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    • 专利摘要:
    Large core photonic crystal fibers for transmitting radiation have a core that includes a substantially transparent core material and has a core diameter of at least 5 μm. The fiber comprises a cladding region surrounding the core material length, the cladding region comprising a substantially transparent cladding material having a first index of refraction, wherein the substantially transparent first cladding material comprises a substantially periodic hole array having a fiber length. The holes are filled with a second cladding material having a second index of refraction less than the first index of refraction, so that radiation entering the optical fiber is transmitted along the length of the core material in a single propagation mode. In a preferred embodiment, the core diameter is at least 20 μm and may be 50 μm. The fibers can transmit higher power radiation than conventional fibers while maintaining a single propagation mode. The core material may be doped with a material that can provide amplification under the action of pump radiation entering the fiber. The present invention relates to fiber lasers and fiber amplifiers comprising doped large core photonic crystal fibers. The fiber is used in a system for transmitting radiation comprising a plurality of lengths of large core photonic crystal fibers separated by a large core photonic crystal fiber amplifier such that the radiation power transmitted through the system is maintained above a predetermined threshold power. .
    公开号:KR20010014256A
    申请号:KR1019997012363
    申请日:1998-06-17
    公开日:2001-02-26
    发明作者:버크스티모시아담；나이트조나단케이브；러셀필립세이트존
    申请人:스켈톤 에스. 알.；더 세크러터리 오브 스테이트 포 디펜스；
    IPC主号:
    专利说明:

    Single mode optical fiber
    The optical fiber is not subjected to linear effects or optical damage as high as a conventional optical fiber at high power. In particular, the optical fiber can be used as a single mode wavelength in a single mode fiber laser or a single mode fiber amplifier.
    Fiber optics are widely used to transfer light from one point to another and can be applied to communication, imaging and sensing. Typically, typical optical fibers are long strands of transparent material that have a refractive index that is uniform along the length but varies across the cross section. For example, a higher refractive index central core region is surrounded by a cladding region having a lower refractive index. The optical fiber may be made of fused silica with pure silica cladding surrounding a core made from silica in which impurities are introduced to raise the refractive index. Light is formed in or near the core by a total internal reflection treatment that occurs at the boundary between the core and the cladding.
    In general, this type of optical fiber may support one or more guided delivery modes formed in a core (ie, multimode fiber). These modes can move along the fiber at different phase speeds. However, if the core is made small enough, only one delivery mode will form a basic mode (ie, a single mode fiber) in the core. In other words, the distribution of light emitted from the optical fiber does not change when the conditions change at the launch end of the optical fiber and the optical fiber itself is subject to disturbances such as cross compression or bending. Typically, an optical fiber designed to carry a single mode having a wavelength of 1500 nm may have several percent germanium dopant in a core having a core diameter of 9 μm.
    Recently, photonic crystal fibers (PCF) have been developed, and the fibers include cladding made of transparent material with a built-in hole array along the length of the optical fiber (JC Knight et al., Opt, Lett 21 (1966) p. 1547. Errata Opt. Lett. 22 (1997) p.484). The holes are laterally arranged in a periodic array and filled with a material having a lower index of refraction than the cladding pedestal, and the core of the optical fiber includes transparent regions that break the cladding periodicity. Typically, both the core and the cladding are made of fused silica and the holes are filled with air. The core diameter is about 5 μm, the flat width of the entire fiber is about 40 μm, and the holes have a spacing of about 2-3 μm. If the air hole diameter of the optical fiber is the pitch or spacing of the small enough portions between the holes, the optical fiber core guides light in a single mode.
    Due to the fact that signals carried by optical fibers travel in only one mode and avoid intermodal distribution problems where they encounter multimode fibers, they are more than multimode fibers in telecommunications, laser power delivery, and many sensor applications. Has an advantage. In addition, the light density across a single mode fiber at a given wavelength is guaranteed to follow one smooth, known unchanging distribution. This does not matter how the light is directed to the fiber or to any impaired fiber (eg, time varying).
    In many applications it is desirable to carry as much optical power as possible. For example, any optical fiber inevitably reduces light while passing through the optical fiber. For example, for a given detector sensitivity, the length of the communication link can be increased by increasing the radiation power input to the optical fiber. As another embodiment, there are many high power laser systems in industrial applications that can be made more simplified if light can be channeled through one optical fiber than using conventional optical systems. However, there is a limitation on the amount of light that can be carried by known optical fibers at a given time.
    In a conventional optical fiber including a core region surrounded by a lower refractive index cladding region, the material from which the optical fiber is made will be greatly damaged if the optical density in the optical fiber exceeds a threshold. Some intensities resulting from nonlinear optical processing at low densities can degrade quality or even damage optical signals, even without optical fiber damage.
