The present disclosure relates to an optical link for high-bandwidth transmission between integrated circuits, and in particular to a dispersion-free coherent optical link.
Modern AI computer systems are bottlenecked by GPU-to-memory bandwidth. This problem is compounded as the distances between chips increases because the achievable bandwidth density decreases. High-bandwidth memory (HBM) is typically placed close to compute application specific integrated circuits (ASICs) because the achievable bandwidth density of the latest-generation HBM achieves more than 800 Gbps/mm of bandwidth per chip edge shoreline. Unfortunately, the HBM electrical links can only reach a few millimeters. For farther reaches, and to access significantly higher quantities of memory, longer-reach electrical interfaces are limited to 400 Gbps/mm of shoreline density. A compute chip will tradeoff the quantity of memory that can be accessed with the total bandwidth to memory. The resulting bottleneck means the highest-bandwidth links are only available to a small amount of total memory due to physical limitations.
Optical links can solve the bottleneck by providing bandwidth densities that can exceed the 800 Gbps/mm short-reach electrical shoreline density while providing hundreds of meters of reach. For example, an optical link includes a local transmitter, optically coupled to a remote receiver via one or more optical fibers. A light source generates a plurality of optical wavelength channels, and a plurality of modulators generate a plurality of modulated optical channel signals. The remote receiver includes a demultiplexer for routing each channel to photodetectors. The optical links can achieve extremely high bandwidth densities, with up to 32 wavelength channels.
The drawback to this optical link architecture is that it is limited by receiver sensitivity and does not efficiently scale to a large number of wavelength channels, even with relatively optimistic insertion loss assumptions.
An object of the present disclosure is to provide an optical link between integrated circuit chips, e.g. memory or ASIC, with improved receiver sensitivity and a large bandwidth-density.
Accordingly, a first apparatus includes an optical link comprising:
In any of the aforementioned embodiments the receiver may be configured for cancelling frequency and phase differences between the second local oscillator signals and the plurality of modulated optical wavelength channels and/or suppressing interference from adjacent wavelength channels.
In any of the aforementioned embodiments the receiver may include analog circuitry with an analog optical-to-electrical bandwidth greater than a bandwidth of each optical wavelength channel but smaller than an optical frequency spacing between adjacent modulated optical wavelength channels, whereby the receiver only transmits the electrical signals that correspond to the modulated optical wavelength channels with a wavelength closest to a wavelength of the second local oscillator signals.
In any of the aforementioned embodiments the one or more multiplexers may be disposed before the plurality of modulators for combining the plurality of input optical signals into a combined laser signal;
In any of the aforementioned embodiments the one or more first splitters may comprise a plurality of LO splitters (233), each of the plurality of LO splitters (233) configured for splitting a respective one of the input optical signals into a plurality (2M) of optical signal portions, a first half of the plurality of optical signal portions forming the first local oscillator signals, and a second half of the plurality of optical signal portions transmitted to the plurality of modulators; and
In any of the aforementioned embodiments the local transmitter further comprises an interleaver configured for combining the plurality of modulated multi-wavelength optical signals onto a single optical fiber; and
In any of the aforementioned embodiments the one or more first splitters may comprise a plurality of first splitters, each one of the plurality of first splitters coupled between the light source and the multiplexer.
In any of the aforementioned embodiments the one or more first splitters may comprise a first splitter coupled between the second splitter and the plurality of modulators.
In any of the aforementioned embodiments the plurality of modulators may comprise a plurality of wavelength dependent modulators.
In any of the aforementioned embodiments the plurality of demultiplexers may comprise a plurality of wavelength dependent optical filters.
