The present disclosure relates to optical communication equipment and, more specifically but not exclusively, to supervisory signal paths for an optical transport system.
This section introduces aspects that may help facilitate a better understanding of the disclosure. Accordingly, the statements of this section are to be read in this light and are not to be understood as admissions about what is in the prior art or what is not in the prior art.
Subsea network operators are facing a fast growth in bandwidth demand, in part due to the development and deployment of cloud-based services. As a result, they need to optimize the capacity and performance of their fiber-optic cable plants to enable the corresponding networks to efficiently handle the increasing data flows. Due to this need, one of the requirements to telecom equipment manufacturers is to provide the network operator(s) with a supervisory system that can be used to monitor the status of the submerged plant elements, e.g., to guarantee fault detection and diagnostics, improved maintainability, good performance characteristics throughout the plant's lifespan, upgradable capacity, and/or any other pertinent benchmarks.
At least some of the above-indicated problems in the state of the art are addressed by various embodiments of a bidirectional optical repeater having two unidirectional optical amplifiers and a supervisory optical circuit connected to optically couple the corresponding unidirectional optical paths. In an example embodiment, the supervisory optical circuit provides three pathways therethrough for supervisory optical signals, the first pathway being from the output of the first optical amplifier to the input of the second optical amplifier, the second pathway being between the input of the first optical amplifier and the input of the second optical amplifier, and the third pathway being from the output of the second optical amplifier to the input of the first optical amplifier. The pathways are arranged such that the remote monitoring equipment of the corresponding optical transport system can use optical time-domain reflectometry, e.g., to determine and monitor, as a function of time, the individual gains of the first and second optical amplifiers.
According to an example embodiment, provided is an apparatus comprising: a first optical amplifier located in a first optical path configured to transmit optical signals in a first direction; a second optical amplifier located in a second optical path configured to transmit optical signals in a second direction, the second direction being opposite to the first direction; and an optical circuit connected to optically couple the first optical path and the second optical path; and wherein the optical circuit comprises: a first optical pathway configured to direct light from an output of the first optical amplifier to an input of the second optical amplifier; and a second optical pathway configured to direct light from an input of the first optical amplifier to the input of the second optical amplifier.
Other aspects, features, and benefits of various disclosed embodiments will become more fully apparent, by way of example, from the following detailed description and the accompanying drawings, in which:
Some embodiments may benefit from the use of features disclosed in the concurrently filed patent application by Omar Ait Sab, entitled “USE OF BAND-PASS FILTERS IN SUPERVISORY SIGNAL PATHS OF AN OPTICAL TRANSPORT SYSTEM,” European Patent Application No. EP17305569.0 filed May 17, 2017, which is incorporated herein by reference in its entirety.
In an example embodiment, wet plant 104 comprises an undersea cable system that includes, inter alia, submersible optical repeaters 1501-150N serially connected by spans 140 of optical fiber, e.g., as indicated in
In the shown embodiment, an optical repeater 150j comprises optical amplifiers 160ja and 160jb, where j=1, 2, . . . , N. Optical amplifier 160ja is configured to amplify optical signals traveling towards landing station 1022. Optical amplifier 160jb is similarly configured to amplify optical signals traveling towards landing station 1021. In an example embodiment, an optical amplifier 160j can be implemented as known in the pertinent art, e.g., using an erbium-doped fiber, a gain-flattening filter, and one or more laser-diode pumps. The laser diodes can be powered by a DC current from the corresponding shore-based power-feeding equipment (PFE, not explicitly shown in
In an alternative embodiment, optical repeaters 150 can be designed for two, three, four, or more pairs of optical fibers 140i connected thereto at each side thereof. For example, an optical repeater 150 designed to be compatible with a four-fiber-pair submarine cable typically includes eight optical amplifiers 160 arranged in four amplifier pairs, each pair being similar to optical amplifiers 160ja and 160jb.
