OPTICAL MODULES HAVING AN IMPROVED OPTICAL SIGNAL TO NOISE RATIO
Consistent with the present disclosure, a photonic integrated circuit (PIC) is provided that has 2 N channels (N being an integer). The PIC is optically coupled to N optical fibers, such that each of N polarization multiplexed optical signals are transmitted over a respective one of the N optical fibers. In another example, each of the N optical fibers supply a respective one of N polarization multiplexed optical signals to the PIC for coherent detection and processing. A multiplexer and demultiplexer may be omitted from the PIC, such that the optical signals are not combined on the PIC. As a result, the transmitted and received optical signals incur less loss and amplified spontaneous emission (ASE) noise. In addition, optical taps may be more readily employed on the PIC to measure outputs of the lasers, such as widely tunable lasers (WTLs), without crossing waveguides
This application is a continuation of and claims priority to U.S. patent application Ser. No. 15/814,346, filed Nov. 15, 2017, which claims priority to U.S. Provisional Patent Application No. 62/422,031, filed on Nov. 15, 2016, the contents of both of which are hereby incorporated by reference herein in their entirety.
BACKGROUNDWavelength division multiplexed (WDM) optical communication systems are known in which multiple optical signals, each having a different wavelength and each modulated to carrying a different data stream, are multiplexed or combined and transmitted on an optical fiber. At a receive end of the fiber, such optical signals are demultiplexed or separated, detected, and the data stream carried by each optical signal is recovered.
WDM optical communication systems including photonic integrated circuits (PICs) are also known. Such PICs, may include various optical devices integrated on a common semiconductor substrate. In a transmitter, such PICs may include lasers, modulators, and optical amplifiers, and an optical combiner or multiplexer, among other devices. At the receive end, the PICs may include optical amplifiers, a power splitter or demultiplexer, and, in the case of a coherent receiver, optical hybrid circuits.
Conventionally, prior to input to the multiplexer, each optical signal may be amplified by a corresponding optical amplifier on the PIC. Each optical amplifier, however, may output, in addition to the optical signal, so-called amplified spontaneous emission (ASE) light at wavelengths other than the optical signal wavelength. Such ASE light may include wavelengths that extend into and overlap with the optical signal wavelengths. When the WDM signal with ASE is provided to an erbium doped fiber amplifier, the optical signals, as well as the ASE may be amplified. Accordingly, ASE light may be a source of noise in WDM optical communication systems and cause errors in transmission. Such noise may contribute to a low launch optical signal to noise ratio (LOSNR) and a low OSNR in a received optical signal (ROSNR).
In addition, the multiplexer may introduce loss into each optical signal when such optical signals are combined. If the multiplexer, such as a power combiner, does not include spectral filtering, power loss may be incurred. Such power loss is typically a function of 1/N, where N is the number of optical signals supplied to the multiplexer. Power loss may result in an additional 1 to 2 dB of loss. Accordingly, an optical signal supplied to such multiplexers may incur a loss of 9-10 dB, but less or more loss may be observed depending on the number of optical signals that are combined by the multiplexer.
SUMMARYConsistent with an aspect of the present disclosure, the multiplexer and demultiplexer may be omitted, such that the optical signals are not combined on the PIC, and each optical signal is transmitted on a corresponding optical fiber coupled to the PIC.
Since the optical signals are not combined, ASE noise is significantly reduced. However, if optical multiplexing is desired, each amplified optical signal may be supplied to a corresponding filter that eliminates or substantially attenuates ASE light at wavelengths other than the optical signal wavelength. As a result, when such filtered optical signals are combined in the multiplexer, the ASE noise is substantially reduced in the output WDM signal compared to a WDM signal including unfiltered amplified optical signals. Since the resulting WDM optical signal has reduced ASE noise, simpler, less expensive erbium doped fiber amplifiers may be provided that do not require further filtering or spectral shaping to lower ASE. Moreover, erbium doped fiber amplifiers in the receiver may be omitted since optical signals supplied to the receiver have improved OSNR, and, therefore, less amplification may be required.
