Patent Application
20240348333
The subject disclosure relates to a method and apparatus for wavelength diversity in free-space optical communications.
In the past decade, there has been a significant rise in the total number of satellites being launched into low-earth orbit (LEO) with the purpose of serving as nodes in a globe-spanning communications network. Leading companies are SpaceX, Amazon, and Telesat. These satellites have initially been provisioned with RF links, but in late 2022, have had their optical backbone links turned on.
The optical challenges associated with space-to-space links are somewhat less severe than optical links that traverse atmosphere due to the lack of atmospheric scintillation. It appears that satellite constellation operators are focused on bringing coherent pluggables into space to counteract high beam spread loss, boost data rate, and leverage a maturing market. It appears 100 Gb/s optical links is the primary focus for near-future deployment.
There are other purely space-based applications, specifically NASA's Laser Communications Relay Demonstration (LCRD) is intended to scope out a possible laser relay system from geosynchronous satellites to the moon and beyond (spacecraft launched further into the solar system).
Recently, several companies such as Alphabet (Sonora, Loon), Meta (Aquila), and Lockheed Martin, have explored the use of optical links employed on high-altitude vehicles (HAVs) above the worst atmospheric turbulence. In some cases, the intended purpose is to mimic LEO satellite constellations to provide internet services to ground customers, with more flexible provisioning. Other applications are motivated by increasing the bandwidth of aircraft passenger internet access, whereby an aircraft would use an optical link to connect to a LEO satellite, instead of directly to the ground. Some of these efforts have been postponed or outright cancelled.
While aerial-to-aerial links can avoid most of the challenges associated with optical turbulence, new practical problems are introduced, such as aircraft vibration effects on pointing and tracking, network provisioning of limited flight-time aircraft, and the need for ground-based connectivity. Aerial-to-ground optical links must traverse the atmosphere at some point, introducing an additional bandwidth bottleneck to be discussed in the “Hybrid Optical Links” section below.
Ground-based optical links are frequently discussed in the context of backhaul applications for last-mile customers or for difficult terrain where laying fiber is impractical. Shorter optical links may also be used for areas with high RF activity or latency/security-constrained environments. Typically, terrestrial links are between 500 m and 5 km, depending on the environment and operate in the near-infrared. Since atmospheric turbulence is highest near the ground, turbulence mitigation techniques are typically employed, increasing the cost of these systems and positioning them as a niche market. Commercial products have been available for several decades and have recently scaled to 10 Gb/s links.
Recently, there has been renewed interest in optical links that traverse multiple of these domains, such as ground-to-air links supporting HAV constellations or ground-to-LEO optical links supporting LEO satellite constellations. In particular, LEO-to-ground optical links may become more prominent in the coming years to address the increase in space-based cross-sectional bandwidth of the constellations. Current traffic-routing solutions utilize RF downlinks from LEO satellites, which are limited by size, weight, and power (SWaP) constraints to around 500 Mb/s.
There are also additional applications that require hybrid optical links besides constellations. Currently, LEO and GEO satellites generate significant amounts of data that must be transmitted to the ground. NASA's Terabyte Infrared Delivery (TBIRD) program is intended to address this bottleneck. However, recent experimental demonstrations have had limited success at transferring data at speeds faster than 5-10 Gb/s aggregate bit rates.
Pointing and tracking between optical terminals has been and continues to be a challenge for modern Free-Space Optical (FSO) systems. Complex control algorithms are required to ensure that the optical beam profile from the transmitter is translated to a receiver beam profile that overlaps with the receiver aperture. While problems plague practical systems, there are well-known and studied techniques for all ranges of free-space optical links.
Weather such as rain, clouds, or fog, can have deleterious effects on a free-space optical link. Frequently, severe weather causes optical links to go down regardless of the amount of optical power available at the transmitter. In these cases, a slower RF backup link is often required. In some cases, networks can be designed to route signals through multiple other paths if one optical link is unavailable, but to ensure a fixed reliability rate, redundant transmitter and receiver terminals are required. This technique is an example of spatial diversity that will be discussed in the “Turbulence Mitigation Techniques” section below.