In any of the aforementioned embodiments each one of the plurality of optical hybrid mixers may comprise a 90° optical hybrid mixer configured for mixing one of the second local oscillator signals with one of the modulated optical wavelength channels producing in-phase (I+ and I−) and quadrature (Q+ and Q−) electrical signals; and
In any of the aforementioned embodiments the remote receiver may also comprise one or more polarization splitters configured for splitting each of the plurality of modulated multi-wavelength optical signals (18) into a respective first orthogonally polarized receiver signal portion and a respective second orthogonally polarized receiver signal portion;
According to a second apparatus an optical device comprises:
In any of the aforementioned embodiments the local receiver may be configured for cancelling frequency and phase differences between the first local oscillator signals and the second plurality of modulated optical wavelength channels and/or suppressing interference from adjacent wavelength channels.
In any of the aforementioned embodiments the local receiver may include analog circuitry with an analog optical-to-electrical bandwidth greater than a bandwidth of each of the second plurality of modulated optical wavelength channels but smaller than an optical frequency spacing between adjacent ones of the second plurality of modulated optical wavelength channels, whereby the local receiver transmits only electrical signals that correspond to the second modulated optical wavelength channels with a wavelength closest to a wavelength of the first local oscillator signals.
In any of the aforementioned embodiments the one or more multiplexers may be disposed before the plurality of modulators for combining the first plurality of input optical signals into a combined laser signal;
In any of the aforementioned embodiments the one or more first splitters may comprise a plurality of first splitters, each one of the plurality of first splitters coupled between the light source and the multiplexer.
In any of the aforementioned embodiments the plurality of modulators may comprise a plurality of wavelength dependent modulators; and wherein the plurality of demultiplexers may comprises a plurality of wavelength dependent optical filters.
In any of the aforementioned embodiments each one of the plurality of optical hybrid mixers may comprise a 90° optical hybrid mixer configured for mixing one of the second local oscillator signals with one of the modulated optical wavelength channels producing in-phase (I+ and I−) and quadrature (Q+ and Q−) electrical signals; and
In any of the aforementioned embodiments the local receiver may include one or more polarization splitters configured for splitting each of the second plurality of modulated multi-wavelength optical signals (18) into a respective first orthogonally polarized receiver signal portion and a respective second orthogonally polarized receiver signal portion;
Some example embodiments will be described in greater detail with reference to the accompanying drawings, wherein:
While the present teachings are described in conjunction with various embodiments and examples, it is not intended that the present teachings be limited to such embodiments. On the contrary, the present teachings encompass various alternatives and equivalents, as will be appreciated by those of skill in the art.
According to a first example embodiment, illustrated in
In some of the embodiments, each of the local receiver 4 and the remote receiver 7 may include a deinterleaver 23 for separating the plurality of multi-wavelength optical signals 181 to 18M onto a plurality of different receiver bus waveguides 24. Each receiver 4 and 7 comprises a demultiplexer, which in the illustrated example embodiment comprises a plurality of wavelength-dependent optical filters 261,1 to 26M,N, one for each optical wavelength in the multi-wavelength optical signal 181 to 18M, are coupled to each receiver bus waveguides 24 configured for separating (demultiplexing) each of the plurality of modulated optical wavelength channels 251,1 to 25M,N in each of the plurality of multi-wavelength optical signals 181 to 18M from each other and onto a respective optical waveguide 27.
Each optical waveguide 27 from each bus waveguide 24 is optically coupled to one of a plurality of 90° optical hybrid mixers 31 (only one shown). The multi-wavelength laser source 11 is also used as a local oscillator (LO) signal generator for generating a local oscillator (LO) signal 321 to 32N that is transmitted to each optical hybrid mixer 31 to be coherently mixed with an incoming RX signal, i.e. one of the modulated optical wavelength channels 251,1 to 25M,N. Each LO signal 321 to 32N and each corresponding RX signal, e.g. the modulated optical wavelength channels 251,1 to 25,N will be on different, but closely-spaced wavelengths and will produce an intradyne beat-signal after mixing in the 90° optical hybrid mixer 31 that produces In-phase (I+ and I−) and Quadrature (Q+ and Q−) signals, see
The LO signals 321 to 32N can be tapped from the local transmitter 3 and the remote transmitter 6 utilizing one or more LO splitters 33, which can be disposed at various locations in the local transmitter 3 and the remote transmitter 6, such as after each laser or the multi-wavelength laser in the light source 11, each LO splitter 33 may tap off one of the plurality (N) of optical wavelength channels 101 to 10N, as in
For the example embodiment of
A complex electrical amplifier 41, such as a transimpedance amplifier (TIA), is configured to perform a sum-of-squares operation. The desired output of the amplifier 41 is to sum the squares of the sum of the in-phase signals and the sum of the quadrature signals, i.e. (I++I−)2+(Q++Q−)2. Accordingly, the output channels of the optical hybrid mixer 31 produce an electrical output that contains no LO-RX beat frequency. In this way, the coherent optical link 1, 201, etc. is free of digital signal processors (“DSP-free”) since the novel nonlinear electrical amplifiers 41 in the local receivers 4 and 204, et al and the remote receivers and 7 and 207, et al are performing DSP functionality in the analog domain.
