So the manner in which the above recited features of the present invention can be understood in detail, a more particular description of the invention, briefly summarized above, may be had by reference to embodiments, some of which are illustrated in the appended drawings. It is to be noted; however, the appended drawings illustrate only typical embodiments of this invention and are therefore not to be considered limiting of its scope, for the invention may admit to other equally effective embodiments.
Capacity of optical communication systems can be improved by launching WDM channels with a pair-wise orthogonal relationship. By selecting channel spacings and polarization states between the channels, spectral efficiency can be improved thereby providing larger system capacity. When receiving the optical channels, channel selectivity may be improved by nulling orthogonal channels adjacent to a selected channel of interest.
Referring to
The laser source 142 may provide the optical signal 150 at the nominal wavelength of the transmitter 140 (or some constant offset therefrom depending on the specific implementations of the modulators 144, 146 and 148). The amplitude modulator 146 may be configured to shape the power envelope of the optical signal 152 so as to provide a shaped optical signal 154. The amplitude modulator 146 may include shaping circuits that transform the clock signal input into a signal that drives the amplitude modulator 146 to achieve the desired shaped optical signal 154. The phase modulator 148 may respond to a clock signal input to generate a “chirped” output optical signal 134. The phase modulator 148 may impart an optical phase angle that is time varying, thereby imparting a frequency shift (and corresponding wavelength shift) to the output optical signal 134. The output optical signal 134 may be received by the multiplexer 132, multiplexed with other output optical signals at different wavelengths, and transmitted via the transmission path 106.
The transmitter 140 may be configured to launch output optical signals on multiple optical channels (e.g., on the transmission path 106) with a pair-wise orthogonal polarization relationship, as shown in
As a result of synchronous optical processing (e.g., amplitude and/or phase modulation), Fourier components or modulation sidebands may be generated around the wavelength of each of the optical channels. Each channel may include an upper modulation sideband and a lower modulation sideband. For example, channel 1 at wavelength λ1 has an upper sideband 202-1 higher than the wavelength λ1 and a lower sideband 204-1 lower than the wavelength λ1. Similarly, channel 2 at wavelength λ2 has an upper sideband 202-2 higher than the wavelength λ2 and a lower sideband 204-2 lower than the wavelength λ2. Accounting for the modulation sidebands, each channel may be associated with a range or band of wavelengths.
According to one embodiment, the channel spacing may be chosen such that the modulation sidebands do not overlap on the same polarization axis. Within the first subset of channels having the first polarization state, for example, the sidebands of adjacent optical channels do not overlap. For example, the upper sideband 202-1 associated with channel 1 does not overlap the lower sideband 204-3 associated with channel 3. Similarly, the sidebands of adjacent optical channels do not overlap within the second subset of channels having the second polarization state. For example, the upper sideband 202-2 associated with channel 2 does not overlap the lower sideband 204-4 associated with channel 4.
To ensure that the modulation sidebands do not overlap within each polarization axis, the channel spacing Δf (e.g., of channels 1, 2, 3, 4, . . . N) may based on an odd number of ½ B steps or increments where B is the line rate in gigabits per second (Gb/s). For example, in a 10 Gb/s (9.9533 Gb/s) system, forward error correction (FEC) coding may be used to provide a 12.3 Gb/s line rate. In such a system, the channel spacing may be calculated as Δf=1.5(12.3 GHz)=18.45 GHz. This results in a spectral efficiency of about (9.9533 Gb/s)/18.45 GHz=0.54(bits/s)/Hz. At a spectral efficiency of about 0.54 (bits/s)/Hz, 128 optical channels, each carrying 10 Gb/s, may be transmitted in a 19 nm bandwidth; or 256 channels, each carrying 10 Gb/s, may be transmitted in a 38 nm bandwidth, both of which fall within the Erbium C-band. Thus, spectral efficiencies may be increased in this example by selecting a channel spacing Δf of 1½ times the line rate B.
