Abstract:
The invention relates to apparatus and methods for transforming a spatial mode of an optical signal. The apparatus includes an optical phase element for imparting a predetermined spatially selective phase delay to the optical signal, and a mask in optical communication with the optical phase element. The mask, in one embodiment, includes an optically attenuating region disposed in a predetermined spatial pattern. In one aspect of the invention, the optical signal is transformed from a first spatial mode to a second spatial mode. In another aspect of the invention, the mask includes an absorbing material arranged in a predetermined spatial pattern. In yet another aspect of the invention, the mask includes a scattering material arranged in a predetermined spatial pattern. The invention also relates to a method for transforming a spatial mode of an optical signal. The method includes the step of receiving the optical signal having a first spatial mode with an intensity distribution and a phase. The method further includes the steps of selectively spatially attenuating the intensity distribution of the first spatial mode of the optical signal, selectively spatially delaying the phase of the optical signal, and propagating the selectively spatially attenuated and delayed optical signal. The first spatial mode of the optical signal is substantially transformed into a second spatial mode.

Description:
FIELD OF THE INVENTION 
     The invention relates to optical communication systems, and more specifically, to devices and methods for selecting spatial modes in optical signals. 
     BACKGROUND OF THE INVENTION 
     Optical signals transmitted through an optical communication fiber are subject to chromatic dispersion, which limits the rate at which data can be transmitted between two points. One or more optical fibers having high negative dispersion, known as dispersion compensation fibers (DCFs) can be used to compensate for the dispersion effect of the communication fiber. Methods and apparatus relating to DCFs are described in pending U.S patent application Ser. Nos. 09/249,830, 09/248,969 and 09/249,920, each filed Feb. 12, 1999, whose contents are incorporated herein by reference and which are assigned to the assignee of this application. In one concept disclosed therein, in order to reduce the length of optical fiber necessary for such compensation and to compensate for the dispersion slope, it is desirable to transform the optical signal from a lower order spatial mode (e.g., LP 01 ) to a higher order spatial mode (e.g., LP 02 ) using a transverse spatial mode transformer before transmitting the optical signal through the DCF. The DCF has been designed to function optimally with a higher order spatial mode. The signal is then transformed back to a lower order spatial mode after exiting the DCF using another transverse spatial mode transformer. The performance of the dispersion compensation device is limited in part by energy lost in unwanted spatial modes resulting from impurities in the compensation fiber, fabrication tolerances in the transverse spatial mode transformers, and alignment of the device with respect to the communication fiber. 
     Uses for higher order spatial modes include special transmission fibers, such as the one described in pending U.S. Provisional Patent Application 60/121,321 filed Feb. 23, 1999. 
     The use of optical elements to produce an optical coordinate transformation has been discussed in the prior art. Two exemplary articles include Bryngdahl, O. “Geometrical Transformations in Optics.”  Journal of the Optical Society of America  (August 1974):1092-1099., and Davidson, N.; Fresem, A.A.; and Hasman, E. “Optical Coordinate Transformations.”  Applied Optics  (March 1992):1067. 
     U.S. Pat. No. 5,760,941 discloses an optical mask utilized as an amplitude mask, which allows certain spectral frequencies to pass. 
     U.S. Pat. No. 4,895,421 discloses the use of a mask to attenuate optical energy radiating from one of two lobes of the LP 11  spatial mode. This acts to assist in the detection of an on or off condition caused by the activation or deactivation of a pump signal. 
     However none of the above references teach a method for removing unwanted spatial modes remaining, or describe a profile for converting in a bi-directional manner spatial modes existing in an optical waveguide to a different spatial mode existing in another waveguide. 
     SUMMARY OF THE INVENTION 
     The invention relates to an apparatus for transforming a spatial mode of an optical signal. The apparatus includes an optical phase element for imparting a predetermined spatially selective phase delay to the optical signal, and a mask in optical communication with the optical phase element. The mask, in one embodiment, includes an optically attenuating region disposed in a predetermined spatial pattern. In another embodiment, the mask is integral with the phase element. In another embodiment, the phase element includes a calcium fluoride window. 
     The apparatus, in one embodiment, includes an optical element in optical communication with the optical phase element. The optical element can be a lens. In another embodiment, the lens is integral with the optical phase element. In another embodiment, the phase element is in optical communication with an optical waveguide. In still another embodiment, the phase element is in optical communication with a second optical waveguide. The apparatus, in another embodiment, includes an optical element disposed between the optical phase element and the optical waveguide. In still another embodiment, an optical element is disposed between the optical phase element and the second optical waveguide. 