Further, since optical multiplexers often have a fixed number of inputs, by omitting such optical multiplexers, additional optical signals may be readily added by providing an additional fiber for each signal. Accordingly, optical communication systems consistent with an aspect of the present disclosure may scale more efficiently than those that include multiplexers or combiners with a fixed number of inputs. Moreover, by removing multiplexers and demultiplexers from the PIC, waveguides that route optical signals on the PIC may be laid out with fewer restrictions, so that such waveguides may have fewer bends and/or a reduced radius of curvature. Moreover, PIC layouts may be made more compact. In addition, optical taps may be more readily employed on the PIC to measure outputs of the lasers, such as widely tunable lasers (WTLs) without crossing waveguides. A novel wavelength locker (WLL) may thus be employed, as described below.
Consistent with a further aspect of the present disclosure, by omitting the multiplexer in the transmit side PICs and the splitter or demultiplexer in the receive side PICs, both transmit and receive PICs may have a simpler layout. Alternatively, additional functionality or circuits may be integrated into the PICs. For example, a receiver for tracking and locking wavelengths of each optical signal may be incorporated into both the transmit and receive PICs, as discussed in greater detail below. In addition, a transceiver PIC may be employed including both receiver devices (such as photodiodes and 90 degree optical hybrids) and transmitter devices (SOAs and modulators) on a common substrate. Such transceiver PICs may include a laser that is used both as a local oscillator and an optical source for the modulators. Alternatively, the transmit and receive portions of the transceiver PIC may include separate lasers.
The following detailed description of example implementations refers to the accompanying drawings. The same reference numbers in different drawings may identify the same or similar elements.
A driver circuit, which may be provided in an integrated circuit (such as one of ICs IC1 to IC8), which may include an application specific integrated circuit (ASIC) or a digital signal processor (DSP) may provide radio frequency (RF) drive signals corresponding to the transmitted data to modulators provided in channel Tx Ch 1 on the Tx PIC. The modulators may receive light from a widely tunable laser (WTL). In addition, the modulators may include Mach Zehnder (MZ) modulators (labeled IQ MZM in
A first MZ modulator of the first pair may modulate part of a first portion the received light from the first side S1 of the WTL in accordance with selected radio frequency (RF) drive signals to provide a first in-phase component of the modulated optical signal and the second MZ modulator of the pair may modulate another part of the first portion of the received light from the first side S1 of the WTL in accordance with other RF drive signals to provide a first quadrature component of the modulated optical signal. Similarly, light output from the second side S2, a second portion of the light output from the WTL, is modulated based on additional RF drive signals supplied to a second IQ MZM to provide second in-phase and quadrature components of another modulated optical in accordance with additional drive signals. As further shown in
Light output from both sides of the WTL has a transverse electric (TE) polarization. In order to further increase capacity of the transmitted optical signal and to minimize interference between the outputs of the IQ MZMs, light output from the first IQ MZM is supplied from the Tx PIC on respective waveguides WG that extend to an edge of substrate 1011. Such light may be directed toward a waveguide on a planar lightwave circuit (Tx PLC) by a pair of lenses L1 and L2 (such as silicon lenses) and an isolator provided between the lenses. Len L1 may be a collimating lens and lens L2 may be a focusing lens that focuses the optical signals onto corresponding waveguides in Tx Block 1 to n of the Tx PLC (planar light wave circuit) on substrate 1014.
Both the Tx PLC and the Tx PIC may be provided on a third substrate or Tx interposer, which may also include a substrate made of silicon or a dielectric, such as silicon dioxide. The PLC may include a substrate made of silicon or a dielectric, such as silicon dioxide, and the devices provided on the PLC may be silicon-based. For example, as shown in
The rotators shown in
The output of the Tx Block 1 may be provided to a variable optical attenuator (VOA) to selectively attenuate the received polarization multiplexed optical signal to have desired power level. Optical taps provided at the input and output of the VOA may be provided to tap off a small portion of the received light and supply such portions to corresponding photodiodes. The photodiodes, in turn, convert the received light portions to corresponding electrical signals which are fed to additional circuitry that can monitor the power, for example, of light input to and output from the VOA.
Thus,
As further shown in
Module 1010 further includes a second substrate 1014 having third N (N being equal to n above) waveguides WG3, each of which being optically coupled to a corresponding one of the first N waveguides WG1 via collimating lens L1, an isolator, and a focusing line L2. The third N waveguides WG3 are provided on second substrate 1020. In addition, fourth N waveguides WG4 are provided on substrate 1014. Each of fourth waveguides WG4 is optically coupled to a corresponding one of the second N waveguides WG2 via a corresponding collimating lens L1, an additional isolator, and a focusing lens L2. The fourth N waveguides WG4 are also provided on the second substrate.