    These problems can be alleviated by reducing the light intensity of the optical fiber for a given power and increasing the size of the fiber core so that large power is carried before reaching the threshold for nonlinear processing. However, if the core diameter is increased, the fiber will be in multimode. This is compensated by reducing the refractive index difference between the core and the cladding. As a result, it becomes difficult to control uniform doping across the core. In addition, fibers with small refractive index differences are liable to lose light when bent. Therefore, there is a limit to the size that increased coder size is used to increase the light capacity of single mode fibers.
    Some nonlinear effects are exacerbated by the presence of dopants in the core that make the material more sensitive to these effects. At higher powers, the doped fibers are severely damaged. Dopants are more easily damaged by ionizing radiation from the nuclear industry. This led to a core made of pure silica. The total internal reflectance is maintained by reducing the refractive index and introducing less dopant into the cladding where less light is carried in the cladding than in the core and more power can be carried. However, this is limited by the fact that some light is carried in the doped cladding.
    In addition, in conventional optical fibers, sufficient coupling of a high power laser towards the optical fiber is a problem when the light needs to be focused at a small point and the intensity at the end face of the optical fiber is greater than that if the core is large. Optical damage at or near the end face of the optical fiber limits the radiation power that can be sent to the optical fiber (S.W.Allison et al., Appl, Opt. 24 (1985) p. 3140). The maximum continuous wave power that can be achieved in a conventional single mode fiber is approximately 15 W.
    The present invention relates to single mode optical fibers that can be used to transmit radiation at substantially higher power than can be achieved using conventional means.
    1 is a schematic diagram of a conventional step index optical fiber.
    2A and 2B are schematic views of photonic crystal optical fibers.
    3A and 3B illustrate the advantages of coupling radiation to a relatively large photonic crystal fiber core.
    4 illustrates a large core photonic crystal fiber amplifier.
    FIG. 5 illustrates a wavelength selective coupler that may be used in the large core photonic crystal fiber amplifier shown in FIG.
    6 and 7 illustrate an optical fiber laser structure including a large core photonic crystal optical fiber.
    8 illustrates lamination and draw processing that may be used to form large core photonic crystal optical fibers.
    9 is an SEM image of the central region in the cleaved large core photonic crystal optical fiber cross section of the present invention.
    FIG. 10 shows a near field pattern at the output of the photonic crystal optical fiber shown in FIG. 9; FIG.
    11A and 11B illustrate near field distribution in cross section of a photonic crystal optical fiber.
    12 shows the effective ν values for photonic crystal fibers.
    The present invention overcomes the incompatibility problem of transmitting high power radiation using conventional optical fibers while maintaining single mode operation. In particular, the optical fiber is used as a waveguide for transmitting radiation from one point to another, or used as an optical fiber amplifier or fiber laser. Fiber optics can support single mode propagation of radiation with maximum power in the 100W-2kW range. In addition, if the core is not doped, the optical fiber does not suffer much damage at high intensity as compared to conventional (doped) optical fiber. The effect of nonlinear optical processing on the optical fiber is reduced and therefore the high power signal output from the optical fiber is degraded. Fiber optics have the added advantage that high power radiation can be efficiently coupled to the fiber without the need to focus on small beam point sizes.
    According to one aspect of the invention, an optical fiber for transmitting radiation,
    A core comprising a substantially transparent core material, having a core refractive index n and a length 1 and having a core diameter of at least 5 μm, and
    A cladding region surrounding the length of the core material, the cladding region comprising a substantially transparent first cladding material having a first index of refraction, wherein the substantially transparent first cladding material has a length of substantially periodic array of holes Is built along the hole, and the hole has a second refractive index equal to or less than the first refractive index,
    The radiation input to the optical fiber is transmitted in single mode propagation along the length of the core material.
    If the holes have a diameter d and are spaced apart by a pitch Λ, the optical fiber may be in single mode regardless of the input radiation wavelength for any pitch Λ value for a substantially fixed d / Λ ratio. . The present invention provides the advantage that the optical fiber can be made in a single mode for any wavelength over an extended wavelength range compared to what can be achieved using conventional optical fibers. This is because the fiber maintains a single mode for a fixed d / Λ ratio for any wavelength over an extended range.
    Preferably, the substantially transparent first cladding material may have a refractive index no less than the core refractive index. In a preferred embodiment, the core diameter may be 10 μm. In another preferred embodiment, the diameter of the core is at least 20 μm.
    In one embodiment of the invention, at least one array hole may be lacking to form an optical fiber core. The holes are arranged in a substantially hexagonal pattern.
    The hole may be a vacuum region or filled with a second cladding material. For example, the second cladding material may be any material that is substantially transparent, may be air or other gas (eg, halogen or hydrocarbon), or liquid (eg, any other water like solution or pigment solution). Or may be a solid (eg, a glass material having a different refractive index than the first cladding material).
    The substantially transparent first cladding material has a substantially uniform first refractive index and the core material has a substantially uniform core refractive index. The core material and the substantially transparent cladding material may be the same material. For example, the at least one core material and the substantially transparent first cladding material may be silica. Preferably, the diameter of the hole is not smaller than the wavelength of light to be guided to the optical fiber.