     In one aspect of the invention, the optical signal is transformed from a first spatial mode to a second spatial mode. The first and second spatial modes, in other embodiments, are the LP 01  spatial mode or the LP 02  spatial mode. 
     In another aspect of the invention, the mask includes an absorbing material arranged in a predetermined spatial pattern. In yet another aspect of the invention, the mask includes a scattering material arranged in a predetermined spatial pattern. In one embodiment, the optically attenuating region includes a sharp profile. In other embodiments, the predetermined spatial pattern is coincident with a minimal energy point of the first or second spatial mode. 
     The invention also relates to a method for attenuating an undesired spatial mode in an optical mode transformer. The method includes the steps of receiving the optical signal having the undesired spatial mode with an intensity distribution, selectively spatially attenuating the intensity distribution of the undesired spatial mode, and propagating the selectively spatially attenuated optical signal. The undesired spatial mode is substantially removed from the optical signal. In one embodiment, the undesired spatial mode is the LP 01  spatial mode. In another embodiment, the undesired spatial mode is the LP 02  spatial mode. 
     The invention further relates to a method for transforming a spatial mode of an optical signal. The method includes the step of receiving the optical signal having a first spatial mode with an intensity distribution and a phase. The method further includes the steps of selectively spatially attenuating the intensity distribution of the first spatial mode of the optical signal, selectively spatially delaying the phase of the optical signal, and propagating the selectively spatially attenuated and delayed optical signal. The first spatial mode of the optical signal is substantially transformed into a second spatial mode. In other embodiments, the first and second spatial modes are the LP 01  spatial mode or the LP 02  spatial mode. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     This invention is pointed out with particularity in the appended claims. The above and further advantages of this invention may be better understood by referring to the following description taking in conjunction with the accompanying drawings, in which: 
     FIG. 1 illustrates one embodiment of a dispersion compensation device according to the present invention. 
     FIG. 2 is a functional diagram of one embodiment of the dispersion compensation device shown in FIG.  1 . 
     FIG. 3 illustrates one embodiment of a mode transformer constructed according to the present invention. 
     FIG. 4 illustrates the radial intensity distribution of the LP 01  spatial mode in an optical beam. 
     FIGS. 5 a  and  5   b  illustrate embodiments of an absorbing mask and a scattering mask, respectively, according to the present invention. 
     FIG. 6 illustrates the radial intensity distribution of the LP 02  spatial mode in an optical beam. 
     FIGS. 7 a  and  7   b  illustrate embodiments of an absorbing mask and a scattering mask, respectively, according to the present invention. 
     FIGS. 8 a  illustrates one embodiment of the radial profile of a first phase element according to the present invention. 
     FIG. 8 b  illustrates the normalized energy intensity of the desired and undesired energy in combination with the radial profile of a first phase element according to the present invention. 
     FIG. 9 a  illustrates one embodiment of the radial profile of a second phase element according to the present invention. 
     FIG. 9 b  illustrates the normalized energy intensity of the desired and undesired energy in combination with the radial profile of a second phase element according to the present invention. 
    
    
     DETAILED DESCRIPTION 
     The invention relates to a device for performing a transverse mode transformation of light energy from one spatial mode substantially completely to another spatial mode, while removing any undesired spatial modes. The device removes uncontrolled effects caused by aberration in the elements or misalignment and ellipticity from an optical signal, while maintaining a desired spatial mode. In one embodiment the device includes a mask having at least one absorbing region or one scattering region disposed in a low intensity region of the desired spatial mode. The mask attenuates energy in the low intensity region of the desired spatial mode. The degree of attenuation for each spatial mode is dependent on the spatial mode&#39;s cross-sectional intensity distribution with respect to the features of the absorbing mask. In another embodiment, the device includes a sharp transition at the end of one or more masks to scatter undesired energy. 
     FIG. 1 shows a block diagram of a dispersion compensation device  10  used to compensate for chromatic dispersion in communication optical fibers  12  and  16 . A spatial mode transformer  18  transforms substantially all of the energy from the LP 01  spatial mode of the signal in the first communication fiber  12  into higher order spatial mode (LP 02 ) utilized in a dispersion compensation fiber  14 . A second spatial mode transformer  20  transforms substantially all of the energy from the higher spatial order mode back to the LP 01  spatial mode for transmission through the second communication fiber  16 . 
