OPTICAL RECEIVER AND OPTICAL AXIS ALIGNMENT METHOD THEREOF
20170237504 · 2017-08-17
Inventors
Cpc classification
H04B10/614
ELECTRICITY
International classification
Abstract
An optical receiver comprises a package provided with an input window; a polarization-maintaining optical fiber fixable to the input window; a polarization beam splitter, disposed on the package, for inputting light outputted from the polarization-maintaining optical fiber and outputting first output light and second output light having respective polarization directions different from each other; a beam splitter, disposed on the package, for splitting the first output light; a first light-receiving element, optically coupled to the beam splitter, having two light-receiving parts corresponding to two kinds of the output light split by the beam splitter; and a second light-receiving element, disposed on the package, for receiving the second output light.
Claims
1.-13. (canceled)
14. An optical axis alignment method of an optical receiver that comprises a package, first and second optical-electrical signal converters, and a polarization-maintaining optical fiber, the first and second optical-electrical signal converters being set within the package, the package having first and second input windows, the polarization-maintaining optical fiber being fixable to the second input window; the method comprising: a first step of adjusting an angle of the polarization-maintaining optical fiber at the second input window according to results of detection by the first and second optical-electrical signal converters; a second step of moving the polarization-maintaining optical fiber from the second input window and to the first input window while keeping the angle of the polarization-maintaining optical fiber; and a third step of aligning an optical axis of the polarization-maintaining optical fiber at the first input window while keeping the angle of the polarization-maintaining optical fiber.
15. The optical axis alignment method according to claim 14, wherein the first step of adjusting the angle of the polarization-maintaining optical fiber is carried out such that an amount of light received by the first optical-electrical signal converter is at least a first threshold while an amount of light received by the second optical-electrical signal converter is not greater than a second threshold.
16. The optical axis alignment method according to claim 15, wherein the package further includes a polarization beam splitter optically coupled with the second input window, the polarization beam splitter receiving light outputted from the polarization-maintaining optical fiber set in the second input window and outputs first output light as TE-polarized light that optically couples with the first optical-electrical signal converter and second output light as TM-polarized light that optically couples with the second optical-electrical signal converter; and wherein the first step of adjusting the polarization-maintaining fiber is carried out such that the TE-polarized light outputted from the polarization-maintaining optical fiber has an angle of polarization of 10° or less.
17. The optical axis alignment method according to claim 14, wherein the second step of moving the polarization-maintaining optical fiber from the second input window includes a step of sliding the polarization-maintaining optical fiber from the second input window to the first input window while keeping its angle.
18. The optical axis alignment method according to claim 14, wherein the first step of adjusting the angle of the polarization-maintaining optical fiber includes a step of inputting light provided from an external local oscillator into the polarization-maintaining optical fiber.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
[0041] In the following, embodiments of the present invention will be explained.
[0042]
[0043] The optical signal processing unit 20 includes a polarization beam splitter (PBS) 22, a beam splitter (BS) 24, a polarization rotator 26, optical hybrids(optical processing unit)28x, 28y, light-receiving units 30, and amplifiers 32 (amplifiers 32x, 32y illustrated in
[0044] The polarization beam splitter 22 splits signal light (SIGNAL) introduced by a single-mode optical fiber (SMF) 12 into X-polarized light and Y-polarized light which are orthogonal to each other. The X-polarized light enters the optical hybrid 28y on the Y side, while the Y-polarized light has its plane of polarization rotated 90° by the polarization rotator 26 so as to become X-polarized light, which then enters the optical hybrid 28x on the X side. For example, TM light and TE light may be used as the X-polarized light and Y-polarized light, respectively, or vice versa.
[0045] The beam splitter 24 splits local oscillator light (LO light) inputted by a polarization-maintaining optical fiber (PMF) 10 from an external local oscillator light source device 14 into X and Y sides. The local oscillator light (LO light) is preset to X-polarized light and enters the optical hybrids 28x, 28y on the X and Y sides.
[0046] Each of the optical hybrids 28x, 28y causes the incident signal light and local oscillator light to interfere with each other in the internal light circuit and outputs the resulting interference light from four ports. Each of the optical hybrids 28x, 28y may be constituted by a silica-based planar lightwave circuit (PLC), for example. The X-polarized signal light (SIGNAL) is combined with the local oscillator light (LO) in the optical hybrid 28x and then is split, into positive (p) and negative (n) in-phase I and quadrature Q components, which are outputted as four optical signals (X-Ip, X-In, X-Qp, X-Qn). the Y-polarized signal light is combined with the local oscillator light (LO light) in the optical hybrid 28y and then is split into positive (p) and negative (n) in-phase I and quadrature Q components, which are outputted as four optical signals (Y-Ip, Y-in, Y-Qp, Y-Qn).
[0047] The light-receiving elements 30 photoelectrically convert the interference light(information signal) outputted from the optical hybrids 28x, 28y into analog electric signals. Each light-receiving element. 30 includes a photodiode (PD), for example. The amplifiers 32 combine and amplify paired positive and negative components of electric signals outputted from the light-receiving elements 30. Each amplifier 32 includes a transimpedance amplifier (TIA), for example. The amplified electric signals are outputted from electric output terminals of the optical signal processing unit 20 and inputted to the electric signal processing unit 40.