Substrate 1014 may further include a plurality (N) polarization elements, such the rotators and associated polarization beam combiners (PBCs) shown in
In the example shown in
Each laser may be tunable. In one example, each of the N lasers is a widely tunable laser that is tunable over a 35 nm range of wavelengths between 1460 nm and 1625 nm. In another example, each of the N lasers is a widely tunable laser that is tunable over a 17.5 nm range of wavelengths between 1460 nm and 1625 nm. Alternatively, each laser may be a distributed feedback (DFB) laser that is tunable over a 2 nm range of wavelengths between 1460 nm and 1625 nm or a widely tunable laser having a grating.
As noted above, each of modulators MZM IQ may be a nested Mach-Zehnder modulator.
As further shown in
Phase adjuster 107-a may be provided to adjust a phase of light propagating in arm 106-a, and amplitude adjuster 107-b may be provided to adjust an amplitude or intensity of such light. Amplitude adjuster 107-b may be a variable optical attenuator, for example. Both phase adjuster 107-a and amplitude adjuster 107-b may be semiconductor devices having a p-i-n structure, for example. Electrode 107-c may be provided to apply an electric field to one or more portions of the waveguide that constitutes arm 107-a to thereby alter or change the refractive index of the waveguide. As a result, when the light propagating in arm 106-a combines in combiner 115 via with light propagating in arm 106-b, the combined optical signal may be phase and/or amplitude modulated in accordance with an I component of the modulated optical signal. Similarly, Mach-Zehnder modulator 112 supplies a component, but the output from modulator 112 is supplied to phase adjuster 109, which, in turn, adjusts the phase of the signal output from modulator 112 by 90 degrees. Accordingly, the output of phase adjuster 109 may be the Q component of the modulated optical. Both I and Q components are combined by combiner 131 and output as one of the first N modulated optical signal to one of waveguides WG1.
Returning to
As further shown in
Respective waveguide WG6 supplies a corresponding one of the rotated optical signals (N such signals) to a corresponding one of waveguides WG7 (inputs, for example) via collimating lens L3 and focusing lens L4. Similarly, respective waveguide WG5 supplies a corresponding one of the TE optical signals (N such signals) to a corresponding one of waveguides WG8 via another collimating lens L3 and another focusing lens L4.
Waveguides WG7 and WG8 (inputs of the RX PIC substrate) supplies respective optical signals to corresponding optical hybrid circuits, which in this example are 90 degree optical hybrid circuits. Each optical hybrid circuit receives first and second power split portion of light output from a side S of a local oscillator laser (WTL). The first and second power split portions are provided from first and second outputs, respectively, of a coupler or splitter coupled to side S of the local oscillator laser WTL.
The received optical signals from waveguides WG7 and WG8 are mixed with light from local oscillator lasers (WTL) in the optical hybrid circuits. The optical hybrids, in turn, supply groups of mixing products to groups of photodiodes. In the example shown in
The groups of photodiodes generate radio frequency (RF) signals that are fed to corresponding ones of integrated circuits (ICs) 1 to 8. The ICs may include known transimpedance amplifiers (TIAs), analog to digital converters (ADCs) and carrier recover circuitry.
In accordance with a further aspect of the present disclosure, a plurality of spot size converters or mode adapters may be provided as part of end portions of each of the above described waveguides. Such spot size converters are shown in
As further shown in
As noted above, by omitting the multiplexer and demultiplexer in modules 1010 and 1012, the advantages noted above may be achieved.
In the examples shown in
In
Optical signals output from the isolator may next be input to a tracking filter that is configured to filter light at wavelengths other than the optical signal wavelength in order to reduce ASE. That is the tracking filter, which may be tunable, has a bandpass that includes the wavelengths of one or more of the transmitted (i.e., modulated) optical signals. A VOA may then be provided to adjust the power of light output from the filter to a desired level and a monitoring tap (2%, for example) and photodiode may be provided at the output of the VOA. In each of the above examples, the attenuation of the VOAs may be adjusted based, at least in part, on the monitored power at the output of each such VOA.