Optical repeater 150j further comprises a supervisory optical circuit (not explicitly shown in
In an example embodiment, each of ME units 1201 and 1202 is configured to use dedicated supervisory wavelengths (labeled λ1 and λ2) to generate respective supervisory signals that can be sent through the corresponding fiber(s) 140 towards the remote landing station 102. The supervisory optical circuit of each optical repeater 150j is configured to loop back, in the opposite direction, at least a portion of a supervisory signal. As a result, ME unit 1201 can receive a looped-back supervisory signal comprising the portions of the original supervisory signal returned to that ME unit by the different supervisory optical circuits of different optical repeaters 1501-150N. Similarly, ME unit 1202 can receive a looped-back supervisory signal comprising the portions of the corresponding supervisory signal returned to that ME unit by the different supervisory optical circuits of different optical repeaters 1501-150N. The looped-back supervisory signals received by ME units 1201 and 1202 can be processed and analyzed to determine the present operating status and/or certain operating characteristics of at least some or all of optical repeaters 1501-150N in wet plant 104. The determined parameters may include but are not limited to: (i) input and output signal levels and the gains of some or all individual optical amplifiers 160ja and 160jb; (ii) non-catastrophic faults in individual optical fibers 140i, such as any gradual loss increases therein; and (iii) catastrophic failures in individual optical repeaters 150j and/or optical fibers 140i.
Landing station 1021 comprises a submarine line terminal equipment (SLTE) unit 1101 and ME unit 1201 connected to wet plant 104 by way of a wavelength multiplexer (MUX) 1301 and a wavelength de-multiplexer (DMUX) 1361 as indicated in
As already indicated above, carrier wavelengths λ1 and λ2 are reserved for supervisory signals and are not used by SLTE unit 1101 for payload transmissions. Carrier wavelengths λ1 and λ2 can be spectrally located at an edge of the spectral range occupied by the payload-carrying WDM channels. For example, in some embodiments, both carrier wavelengths λ1 and λ2 can be smaller than any of carrier wavelengths λ3-λn. In some other embodiments, both carrier wavelengths λ1 and λ2 can be larger than any of carrier wavelengths λ3-λn. In some alternative embodiments, carrier wavelength λ1 can be smaller than any of carrier wavelengths λ3-λn, and carrier wavelength λ2 can be larger than any of carrier wavelengths λ3-λn.
In an example embodiment, carrier wavelengths can be selected in accordance with a frequency (wavelength) grid, such as a frequency grid that complies with the ITU-T G.694.1 Recommendation, which is incorporated herein by reference in its entirety. The frequency grid used in system 100 can be defined, e.g., in the frequency range from about 184 THz to about 201 THz, with a 100, 50, 25, or 12.5-GHz spacing of the channels therein. While typically defined in frequency units, the parameters of the grid can equivalently be expressed in wavelength units. For example, in the wavelength range from about 1528 nm to about 1568 nm, the 100-GHz spacing between the centers of neighboring WDM channels is equivalent to approximately 0.8-nm spacing. In alternative embodiments, other fixed or flexible (flex) frequency grids can be used as well.
In operation, MUX 1301 multiplexes the optical signals of carrier wavelengths λ3-λn, generated by SLTE unit 1101 and the supervisory optical signals of carrier wavelengths λ1 and λ2, and applies the resulting multiplexed optical signal to optical fiber 1401a. DMUX 1361 de-multiplexes a multiplexed optical signal received from optical fiber 140ib into two portions. The first portion has optical signals of carrier wavelengths λ3-λn and is directed to SLTE unit 1101. The second portion has the looped-back supervisory optical signals of carrier wavelengths λ1 and λ2 and is directed to ME unit 1201.
In an example embodiment, ME unit 1201 comprises an optical time-domain reflectometer (OTDR, not explicitly shown in
Landing station 1022 is analogous to landing station 1021 and comprises an SLTE unit 1102, ME unit 1202, a MUX 1302, and a DMUX 1362. The analogous elements/components of the two landing stations are labeled in
In various embodiments, each of landing stations 1021 and 1022 may further include one or more of the following conventional elements/components: (i) power feeding equipment; (ii) system supervisory equipment; (iii) network management equipment; (iv) cable termination boxes; (v) network protection equipment; and (vi) various interface circuits.