[0048] In the electric signal processor 40, the analog-digital converters 42 convert the analog electric signals outputted from the optical signal processing unit 20 into digital signals by analog-digital conversion. The digital signal processor 44 subjects the converted digital signals to various kinds of signal processing such as signal demodulation. The foregoing processing can perform digital coherent communications.
First Embodiment
[0049]
[0050] As illustrated in
[0051] The polarization-maintaining optical fiber 10 is fixed to the first input window 52. The TE light emitted from the polarization-maintaining optical fiber 10 is converted into collimated light by a lens 86 within a lens holder 84 and then enters the polarization beam splitter 72 within the package 50. The light having advanced straight through the polarization beam splitter 72 becomes TE light, which is inputted to the beam splitter 24. The light reflected 90° by the polarization beam splitter 72 becomes TM light, which is inputted to the light-receiving element 74. The TE light emitted from the polarization-maintaining optical fiber 10 may have an angle of polarization of 10° or less, for example.
[0052] The light having advanced straight through the beam splitter 24 passes through the skew adjustment element 56x and is condensed by the collimator lens 60a, so as to enter the optical hybrid 28x on the X side. The structure indicated by signs 28x, 30x in the drawing is one integrating the optical hybrid 28x and light-receiving element 30x on the X side.
[0053] On the other hand, the light reflected 90° by the beam splitter 24 is reflected 90° again by the mirror 58y and then condensed by the collimator lens 60c, so as to enter the optical hybrid 28y on the Y side. The structure indicated by signs 28y, 30y in the drawing is one integrating the optical hybrid 28y and light-receiving element 30y on the Y side.
[0054] The single-mode optical fiber 12 is fixed to the second input window 54. The light emitted from the single-mode optical fiber 12 is converted into collimated light by a lens 83 within a lens holder 81 and then enters the polarization beam splitter 22 within the package 50. The light entering the polarization beam splitter 22 has random polarization directions (indicated by Rand). The light having advanced straight through the polarization beam splitter 22 becomes TE light, which passes through the skew adjustment element 56y and then is condensed by the collimator lens 60d, so as to enter the optical hybrid 28y on the Y side.
[0055] On the other hand, the light reflected 90° by the polarization beam splitter 22 once becomes TM light, but is converted into YE light by passing through the polarization rotator 26. It is reflected 90° again by the mirror 58x and then condensed by the collimator lens 60b, so as to enter the optical hybrid 28x on the X side.
[0056] Of the local oscillator light LO coming from the polarization-maintaining optical fiber 10, the part entering the Y-side optical hybrid 28y has an optical path length longer than that of the part entering the X-side optical hybrid 28x by the distance between the beam splitter 24 and the mirror 58y. Therefore, the skew adjustment clement 56x arranged on the X side delays the phase of light on the X side such that the local oscillator light has the same optical path length on the X and Y sides.
[0057] Of the signal light coming from the single-mode optical fiber 12, the part entering the X-side optical hybrid 28x has an optical path length longer than that of the part entering the Y-side optical hybrid 28y by the distance between the polarization beam splitter 22 and the mirror 58x. Therefore, the skew adjustment element 56y arranged on the Y side delays the phase of light on the Y side such that the signal light has the same optical path length on the X and Y sides. As the skew adjustment elements 56x, 56y, materials (e.g., glass) having a refractive index higher than that of air may be used.
[0058]
[0059] As illustrated in
[0060] Here, the ferrule 80 has degrees of freedom of adjustment in the Z, θ, and φ axes. The ferrule holder 82 and lens holder 84 have degrees of freedom of adjustment in the X and Y axes. Thus, the polarization-maintaining optical fiber 10 has various degrees of freedom of adjustment for fixing the same, whereby angular shifts may occur in the process of aligning the optical axis of the polarization-maintaining optical fiber 10.
[0061]
[0062] Next, as illustrated in
[0063]
[0064] In the first light-receiving element receiving the TE light, as illustrated in
[0065] In view of the foregoing, it is preferred for the angle of the polarization-maintaining, optical fiber 10 to be adjusted such as to maximize and minimize the PD currents (received light amounts) in the first and second light-receiving elements, respectively, thereby making the angular shift as small as possible. The angle of the polarization-maintaining optical fiber 10 may be adjusted such that the PD currents received light amounts) in the first and second light-receiving elements become at least a first threshold and not greater than a second threshold, respectively. The first and second thresholds may be predetermined fixed values or variable values which are changed as appropriate.
[0066] Letting θ(°) be the angular shift from the T E-polarized light, the transmittance of optical power is cos.sup.2θ and sin.sup.2θ for rectilinear light and reflected light, respectively. When θ=5, the transmittance of optical power is 0.99 and 0.01 for the rectilinear light. (cos.sup.2θ) and reflected light (sin.sup.2θ), respectively. When θ=10, the transmittance of optical power is 0.97 and 0.03 for the rectilinear light (cos.sup.2θ) and reflected light (sin.sup.2θ), respectively. When θ=20, the transmittance of optical power is 0.88 and 0.12 for the rectilinear light (cos.sup.2θ) and reflected light (sin.sup.2θ), respectively.