Clear-air turbulence is among a class of atmospheric conditions where attenuation of and optical signal is relatively low, compared to vacuum, but atmospheric effects due to air movement, temperature, and pressure, distorts the optical signals in various ways that make reception of the signal difficult. Frequently, clear-air turbulence results in fading, whereby the received intensity of an optical signal decreases rapidly below the receiver sensitivity due to multi-path interference effects in the atmosphere. The observed statistical nature of the received optical intensity through the atmosphere is the basis for many theoretical models.
The most prominent theory of atmospheric turbulence is Kolmogorov's Theory of Turbulence, where the atmosphere is treated as a viscous liquid undergoing turbulent flow. Furthermore, the atmosphere is assumed to be composed of eddies of varying sizes, and in thermal equilibrium there is a distribution of eddies sizes, which, given various other parameters such as wind speed and pressure, determine the total effects of refraction and interference of an optical signal as it traverses the atmosphere. Specifically, the index of refraction structure function, which describes the correlation of the refractive index in the receiver plane, is Φn(K)=0.033 Cn2K−11/3, where K is the spatial frequency and Cn2 is the refractive index structure constant which describes the overall strength of the turbulence. This theory has led to the theoretical and experimental exploration of the effects of atmosphere on optical transmission, including the optical phase. Additional models have been built up on this theory, such as the Gamma-Gamma model, which will be used later, where atmospheric turbulence is characterized primarily by the size of the smallest and largest atmospheric eddies. These length scales, derived from Cn2, are then used to predict the distribution of the intensities at the receiver plane.
Finally, in the context of free-space optical heterodyne receivers, statistical information about the phase of the received optical signal can be ascertained. Specifically, the coherence length is defined roughly as the length in the receiver plane between points where the phase of the optical signal is well-correlated, which is critical for coherent optical communications systems. The coherence length is related to the link length, wavelength, and turbulence strength: r0=1.68(Cn2Lk2)−3/5, valid for a plane wave.
One technique to avoid intensity fading of an optical signal is to send additional optical power from the transmitter aperture. The ratio of average received optical power to the receiver sensitivity is called the fade threshold. Increasing the fade threshold decreases the probability of a fading event dropping the received signal intensity below the receiver sensitivity, resulting in a link outage. The obvious drawbacks to this method are a decrease in efficiency, decrease in signal to noise ratio (SNR) and potential limitations due to eye-safety concerns. Importantly, some optical links under conditions of high turbulence can experience very deep fades, on the order of tens of dBs, much higher than practical fad thresholds.
Another technique by which atmospheric turbulence can be mitigated is aperture averaging. By increasing the aperture size, additional light is collected and combined in the receiver waveguide. For coherent communications, increasing the aperture size within the coherence length increases the SNR, while aperture averaging is limited past the coherence length.
One compensatory optical technique is adaptive optics, whereby the received optical wavefront is measured and compensated so that the discretized wavefront is coherently summed in the receiving waveguide. By sensing the wavefront, such as with a Shack-Hartmann wavefront sensor, the relative phases of the pixelized wavefront can be estimated and corrected. Necessarily, the use of adaptive optics requires constant temporal updates to the wavefront correcting element as the atmosphere changes.
For many FSO systems, the primary impairment is temporal fading. Depending on the length of the link and the strength of the turbulence, mean fading times can occur on the time scales of tens of microseconds to 10s of milliseconds4. Some systems implement automatic repeat requests (ARQ) so that if packets are dropped in the FSO link, they may be transmitted. Similarly, some links shift the complexity to signal coding and introduce temporal redundancy with various type of repetition coding. In the latter case, the statistical nature of fading is used to reduce the likelihood of an outage, while in the former, fading is dealt with by a higher protocol. Both methods significantly increase the latency of the FSO link.