    In one embodiment of the invention, the substantially transparent core material comprises a dopant material, for example rare earth oxide ions such as erbium.
    According to a second aspect of the invention, an optical fiber amplifier for amplifying signal radiation,
    An optical fiber length as described herein for receiving signal radiation of a selected wavelength and transmitting radiation along the length of the optical fiber, the core material comprises a dopant material along at least a portion of the length,
    A portion of the doped core material comprises a radiation source for directing pump radiation of another selected wavelength for input to the length of the optical fiber to amplify the signal radiation under the action of the pump radiation, and
    Wavelength selective transmission means for selectively transmitting pump radiation over the length of the optical fiber and selectively outputting the signal radiation amplified from the optical fiber amplifier.
    For example, the wavelength selective transmission means includes an input lens and an output lens for focusing the radiation, and a dichroic mirror for selectively reflecting the pump radiation to the optical fiber and selectively transmitting the amplified input radiation to be output from the optical fiber amplifier. . Optionally, the wavelength selective transmission means comprises an optical fiber directional coupler having a wavelength dependent response.
    The dopant material may comprise rare earth oxide ions, such as erbium ions.
    According to another aspect of the invention, an optical fiber laser for outputting laser radiation,
    An optical fiber length as described herein for selectively transmitting laser radiation having a selected wavelength along the optical fiber length, at least a portion of the core material length comprising a dopant material,
    The doped core material comprises a radiation source for radiating pump radiation of different selected wavelengths for input into the optical fiber length to amplify the laser radiation under pump radiation action,
    Wavelength selective transmission means for selectively transmitting pump radiation over the length of the optical fiber and selectively outputting the laser radiation amplified from the optical fiber laser, and
    Feedback means for selectively supplying a portion of the amplified laser radiation such that the amplified laser radiation passes periodically along the length of the optical fiber and is further amplified.
    The dopant material may include rare earth oxides such as erbium ions.
    In one embodiment of the fiber laser, the wavelength selective transmission means and the feedback means may comprise two dichroic mirrors, each dichroic mirror disposed at different locations along the length of the optical fiber and the doped core material being two It is arranged between the positions of two dichroic mirrors.
    In another embodiment of the fiber laser, the feedback means and the wavelength selective transmission means may comprise two gratings formed at two different locations along the optical fiber length such that the doped core material is disposed between the two optical fiber gratings.
    In another embodiment of the above-described aspect of the invention, the fiber laser is a ring resonator fiber laser and wherein the feedback means is
    And means for directing light radiating from one end of the optical fiber length having the doped core material to the other end of the optical fiber length.
    According to another aspect of the invention, a system for transmitting radiation in a single propagation mode,
    Each optical fiber length comprises a plurality of optical fiber lengths arranged in series to receive input radiation from the previous length of the optical fiber in series and to transmit the output radiation at a later length in the optical fiber, each length being greater than or equal to a predetermined power to the optical fiber length. Separated by an amplifying means for amplifying the radiation output from the optical fiber length to maintain the power of the radiation transmitted by it.
    In a preferred embodiment, the amplifying means comprises a fiber optic amplifier as described herein.
    The invention will be described with reference to the following figures.
    Referring to FIG. 1, a typical step index fiber 1 comprises a circular core 2 of radius r surrounded by a cladding material 3 of uniform refractive index n1 and uniform refractive index n2. . The number of guided modes that the step index fiber 1 supports for light of wavelength lambda is determined by the value of V, where V is as follows.
    ... (1)
    The step index fiber is single mode if V is less than or equal to 2.405. Thus, a conventional single mode step index fiber is typically operated such that V is less than or equal to 2.405.
    In a typical step index fiber as shown in FIG. 1, if the light intensity propagating along the fiber exceeds the threshold, the material from which the fiber is made is ultimately subject to irreparable damage. For light of lower intensity, a number of nonlinear optical treatments occur, degrading or damaging the quality of the optical signal. Although these problems are alleviated by increasing the size of the core 2 of the optical fiber 1, if the core radius is increased, the optical fiber will be in multiple mode. The refractive index difference between the core 2 and the cladding 3 should be reduced simultaneously for compensation.
    The refractive indices of the core 2 and the cladding 3 can be controlled by introducing the dopant into the material. However, in the end, it becomes difficult to control uniform doping across the core region 2. In addition, optical fibers with small index differences are affected by light loss when bent. This limits the power that the optical fiber can transmit, or the range that can be increased to increase the power capacity of the optical fiber. 2 (a) shows an optical fiber 4 of the present invention that overcomes the low power capacity problem associated with conventional fibers. The optical fiber 4 comprises a cladding of the first material 5 which is substantially transparent, wherein the array of holes 6 is embedded along the length 1 of the fiber. The holes 6 are laterally arranged in a periodic array and filled with a second material having a refractive index smaller than that of the first cladding material. This second material may be a solid, liquid or gaseous material. The hall may be empty. For example, the core material 7 and the first cladding material 5 may be made of pure fuse silica and the holes 6 may be filled with air.