The link architecture enables an order-of-magnitude improvement in receiver sensitivity and bandwidth-density. Reserving some fraction of optical power that does not need to couple to a fiber, route through an optical network, and couple into another chip results in efficient & high-yield optical gain as well as excellent wavelength selectivity through coherent intradyne mixing.
In some embodiments, a 90° hybrid optical mixer 31 is used, in which each of the four outputs is connected to a respective photodetector: I+ photodetector 35, I− photodetector 36, Q+ photodetector 367 and Q− photodetector 38 for converting the plurality of modulated optical wavelength channels 25 to electrical signals. The I+ photodetector 35 and I− photodetector 36 currents are summed, as are the Q+ photodetector 37 and Q− photodetector 38 currents. The AC photocurrent generated by a mixing process in the 90° optical hybrid mixer 31 with the balanced photodetector pairs of photodetectors 34 and 35, and 36 and 37 and sinusoidal waveforms is approximately:
Where ILO and IRX are the RMS instantaneous DC photocurrent outputs of the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25M,N, and the LO signal 321 to 32N from the photodetector pairs 35/36 and 37/38, and Δω(t) and Δϕ(t) are the time-varying frequency and phase differences in the LO and RX optical frequencies and phases. For amplitude modulation, IRX will vary with time and so the output amplitude will be proportional to the square root amplitude of the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25N,M. One interesting phenomenon is that the sum of the squares of the cosine and sine terms from the output from the 90° hybrid mixer 31 should be linearly proportional to the amplitude of the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25N,M, like in a direct detect receiver, but with the added benefit of a multiplicative gain from the local oscillator signal 321 to 32N. In this way, the frequency and phase differences between the LO signal 321 to 32N and the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25N,M, can be effectively canceled with appropriate analog circuitry provided in the receivers 4, 7, 204, 207, etc. by selecting appropriate analog electrical bandwidths from input to output corresponding to the difference in optical wavelengths in wavelength channels 251,1 to 25N,M. As will be shown below, the mixing products of the LO signal 321 to 32N and the RX signal that result through the input of an optical mixer, such as a 90° hybrid mixer 31 or a 120° hybrid mixer 131, followed by photodetectors 35-38 or 135-137, create an electrical signal with a total bandwidth corresponding to the total bandwidth of the RX signal. The mixing products that results from the RX signal channel closest in optical wavelength to the LO wavelength will have the lowest electrical frequency, while the mixing products from all other RX signal channels and the LO wavelength will have higher electrical frequencies. By choosing the analog optical-to-electrical bandwidth of the analog circuitry in the receiver 2, 4, 102, 104 etc. appropriately, such as greater than the bandwidth of the RX signal but smaller than the optical frequency spacing between adjacent RX signal channels, the analog circuitry will effectively transmit only the electrical signal that corresponds to the RX signal with wavelength closest to the LO wavelength. The analog optical-to-electrical bandwidth of the receiver 2, 4, 102, 104 etc. is typically determined by the overall transfer function of the components within it: the optical transmission of the optical components, where present, e.g. the optical fibers 8, the polarization splitter 105, the deinterleavers 125, the filters 26, the photodetectors 35 to 38 and 135 to 137, the electrical amplifier 41, and any other electrical components that may follow the electrical interconnects following the output of the receiver 2, 4, 102, 104 etc. In practice, it is typical that the optical components have very wide bandwidths and that the dominant limitation on optical-to-electrical bandwidth will be principally determined by the electrical bandwidth of the electrical amplifier 41.