[0067] In the graph of
[0068] Referring to
[0069] The optical axis alignment of the polarization-maintaining optical fiber 10 in an optical receiver in accordance with a comparative example will now be studied.
[0070]
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[0072] When the position or angle of the polarization-maintaining optical fiber 10 shifts in the comparative example, light other than the TE-polarized component is cut off by the polarizer 160, whereby optical losses occur in the light-receiving elements 30x, 30y according to the magnitude of the angular shift. Specifically, letting θ(°) be the angular shift from the TE-polarized light, the transmittance of optical power is cos.sup.2θ. When θ=5, the transmittance of optical power is cos.sup.2θ=0.99. When θ=10, the transmittance of optical power is cos.sup.2θ=0.97. When θ=20, the transmittance of optical power is cos.sup.2θ=0.88. Thus, monitoring the light-receiving elements 30x, 30y makes it possible to detect shifts in the position or angle of the polarization-maintaining optical fiber. Adjusting, the position and angle of the polarization-maintaining optical fiber 10 such as to maximize the received light amounts (PD currents) in the light-receiving elements 30x, 30y can maximize the amount of TE light incident on the optical hybrid 28x.
[0073] However, as illustrated in
[0074] When the end face 11 of the polarization-maintaining optical fiber 10 is tilted as illustrated in
[0075] By contrast, the optical receiver in accordance with this embodiment can accurately calculate the magnitude of angular shift from the output ratio of PD currents in the first and second light-receiving elements. As a result, the angular shift at the time of adjustment can be reduced. For example, the angular shift, which is up to about 20° in the comparative example, can be suppressed to 10° or less in this embodiment. In terms of optical loss, it can greatly be improved from 12% in the comparative example to about 3% in this embodiment.
[0076] In view of the foregoing, the optical receiver and its optical axis alignment method in accordance with this embodiment can enhance the accuracy in optical axis alignment of the polarization-maintaining optical fiber 10.
Second Embodiment
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[0081] Next, the dummy element with the light regulation unit 90 is removed (step S34). Thereafter, the dummy element is replaced with the actual element (step S36). The steps S34 and S36 keep the angle of the polarization-maintaining optical fiber 10 determined by the step S32. After the mounting of the actual element is completed, optical axes of the actual elements of the polarization-maintaining optical fiber 10 are aligned (step S38). At this time, the position of the polarization-maintaining optical fiber 10 or the positions or angles of the other optical elements may be changed, but the angle of the polarization-maintaining optical fiber 10 is kept unchanged.
[0082] The optical receiver and its optical axis alignment method in accordance with the second embodiment, adjust the angle of the polarization-maintaining optical fiber 10 by using the dummy element at the time of assembling and replace the dummy element with the actual element while keeping the angle. This can suppress the angular shift in the polarization-maintaining optical fiber 10 and improve the accuracy in optical axis alignment as with the first embodiment.
[0083] The structure in accordance with the second embodiment finally removes the dummy light regulation unit including the polarization beam splitter 92 and thus can make the number of components smaller than that in the first embodiment, thereby cutting cost down. In the structure in accordance with the second embodiment, the first and second light-receiving elements 94, 96 are arranged equidistantly from the polarization beam splitter 92. This can reduce the difference in light-receiving sensitivity between two light-receiving elements 94, 96, thereby making it possible to detect the angular shift of the polarization-maintaining optical fiber 10 more accurately.
Third Embodiment
[0084]
[0085] As illustrated in
[0086] The TM light as the second output light from the polarization beam splitter 22 is inputted to the light-receiving element 30x by way of the polarization rotator 26, mirror 58x, and lens 60b. In this embodiment, the light-receiving element 30x functions as the second light-receiving element for receiving, the second output light.
[0087]
[0088] Next, as illustrated in
[0089] The optical receiver and its optical axis alignment method in accordance with the third embodiment can monitor the TE tight and TM light by utilizing the polarization beam splitter 22 and light-receiving elements 30x, 30y, which constitute an optical system on the signal light side. This can suppress the angular shift of the polarization-maintaining optical fiber 10 and improve the accuracy in optical axis alignment as with the first embodiment.
[0090] The structure in accordance with the third embodiment does not use constituents such as the light regulation unit 70 in the first embodiment and the dummy light regulation unit 90 in the second embodiment and thus can thither cut the manufacturing cost down as compared with the first and second embodiments.
[0091] While the first to third embodiments set forth TE light, as an example of the local oscillator light (LO) introduced from the polarization-maintaining optical fiber 10, TM light can be used in place of the TE light.
[0092] While embodiments of the present invention are explained in detail in the foregoing, the present invention is not limited to such specific embodiments but can be modified and altered within the scope of the gist thereof set forth in claims.