In some embodiments, a single respective carrier wavelength can be used at each of ME units 1201 and 1202 to generate supervisory optical signals. In some other embodiments, more than two carrier wavelengths of the WDM set λ1-λn can be allocated for supervisory functions. A person of ordinary skill in the art will understand, without undue experimentation, how to modify MUXes 130, DMUXes 136, and/or other pertinent system components to be compatible with such alternative WDM-channel allocations for supervisory functions.
As can be seen in
A person of ordinary skill in the art will understand that the OTDR traces acquired by ME unit 1202 (
In some embodiments, the OTDR traces similar to those shown in
Circuit 300 comprises (i) four optical taps that are labeled in
Optical tap 3101a is located on optical path 340a upstream from an input port 358a of optical amplifier 160ja. Optical tap 3102a is located on optical path 340a downstream from an output port 362a of optical amplifier 160ja. Optical tap 3101b is located on optical path 340b downstream from an output port 362b of optical amplifier 160jb. Optical tap 3102b is located on optical path 340b upstream from an input port 358b of optical amplifier 160jb. Optical taps 3101a and 3102b are connected to one another by way of an optical fiber or waveguide 314, as indicated in
Optical combiner 330a is located at input port 358a of optical amplifier 160ja and is configured to apply thereto an optical signal generated by that optical combiner at the output thereof in response to the optical signals applied to its inputs by optical fiber 140ja and optical tap 3101b. Optical combiner 330b is located at input port 358b of optical amplifier 160jb and is configured to apply thereto an optical signal generated by that optical combiner at the output thereof in response to the optical signals applied to its inputs by optical fiber 140(j+1)b and optical tap 3102a. Optical tap 3101b and optical combiner 330a are connected to one another by way of an optical fiber or waveguide 312. Optical tap 3102a and optical combiner 330b are connected to one another by way of an optical fiber or waveguide 316.
Circuit 300 further comprises wavelength-selective reflectors 3201a, 3201b, 3202a, and 3202b that are coupled to optical taps 3101a, 3101b, 3102a, and 3102b, respectively, as indicated in
In operation circuit 300 provides the following loop-back paths for the supervisory optical signals of carrier wavelengths λ1 and λ2.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received through optical fiber 140ja to optical tap 3101a. Optical tap 3101a operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3201a that selectively reflects the λ1 component thereof and essentially absorbs all other spectral components thereof. The reflected λ1 component travels through optical fiber 314 to optical tap 3102b that operates to couple a portion of that component into optical path 340b. Optical path 340b then directs the coupled portion to optical amplifier 160jb, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362b of optical amplifier 160jb to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received through optical fiber 140ja to optical amplifier 160ja, where the latter undergoes optical amplification. The resulting amplified signal is directed from output port 362a of optical amplifier 160ja to optical tap 3102a. Optical tap 3102a operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3202a that selectively reflects the λ2 component thereof and essentially absorbs all other spectral components thereof. The reflected λ2 component travels through optical fiber 316 to optical combiner 330b that applies the latter to optical amplifier 160jb. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362b of optical amplifier 160jb to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received through optical fiber 140(j+1)b to optical tap 3102b. Optical tap 3102b operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3202b that selectively reflects the λ2 component thereof and essentially absorbs all other spectral components thereof. The reflected λ2 component travels through optical fiber 314 to optical tap 3101a that operates to couple a portion of that component into optical path 340a. Optical path 340b then directs the coupled portion to optical amplifier 160ja, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362a of optical amplifier 160ja to optical fiber 140(j+1)a.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received through optical fiber 140(j+1)b to optical amplifier 160jb, where the latter undergoes optical amplification. The resulting amplified signal is directed from output port 362b of optical amplifier 160jb to optical tap 3101b. Optical tap 3101b operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3201b that selectively reflects the λ1 component thereof and essentially absorbs all other spectral components thereof. The reflected λ1 component travels through optical fiber 312 to optical combiner 330a that applies the latter to optical amplifier 160ja. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362a of optical amplifier 160ja to optical fiber 140(j+1)a.
In some embodiments, the following approximation can be used to obtain the individual gains of optical amplifiers 160ja and 160jb of the optical repeater 150j shown in
The above-mentioned approximation relies on the assumption that circuit 300 has the same optical loss for each of the above-described loop-back paths for both wavelengths λ1 and λ2. The approximation further relies on the assumption that the gains of optical amplifiers 160ja and 160jb are spectrally flat and do not depend on the signal wavelength. The approximation further relies on the assumption that the supervisory optical signals of both carrier wavelengths λ1 and λ2 have the same power level P at the remote end of optical fiber 140ja configured to feed optical repeater 150j.
