diameter of the signal is constant through proximal portion 216 of signal fiber 200. Second mode profile 214 can be such that the mode field diameter increases along distal portion 218 of signal fiber 210. In such embodiments, the increase in mode field diameter can be adiabatically tapered so that transmission losses associated with the transformation of the mode profile are negligible.
Distal portion 218 of signal fiber 210 includes a mode expansion region. The length of the mode expansion region can vary. In some embodiments, the length of the mode expansion region can be about one millimeter. In other embodiments, the length of the mode expansion region can be between about 100 microns and about ten millimeters. The mode expansion region can expand the mode field diameter of a signal for an amount between about ten percent expansion and about 400 percent expansion. The amount of expansion of the mode field diameter through the mode expansion region can be based on, for example, the length of the mode expansion region, characteristics of the waveguide structure of the signal fiber 210, how the distal portion of the signal fiber was altered, the substantially constant outer diameter D1 of the signal fiber, and/or combinations of the above.
Lens fiber 230 can include a coreless structure, e.g., may not have a waveguide structure to reduce or prevent diffraction. In this manner, lens fiber 230 can include a nominally homogenous refractive index. Lens fiber 230 supports mode profile 232 and includes lens 234. In some embodiments, the coreless structure of lens fiber 230 can allow the mode field diameter of a signal to expand by diffraction. In this manner, the mode field diameter of the signal can increase along a length of lens fiber 230. Lens 234 of lens fiber 230 can be curved to collimate the signal light exiting lens fiber 230. In some embodiments, lens 234 can be curved such that the signal mode field diameter increases, decreases, or is collimated as it propagates away from the lens fiber 230, e.g., to expand or to reduce the signal mode field diameter. In such embodiments, increasing the radius of curvature of lens 234 can increase the mode field diameter of the signal as it propagates away from lens fiber 230, and decreasing the radius of curvature can reduce the mode field diameter of the signal as it propagates away from the lens fiber.
Lens fiber 230 includes a substantially constant outer diameter D2. In some embodiments, the substantially constant outer diameter D2 of lens fiber 230 can be larger than the substantially constant outer diameter D1 of signal fiber 210. In such embodiments, the substantially constant outer diameter D2 of the lens fibers can be, for example, less than about three times as large as the substantially constant outer diameter D1 of signal fiber 210. In this manner, lens fibers 230 can be more easily spliced/fused to signal fiber 210, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments the substantially constant outer diameter D2 of lens fiber 230 can be larger or smaller than three times the substantially constant outer diameter D1 of signal fiber 210. In some embodiments, the outer diameter of lens fiber 230 can be at least twice the size of the mode field diameter of the signal. In such embodiments, the outer diameter of the lens fiber 230 can be at least three times the size of the mode field diameter of the signal. While shown in
Intermediate fiber 550 can include a coreless structure, e.g., may not have a waveguide structure to reduce or prevent diffraction. In this manner, intermediate fiber 550 is represented by a nominally homogenous refractive index. Intermediate fiber 550 can support mode profile 552 at a distal end. In some embodiments, the coreless structure of intermediate fiber 550 can allow the mode field diameter of a signal to expand by diffraction. In this manner, mode profile 552 can be such that the mode field diameter of the signal can increase along the intermediate fiber 550 (in the direction of the signal shown in
Intermediate fiber 550 includes a substantially constant outer diameter D4. In some embodiments, the substantially constant outer diameter D4 of intermediate fiber 550 can be larger than the substantially constant outer diameter D1 of signal fiber 510. In such embodiments, the substantially constant outer diameter D4 of the intermediate fiber can be less than about three times as large as the substantially constant outer diameter D1 of signal fiber 510. In this manner, intermediate fiber 550 can be more easily spliced/fused to signal fiber 510, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments the substantially constant outer diameter D4 of intermediate fiber 550 can be larger or smaller than three times the substantially constant outer diameter D1 of signal fiber 510.