    There is a core region 7 of substantially transparent material that substantially interrupts the array periodicity of the holes 6 in the center of the optical fiber cross section. For example, the central hole of the array is where the first cladding material region forms the core 7 of the optical fiber 4 around the location and location of the empty hole. The optical fiber core has a diameter c as shown in FIG. 2B. For this explanation, the core diameter of the optical fiber c is obtained by the distance between the center of one hole adjacent to the core and the diagonally opposite hole adjacent to the core.
    The array of holes forms a hexagonal pattern (eg, as shown in FIG. 2A) but other hole patterns can be envisioned.
    In conventional photonic crystal fibers, the outer width of the optical fiber w is on the order of 40 mu m, and the center to center spacing of the holes (pitch Λ) is about 2 mu m. The solid core region typically has a 4 μm diameter smaller than the core diameter of a conventional single mode fiber (see FIG. 1) as used in telecommunication applications. However, photonic crystal fibers of this diameter can only transmit radiation having a power of 10-20 W. Therefore, the fiber is not suitable for use in high power laser systems that can have an output power of at least 1 kW.
    According to one aspect of the invention, a single mode optical fiber for transmitting radiation from one point to another comprises photonic crystal fibers as shown in FIG. 2, wherein the diameter of the core 7 is at least 5 μm and Preferably at least 10 μm. Increasing the core diameter of the photonic crystal fiber causes an increase in the amount of power that can be transmitted and is still preferred for the large core diameter in the 20-50 μm region, depending on the particular application of the optical fiber. To illustrate this, photonic crystal fibers with a central core 7 having a diameter of at least 5 μm are called “large core photonic crystal fibers”.
    In addition, large core photonic crystal fibers can propagate radiation in a single mode. Therefore, fibers are used to transmit higher power radiation due to the larger core size in a single propagation mode than can be achieved using conventional optical fibers.
    Large core photonic crystal fibers with a core diameter of 50 μm can support continuous wave radiation with a power of approximately 2 kW. This corresponds to the value obtained by estimating the best experimental result achieved for a conventional optical fiber. In a typical silica step index fiber as shown in FIG. 1, the maximum continuous wave intensity of radiation that can be transmitted before permanent damage signs is 100 MW cm- 2 (W.Luthy, Optical Engineering 34 (1995) pp. 2361- 2364). For a core diameter of 12 μm, this corresponds to a theoretical maximum power of approximately 100 W. In practice, however, the theoretical maximum power is greatly reduced by the loss resulting from the radiation coupling to the optical fiber and the fact that the maximum continuous wave power achieved in conventional single mode fibers is approximately 15 W.
    An additional advantage of large core photonic crystal fibers is that the coupling of radiation to the optical fiber can be made easier. 3A and 3B are schematic representations of laser radiation 8 input to a conventional photonic crystal fiber (a) having a relatively small core and a large core photonic crystal fiber (b) by means of a lens or lens arrangement 9. Drawing. With reference to FIG. 3B, if the core of the large core photonic crystal fiber 7 is compared with the diameter of the laser beam beam, it is possible to input radiation 8 into the optical fiber without the need for a lens 9.
    Single mode large core photonic crystal fibers are applied to high power laser systems used in the industry as used in laser device applications where there is a need to direct high power laser radiation to the material to be processed. This is inconvenient and it is not practical to move the laser to direct the laser beam so conventional optics are used to guide the laser beam in the required direction. The large core photonic crystal fiber can enable high power laser beams to be delivered without the need for complicated and large optics.
    Large core photonic crystal fibers are used for telecommunication applications. Typically, the length of a conventional optical fiber (shown in FIG. 1) is used to guide radiation from one point to another. Since the intensity of the radiation decreases as it is transmitted along its length, an optical fiber amplification device, or repeater, is used at various points along the optical fiber length to improve the power of the periodically transmitted radiation. The device detects a weak signal (i.e., reduced power signal) radiating from the optical fiber link cross section, amplifies it and sends the amplified signal to a later cross section of the link. The greater the power that can be supported by the fiber, the further the signal can transmit through the optical fiber before amplification is required. Thus, the maximum power carried by the optical fiber determines the spacing of the repeaters. However, the maximum power carried by the fiber is limited by the intensity which depends on the nonlinear optical effects which can degrade the signal quality. Larger core regions allow for increased power for a given intensity. The maximum fiber core area that can be used to achieve a single propagation mode limits the repeater spacing to a minimum.