Let Pin and Pout denote the power levels at input port 358a and output port 362a, respectively, of optical amplifier 160ja. Using the above-indicated assumptions, Pin and Pout can be expressed using Eqs. (1)-(2):
Pin=P−Aja+Gb−Ajb (1)
Pout=P−Aja+Ga+Gb−Ajb (2)
where Aja is the signal attenuation in optical fiber 140ja; Ga and Gb are the gains of optical amplifiers 160ja and 160jb, respectively; and Ajb is the signal attenuation in optical fiber 140jb. It is evident from Eqs. (1)-(2) that the gain Ga of optical amplifier 160ja can be obtained by determining the difference between Pout and Pin, i.e.:
Ga=Pout−Pin (3)
As already indicated above, the values of Pin and Pout can be experimentally measured using the amplitudes of the corresponding peaks in the OTDR traces analogous to those shown in
A person of ordinary skill in the art will understand that the OTDR traces measured by ME unit 1202 using carrier wavelengths λ1 and λ2 can similarly be used to obtain the present-time values of the individual gains for all of optical amplifiers 1601b-160Nb in wet plant 104.
The above-indicated ability to obtain and monitor, as a function of time, the individual gains of optical amplifiers 1601a-160Na and 1601b-160Nb is advantageous, e.g., because, unlike circuit 300, conventional optical supervisory circuits used in submersible optical repeaters typically do not allow unambiguous determination of the individual amplifier gains and, instead, allow the system operator to only measure some indicator value that depends on two or more individual amplifier gains in some convoluted manner. The above-indicated ability to obtain and monitor the individual gains of optical amplifiers 1601a-160Na and 1601b-160Nb can be beneficial, e.g., because it enables the system operator to take appropriate (e.g., re-configuration and/or repair) actions in a better-informed and targeted manner.
The embodiment of optical repeater 150j shown in
In the embodiment of optical repeater 150j shown in
In operation circuit 400 provides the following loop-back paths for the supervisory optical signals of carrier wavelengths λ1 and λ2.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received through optical fiber 140ja to Bragg reflector 4201a. Bragg reflector 4201a reflects a portion of the λ1 component of that optical signal and passes through the remainder of that optical signal. Optical coupler 4101a couples a portion of the reflected λ1 component into optical fiber 314 that delivers it to optical coupler 4102b. Optical coupler 4102b operates to couple a portion of the received λ1 component into optical path 340b. Optical path 340b then directs the coupled portion, through Bragg reflector 4202b, to optical amplifier 160jb, where the latter portion undergoes optical amplification. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362b of optical amplifier 160jb, through Bragg reflector 4201b, to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received from optical fiber 140ja through Bragg reflector 4201a to optical amplifier 160ja, where the corresponding optical signal undergoes optical amplification. The resulting amplified signal is directed from output port 362a of optical amplifier 160ja to Bragg reflector 4202a. Bragg reflector 4202a reflects a portion of the λ2 component of that optical signal and passes through the remainder of that optical signal. Optical coupler 4102a couples a portion of the reflected λ2 component into optical fiber 316 that delivers it to optical combiner 330b. Optical combiner 330b applies the received λ2 component to optical amplifier 160jb. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362b of optical amplifier 160jb, through Bragg reflector 4201b, to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received through optical fiber 140(j+1)b to Bragg reflector 4202b. Bragg reflector 4202b reflects a portion of the λ2 component of that optical signal and passes through the remainder of that optical signal. Optical coupler 4102b couples a portion of the reflected λ2 component into optical fiber 314 that delivers it to optical coupler 4101a. Optical coupler 4101a operates to couple a portion of the received λ2 component into optical path 340a. Optical path 340a then directs the coupled portion, through Bragg reflector 4201a, to optical amplifier 160ja, where the latter portion undergoes optical amplification. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362a of optical amplifier 160ja, through Bragg reflector 4202a, to optical fiber 140(j+1)a.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received from optical fiber 140(j+1)b through Bragg reflector 4202b to optical amplifier 160jb, where the corresponding optical signal undergoes optical amplification. The resulting amplified signal is directed from output port 362b of optical amplifier 160jb to Bragg reflector 4201b. Bragg reflector 4201b reflects a portion of the λ1 component of that optical signal and passes through the remainder of that optical signal. Optical coupler 4101b couples a portion of the reflected λ1 component into optical fiber 312 that delivers it to optical combiner 330a. Optical combiner 330a applies the received λ1 component to optical amplifier 160ja. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362a of optical amplifier 160ja, through Bragg reflector 4202a, to optical fiber 140(j+1)a.