As further shown in
The transceiver shown in
A second portion of the light output from the Align DFB may be supplied to a receiver including delay line interferometer including a splitter, a first waveguide having an optical length longer (i.e., a delay line) than a second waveguide, and 90 degree optical hybrid. The wavelength of each optical signal may be locked individually. That is, in order to lock the wavelength of light output from WTL1, the VOAs associated with each of remaining lasers WTL2 to WTLn are controlled to effectively block light supplied from such remaining lasers. Accordingly, a portion of light output from WTL1 via a tap provided between a first IQ MZM and an SOA is supplied to a VOA (for power adjustment) and a second tap as an input to the Delay Line Interferometer. The delay line in conjunction with the 90 degree optical hybrid and splitter may generate mixing products indicative of the difference in wavelength between the Align DFB light and the light output from WTL1. Such mixing products are sensed by photodiodes, which generate electrical signals that are subject to further processing to generate control signals for adjusting the wavelength of light output from WTL1 so that the difference between that wavelength and the wavelength of light output from the Align DFB is a desired value. At which point, the wavelength of the WTL1 light may be locked. In a similar fashion, VOAs shown in
The Delay Line Interferometer has a 25 GHz free spectral range (FSR), which is indicative of the of the capture range of the wavelength locker.
VOA monitoring optical taps and photodiodes, as shown in
Further, the polarization of the TE and TM components of each optical signal may be monitored and adjusted or calibrated with per polarization VOAs and SOAs.
MZ modulator control may be achieved by further modulating optical signals output from the modulators with a low frequency tone and detecting those tones to isolate the modulation of an optical signal having a particular wavelength. Based on such tone monitoring, the modulators bias point, for example, may be adjusted or controlled. Such control may be achieved on a per wavelength or per optical signal basis.
In greater detail,
Module 310 also includes a plurality of second optical waveguides WG2, each of which being optically coupled to a corresponding one of the second IQ MZMs and receiving a second portion of light supplied from side S2 of each WTL. Each of waveguides WG2 also extending to edge E1 of the TX PIC substrate and being optically coupled to a respective one of the second IQ MZMs.
A plurality of taps (tap 1 to tap n) are provided on the TX PIC substrate. Each of the plurality of taps supplying a power split portion of each of a first plurality of optical signals supplied by a corresponding one of the IQ MZMs coupled to a side S1 of a respective WTL. A plurality of variable optical attenuators (VOA 1 to VOA n) are also provided on the substrate, and each receives a corresponding one of the power split portions from a corresponding one of the taps (tap 1 to tap n). The outputs of each VOA are fed by a combiner or tap to a third waveguide WG3, which in turn supplies the VOA outputs to a receiver circuit.
As noted above, in operation, each VOA is controlled, such that one VOA at any given time is controlled to pass the power split portion of light it receives to the WG3 and on to the receiver circuit, so that the VOAs selectively pass such light to the receiver circuit. Based on an outputs of the receiver circuit, a control circuit may adjust the wavelength of each WTL, for example by adjusting the temperature of a heater adjacent each WTL.
As further noted above, an alignment laser may be provided that supplies light to an additional VOA that selectively supplies light to a splitter or coupler having a first output coupled to waveguide WG3 (and on to the receiver circuit) and a second output coupled to an athermal wavelength locker 312 via an optical path that traverses the TX PLC substrate. Wavelength locker 312 may include a beam splitter and associated first photodiode, Fabry-Perot (FP) etalon and a second photodiode to lock alignment DFB in a known manner. The wavelength of the alignment DFB laser serves as a reference for the wavelengths of light output from each of the WTLs. Although a coupler is shown for supplying power split portion of the light output form the alignment laser to wavelength locker 312 and the receiver circuit, it is understood that light from opposing sides of the alignment laser may be supplied to wavelength locker 312 and the receiver circuit, respectively.
The receiver circuit includes a delay line interferometer, which includes a splitter having first and second output coupled to first ends waveguides WG4 and WG5, respectively. Waveguide WG4 has a longer length than WG5 and thus constitutes a delay line. Second ends of waveguides WG4 and WG5 are coupled to input of a 90 degree hybrid, for example, which may include a multimode (MMI) coupler. The 90 degree optical hybrid has a plurality of outputs (four in this example), each of which be coupled to a respective photodiode, which may be provided on the Tx PIC substrate.