The sum of the squares of the 90° hybrid outputs are: (I++I−)2+(Q++Q−)2=64 ILOIRX(COS2(Δω(t)+Δϕ(t))+sin2(Δω(t)+Δϕ(t)))
Which then simplifies to: (I++I−)2+(Q++Q−)2=64 ILOIRX.
In another example embodiment, illustrated in
Each first demultiplexer 125a separates the first polarized multi-wavelength optical signal portion 18−1 into separate signals, each comprising a first polarized portion of a respective one of the modulated optical wavelength channels, e.g. 25−1,1 to 25−1.N, and each second demultiplexer 125b separates the second polarized multi-wavelength optical signal 18+1 into separate signals, each comprising a second polarized portion of a respective one of the modulated optical wavelength channels, e.g. 25+1,1 to 25+1,N Each of the first and second demultiplexers 125a and 125b includes a plurality of outputs (N), one for each of polarized portion of the modulated optical wavelength channels 251,1 to 251,N. Each of the plurality of outputs of the demultiplexers 125a and 125b is coupled to a respective 120° hybrid optical mixer 131, whereby each 120° hybrid optical mixer 131 receives the first and second polarized portions of a respective modulated optical wavelength channel 251,1 to 25M,N along with a LO signal 341 to 34N. The advantage of the 120° optical hybrid mixer 131 is that it enables a polarization-independent data signals incident on the local receiver 304 and the remote receiver 307.
The 120° hybrid optical mixer 131 has three outputs, each connected to a respective photodetector 135, 136 and 137, generating photocurrents I1, I2, and I3, respectively. The AC photocurrents I1, I2, and I3, generated by a mixing process in the 120° optical hybrid mixer 131 are calculated below, where rj(t) is the amplitude of the jth channel (in a WDM configuration with j channels):
Similar to the 120° hybrid case, the sum of the squares of the photodetector currents I1, I2, and I3, from photodetectors 135, 136, and 137, respectively, are below: (where f22(t) is the intensity one of the modulated optical wavelength channels 251,1 to 25M,N, foffset is the frequency offset between the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25M,N and the corresponding LO signal 321 to 32N:
In the case of the 120° hybrid mixer 131, it can be shown that if the frequency offset between the LO signal 321 to 32N and the RX signal, e.g. the modulated optical wavelength channels 251,1 to 25M,N is greater than the optical-to-electrical bandwidth of the photodetectors 135, 136 and 137, and the electrical amplifier (TIA) 141, then the spurious term r21(t)sin ϕ sin(4πfoffset(t)+ψ+π/6) can be suppressed, along with interference from adjacent wavelength channels r21(t)+r23(t)+2r1(t)r3(t)cos(4γfoffset(t)) using suitable circuitry provided in the electrical amplifier (TIA) 141. The “cancellation” in the circuitry is a result of the finite optical-to-electrical bandwidth of the receiver electronics. For example, the terms cos(Δω(t)) (as above) and cos(4πfoffset) will produce frequencies above the optical-to-electrical bandwidth of the receiver, e.g. receivers 4, 7, 104, 107, 204, 207 etc, and will thus be attenuated, assuming that the receiver optical-to-electrical bandwidth is less than the channel spacing of the modulated optical wavelength channels 251,1 to 25M,N.
Accordingly, the sum equals: 2/3 R2 ELO2 r22(t), where R is the responsivity of the photodetectors, ELO is the electric field intensity of the LO signal 341 to 34N, and r2 is optical intensity of one of the modulated optical wavelength channels 251,1 to 25M,N.