    For the discovery criteria, the repeater spacing for standard fibers is 30 km (O. Audouin et al., IEEE Photonics Techonolgy Letters (1995) pp. 1363-1365). Using large core photonic crystal fibers with a fiber core diameter of approximately 50 μm to transmit radiation, repeater spacings as large as 160 km are sufficient (presuming attenuation of power in photonic crystal fibers and conventional fibers is estimated. similar). Thus, transmission of optical signals can be achieved over large distances using photonic crystal fibers, which are more convenient and less expensive. In addition, large core photonic crystal fibers eliminate the need for repeaters for optical fiber links over distance, where repeaters are required when using the prior art.
    Referring to FIG. 4, large core photonic crystal fibers are used in fiber amplifier systems. The large core photonic crystal amplifier includes the length of the fiber 4 having a core (not shown) doped with a small amount of dopant material such as erbium. The fiber amplifier includes a wavelength selective coupler (WSC) 12 and a pump radiation source 13 for radiating pump radiation 14. The pump radiation 14 has a shorter wavelength compared to the input radiation 10 and is led through the WSC 12 to one end of the length of the optical fiber 4. The input signal radiation 10 from the radiation source 11, or the previous length of the optical fiber, is input to the length of the optical fiber 4 on the opposite side.
    The purpose of the WSC 12 is to insert radiation of one wavelength (ie pump wavelength) without transmitting radiation of another wavelength (ie input radiation wavelength). Thus, the pump radiation 14 is input along the same fiber 4 as the signal radiation 10 without sending any signal radiation 10 out of the fiber 4. The pump radiation 14 excites the dopant ions of the core of the fiber 4 and provides a benefit for the longer wavelength of the input radiation 10. Input radiation 10 is amplified. Wavelength sensing coupler 12 optionally transmits long wavelength input radiation, thus producing an amplified output signal 16. This output signal 16 is output through the length of the optical fiber 15.
    Typically, available wavelength selective couplers include the length of the input and rule force fibers, which input fibers are conventionally doped fibers (as in FIG. 1). In the large core photonic crystal fiber amplification shown in FIG. 4, it is preferable to include only large core photonic crystal fibers in order to avoid loss of intensity when the signal is inputted and outputted to the WSC 12.
    WSC 12 is any fiber device, such as a fused coupler, or any fiber directional coupler device with a wavelength dependent response. Optionally, FIG. 5 shows an optical device 17 that can be used as the wavelength selection coupler. For example, the optical device includes input and output lenses 18a and 18b and a dichroic mirror 19, respectively. The mirror 19 is angled such that it reflects the pump radiation 14 towards the input lens 18a and transmits the input signal radiation 10.
    In a fiber amplifier containing a step index optical fiber (as shown in FIG. 1) having a core diameter of 20 μm, which represents a limitation of the conventional technique of transmitting pulsed radiation having a pulse length of 1 ns, a peak power of 100 kW is achieved. (P. Nouchi et al., Proc. Conference on optical fiber communication (1995) pp. 260-261). Using the photonic crystal fiber amplifier shown in FIG. 4 in which the optical fiber 4 has a core diameter of approximately 50 μm, pulse radiation having a 1 ns pulse and a peak power of at least 600 kW is transmitted.
    Another application of large core photonic crystal fibers is fiber lasers. Although there are many other structures of fiber lasers in which large core photonic crystal fibers are used, two possible structures of fiber lasers are shown in FIGS. 6 and 7. For example, large core photonic crystal fibers are used in ring resonator fiber lasers, where the ends of the fibers are joined together such that laser radiation is transmitted around the “ring” of the fiber and continuously amplified.
    Referring to FIG. 6, a fiber laser capable of outputting high power radiation includes a large core photonic crystal fiber 4 length having a small amount of dopant material such as erbium in the core region (not shown). The fiber laser comprises two dichroic mirrors, an input mirror 22 and an output mirror 23 on either side of the fiber 4. Radiation 24 from the source of the pump radiation 25 (eg a laser) is input through the input mirror 22. This creates a gain in the doped fiber region 4 between the mirrors 22, 23 by exciting the erbium ions of the fiber core. Any radiation from the excited erbium ions produces a small amount of signal radiation in the fiber 4 (not shown in the fiber) having a wavelength longer than the pump radiation 24. This signal radiation is amplified and reflected by the mirrors 22 and 23 as it returns back and moves forward along the fiber.
    Typically, the dichroic mirror 22 is designed to reflect approximately 99% of the signal radiation during transmission of the pump radiation 24 and the output dichroic mirror 23 is adapted to reflect approximately 80% of the laser radiation. Is designed. Thus, at each time the signal radiation will be reflected at the output mirror 23 and a portion will radiate as the output signal 25.
    Fiber lasers are needed when providing a source of laser radiation in the form of fibers that can easily be coupled to later lengths of optical fibers. Due to the high power capacity of the large core photonic crystal fibers, more powerful fiber laser power can be more achieved using conventional optical fibers.