Some FSO systems utilize adaptive coding to adapt to the unpredictable FSO channel. Frequently in these implementations, a RF back-channel is used to convey information about the FSO channel, which is used to reduce or increase the modulation format order. This requires synchronization at both transmitter and receiver ends as well as a reliable estimator for the channel. In addition, this method is not necessarily compatible with fixed rate networks where optical links are expected to be able to support a specific maximum data rate at any given time.
A method of decreasing the outage probability of and FSO link is by utilizing transmitter or receiver diversity. In its simplest form, identical or similar information is sent across multiple independent of sufficiently uncorrelated channels to increase the probability that the information is successfully transmitted and received.
A form of diversity is temporal diversity to decrease the outage probability. While repetition coding is an example of time-diversity, any uncorrelated channels can be used to re-transmit information. For example, a sometimes-used method is subcarrier intensity modulation (SIM) whereby different subcarriers of an intensity-modulated signal are used to transmit independent data streams. In one implementation, the same information, but time-delayed, is transmitted on each subcarrier.
Spatial diversity techniques often leverage the spatial decorrelation of the atmosphere to reduce the likelihood of an outage and increase the BER. Various implementations use one or multiple transmit apertures focused onto one or multiple receiver apertures in either the near-field or far-field. Without loss of generality, we consider receiver diversity schemes, though the methods can also be used for a combination of receiver and transmitter diversity schemes. If multiple copies of the transmitted optical signal are received, then the information can be gathered and processed to determine the original signal. Some common methods are: maximal ratio combining (MRC), equal gain combining (EGC), or selective combining (SC). Transmitter and receiver methods may use multiple separate apertures or utilize a single aperture that can transmit or receive multiple spatial modes, such as coupling into few-mode fiber. These methods can be used with both coherent optical links as well as optical links based on direct detection. The methods are described briefly below:
The above methods can be done in either the optical domain or the electrical domain. If the signals are combined in the optical domain, they are typically combined with interferometric devices, either concatenated Mach-Zehnder (MZ) modulators, or meshes of MZ modulators, whose relative path length differences are adjusted to align the phase of one or more received optical signals. In recent years there have been several theoretical and experimental studies of optical phase alignment algorithms for spatial diversity receivers.
Similarly, phase alignment can also occur in the electrical domain after the optical signals have been down converted. There is often more flexibility in the digital domain and FSO spatially diverse receivers have been demonstrated for both coherent and noncoherent detection methods. One downside of digital combining is that the number of independent receivers scales with the number of receiver apertures, which may or may not increase cost and complexity.
Like other diversity techniques, multiple wavelengths can transmit identical or similar information and traverse a unique or shared path. If the path length is long enough, then a shared path through the atmosphere can introduce decorrelation between optical wavelengths. This effect has been studied via two-frequency mutual coherence functions. Interestingly, only for very long links, such as LEO-to-ground, and high optical turbulence, can two frequencies transmitted and received through the same aperture become significantly decorrelated. For this reason, many previous wavelength diversity systems use optical wavelengths very far apart, such as 800 nm and 1550 nm to ensure decorrelation. Demonstrations of wavelength diversity have been shown for both direct detection and coherent detection-based systems where the wavelengths are separated by wavelength-selective devices, processed by separate receivers, and optimally combined. Some implementations rely on coding across multiple wavelengths of a wavelength-division multiplexed channel.
Reference will now be made to the accompanying drawings, which are not necessarily drawn to scale, and wherein:
As described above, due to atmospheric fading, FSO communications links can experience power drops for long periods on the scale of communications systems (100 microseconds to 10 milliseconds). The architectures below mitigate the effect of atmospheric fading using wavelength diversity and other diversity techniques. Importantly, these techniques may be used together or separately to completely resolve or partially mitigate the effects of atmospheric turbulence. In the cases where atmospheric effects can be completely mitigated, real-time optical links can be implemented without additional ARQ layers.