Variations in wavelength cause each photodiode the receive different amounts of light. Accordingly, by detecting the photocurrent generated by each photodiode in the control circuit, the wavelength of each WTL laser may be monitored and adjusted, as noted above.
As further shown in
In the example shown in
Further, light output (a first portion) from one side of each WTL in
In addition, a splitter may be provided to supply a portion of light output from ALN laser 2 on the pass through waveguide, for example, to a wavelength locker circuit (second control circuit) to control the wavelength of ALN laser 2 in a manner similar to that discussed above.
Turning to
Each VOA selectively supplies the third portion of light from each local oscillator WTL to a corresponding input of the multiplexer, and the multiplexer, in turn, provides the selected third portion to a receiver including a DLI interferometer and having structure similar to or the same as that described above for wavelength control. In the example shown in
Moreover, in the example shown in
Further, as in
In addition, a splitter may be provided to supply a portion of light output from ALN laser 2 on the pass through waveguide, for example, to a wavelength locker circuit (second control circuit) to control the wavelength of ALN laser 2 in a manner similar to that discussed above. Also, light from ALN laser 1 may be passed across the Rx PLC in a manner similar to that discussed above in connection with
In each of the above-described embodiment, the elements that provide the optical outputs of the TX PIC or provide optical inputs to the RX PIC are formed on a PLC substrate. Consistent with the present disclosure, free space optics (FSO) including lenses, polarization rotators, PBCs, PBSs, and isolators may be provided as bulk or individual devices which are not integrated on a substrate. Various FSO configurations will next be described with reference to
In
Further, in
Alternative package configurations are shown in
In greater detail, waveguides WG1 and WG2 as shown in
In a receive configuration, the optical signal flow described above may be reversed. For example, each of N polarization multiplexed optical signals may be input from a corresponding optical fiber in the SMF array, and each such signal may be supplied to a corresponding one of N lenses in the Fiber Lens Array. Each such lens, when configured to receive optical signals from the SMF array, collimates such optical signals and supplies the signals to Block 1. The splitter/combiner plate or component (e.g., a beam splitter or reflector) is configured to reflect TM polarized light (signal) or component of each polarization multiplexed optical signal while allowing the TE polarized light (signal) or component to pass to Array 1. The TM signal is reflected off of the mirror in Block 1 and directed toward the rotator of half wave plate, which rotates the polarization of the TM signal to have a TE polarization. The rotated optical signals are then fed to a corresponding one of N lenses Array2, and, as noted above, the received TE signals are supplied to a corresponding one of lenses in Array1.
Each lens in Array1 and Array2 is configured to focus, in this example, the received optical signals onto a corresponding one of the waveguides (WG) on the RX PIC, as described above in connection with
In the above example, each of the lenses in Array1 and Array2 is tilted relative to facet F1, for example. However, in the embodiment shown in
In addition, although a block is shown having bulk components, such as the half wave plate, isolator, and combiner splitter that rotate and combine each of the received optical signals, it is understood that individual polarization rotators, combiners and splitters may be provided on a channel by channel basis. For example, the individual polarization rotators, combiners, and splitters shown in
In addition, waveguides WG1 and WG2 may be provided perpendicular to the PIC facet, as shown in
In
In greater detail, waveguides WG1 and WG2 as shown in
A rotator in each block, such as a half wave plate, rotates the polarization of each TE's signal, such that each TE′ signal has a TM polarization. The rotated signal in each block is next provided to a mirror, which reflects the rotated signal to a combiner. The combiner in each block also receives a corresponding one of the TE signals, such that corresponding TE signal passes through the combiner, while the rotated TE′ signal (now TM) is reflected by the combiner, as shown in
An additional waveguide (WG (align)) may be provided to supply light for alignment of the PIC, PIC lens array, blocks, fiber lens array and fiber.
In a receive configuration, the optical signals propagate in the reverse direction relative to that described above to an RX PIC. Namely, each of N polarization multiplexed optical signals are supplied by a corresponding one of N optical fibers via a corresponding lens in the fiber lens array to a respective block. In the receive configuration, each lens in the fiber lens array collimates the received optical signal. The splitter in each block or grouping passes a respective one of the received TE polarized optical signals or components of the polarization multiplexed signal, but reflects the corresponding TM optical signal or component to the mirror, which directs the TM optical signal to the rotator or half waveplate in the block. The rotator, in turn rotates the polarization of the TM signal, such that the TM signal has a TE polarization and the rotated signal is directed to a corresponding one of waveguides WG2 as a TE's optical signal. The TE optical signal is supplied from the splitter and output to a corresponding one of waveguide TE. Both optical signals are then subject to mixing with local oscillator late, conversion to electrical signals and further processing, as discussed above.