    With reference to FIG. 7, another structure of the fiber laser may include a fiber grating 26 having the function of a dichroic mirror (FIG. 8). This structure has advantages in all fiber devices. There are many structures of fiber lasers in which large core photonic crystal fibers are included and the use of the fibers in the device is not intended to be limited to the two illustrated embodiments. In another embodiment, a large core photonic crystal fiber is used in a ring resonator fiber laser such that one end of the large core photonic crystal fiber is connected to the other and thus laser radiation is directed around the "ring" of the large core photonic crystal fiber. Pass continuously and amplify successively.
    Typically, large core photonic crystal fibers 94 can be made using repeated lamination and draw processes from a rod of fused silica as shown in FIG. 8 (JC Knight et al., Opt. 21 (1996) p. 1547. Errata: Opt.Lett 22 (1997) p. 484). FIG. 8A shows a cylindrical rod of fused silica 27 with a hole 6 (FIG. 8B) drilled centrally along the length of the rod 8. Six plates are milled on the outside of the rod at an angular distance from the hole and provide a rod 27 of hexagonal cross section near the central hole 6. The rod 27 is pulled into a cane 28 using a fiber drawing tower and cut to the required length. The canes 28 are stacked to form a hexagonal cane array as shown in FIG. 8C, which forms the fibers 4. At the center of the array the kane has no holes lifted through the center and forms the core 7 of the fiber 4. Kane's complex stack is pulled down to the final fiber using a fiber drawing tower.
    Other fabrication techniques can be used if cylindrical silica capillaries are used and they can be used as basic fiber elements (ie, capillaries having the form of Kane 28). The need for hole drilling and milling steps in the above-mentioned stack draw process is eliminated.
    The fiber 4 comprises a first cladding material that is substantially transparent and can be stretched into a fiber (as shown in FIG. 8B). The core material is any material that is substantially transparent but need not be the same material as the first cladding material. Preferably, the refractive index of the first cladding material is smaller than the core material.
    The hole 6 may be filled with empty or any material, a second cladding material which has a refractive index smaller than the first cladding material and can be stretched into fibers, or any material that can be inserted into the hole when stretched to a smaller size. have. For example, the holes may be air or other gases (eg hydrogen or hydrocarbons), solid materials (eg other glass materials with a different refractive index than the first cladding material) or liquids (eg water, aqueous solutions). Or a dye solution). The second cladding material in the hole does not necessarily need to be transparent. As is apparent from the above description, "hole" is not limited to meaning a member area in the first cladding material.
    If the air hole diameter of the fiber is a sufficiently small portion of the pitch or spacing between the holes, the fiber core is guided in a single mode. Preferably, the diameter of the air holes is not smaller than the wavelength of light to be led into the fiber. The spacing between the holes is not less than 1/4 of the core diameter and no greater than 1/2 of the core diameter. Typically, the spacing between the holes is one half of the core diameter.
    The first cladding material and the core have a uniform refractive index or have a variable refractive index. For example, not only the center hole of the array is empty, or holes smaller or larger than other holes may be empty or filled with other materials. The core 7 is doped with a dopant material, for example of erbium or rare earth oxide elements, as in the fiber laser device shown in FIGS. 6 and 7.
    9 shows an SEM image of the central region in the cross section of the cleaved PCF. The central hole was empty leaving a core having a diameter of 22 μm bounded by the innermost 6 holes. The fiber is 180 μm and the associated hole size (d / Λ) is 0.12. FIG. 10 shows the near field pattern at the output of the large core PCF shown in FIG. 9 for incident light of wavelength 458 nm. The image is saturated at the center of the pattern to show weaker features at the edges. The perimeter of the pattern is concave when adjacent to the six innermost air holes.
    Light at a wavelength of 458 nm starts off into the fiber and an index matching fluid is applied to the structure to strip the cladding mode. The output is observed when the starting conditions vary. Many modes are not excited in the near field pattern and the PCF output as shown in FIG. 5 is not affected. Although the core diameter is 50 times the incident light wavelength, the fiber remains in a single mode. This ratio results in a wavelength of 1550 nm, and similar PCFs with a core diameter of 75 μm are single mode.
    The action of the large core photonic crystal fibers of the present invention is understood in terms of the effective refractive index n 2 of the cladding 5 at different wavelengths. 11A and 11B show the near field distribution at the end face 28 of the photonic crystal fiber 4, where the core material 7 and the first cladding material are silica and the holes 6 are airborne. Is charged.
    Referring to FIG. 11B, at long wavelengths (eg, 1500 nm), the strong transmission through the optical fiber 4 poorly magnetizes the array of holes (FIG. 3B) and thus some of the light proceeds to the air holes 6. do. The effective refractive index of the cladding material 5, for example silica and air cladding material 5, is reduced compared to the refractive index of pure silica n 1 (ie the refractive index of core 7). With reference to FIG. 11, the light traveling along the fiber 4 at short wavelengths (eg 600 nm) clearly images the array of holes 6 and does not substantially travel through the holes. The effective refractive index n 2 of the silica cladding 5 surrounding the core 7 is closer to pure silica (ie the refractive index of core 7) n 1 .