Transmitting identical or similar information on two different wavelengths has a diversity advantage without, in principle, increasing the latency or increasing the number of transmitter and receiver apertures. Here we describe three FSO Communications (FSOC) architectures that leverage this performance improvement.
Note, in the following figures λN represents the N'th single-wavelength source (such as a laser) while {tilde over (λ)}N represents an optical signal at the same center wavelength, λN, that has been modulated.
Due to wavelength-dependent phase variations due to atmospheric turbulence, optical path lengths, mechanical tolerance, etc. phase alignment of the local oscillator wavelengths allows for the down conversion process to generate electrical signals that sum coherently. Due to this coherent summation, the electrical signal-to-noise ratio is greater than that of any of the single wavelength signals. Importantly, the probability of a fade decreases dramatically because each wavelength experiences independent or only partially correlated turbulence, resulting in wavelength diversity.
This design uses a processor that receives input from the modem, which receives the analog electrical signals from the optical hybrid. In this architecture, the processor uses an algorithm to determine the optimal phase alignment for each of the local oscillator wavelengths. Then the processor sends electrical control signals to the optical phase alignment stage, discussed below, to align the phases of the local oscillator optical wavelengths. Moreover, the algorithms track various temporal phase effects that may occur due to turbulence, temperature, pressure, etc. so that the aligned phases remain matched to the transmitted signals. The processor also sends feedback to the local oscillator multi-wavelengths source necessary to track the per-channel optical frequencies and phases due to optical phase noise in the source, or other fast phase effects.
The phase alignment technique can also take place solely in the electric domain.
The phase alignment technique can also take place in the digital domain. For example, when the wavelengths of the Rx optical source are slightly staggered relative to the Tx optical source, the Intermediate Frequencies after optical mixing will be staggered in frequency. Digital processing can recover the phase from each of these and then a unitary transform such as a Hadamard matrix can combine the signals for decoding.
In another implementation, wavelength-diversity can be used in FSOC architectures based on direct detection as depicted in
The transmitter multi-wavelength source may be coherent or incoherent. Here we define “coherent” to mean having a known, consistent phase relationship.
In
In
In
Incoherent sources of multiple wavelengths can still be used in this configuration, though it shifts complexity to the receiver-side (per-wavelength fast phase tracking may be required).
For the incoherent multi-wavelength approach, it is necessary to modulated separate wavelengths with the same or similar information with different electrical carrier frequencies.
In the architectures presented here, multiple wavelengths are detected simultaneously in a single detector. The detection may be based on coherent detection or intensity detection. In both cases, it is necessary that the optical detectors be responsive at the desired wavelengths. Similarly, optical devices intended for multi-wavelength usage may need to be designed to support the wavelengths under operation.
Coherent detection may occur in a coherent optical hybrid whereby the phase, amplitude, or both are detected and converted to electrical signals. The hybrid may support multiple polarizations, may be homodyne or heterodyne, and may support single- or dual-quadrature detection.
Intensity detection may occur in a single optical detector or multiple optical detectors designed for specific wavelengths. Typically, a photodiode is used, though avalanche photodetectors or single photon avalanche diodes may be used.
Similar to the transmitter multi-wavelength source, the receiver local oscillator multi-wavelength source can be either coherent or incoherent. If the source is incoherent, additional processing is required on the processor in order to phase-align the wavelengths with the received signal wavelengths.
Similarly, incoherent multi-wavelength sources can be used as the receiver local oscillator.
A general schematic of a modem is shown in
Generally, the transmitter multi-wavelength optical sources will have some fast frequency and phase noise that will need to be tracked by the receiver local oscillator wavelengths. For multi-wavelength sources that are coherent, it is possible to use a single tracking loop such as an optical phase-locked loop to track the frequency and phase of the input carriers. For incoherent multi-wavelength sources, the frequency-tracking may need to be parallelized. For coherent sources, phase and frequency tracking can be accomplished inside the modem, with feedback to the local oscillator multi-wavelength source.