In terms of total power (i.e., without regard for polarization), the modulation sidebands of adjacent optical channels may overlap. The lower modulation sideband 204-2 associated with channel 2, for example, may overlap with the upper modulation sideband 202-1 associated with channel 1. Similarly, the lower modulation sideband 204-3 associated with channel 3 may overlap with the upper modulation sideband 202-2 associated with channel 2. Because of this overlap, the channels transmitted with a pair-wise orthogonal relationship may not be completely separated at the receiver using typical filtering techniques without causing some receiver impairments.
Referring to
The polarization control loop 312 may include a polarization controller 322, such as a waveplate or electro-optic polarization controller, a polarization beamsplitter 324, an optical-to-electrical converter 326, and a control circuit 328. An optical signal 302 received on the channel selected by the filter 310 is passed to the polarization controller 322, which rotates the optical signal before the polarization beamsplitter 324. The beamsplitter 324 splits the optical signal into first and second optical components 304, 306 having different polarization states. The polarization controller 322 should orient the received optical signal 302 such that the first optical component 304 has a polarization state generally aligned or consistent with the polarization state of the selected channel and the second optical component 306 has a polarization state generally aligned or consistent with the polarization state of an adjacent channel orthogonal to the selected channel.
The first optical component 304 includes the selected channel and is passed to an optical-to-electrical (O/E) converter 330 to convert the optical signal received on the selected channel into an electrical signal on a data path 308. After the O/E converter 330, the electrical signal may be coupled to conventional detection and decoding circuitry (not shown), as is known to those skilled in the art. The second optical component 306 is converted into an electrical signal by the O/E converter 326 and is passed to the control circuit 328. In response to the electrical signal, the control circuit 328 controls the polarization controller 322 such that the power of the second optical component 306 is maximized, thereby minimizing the power of the orthogonal polarization within the first optical component 304 including the selected channel. By minimizing the power of the orthogonal polarization within the first optical component 304, the polarization control loop 312 maximizes throughput to the data path because the selected channel is effectively separated from overlapping adjacent channels. As a result, the polarization control loop 312 essentially “nulls” the orthogonal channel(s) adjacent to the selected channel. As used herein, the term “null” refers to the minimizing of the power in the adjacent orthogonal channel but does not necessarily require the power to be minimized to zero.
Although the exemplary optical receiver 300 is configured to select one channel, additional receivers similar to the optical receiver 300 may be configured to select each channel within a plurality of multiple WDM channels. Those skilled in the art will also recognize that other implementations of the receiver 300 are possible. The filter 310, for example, may be implemented as part of a demultiplexer. The dispersion compensation may be performed in other locations within the receiver or outside of the receiver. Those skilled in the art will also recognize that the control circuit 328 may be implemented in hardware, software, firmware or any combination thereof.
Referring to
The polarization selecting unit 420 is configured to separate the optical signal 402 into the polarization states of the orthogonal channels. The polarization selecting unit 420 may include a polarization controller 422 and a polarization beam splitter 424. The polarization controller 422 rotates or orients the polarization of the optical signal 402 according to a control signal received from the control circuit 428. The polarization beam splitter 424 splits the optical signal into first and second optical components 460, 462 having different polarization states. The optical filters 440, 442 receive the first and second optical components 460, 462, respectively, and select adjacent channels (e.g., a channel at wavelength λ1 and a channel at wavelength λ2) within the respective optical components 460, 462.
The filter 440 may be, for example, an interference filter, fiber Bragg grating or other optical filter having a high transmission characteristic associated with a particular wavelength or band of wavelengths associated with one channel (e.g., channel 1 at wavelength λ1) and a high reflectivity characteristic associated with other wavelengths. Similarly, the filter 442 may be, for example, an interference filter, fiber Bragg grating or other optical filter having a high transmission characteristic associated with a wavelength or band of wavelengths associated with an adjacent channel (e.g., channel 2 at wavelength λ2) and a high reflectivity characteristic associated with other wavelengths.