    Thus, referring again to Equation 1, when the wavelength of light traveling through the fiber 4 is reduced, the V value is apparently increased in accordance with the wavelength [lambda]. This increase is a factor Partially compensated by the reduction of n 1 and n 2 are the effective refractive index of the silica cladding and the refractive index of pure silica (and core 7). This makes the V value less dependent on wavelength, thus making the possible extended wavelength range where V is below the threshold for multimode guidance to the structure.
    The wavelength dependence of V is not only reduced but also completely out of the limits of the short wavelength. This is shown in FIG. 12, which shows an effective V value (V eff ) graph of the fiber when the ratio of hole pitch Λ to wavelength λ varies . Each curve corresponds to the diameter d ratio of the hole 6 to the pitch Λ. The V eff -d / Λ curve is calculated by first calculating the effective refractive index n 1 of the cladding material 5 and calculating V eff from Eq. The calculation assumes that the radius of the core 7 is equal to the pitch Λ.
    FIG. 12 shows that for each ratio of d / Λ, when the ratio Λ / λ is infinity, the V is delimited above the value. This behavior contrasts with conventional step index fibers where V is infinity when r / λ is infinity. Unlike conventional step index fibers, large core photonic crystal fibers can be aqueous to be single mode for structures of any size. The fiber is in single mode for any value of the pitch Λ provided so that the ratio of d / Λ is fixed when d is the diameter of the hole 6.
    The properties of large core photonic crystal fibers are suitable for use in some applications, including applications as high power communication links, high power fiber amplifiers, and high power fiber lasers. Fibers are used to deliver large optical power for industrial applications such as laser processing, and mechanical applications.
    权利要求:
    Claims (31)
    [1" claim-type="Currently amended] In an optical fiber for transmitting radiation,
    A core comprising a substantially transparent core material, having a core refractive index n and a length l, the core having a core diameter of at least 5 μm; And
    A cladding region surrounding the core material length, the cladding region comprising a first cladding material that is substantially transparent and having a first refractive index, wherein the first cladding material that is substantially transparent is substantially periodic along the length of the fiber. A conventional array of holes, the holes having a second refractive index less than the first refractive index,
    Radiation for an optical fiber is transmitted along the length of the core material in single propagation mode.
    [2" claim-type="Currently amended] 2. The method of claim 1, wherein the holes have a diameter d, spaced apart by a pitch Λ, and the optical fiber has an input radiation wavelength for an arbitrary value of pitch Λ for a substantially fixed d / Λ. Fiber optics regardless of single mode.
    [3" claim-type="Currently amended] The optical fiber of claim 1, wherein the substantially transparent first cladding material has a refractive index no less than a core refractive index.
    [4" claim-type="Currently amended] The optical fiber of claim 1, wherein the core diameter is at least 10 μm.
    [5" claim-type="Currently amended] The optical fiber of claim 4 wherein the core diameter is at least 20 μm.
    [6" claim-type="Currently amended] The optical fiber of claim 1, wherein at least one array hole is empty to form an optical fiber core.
    [7" claim-type="Currently amended] The optical fiber of claim 1, wherein the substantially transparent first cladding material has a first uniform refractive index.
    [8" claim-type="Currently amended] The optical fiber of claim 1, wherein the core material has a substantially uniform core refractive index.
    [9" claim-type="Currently amended] The optical fiber of claim 1 wherein the core material and the substantially transparent first cladding material are the same.
    [10" claim-type="Currently amended] The optical fiber of claim 1 wherein the at least one core material and the substantially transparent first cladding material is silica.
    [11" claim-type="Currently amended] The optical fiber of claim 1, wherein the diameter of the hole is not smaller than the wavelength of light to be guided to the fiber.
    [12" claim-type="Currently amended] The optical fiber of claim 1, wherein the hole is empty.
    [13" claim-type="Currently amended] The optical fiber of claim 1 wherein the holes are filled with a second cladding material.
    [14" claim-type="Currently amended] The optical fiber of claim 13, wherein the second cladding material is air.
    [15" claim-type="Currently amended] The optical fiber of claim 13 wherein the second cladding material is a liquid.
    [16" claim-type="Currently amended] The optical fiber of claim 13 wherein the second cladding material is a substantially transparent material.
    [17" claim-type="Currently amended] The optical fiber of claim 1 wherein the substantially transparent core material comprises a dopant material.
    [18" claim-type="Currently amended] The optical fiber of claim 1, wherein the holes are arranged in a substantially hexagonal pattern.
    [19" claim-type="Currently amended] A fiber amplifier for amplifying signal radiation,
    A fiber length according to any one of claims 1 to 5 for receiving signal radiation of a selected wavelength and transmitting said input radiation along the length of the fiber, wherein said core material comprises a plate along a portion of the fiber. Contains the raw material,
    A radiation source for radiating pump radiation of another selected wavelength for input into an optical fiber length such that a portion of the doped core material amplifies signal radiation under the action of pump radiation, and
    And wavelength selective transmission means for selectively transmitting pump radiation over the length of the optical fiber and selectively outputting amplified signal radiation from the fiber amplifier.