In several described implementations, it is possible to generate multiple wavelengths with a fixed spacing between them (typically in the frequency domain). If such a source is used in both the transmitter and receiver then it is possible to align all of the wavelengths used for wavelength diversity by tracking the frequency spacing between wavelengths (in addition to the absolute wavelength of one of the input wavelengths). For example, if using a resonator-based optical frequency comb, the free-spectral range of the resonator typically determines the frequency spacing, but the transmitter and receiver comb generators may differ slightly due to fabrication tolerances. Moreover, the size of the ring may change based on external factors such as temperature. By tracking the frequency spacing of the received multi-wavelength source, a control signal can be sent to the receiver local oscillator multi-wavelength source to align the transmitted and received frequency spacing to ensure efficient overlap in the coherent hybrid.
Thermal drift, pressure, and importantly, turbulence can change the relative phases of the received wavelengths. If a joint coherent fast phase and frequency tracking is used, then fast phase fluctuations for each of the receiver wavelengths are corrected, but slower-scale wavelength-dependent phases are not. This necessitates additional frequency and phase alignment, which are detailed in the following section.
As shown in
The phase alignment algorithm may include an acquisition phase, where a known set of symbols is transmitted. During operation, the processor may overlay a low-speed low-amplitude dither to the phase modulators to determine the mean phase direction to apply. Similarly, pilot tones can be sent on various wavelengths and extracted in the Tx filtering and processing stage in order to align different wavelengths.
The phase alignment dithers or pilot tones can be implemented either electrically in the transmitter or optically by wavelength demultiplexing and multiplexing. Wavelength (de)multiplexing options include AWGs, free-space filtering, or single-waveguide ring-resonator/busses. Additionally, a pilot tone or dither can be applied in the multi-wavelength source generation process. For some multi-wavelength processes, a dither applied on the input wavelength can “cascade” to other wavelengths but exist at a higher harmonic or other portion of the baseband frequency spectrum. This is one way to “tag” specific wavelengths in the receiver with a pilot tone or dither.
Combination with Other Diversity Techniques
The techniques here can also be combined with other turbulence mitigation techniques including:
While for purposes of simplicity of explanation, the respective processes are shown and described as a series of blocks in
In one embodiment, the additional information comprises signal-to-noise ratio of the electrical signals, modulation error ratio of the electrical signals, error vector magnitude of the electrical signals, bit error ratio of the electrical signals, Q factor of the electrical signals, power of the electrical signals, noise calculation of the electrical signals, a portion of the electrical signals, or combinations thereof.
In one embodiment, the transmitter is further configured to modulate the multiple optical wavelengths with one or more additional signals, wherein at least a portion of the one or more additional signals is included in the additional information generated by the modem, and wherein the additional information enables the processor to identify each of the multiple optical wavelengths.
In one embodiment, the processor identifies each of the multiple optical wavelengths from the additional information based on pilot signals, pilot symbols, dithers or combinations thereof inserted in the correlated optical signals.
In one embodiment, the processor identifies each of the multiple optical wavelengths from the additional information based on dithering applied by the processor to the one or more control signals, extraction by the processor of pilot signals, pilot symbols, or dithers included in the additional information, or combinations thereof.
In one embodiment, the multiple optical wavelengths are generated by a single-wavelength input, wherein the single-wavelength input comprises in a Kerr resonator frequency comb, electro-optic resonant comb, a cascaded electro-optic frequency comb, or combinations thereof.
In one embodiment, the multiple optical wavelengths are generated by a multi-wavelength mode-locked laser, gain-switched laser or a combination thereof.
In one embodiment, the multiple optical wavelengths are generated by separate single-wavelength sources.