Similar to circuit 300, circuit 400 enables the system operator to obtain and monitor the individual gains of optical amplifiers 1601a-160Na and 1601b-160Nb, e.g., as described above in reference to
The embodiment of optical repeater 150j shown in
In the embodiment of optical repeater 150j shown in
Also shown in
Optical isolators 5241 and 5242 and optical attenuators 5281-5283 may be used in some embodiments to prevent spontaneous light generation in the “ring laser” that may be formed and become active due to the presence of output-to-input optical paths between optical amplifiers 160ja and 160ja provided by circuit 500. A person of ordinary skill in the art will understand that such spontaneous light generation may render optical repeater 150j unusable, e.g., due to the high noise level caused thereby. The use of these and possibly other optional elements for the indicated purpose is not limited to the embodiment of optical repeater 150j shown in
In operation circuit 500 provides the following loop-back paths for the supervisory optical signals of carrier wavelengths λ1 and λ2. For brevity, the description of these loop-back paths is given for an embodiment of circuit 500 in which the above-indicated optional elements are not present.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received through optical fiber 140ja to optical tap 3101a. Optical tap 3101a operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3201a that selectively reflects the λ1 component thereof and essentially absorbs all other spectral components thereof. A portion of the reflected λ1 component reaches optical tap 3102b by way of power splitter/combiner 5301, optical fiber 314, and power splitter/combiner 5302. Optical tap 3102b operates to couple a portion of the received λ1 component into optical path 340b. Optical path 340b then directs the coupled portion to input port 358b of optical amplifier 160jb, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362b of optical amplifier 160jb to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140ja can be looped back into optical fiber 140jb, e.g., as follows. Optical path 340a directs the optical signal received through optical fiber 140ja to optical amplifier 160ja, where the latter undergoes optical amplification. The resulting amplified signal is directed from output port 362a of optical amplifier 160ja to optical tap 3102a. Optical tap 3102a operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3202a that selectively reflects the λ2 component thereof and essentially absorbs all other spectral components thereof. A portion of the reflected λ2 component reaches optical tap 3102b by way of power splitter/combiner 5302. Optical tap 3102b operates to couple a portion of the received λ2 component into optical path 340b. Optical path 340b then directs the coupled portion to input port 358b of optical amplifier 160jb, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362b of optical amplifier 160jb to optical fiber 140jb.
A portion of a supervisory optical signal of carrier wavelength λ2 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received through optical fiber 140(j+1)b to optical tap 3102b. Optical tap 3102b operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3202b that selectively reflects the λ2 component thereof and essentially absorbs all other spectral components thereof. A portion of the reflected λ2 component reaches optical tap 3101a by way of power splitter/combiner 5302, optical fiber 314, and power splitter/combiner 5301. Optical tap 3101a operates to couple a portion of the received λ2 component into optical path 340a. Optical path 340a then directs the coupled portion to input port 358a of optical amplifier 160ja, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ2 is then directed from output port 362a of optical amplifier 160ja to optical fiber 140(j+1)a.