    [20" claim-type="Currently amended] The method of claim 19, wherein the wavelength selective transmission means,
    Input and output lenses for radiation and focusing radiation, and
    And a dichroic mirror for selectively reflecting pump radiation into the optical fiber and selectively transmitting amplified signal radiation output from the fiber amplifier.
    [21" claim-type="Currently amended] 20. The fiber amplifier of claim 19 wherein the wavelength selective transmission means comprises a fiber directing coupler having a wavelength dependent response.
    [22" claim-type="Currently amended] 22. The fiber amplifier of any of claims 19-21, wherein the dopant material is rare earth oxide ions.
    [23" claim-type="Currently amended] The fiber amplifier of claim 22 wherein the rare earth oxide ions are erbium ions.
    [24" claim-type="Currently amended] In a fiber laser for outputting laser radiation,
    A fiber length according to any one of claims 1 to 5 for selectively transmitting laser radiation having a selected wavelength along a fiber length, wherein a portion of the length of the core material comprises a dopant material,
    A radiation source for radiating pump radiation of different selected wavelengths for input into the optical fiber length such that the doped core material amplifies the laser radiation under the action of the pump radiation,
    Wavelength selective transmission means for selectively transmitting pump radiation in the length of the optical fiber and selectively outputting the laser radiation amplified from the fiber laser, and
    And feedback means for selectively refeeding a portion of the amplified laser radiation such that the amplified laser radiation passes repeatedly along the optical fiber length and is further amplified.
    [25" claim-type="Currently amended] 25. The fiber laser of claim 24, wherein the dopant material comprises rare earth oxide ions.
    [26" claim-type="Currently amended] 27. The fiber laser of claim 25, wherein the rare earth oxide ions are erbium.
    [27" claim-type="Currently amended] 25. The apparatus of claim 24, wherein the wavelength selective transmission means and the feedback means comprise two dichroic mirrors, each dichroic mirror disposed at different locations along the length of the optical fiber, and the doped core material being two dichroic. Fiber laser placed between mirror positions.
    [28" claim-type="Currently amended] 25. The fiber laser of claim 24, wherein the feedback means and the wavelength selective transmission means comprise two fiber gratings formed at two locations along the optical fiber length such that the doped core material is disposed between the two fiber gratings.
    [29" claim-type="Currently amended] 25. The fiber laser of claim 24, wherein the feedback means comprises means for directing light radiating from one end of the length of the optical fiber having the doped core material to the other end of the optical fiber length.
    [30" claim-type="Currently amended] A system for transmitting radiation in a single propagation mode,
    Each fiber length in series to receive input radiation from the previous length of the fiber and transmit the output radiation to the subsequent length of the fiber in series, and each length maintain the radiation power transmitted by the fiber length above the predetermined power A system comprising a plurality of lengths of optical fibers according to any one of claims 1 to 5 arranged in series to be separated by amplifying means for amplifying the radiation output from the optical fiber lengths.
    [31" claim-type="Currently amended] 32. The system of claim 30, wherein said amplifying means comprises a fiber amplifier according to any of claims 19-23.
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    同族专利:
    公开号 | 公开日
    GB9929482D0|2000-02-09|
    US20020122644A1|2002-09-05|
    DE69827630T2|2005-12-22|
    EP1443347A2|2004-08-04|
    EP0991967A1|2000-04-12|
    CN1269020A|2000-10-04|
    JP2002506533A|2002-02-26|
    AU8116998A|1999-01-19|
    US6603912B2|2003-08-05|
    GB9713422D0|1997-08-27|
    EP1443347A3|2004-12-22|
    GB2341457B|2002-04-24|
    KR100509720B1|2005-08-26|
    CN1143147C|2004-03-24|
    GB2341457A|2000-03-15|
    DE69827630D1|2004-12-23|
    JP4593695B2|2010-12-08|
    GB2341457C|2002-04-24|
    EP0991967B1|2004-11-17|
    US6334019B1|2001-12-25|
    WO1999000685A1|1999-01-07|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    法律状态:
    1997-06-26|Priority to GB9713422A
    1997-06-26|Priority to GB9713422.5
    1998-06-17|Application filed by 스켈톤 에스. 알., 더 세크러터리 오브 스테이트 포 디펜스
    1998-06-17|Priority to PCT/GB1998/001782
    2001-02-26|Publication of KR20010014256A
    2005-08-26|Application granted
    2005-08-26|Publication of KR100509720B1
    优先权:
    申请号 | 申请日 | 专利标题
    GB9713422A|GB9713422D0|1997-06-26|1997-06-26|Single mode optical fibre|
    GB9713422.5|1997-06-26|
    PCT/GB1998/001782|WO1999000685A1|1997-06-26|1998-06-17|Single mode optical fibre|
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