     The description of the transformation is described below as being in the direction of converting LP 01  to the LP 02  spatial mode. It is to be understood that the elements can be designed to function in a bi-directional fashion by coordinate transformation, by numerical iterations, by a combination of these methods or any other method, with the same principles applied for converting the LP 02  spatial mode to the LP 01  spatial mode. The invention is described in relation to a specific higher order spatial mode, namely the LP 02  spatial mode, and a specific lower order spatial mode, namely the LP 01  spatial mode. However, this is not intended to be limiting in any way. In other embodiments, the invention is used to convert between any two or more spatial modes. The description of the transformation is described below in connection with one embodiment of a dispersion compensation management device. In other embodiments, the invention is utilized without a second device for retransformation to the original spatial mode, or for example, in combination with a transmission fiber as described in pending U.S. Provisional Patent Application 60/121,321. 
     FIG. 2 is a functional diagram of one embodiment of the device  10  of FIG. 1 indicating the coupling mechanism between two spatial modes. Splitters  22  and  24  represent spatial mode coupling at the spatial mode transformers  18  and  20 , respectively. After transformation, the dispersion compensation fiber  14  includes both the desired LP 02  spatial mode and unwanted spatial modes LP 01 , LP 11 , LP 21 , and LP 03 , which are shown traveling in separate paths in dispersion compensation fiber  14 . It is to be understood, however, that both paths exist in the single dispersion compensation fiber  14 , and interactions between the desired and undesired spatial modes shown as arrow  15 , and known as multipath interference (MPI), cause significant reduction in signal quality. Thus, it is desirable to implement a method for filtering out the unwanted spatial modes and aberrations resulting from the coupling, especially at the spatial mode transformers  18  and  20  of FIG.  1 . 
     FIG. 3 depicts one embodiment of a spatial mode transformer  18 ′ for efficiently transforming the LP 01  spatial mode to the LP 02  spatial mode while suppressing other undesired spatial modes from entering dispersion compensation fiber  14 . In this embodiment, the spatial mode transformer  18 ′ includes a lens  28  for collimating the optical output of the single mode fiber (SMF)  12 , a pair of phase elements  30  and  34  which selectively spatially delay the collimated beam  32  in one or more predetermined regions to cause a transformation from the LP 01  spatial mode to the LP 02  spatial mode, and a coupling lens  46  for transmitting the optical energy into a dispersion compensation fiber  14 . It is to be understood that the LP 01  and LP 02  spatial modes do not physically exist outside of the optical waveguide, however the field distribution, which is similar to these spatial modes is meant. Phase elements  30  and  34  are produced from any appropriate optical material, including but not limited to a calcium fluoride (CaF 2 ) window. In additional embodiments, lens  28  and lens  46  are physically combined with phase element  30  and  34 , respectively. Mask  36 , in one embodiment, is shown substantially attached to phase element  30 . In another embodiment, mask  36  is not attached to phase element  30  (not shown). Mask  36  attenuates selected spatial modes in collimated beam  32 . Mask  42 , in one embodiment, is shown substantially attached to phase element  34 . In another embodiment, mask  42  is not attached to phase element  34  (not shown). Mask  42  attenuates selected spatial modes in collimated beam  32 . Embodiments of masks  36  and  42  will be described in greater detail. 
     FIG. 4 depicts the radial intensity distribution of the desired LP 01  spatial mode at the first phase element  30 . There is negligible optical energy under the curve where the radius is greater than r c . Therefore, nearly all of the energy exists inside a radius r c . By introducing an absorbing or scattering mask which has high absorption or scattering in the area with radius greater than r c , spatial modes or spurious energies in this area are significantly attenuated and the attenuation of the LP 01  spatial mode is negligible. 
     FIG. 5 a  shows an absorbing mask  36  located on or near the first phase element  30  having an absorbing region  38  which has no significant influence on the desired LP 01  spatial mode but can substantially attenuate modes with energy outside a radius r c . In another embodiment of the invention, an absorbing material can be integrated into the phase element  30 . 
     FIG. 5 b  shows a scattering mask  36 ′ located on or near the first phase element  30  having a scattering region  38 ′ which also includes a surface profile having a sharp pattern for scattering a substantial portion of the optical energy in region  38 ′ out of the optical path. The region  38 ′ has no significant influence on the desired LP 01  spatial mode. The surface profile, in one embodiment, is part of the surface profile of the phase element  30 . Both absorbing mask  36  and scattering mask  36 ′ can be placed on either side of phase element  30 , and can be used together if desired. 