In any embodiment, either a 120° hybrid mixer 131 or a 90° hybrid mixer 31 followed by an electrical amplifier 141 or 41, respectively, sums the squares of the 4 outputs of the 90° hybrid mixer 31 or the 3 outputs of a 120° hybrid mixer 131.
Using a 120° optical hybrid mixer 131 or a 90° optical hybrid mixer 31 has the following advantages: (1) the amplitude of the received signal is amplified by the local oscillator signal 321 to 32N, (2) if multiple signals impinge on the optical hybrid mixer 31 or 131, as long as the channel-to-channel frequency spacing of each signal is greater than the receiver optical-to-electrical bandwidth, then the mixing products from the out-of-band signals are effectively filtered out. Thus, the use of a LO signal 321 to 32N, optical hybrid mixer 31 or 131, and sum-of-squares electrical amplifier 41 or 141 creates a very effective wavelength demultiplexer, (3) the use of the optical hybrid mixer 31 or 131 as a demultiplexer relaxes the demultiplexer requirements elsewhere in the silicon photonic circuits. For example, a first demultiplexer, e.g. 261,1 to 261,N or 125, can be used to split the incoming WDM signal, e.g. 181, between multiple optical hybrid mixers 31 or 131. Then, the optical hybrid mixer/LO/sum-of-squares amplifier 41 or 141 act as a second filter. The design of a demultiplexer without regard for optical crosstalk is superior to a similar design with improved crosstalk.
In other exemplary embodiments, illustrated in
For embodiments with an interleaver 21, the local receiver 404 and the remote receiver 407 include a deinterleaver 23 for separating the interleaved multiplexed modulated optical signals 181 to 18M onto separate output waveguides 24 coupled to different demultiplexers 1251 to 125M. The local receiver 404 and the remote receiver 405 include a plurality of demultiplexers 1251 to 125M configured for demultiplexing the multiplexed modulated optical signals 181 to 18M. Each demultiplexer 1251 to 125M has a plurality of outputs, e.g. M, which are each coupled to a 90° optical hybrid mixer 31 and amplifier 41, as hereinbefore described.
With reference to
With reference to
With reference to
The light source 11 may comprise an external fixed-wavelength laser with N wavelengths combined into one lane and split M-ways (N>=1, M>=1); an external fixed-wavelength laser with N wavelengths with multiplexing to occur on-chip; an external tunable-wavelength laser with N wavelengths combined into one lane and split M-ways (N>=1, M>=1); a comb laser with N wavelength comb lines as output; or an external tunable wavelength laser with N wavelengths with multiplexing to occur on-chip. Finally, in any of these cases, the light source 11 may be tunable. Tunability will alleviate the design of an on-chip demultiplexer for both the LO path as well as the signal path. It will also alleviate optical-to-electrical bandwidth requirements on the nonlinear sum-of-squares TIA.
The optical fibers 81 to 8M may comprise a polarization-maintaining fiber, a standard single mode fiber (SMF) or a multi-core fiber.
The demultiplexers 34 or 125 may comprise deinterleavers; ring resonator add-drop; multi-ring add-drop filters; cascaded Mach-Zehnders filters; arrayed waveguide gratings; echelle gratings; thin-film filters of arbitrary order; or any combination of the above cascaded in series or parallel with one another.
The modulator 17 and 117, may comprise resonant modulators on a common bus (such as single-ring, double-ring, multi-ring, Fabry-Perot, coupling modulators, multi-segment ring coupling modulators, and more). These resonant modulators require that the laser sources are multiplexed prior to the modulator or modulators not on a common bus, which may be one of many possible types in literature, such as any resonant modulator, Mach-Zehnder modulator, dual-nested Mach-Zehnder, resonantly-assisted Mach-Zehnder (not necessarily single-rings), Michelson modulators, and more.
The foregoing description of one or more example embodiments has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form disclosed. Many modifications and variations are possible in light of the above teaching. It is intended that the scope of the disclosure be limited not by this detailed description.
Number | Date | Country | |
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63608238 | Dec 2023 | US |