In the above examples, the lenses provided in the PIC lens array and the Fiber Lens array may be attached to one another, be mounted on a support. Alternatively, the lenses may collectively be formed as a unitary in or integral unit, as shown in the figures above. In addition, the lenses may be provided as part of a complex lens.
In the above examples, N lasers are provided, and optical signals are supplied to N optical fibers. It is understood, however, the free space optics and PLC implementations discussed above may couple to more than N or less than N optical fibers. For example, additional optical fibers that do not carry optical signals may be provided as spare fibers to carry optical signals in the event of a fault in a working fiber or may be used in the event additional capacity is required. Accordingly, coupling to M optical fibers is also contemplated herein where is an integer less than N or greater than N.
A further embodiment of the present disclosure will next be described with reference to
If the PIC is an RX PIC, the same or similar connections DC and RF connections would be made. The transmission lines, however, may carry RF signals from the above-described photodiodes to the ASIC for further processing by, for example, transimpedance amplifiers, analog-to-digital conversion, and carrier recovery. As noted above, such photodiodes receive modulated optical signal mixed with local oscillator light from the optical hybrid circuits. The photodiodes may have a relative short length and may thus constitute lumped elements. Alternatively, the photodiodes may have a relative long length and constitute travelling wave elements, in which case, a termination impedance or resistance may be provided on or off the PIC, as noted above.
In one example, the PIC and the ASIC are flip chip bonded to interposer substrate. For ease of explanation, optical outputs of the PIC, the optical fibers, and the coupling to the optical fibers described above are not shown in
Other embodiments will be apparent to those skilled in the art from consideration of the specification. It is intended that the specification and examples be considered as exemplary only.
Claims
1. An optical device, comprising:
- a substrate;
- 2N inputs/outputs on the substrate, N being an integer, each of the 2N inputs/outputs including a respective one of 2N waveguides, each of the 2N waveguides carrying a respective one of 2N optical signals, each of the 2N optical signals including an in-phase component and a quadrature component, each of the 2N waveguides extending to an edge of the substrate;
- N lasers provided on the substrate;
- each of first N waveguides of the 2N waveguides being: (1) optically coupled to a respective one of the N lasers, each of the first N waveguides supplying a first portion of the light generated by a respective one of the N lasers, or (2) configured to supply a corresponding one of first N optical signals of the 2N optical signals, which is mixed with a first portion of the light generated by a respective one of the N lasers; and
- each of second N waveguides of the 2N waveguides being: (1) optically coupled to a respective one of the N lasers, each of the second N waveguides supplying a second portion of the light generated by a respective one of the N lasers, or (2) configured to supply a corresponding one of second N optical signals of the 2N optical signals, which is mixed with the second portion of the light generated by a respective one of the N lasers.
2. An optical device in accordance with claim 1, wherein the substrate is a first substrate, the optical device further including:
- a second substrate;
- third N waveguides, each of which being optically coupled to a corresponding one of the first N waveguides, the third N waveguides being provided on the second substrate;
- fourth N waveguides, each of which being optically coupled to a corresponding one of the second N waveguides, the fourth N waveguides being provided on the second substrate; and
- N polarization elements provided on the substrate, each of which having a first port optically coupled to a respective one of the third N waveguides, a second port optically coupled to a respective one of the fourth N waveguides, and a third port.
3. An optical device in accordance with claim 1, wherein the substrate includes one of a Group III-V material or silicon.
4. An optical device in accordance with claim 1, wherein the first portion of the light is supplied by a first side of a corresponding one of the N lasers and the second portion of the light generated by a second side of said corresponding one of the N lasers.
5. An optical device in accordance with claim 1, further including:
- N splitters on the substrate, each of which receiving the light output from a corresponding one of the N lasers, each of the N splitters having a first output that supplies the first portion of the light generated by a respective one of the N lasers and a second output that supplies the second portion of the light generated by said respective one of the N lasers.