Lens fiber 530 includes a substantially constant outer diameter D2. In some embodiments, the substantially constant outer diameter D2 of lens fiber 530 can be larger than the substantially constant outer diameter D4 of intermediate fiber 550. In such embodiments, the substantially constant outer diameter D2 of the lens fibers can be less than about three times as large as the substantially constant outer diameter D4 of intermediate fiber 550. In this manner, lens fibers 530 can be more easily spliced/fused to intermediate fiber 550, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments the substantially constant outer diameter D2 of lens fiber 530 can be larger or smaller than three times the substantially constant outer diameter D4 of intermediate fiber 550.
A signal propagating through optical fiber assembly 500 can have a first mode field diameter in a proximal portion 516 of signal fiber 510, represented by first mode profile 512. The signal can have a mode field diameter expanding from the first mode field diameter to a second mode field diameter in distal portion 518 of signal fiber 510, represented by second mode profile 514. The signal can have a mode field diameter expanding from the second mode field diameter to a third mode field diameter in intermediate fiber 550, represented by mode profile 552. The signal can have a mode field diameter expanding from the third mode field diameter to a fourth mode field diameter in lens fiber 530, represented by mode profile 532. Lens 534 can collimate the signal into a collimated beam propagating in free space with a substantially constant outer diameter D3.
Tapered fiber 670 can include a coreless structure, e.g., may not have a waveguide structure to reduce or prevent diffraction. In this manner, tapered fiber 670 can include a nominally homogenous refractive index. Tapered fiber 670 can support mode profile 672 at a distal end. In some embodiments, the coreless structure of tapered fiber 670 can allow the mode field diameter of a signal to expand by diffraction. In this manner, mode profile 672 can represent an expanding mode profile corresponding to the mode field diameter of the signal increasing along the tapered fiber 670. In some embodiments, tapered fiber 670 can include a waveguide structure (not shown) defining a core (not shown). In such embodiments, a diameter of the core can be larger than the mode field diameter of the signal at any point within tapered fiber 670. In such embodiments, the core of tapered fiber 670 may not prevent the expansion of the mode field diameter of a signal passing through tapered fiber 670.
Tapered fiber 670 includes a tapered outer diameter. The tapered outer diameter of tapered fiber can increase from a first outer diameter D1 to second outer diameter D2. In some embodiments, the first outer diameter D1 of tapered fiber 670 can be substantially the same as the substantially constant outer diameter D1 of signal fiber 610. In this manner, tapered fiber 670 can be more easily spliced/fused to signal fiber 610, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments the first outer diameter of tapered fiber 670 can be larger or smaller than the substantially constant outer diameter D1 of signal fiber 610.
Lens fiber 630 includes a substantially constant outer diameter D2. In some embodiments, the substantially constant outer diameter D2 of lens fiber 630 can be substantially the same as the second outer diameter D2 of tapered fiber 670. In this manner, lens fibers 630 can be more easily spliced/fused to tapered fiber 670, and the splice/fuse can be stronger, e.g., less likely to fail. In some embodiments the substantially constant outer diameter D2 of lens fiber 630 can be larger or smaller than the second outer diameter of tapered fiber 670.
A signal propagating through optical fiber assembly 600 can have a first mode field diameter in a proximal portion 616 of signal fiber 610, represented by first mode profile 612. The signal can have a mode field diameter expanding from the first mode field diameter to a second mode field diameter in distal portion 618 of signal fiber 610, represented by second mode profile 614. The signal can have a mode field diameter expanding from the second mode field diameter to a third mode field diameter in tapered fiber 670, represented by mode profile 672. The signal can have a mode field diameter expanding from the third mode field diameter to a fourth mode field diameter in lens fiber 630, represented by mode profile 632. Lens 634 can collimate the signal into a collimated beam propagating in free space with a substantially constant outer diameter D3.
A signal traveling through optical fiber assembly 700 can have a first mode field diameter in a proximal portion 716 of signal fiber 710, as represented by first mode profile 712. The signal can have a mode field diameter expanding from the first mode field diameter to a second mode field diameter in distal portion 718 of signal fiber 710, as represented by second mode profile 714. The signal can have a mode field diameter expanding from the second mode field diameter to a third mode field diameter in intermediate fiber 750, as represented by mode profile 752. The signal can have a mode field diameter expanding from the third mode field diameter to a fourth mode field diameter in tapered fiber 770, as represented by mode profile 772. The signal can have a mode field diameter expanding from the fourth mode field diameter to a fifth mode field diameter in lens fiber 730, as represented by mode profile 732. Lens 734 can collimate the signal into a collimated beam propagating in free space with a substantially constant outer diameter D3.