A portion of a supervisory optical signal of carrier wavelength λ1 received from optical fiber 140(j+1)b can be looped back into optical fiber 140(j+1)a, e.g., as follows. Optical path 340b directs the optical signal received through optical fiber 140(j+1)b to optical amplifier 160jb, where the latter undergoes optical amplification. The resulting amplified signal is directed from output port 362b of optical amplifier 160jb to optical tap 3101b. Optical tap 3101b operates to cause the tapped optical signal to impinge onto wavelength-selective reflector 3201b that selectively reflects the λ1 component thereof and essentially absorbs all other spectral components thereof. A portion of the reflected λ1 component reaches optical tap 3101a by way of power splitter/combiner 5301. Optical tap 3101a operates to couple a portion of the received λ1 component into optical path 340a. Optical path 340a then directs the coupled portion to input port 358a of optical amplifier 160ja, where the latter undergoes optical amplification. The resulting amplified signal of carrier wavelength λ1 is then directed from output port 362a of optical amplifier 160ja to optical fiber 140(j+1)a.
Similar to circuit 300, circuit 500 enables the system operator to obtain and monitor the individual gains of optical amplifiers 1601a-160Na and 1601b-160Nb, e.g., as described above in reference to
According to an example embodiment disclosed above in reference to
In some embodiments of the above apparatus, the first optical pathway is coupled to a first wavelength-selective reflector (e.g., 3202a,
In some embodiments of any of the above apparatus, the first wavelength-selective reflector comprises a first Bragg reflector (e.g., 4202a,
In some embodiments of any of the above apparatus, each of the first and second optical amplifiers is configured to amplify a respective WDM signal transmitted therethrough by way of a respective one of the first and second optical paths, the respective WDM signal configured to include a component having the first wavelength, a component having the second wavelength, and a plurality of additional components, each of the additional components having a respective wavelength (e.g., λ3-λn,
In some embodiments of any of the above apparatus, at least some of the respective wavelengths are spectrally located between the first wavelength and the second wavelength.
In some embodiments of any of the above apparatus, at least some of the respective wavelengths are smaller than either of the first wavelength and the second wavelength.
In some embodiments of any of the above apparatus, at least some of the respective wavelengths are greater than either of the first wavelength and the second wavelength.
In some embodiments of any of the above apparatus, the optical circuit further comprises a third optical pathway (e.g., 312,
In some embodiments of any of the above apparatus, the second optical pathway is further configured to direct light from the input of the second optical amplifier to the input of the first optical amplifier.
In some embodiments of any of the above apparatus, the first optical pathway is coupled to a first wavelength-selective reflector (e.g., 3202a,
In some embodiments of any of the above apparatus, the first wavelength-selective reflector comprises a first Bragg reflector (e.g., 4202a,
In some embodiments of any of the above apparatus, the apparatus further comprises monitoring equipment (e.g., 1201/1202,
In some embodiments of any of the above apparatus, the monitoring equipment is configured to determine an optical gain of the first optical amplifier using the first looped-back optical signal (e.g., as described in reference to Eqs. (1)-(3)); and the monitoring equipment is further configured to determine an optical gain of the second optical amplifier using the second looped-back optical signal (e.g., as described in reference to Eqs. (1)-(3)).
In some embodiments of any of the above apparatus, the optical circuit further comprises a first optical power combiner (e.g., 5302,
In some embodiments of any of the above apparatus, the optical circuit further comprises an optical power combiner (e.g., 5302,
In some embodiments of any of the above apparatus, the first optical amplifier, the second optical amplifier, and the optical circuit are parts of a first optical repeater (e.g., 150j,
In some embodiments of any of the above apparatus, the first optical repeater is submersible.
In some embodiments of any of the above apparatus, the apparatus further comprises one or more additional optical repeaters (e.g., 1502-150N,
In some embodiments of any of the above apparatus, the apparatus further comprises monitoring equipment (e.g., 1201,
In some embodiments of any of the above apparatus, the monitoring equipment is configured to determine an optical gain of the first optical amplifier using the looped-back optical signal (e.g., as described in reference to Eqs. (1)-(3)).
While this disclosure includes references to illustrative embodiments, this specification is not intended to be construed in a limiting sense.
For example, although various embodiments are described above in reference to wet plant 104 and submersible optical repeaters 150, the invention is not so limited. From the provided description, a person of ordinary skill in the art will understand how to make and use embodiments that are suitable for use in a terrestrial optical network, wherein at least one optical repeater 150 is located in a remote or difficult-to-access area that is not necessarily under water.