In one embodiment, the multiple optical wavelengths are coherent.
In one embodiment, the multiple optical wavelengths are incoherent.
In one embodiment, the modulation of the multiple optical wavelengths is performed according to both phase and amplitude.
In one embodiment, the modulation of the multiple optical wavelengths is performed according to intensity modulation.
In one embodiment, the single-wavelength source generates a plurality of optical signals that are modulated and thereafter converted to the multiple optical wavelengths.
In one embodiment, the single-wavelength source generates a plurality of optical signals that are converted to the multiple optical wavelengths and thereafter modulated.
In one embodiment, an additional electrical frequency shift is applied to the modulation of each wavelength of the multiple optical wavelengths.
In one embodiment, the transmission medium is a terrestrial optical link.
In one embodiment, the transmission medium is a ground to low-earth orbit link.
In one embodiment, the transmission medium is a space-to-space link.
In one embodiment, the transmission medium is an underwater link.
In one embodiment, the transmitter has a single transmitter aperture, wherein the single transmitter aperture transmits one or more multiple optical modes.
In one embodiment, the transmitter has multiple transmitter apertures.
In one embodiment, the correlated optical signals are routed through the multiple transmitter apertures configured as an optical phased array or in a manner of coherent optical beam combining.
In one embodiment, the correlated optical signals are time-delayed to introduce time diversity with optical delay lines.
In one embodiment, the modulation of the multiple optical wavelengths is time-delayed via analog or digital delays to introduce time-diversity.
In one embodiment, the optical signals are received via a single receiver aperture, and wherein the single receiver aperture receives one or more multiple optical modes.
In one embodiment, the optical signals are received via multiple receiver apertures.
In one embodiment, the optical signals from the multiple receiver apertures are optically combined via feedback from the processor to improve signal quality through spatial diversity techniques including equal gain combining, selective combining, maximal ratio combining, or combinations thereof.
In one embodiment, the optical signals from each receiver aperture of the multiple receiver apertures are processed and converted to electrical signals separately and then combined electrically to improve signal quality through spatial diversity techniques including equal gain combining, selective combining, maximal ratio combining, or combinations thereof.
In one embodiment, the optical signals are time-delayed to compensate for the optical delays in the transmitter and to achieve time diversity.
In one embodiment, additional analog or digital delays are applied to the multiple optical wavelengths to compensate for the time-delayed modulation.
In one embodiment, the optical to electrical conversion is performed according to a combination of the received optical signals with a local oscillator optical signal in an optical hybrid to produce the electrical signals, and wherein the local oscillator optical signal comprises other multiple optical wavelengths and is generated by an unmodulated multi-wavelength optical source.
In one embodiment, the optical to electrical conversion is performed according to intensity detection, the intensity detection including a photodiode, an Avalanche Photo Diode (APD), a Single Photon Avalanche Diode (SPAD), or combinations thereof.
In one embodiment, the other multiple optical wavelengths are generated in a similar fashion to a method used to generate the multiple optical wavelengths.
In one embodiment, the other multiple optical wavelengths are generated according to a different method than a technique used by the transmitter to generate multiple optical wavelengths, the technique comprising at least one of the aforementioned embodiments.
In one embodiment, the other multiple optical wavelengths are aligned with the received optical signals via the one or more control signals being directed to the unmodulated multi-wavelength optical source, which could be accomplished with tailoring of electrical drive signals to cascaded electro-optic modulators.
In one embodiment, the other multiple optical wavelengths are aligned with the received optical signals via the one or more control signals from the processor sent to the unmodulated multi-wavelength optical source as well as an optical phase alignment stage.
In one embodiment, the modem processes the electrical signals coherently.
In one embodiment, the modem processes the electrical signals as intensity-detected signals.
In one embodiment, the additional information comprises analog or digital information, and wherein the modem outputs the analog or digital information from any of the modem subsystem blocks or raw samples from a DAC or ADC of the modem.