Intermediate fiber 850 can include a waveguide structure (not shown) defining a core (not shown), and includes a proximal portion 856 that supports a first mode profile substantially similar to mode profile 814, and a distal portion 858 that supports a second mode profile 854 at the distal end. In some embodiments, intermediate fiber 850 can have a substantially constant outer diameter D4. The waveguide structure of distal portion 858 of intermediate fiber 850 is altered, such as, for example, by applying heat to distal portion 858 of intermediate fiber 850, such that the waveguide structure of distal portion 858 of intermediate fiber 850 is altered. The waveguide structure can be altered prior to fusing/splicing with signal fiber 810 and to lens fiber 830, and/or can be altered after fusing/splicing with signal fiber 810 and to lens fiber 830. In such embodiments, first mode profile (not shown) can be different from second mode profile 854. The first mode profile includes a constant mode profile representing that the mode field diameter of the signal is constant through first portion 856 of intermediate fiber 850, and second mode profile 854 is an expanded mode profile representing that the mode field diameter of a signal increases along distal portion 858 of intermediate fiber 850.
Distal portion 858 of intermediate fiber 850 includes a mode expansion region. The length of the mode expansion region can vary. In some embodiments, the length of the mode expansion region can be about one millimeter. In other embodiments, the length of the mode expansion region can be between about 100 microns and about ten millimeters. The mode expansion region can expand the mode field diameter for an amount between about ten percent expansion and about 400 percent expansion. The amount of expansion of the mode field diameter through the mode expansion region can be based on the length of the mode expansion region, characteristics of the waveguide structure of the intermediate fiber 850, how the distal portion of the signal fiber was altered, the substantially constant outer diameter D4 of intermediate fiber 850, and/or combinations of the above.
A signal traveling through optical fiber assembly 800 can have a first mode field diameter in a proximal portion 816 of signal fiber 810, represented by first mode profile 812. The signal can have a mode field diameter expanding from the first mode field diameter to a second mode field diameter in distal portion 818 of signal fiber 810, represented by second mode profile 814. The signal can include a substantially constant third mode field diameter in a proximal portion 856 of intermediate fiber 850, represented by first mode profile 814. The signal can have a mode field diameter expanding from the third mode field diameter to a fourth mode field diameter in distal portion 858 of intermediate fiber 850, represented by second mode profile 854. The signal can have a mode field diameter expanding from the fourth mode field diameter to a fifth mode field diameter in lens fiber 830, represented by mode profile 832. Lens 834 can collimate the signal into a collimated beam propagating in free space with a substantially constant outer diameter D3.
In some embodiments, any of optical fiber assemblies 100-800 can be built into a connector assembly (not shown), for example, a housing configured to mechanically align the optical fiber assembly within a standardized connection, and/or to another of optical fiber assemblies 100-800. In such embodiments, the signal fiber, intermediate fiber, tapered fiber, and/or lens fiber can be secured by, for example, a ferrule, such that inserting the ferrule into a matching connection can mechanically align the optical fiber assembly.
While various embodiments have been described above, it should be understood that they have been presented by way of example only, not limitation, and various changes in form and details may be made. For example, while
Where methods described above indicate certain events occurring in certain order, the ordering of certain events can be modified. Additionally, certain of the events can be performed concurrently in a parallel process when possible, as well as performed sequentially as described above. Any portion of the apparatus and/or methods described herein may be combined in any combination, except mutually exclusive combinations. The embodiments described herein can include various combinations and/or sub-combinations of the functions, components and/or features of the different embodiments described. Furthermore, values for various dimensions and/or wavelengths are given for exemplary purposes only. For example, while a signal can be described as being centered about a visible wavelength, for example, between centered about 630 nm, signals can be centered about other wavelengths.
This application claims priority to U.S. Provisional Application No. 61/380,927 filed Sep. 8, 2010, and entitled “OPTICAL FIBER WITH END-CAP LENS AND METHOD FOR MAKING THE SAME,” the contents of which are herein incorporated by reference in its entirety.
Number | Date | Country | |
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61380927 | Sep 2010 | US |