Various modifications of the described embodiments, as well as other embodiments within the scope of the disclosure, which are apparent to persons skilled in the art to which the disclosure pertains are deemed to lie within the principle and scope of the disclosure, e.g., as expressed in the following claims.
Unless explicitly stated otherwise, each numerical value and range should be interpreted as being approximate as if the word “about” or “approximately” preceded the value or range.
It will be further understood that various changes in the details, materials, and arrangements of the parts which have been described and illustrated in order to explain the nature of this disclosure may be made by those skilled in the art without departing from the scope of the disclosure, e.g., as expressed in the following claims.
Reference herein to “one embodiment” or “an embodiment” means that a particular feature, structure, or characteristic described in connection with the embodiment can be included in at least one embodiment of the disclosure. The appearances of the phrase “in one embodiment” in various places in the specification are not necessarily all referring to the same embodiment, nor are separate or alternative embodiments necessarily mutually exclusive of other embodiments. The same applies to the term “implementation.”
Also for purposes of this description, the terms “couple,” “coupling,” “coupled,” “connect,” “connecting,” or “connected” refer to any manner known in the art or later developed in which energy is allowed to be transferred between two or more elements, and the interposition of one or more additional elements is contemplated, although not required. Conversely, the terms “directly coupled,” “directly connected,” etc., imply the absence of such additional elements.
The described embodiments are to be considered in all respects as only illustrative and not restrictive. In particular, the scope of the disclosure is indicated by the appended claims rather than by the description and figures herein. All changes that come within the meaning and range of equivalency of the claims are to be embraced within their scope.
Number | Date | Country | Kind |
---|---|---|---|
17305570 | May 2017 | EP | regional |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/EP2018/061511 | 5/4/2018 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2018/210586 | 11/22/2018 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
6414769 | Meli | Jul 2002 | B1 |
6708004 | Homsey | Mar 2004 | B1 |
8280253 | Genay et al. | Oct 2012 | B2 |
8502964 | Wang et al. | Aug 2013 | B2 |
8805183 | Dvir | Aug 2014 | B2 |
8837938 | Liu et al. | Sep 2014 | B2 |
8942556 | Zhao et al. | Jan 2015 | B2 |
9008503 | Urban et al. | Apr 2015 | B2 |
9036991 | Aguren | May 2015 | B2 |
9042721 | Randel et al. | May 2015 | B2 |
9143228 | Sandstrom | Sep 2015 | B2 |
9170173 | Perron et al. | Oct 2015 | B2 |
9240836 | Chen | Jan 2016 | B1 |
9310274 | Nagel et al. | Apr 2016 | B2 |
9341543 | Viswanathan | May 2016 | B2 |
20050226614 | Ogiwara | Oct 2005 | A1 |
20090324249 | Zhang | Dec 2009 | A1 |
20110216996 | Rogers | Sep 2011 | A1 |
20120136660 | Harman et al. | May 2012 | A1 |
20130216176 | Li et al. | Aug 2013 | A1 |
20140212130 | Urban et al. | Jul 2014 | A1 |
20140212131 | Zhang | Jul 2014 | A1 |
20150280855 | Mertz | Oct 2015 | A1 |
Number | Date | Country |
---|---|---|
0981215 | Feb 2000 | EP |
1591768 | Nov 2005 | EP |
2685641 | Jan 2014 | EP |
3404855 | Nov 2018 | EP |
Entry |
---|
“Spectral Grids for WDM Applications: DWDM Frequency Grid”, Series G: Transmission Systems and Media, Digital Systems and Networks Transmission Media and Optical Systems Characteristics—Characteristics of Optical Systems, ITU-T G.694.1 Recommendation, Feb. 2012, 16 pages. |
Bao et al., “Recent Progress in Distributed Fiber Optic Sensors”, Sensors, vol. 12, No. 7, 2012, pp. 8601-8639. |
Extended European Search Report received for corresponding European Patent Application No. 17305570.8, dated Oct. 27, 2017, 9 pages. |
International Search Report and Written Opinion received for corresponding Patent Cooperation Treaty Application No. PCT/EP20181061511, dated Jul. 4, 2018, 13 pages. |
Number | Date | Country | |
---|---|---|---|
20200127735 A1 | Apr 2020 | US |