Although one pair of filters 440, 442 may be used for two adjacent channels (e.g., at wavelengths λ1 and λ2), multiple pairs of filters (not shown) may be used for multiple pairs of adjacent channels (e.g., λ1 and λ2, λ3 and λ4, λ5 and λ6 . . . ). The system 400 may include 1×N couplers 430, 432 to provide the first and second optical components 460, 462, respectively, to the multiple pairs of filters (not shown) associated with the multiple pairs of adjacent channels.
The system 400 may include optical taps 470, 472 to tap a portion (e.g., about 5-10%) of respective filtered optical components 480, 482 associated with the selected adjacent channels (e.g., channels at wavelengths λ1 and λ2). The remaining portion of the filtered optical components 480, 482 associated with the adjacent channels is passed on for detection and decoding. The tapped portions of the filtered optical components 480, 482 are supplied to the respective optical-to-electrical (O/E) converters 450, 452. The O/E converters 450, 452 (e.g., photodectors) convert the filtered optical components 480, 482 to corresponding electrical signals 490, 492. The electrical signals 490, 492 from the O/E converters 450, 452 are supplied to the control circuit 428. The control circuit 428 may include, for example, a difference amplifier circuit that receives the electrical signals 490, 492 and produces an error signal 494 to control the polarization controller 422 such that the detected power of the two adjacent channels (e.g., channel 1 at λ1 and channel 2 at λ2) is maximized.
The error signal 494 will thus cause the polarization controller 422 to be oriented such that the optical components 460, 462 from the beamsplitter 424 have polarization states consistent with the first and second polarization states of the channels launched with the pair-wise orthogonal relationship. When the detected power of the two adjacent channels is maximized, for example, the beamsplitter 424 produces a first optical component 460 with a polarization state consistent with the polarization state of the odd channels on the ‘Y’ axis shown in
According to an alternative embodiment, a system for nulling adjacent orthogonal optical channels may control a polarization controller without converting the optical component(s) into an electrical signal. The wavelengths of adjacent channels (e.g., channels 1 and 2) within the optical component(s) may be detected (e.g., with an OSA) and the intensity difference between the adjacent channels may be determined. The polarization controller may be rotated or controlled (e.g., using hardware or software) such that the intensity difference between the adjacent channels is maximized.
Accordingly, an optical communication system, consistent with one aspect of the present invention, includes an optical transmitter configured to generate a plurality of optical channels with a pair-wise orthogonal relationship such that a first subset of the optical channels has a first polarization state and a second subset of the optical channels has a second polarization state orthogonal to the first polarization state. The optical transmitter is configured to generate the optical channels at different wavelengths and with a channel spacing such that modulation sidebands of adjacent optical channels do not overlap within each of the first and second subsets of optical channels and such that modulation sidebands of adjacent optical channels overlap within the plurality of optical channels. The optical communication system also comprises an optical receiver configured to receive at least some of the plurality of optical channels having the pair-wise orthogonal relationship, to select at least one channel of interest, and to detect an optical signal on the channel of interest. An optical transmission path may be coupled between the transmitter and the receiver.
Consistent with another aspect of the present invention, a system includes a polarization controller configured to receive an optical signal on at least one selected channel having a band of wavelengths and configured to orient a polarization of the optical signal. A polarization beamsplitter may be coupled to the polarization controller and configured to split the optical signal into first and second optical components having different polarization states. A control circuit may be coupled to the polarization controller and configured to control the polarization controller such that power of orthogonal channels adjacent to the selected channel in one of the optical components is minimized.
Consistent with a further aspect of the present invention, a method includes: receiving a plurality of optical channels having a plurality of associated wavelengths, the optical channels being generated with a pair-wise orthogonal relationship; selecting at least one channel of interest from the plurality of optical channels; minimizing power of the channels adjacent to and orthogonal to the at least one channel of interest; and detecting an optical signal on the at least one channel of interest.
While the foregoing is directed to embodiments of the present invention, other and further embodiments of the invention may be devised without departing from the basic scope thereof, and the scope thereof is determined by the claims that follow.