In one embodiment, the analog or digital information includes per-subcarrier data information.
In one embodiment, a first portion of the one or more controls signals are configured for fast phase alignment of the received optical signals to compensate for phase noise of the received optical signals, and wherein a second portion of the one or more controls signals are configured for slow phase alignment of the received optical signals to compensate for atmospheric effects caused by the turbulent channel on the received optical signals.
In one embodiment, the fast phase alignment between the received optical signals and the local oscillator optical signal is accomplished with an optical phase locked loop.
In one embodiment, the fast phase alignment between the received optical signals and the local oscillator optical signal is accomplished with optical injection locking.
In one embodiment, the fast phase alignment is performed according to independent control signals of the one or more control signals on each wavelength of the local oscillator optical signal.
In one embodiment, the fast phase alignment is performed by at least one control signal of the one or more control signals applied to multiple wavelengths of the local oscillator optical signal.
In one embodiment, the fast phase alignment is performed by tracking the frequency spacing between wavelengths of the received optical signals and fast phase noise of at least one wavelength in the received optical signals.
In one embodiment, the phase alignment stage comprises an optical phase alignment module, an unmodulated multi-wavelength optical source, an electrical phase alignment module or combinations thereof.
In one embodiment, the electrical phase alignment module performs digital phase alignment, analog phase alignment or a combination thereof.
In one embodiment, entropy of the additional information is greater than 1 giga bits per second.
In one embodiment, the additional information supplied to the processor is digital information.
In one embodiment, a bit-rate of the additional information is greater than 10 giga bits per second.
In one embodiment, a bit-rate of the additional information is greater than 100 giga
bits per second.
In one embodiment, latency of the additional information is less than 10 microseconds.
In one embodiment, latency of the additional information is less than 1 microsecond.
In one embodiment, latency of the additional information is less than 10 nanoseconds.
In one embodiment, latency of the additional information is less than 1 nanosecond.
In one embodiment, the wavelength-diverse optical communication link is bidirectional.
In one embodiment, portions of the wavelength-diverse optical communication link are configured for wavelength diversity, spatial diversity, time diversity, or combinations thereof.
In one embodiment, an apparatus can comprise a processing system including a processor; and a memory that stores executable instructions that, when executed by the processing system, facilitate performance of operations, comprising receiving optical signals, wherein the optical signals are generated by a transmitter, wherein the transmitter generates multiple optical wavelengths, wherein the transmitter modulates the multiple optical wavelengths from digital input data to create correlated optical signals, and wherein the transmitter transmits the correlated optical signals across a transmission medium having characteristics of a turbulent channel; converting of the optical signals to electrical signals; processing of the electrical signals in a modem to produce output data and additional information; supplying the additional information to a processor; and based on the additional information, the processor generating one or more control signals directed to a phase alignment stage for compensating turbulent effects experienced by the optical signals while propagating through the turbulent channel.
In one embodiment, a machine-readable medium, can comprise executable instructions that, when executed by a processing system including a processor, facilitate performance of operations, comprising receiving optical signals, wherein the optical signals are generated by a transmitter, wherein the transmitter generates multiple optical wavelengths, wherein the transmitter modulates the multiple optical wavelengths from digital input data to create correlated optical signals, and wherein the transmitter transmits the correlated optical signals across a transmission medium having characteristics of a turbulent channel; converting of the optical signals to electrical signals; processing of the electrical signals in a modem to produce output data and additional information; supplying the additional information to a processor; and based on the additional information, the processor generating one or more control signals directed to a phase alignment stage for compensating turbulent effects experienced by the optical signals while propagating through the turbulent channel.
The present application claims the benefit of priority to U.S. Provisional Application No. 63/496,239 filed on Apr. 14, 2023, which is hereby incorporated herein by reference in its entirety.
| Number | Date | Country | |
|---|---|---|---|
| 63496239 | Apr 2023 | US |