     FIG. 6 depicts the desired radial intensity distribution of the LP 02  spatial mode at the output of second phase element  34 . There is negligible optical energy in the cross-sectional areas  44  where the radius is approximately r a . Similarly, there is negligible optical energy in the cross-sectional area  46  whose radius is greater than r b . By introducing an absorbing mask or a phase element profile which has high absorption or scattering in areas  44  and  46 , spatial modes having significant energy in areas  44  and  46  are significantly attenuated while the attenuation of the LP 02  spatial mode is negligible. 
     FIG. 7 a  depicts the front view of an absorbing mask  42  located on or near the second phase element  34  having an absorbing ring  44  and an outer absorbing region  46 . The rejection of unwanted spatial modes is improved as the width Δr a  of the absorbing ring  44  is increased. Unfortunately, the desired spatial mode is also attenuated as the width Δr a  increases. As a result, the width Δr a  of the absorbing ring is typically limited by the acceptable attenuation loss (e.g., 0.2 dB or less) to the desired spatial mode. Outer absorbing ring  46  rejects unwanted energy, which can consist of errors in the transformation caused by inexactitude in the elements or their placement, as well as undesired modal energies. In one embodiment, absorbing ring  44  and absorbing ring  46  are constructed of an absorbing material. In one embodiment, phase elements  30  and  34  are produced by surface relief methods, such as diamond turning or photolithography. Integrating an absorbing material into the phase elements  30  and  34  requires implementation of an additional process and results in increased fabrication time and cost. 
     FIG. 7 b  shows mask  42 ′, which has high loss in scattering regions  44 ′ and  46 ′. These loss regions  44 ′ and  46 ′ include a sharp change in the surface profile, which scatters most of the optical energy in the regions  44 ′ and  46 ′ out of the optical path. Mask  42 ′ can, in different embodiments, be near, on, or substantially part of the surface profile of second phase element  34 . The rejection of unwanted spatial modes is improved as the width Δr a  of the scattering ring  44 ′ is increased. Unfortunately, the desired spatial mode is also attenuated as the width Δr a  increases. As a result, the width Δr a  of the scattering ring is typically limited by the acceptable attenuation loss (e.g., 0.2 dB or less) to the desired spatial mode. Outer scattering ring  46 ′ rejects unwanted energy which can consist of errors in the transformation caused by inexactitude in the elements or their placement, as well as undesired modal energies. Construction of a narrow sharp profile in the middle of a phase element requires a complex manufacturing process, whereas constructing a sharp profile at a radial section proceeding towards the outer limit of an element is, typically, more easily achieved. 
     It is to be understood that absorbing ring  44  can be combined on a single element with scattering ring  46 ′, or absorbing ring  46  with scattering ring  44 ′. In addition absorbing ring  46  or scattering ring  46 ′ can be utilized without absorbing ring  44  or scattering ring  44 ′ to achieve selectivity. Conversely, absorbing ring  44  or scattering ring  44 ′ can be utilized without absorbing ring  46  or scattering ring  46 ′. Furthermore, rings  46 ,  46 ′,  44  and  44 ′ can each be placed on, near or as part of either side of second phase element  34 . Absorbing ring  44 , in another embodiment, is used in combination with scattering ring  44 ′. In yet another embodiment, absorbing ring  46  is used in combination with scattering ring  46 ′. 
     By integrating the two absorbing masks  36  and  42 , or scattering masks  36 ′ and  42 ′ or any combination of the masks, with their respective phase elements  30  and  34 , a spatial mode transformer  18  having significant mode selectivity is realized. In addition, the spatial mode transformer  18  has reduced sensitivity to variations and distortions of the phase elements  30  and  34 . Thus, noise due to interference caused by undesired spatial modes, uncontrolled energy at the ends, aberrations in the elements, misalignment and any ellipticity is minimized. It is to be understood that mask  36 ,  36 ′,  42  or  42 ′ can also be used alone to achieve significant mode selectivity. 
     In one embodiment, the absorbing masks  36  and  42  are partially absorbing. The absorption varies spatially according to a predetermined mode selectivity. In another embodiment, the absorption is replaced by random phase distortion (i.e., optical diffusion) in the absorbing regions  38 ,  44  and  46 . The absorbing masks can be implemented in other spatial mode transformers having any number of optical phase elements. 