6. An optical device in accordance with claim 1, wherein the light generated a respective one of the N lasers has a corresponding one of N wavelengths.
7. An optical device in accordance with claim 1, wherein each of the first N waveguides is coupled to a corresponding one of N optical amplifiers.
8. An optical device in accordance with claim 7, wherein each of the N optical amplifiers is provided on the substrate.
9. An optical device in accordance with claim 8, wherein each of the N amplifiers is a semiconductor optical amplifier.
10. An optical device in accordance with claim 1, wherein each of the N lasers is tunable.
11. An optical device in accordance with claim 1, further including:
- first N amplifiers and second N amplifiers, each of the first N waveguides is coupled to a corresponding one of the first N amplifiers, and each of the second N waveguides is coupled to a corresponding one of the second N amplifiers.
12. An optical device in accordance with claim 11, wherein each of the first N amplifiers is provided on the substrate and each of the second N amplifiers is provided on the substrate.
13. An optical device in accordance with claim 12, wherein each of the first N amplifiers and each of the second N amplifiers is a semiconductor optical amplifier.
14. An optical device in accordance with claim 1, further including a N optical taps, each of which being coupled to a respective one of the first N waveguides, each of the N taps has a first output that provides part of the light generated by a corresponding one of the N lasers and a second output that provides the first portion of the light generated by a respective one of the N lasers.
15. An optical device in accordance with claim 14, further including N photodiodes, each of which being coupled to a respective one of the first outputs of the N optical taps.
16. An optical device in accordance with claim 1, further including:
- first N optical taps, each of which being coupled to a respective one of the first N waveguides, each of the first N taps has a first output that provides a first part of the light generated by a corresponding one of the N lasers and a second output that provides the first portion of the light generated by a respective one of the N lasers; and
- second N optical taps, each of which being coupled to a respective one of the second N waveguides, each of the second N taps has a first output that provides a second part of the light generated by a corresponding one of the N lasers and a second output that provides the second portion of the light generated by a respective one of the N lasers.
17. An optical device in accordance with claim 16, further including:
- first N photodiodes, each of which being coupled to a respective one of the first outputs of the first N optical taps; and
- second N photodiodes, each of which being coupled to a respective one of the first outputs of the second N optical taps.
18. An optical device in accordance with claim 1, further including:
- N semiconductor optical amplifiers, each of which being coupled to a corresponding one of the first N waveguides; and
- N optical taps, each of which being coupled to an output of each of the N semiconductor optical amplifiers.
19. An optical device in accordance with claim 18, further including N photodiodes, each of which being coupled to a respective one of the N optical taps.
20. An optical device in accordance with claim 1, further including:
- first N semiconductor optical amplifiers, each of which being coupled to a corresponding one of the first N waveguides;
- second N optical amplifiers, each of which being coupled to a corresponding one of the second N waveguides;
- first N optical taps, each of which being coupled to an output of each of the first N semiconductor optical amplifiers;
- second N optical taps, each of which being coupled to an output of each of the second N semiconductor optical amplifiers;
- first N photodiodes, each of which being coupled to a respective one of the first N optical taps; and
- second N photodiodes, each of which being coupled to a respective one of the second N optical taps.
21. An optical device in accordance with claim 10, wherein each of the N lasers is a widely tunable laser that is tunable over a at least a 35 nm range of wavelengths between 1460 nm and 1625 nm.
22. An optical device in accordance with claim 10, wherein each of the N lasers is a widely tunable laser that is tunable over at least a 17.5 nm range of wavelengths between 1460 nm and 1625 nm.
23. An optical device in accordance with claim 1, wherein each of the N lasers is a distributed feedback (DFB) laser that is tunable over at least 2 nm range of wavelengths between 1460 nm and 1625 nm.
24. An optical device in accordance with claim 3, wherein the Group III-V material includes indium phosphide (InP) or gallium arsenide (GaAs).
25. An optical device in accordance with claim 1, wherein each of the N lasers is a widely tunable laser including a grating.
Type: Application
Filed: Nov 13, 2018
Publication Date: Mar 14, 2019
Inventors: Jeffrey T. Rahn (Sunnyvale, CA), Fred A. Kish (Palo Alto, CA), Michael Reffle (Center Valley, PA), Peter W. Evans (Mountain House, CA), Vikrant Lal (Sunnyvale, CA)
Application Number: 16/189,074