     Referring to FIG. 8 a , therein is shown a graph of surface profile  50  of phase element  30  of FIG.  3 . One embodiment of mask  38 ′ of FIG. 5 b  is also shown as scattering profile  54 . The X-axis represents the radial distance in microns of the phase element, and the Y-axis represents the depth in microns. The fixed portion of the phase element is not shown for clarity. The profile is designed as part of a system to convert the energy from one spatial mode, for example, the LP 01  spatial mode, to a second spatial mode, for example, the LP 02  spatial mode, for transmission into a dispersion compensation fiber. The surface profile  50  of phase element  30  is designed to operate in combination with second phase element  34  of FIG. 3, which is typically at a distance on the order of the Rayleigh range, and preferably less than the Rayleigh range to complete the conversion between spatial modes with very high efficiency. The exact profile is a function of the actual LP 02  spatial mode cross sectional profile of dispersion compensation fiber  14 , the actual LP 01  spatial mode cross sectional profile of single mode fiber (SMF)  16 , the distances between the elements, and the exact profile of the collimating lenses. Once the above factors are known, the exact profile is chosen in a manner known to those skilled in the art so as to steer the energy from the input spatial mode to the desired output spatial mode. This is accomplished by analytic coordinate transformation, by an iterative numerical process, by a combination of these processes, or by any other method known to those skilled in the art. 
     Referring now to FIG. 8 b , therein is shown a graph of the normalized energy intensity superimposed on the phase element  30 . It should be noted that the Y-axis of the graph in FIG. 8 b  is a mixture of both normalized energy intensity and depth of the lens used, and the X-axis represents the lens radius. Curve  58  represents undesired energy, which will be reshaped and directed by the shape of the element, line  54  represents the profile of element  30 , and line  56  represents energy of the desired spatial mode. It should be noted that curves  56  and  58  are independently normalized and do not represent similar energy levels. Since the input spatial mode is the LP 01  spatial mode, which as mentioned above can be the output of the transformer in reverse operation, a sharp change  60  in profile is constructed towards the outer part of the lens, at a point where the LP 01  spatial mode has relatively low energy. The effect of the sharp change  60  in profile is to scatter all optical energy located in the area of the sharp change  60 . Scattering in this region is useful to compensate for misalignment of the optical elements as well as any ellipticity in the fibers, and is primarily functions to eliminate uncontrolled energy. In one embodiment, the technique of sharply changing the profile to scatter the energy could be used as an alternative to using a scattering or absorbing mask as depicted in FIG. 5 a.    
     FIG. 9 a  shows a graph of one embodiment of a surface profile of phase element  34  FIG.  3 . The X-axis represents the radial distance in microns of the phase element, and the Y-axis represents the depth in microns. The fixed portion of the phase element is not shown for clarity. The profile  62  of second phase change element is shown with a sharp discontinuity  64 , which causes the phase shift described in the aforementioned pending applications. The sharp profile  66  represents mask  46 ′ of FIG. 7 b , while the remainder of profile  62  functions to complete the steering of energy to the desired LP 02  spatial mode at the output of phase element  34 . The energy is focused by optical element  46  into dispersion compensating fiber  14 . In the reverse direction, optical element  46  collimates the optical energy received from dispersion compensating fiber  14 . 
     Referring now to FIG. 9 b , therein is shown a graph of the energy superimposed on the phase element  34 . It should be noted that the Y-axis of the graph in FIG. 12 is a mixture of both normalized energy intensity and the depth of the lens used. The X-axis represents the radius. Curve  66  represents the phase element profile. Curve  70  represents the desired energy in the LP 02  spatial mode, and curve  68  represents the undesired energy primarily in the LP 01  spatial mode. It should be noted that curves  68  and  70  are independently normalized and do not represent similar energy levels. Since the output spatial mode is the LP 02  spatial mode, which as mentioned above can be the input of the transformer in reverse operation, a sharp change  72  in profile is constructed towards the outer part of the lens, at a point where the undesired mode intensity is relatively low. The effect of the sharp change  72  in profile is to scatter all optical energy located in the area of the sharp change  72 . Scattering in this region is useful to compensate for misalignment of the optical elements as well as any ellipticity in the fibers, and is primarily functions to eliminate uncontrolled energy. In one embodiment, it is possible to avoid the use of masks such as depicted in FIG. 7 a , and instead use sharp profile changes to scatter the light energy. It is to be noted that ring  44  or  44 ′ are not shown in FIG. 9 b . Phase element discontinuity  74  functions to introduce a step function to the wavefront such that the center region of the wavefront is retarded with respect to the outer region of the wavefront. 
     Having described and shown the preferred embodiments of the invention, it will now become apparent to one of skill in the art that other embodiments incorporating the concepts may be used and that many variations are possible which will still be within the scope and spirit of the claimed invention. It is felt, therefore, that these embodiments should not be limited to disclosed embodiments but rather should be limited only by the spirit and scope of the following claims.