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Curr. Opt. Photon. 2023; 7(1): 15-20

Published online February 25, 2023 https://doi.org/10.3807/COPP.2023.7.1.15

Copyright © Optical Society of Korea.

Coherent Optical Receiver for Real-time CO-ORMDM Systems

Jae Seung Lee

Department of Electronic Engineering, Kwangwoon University, Seoul 01897, Korea

Corresponding author: *jslee@kw.ac.kr, ORCID 0000-0002-3927-9200

Received: August 19, 2022; Revised: November 22, 2022; Accepted: November 29, 2022

This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/4.0/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

We propose a new coherent optical receiver (COR) to detect optical receiver mode (ORM) subchannels selectively in coherent optical (CO) ORM division multiplexing (ORMDM) systems. In the COORMDM systems, each optical channel is a linear sum of ORM subchannels, to obtain high spectral efficiencies (SEs). The COR uses an ORM subcarrier as its local oscillator (LO) and reads the transmitted data at the origin times of ORM signals. For example, if the mth ORM subcarrier is used as the LO, then the COR reads the data of the mth ORM subchannel. The proposed COR is fast and can make COORMDM systems useful for real-time optical communication with high SE.

Keywords: Coherent optical communication, Optical fiber communication, Optical receivers, Wavelength division multiplexing (WDM)

OCIS codes: (060.0060) Fiber optics and optical communications; (060.2330) Fiber optics communications; (060.2360) Fiber optics links and subsystems; (060.4510) Optical communications

As data-traffic demands grow in areas such as the Internet of Things and artificial intelligence, it is important to increase the spectral efficiencies (SEs) of optical-fiber transmission systems [1, 2]. With the advent of coherent optical (CO) communication systems [3, 4], the SEs of optical communication systems have grown remarkably, greater than 10 bit s−1 Hz−1. The CO communication systems can discriminate the differences in polarizations, amplitudes, frequencies, and phases of received optical signals.

The SE can be enhanced when CO communication systems use the orthogonal frequency-division multiplexing (OFDM) technique [5]; these are called CO-OFDM systems. OFDM uses many closely spaced subcarriers that are modulated independently. CO-OFDM systems have produced high SE records [6, 7], because the CO-OFDM subcarriers are orthogonal to each other and form a complete set. Usually the modulation speed for subcarriers is low, which helps to overcome the optical fiber’s dispersion. However, CO-OFDM suffers from a high peak-to-average power ratio (PAPR) and is sensitive to the phase noises of laser diodes. Most of all, it requires heavy use of digital signal processing (DSP) circuits, which makes its real-time operation difficult [6, 7].

Recently it has been suggested to use a linear sum of optical receiver modes (ORMs) as an optical signal, called an ORM signal [8, 9]. We refer to this kind of multiplexing as ORM division multiplexing (ORMDM). Let’s assume that ORMDM is used in CO-ORMDM systems. Then, the ORMs are inherent modes of the coherent optical receiver (COR) in the CO-ORMDM system [1013]. They are orthogonal to each other and form a complete set as well. Thus the CO-ORMDM can yield high SE values.

In a CO-ORMDM system the optical channel is a linear sum of ORM subchannels, as will be explained in Section II. The ORM subchannels have wider spectra and higher baud rates than those of CO-OFDM systems. Thus the foregoing PAPR and phase noise problems can be mitigated, as in wavelet OFDM [14, 15]. In this case, how is one to detect each ORM subchannel separately, in real time? To this end, we propose a new COR that uses an ORM subcarrier as its local oscillator (LO).

Let us consider the ith optical channel in a CO-ORMDM system. The electric field of this optical channel can be written as e(t) = Re{E(t)exp( it)}, where ωi is the center angular frequency of the ith optical channel, and E(t) is the complex electric field amplitude (CEFA). For a single ORM signal localized at t = 0, E(t) is a linear sum of ORM mode functions ψn(t){n = 0, 1, 2, …} [8]

E(t)=n=0M1anψn(t)

where M is the number of ORMs used for the ORMDM. The complex mode coefficient an includes the data to be transmitted. We call the t = 0 time the origin of this ORM signal [8, 9]. The mode functions are real and complete, satisfying the orthogonality relation [8]

dtψm(t)ψn(t)=δmn

where δmn is the Kronecker delta function.

Taking the Fourier transform of both sides of Eq. (1), we have an alternative form of the ORM signal that is more convenient than Eq. (1) in many cases: ε(ω)= n=0 M1anϕn(ω), where ε(ω) and ϕn(ω) are the CEFA and the nth ORM mode function in the optical frequency domain respectively [8]. The mode functions ϕn(ω){n = 0, 1, 2, …} are also complete and satisfy the orthogonality relation dωϕm*(ω)ϕn(ω)=2πδmn−∞ dωϕ*m(ω)ϕn(ω) = 2πδmn.

With all ORM signals present, the full expression for E(t) can be written as

E(t)= n=0 M1l=a n,lψn(tlT)

where T is the period of the ORM signal, and we use the simplification an,0 = an. The optical channel is a linear sum of ORM subchannels. The CEFA of the mth ORM subchannel is l=am,lψm(tlT). The mth ORM subchannel before its modulation is the mth ORM subcarrier, the CEFA of which is given by l=ψm(tlT). The CEFA of the ORM subcarriers and the origin times are shown in Fig. 1, for the three lowest-order ORMs.

Figure 1.Complex electric field amplitudes of the three lowest-order optical receiver mode subcarriers.

In Fig. 2, we illustrate the proposed COR that detects the mth ORM subchannel of the ith optical channel. This COR will be denoted as CORi,m. Let us first discuss the characteristics of the direct-detection unit (DDU) within the dotted box in Fig. 2. The DDU defines the ORM set, and is the key element of the COR. The optical filter (OF) demultiplexes the received optical wavelength division multiplexing (WDM) channels. The photodetector (PD) is an ideal one, and its frequency response is absorbed by the electrical filter (EF). The EF filters out beat noises generated by the amplified spontaneous emission (ASE) optical noise. The ORMs and related quantities are dependent on the optical channel index i, but we will not use the optical channel index here explicitly, except in CORi,m.

Figure 2.The CORi,m that detects the mth ORM subchannel within the ith optical channel. COR, coherent optical receiver; ORM, optical receiver mode; WDM, wavelength division multiplexing; LO, local oscillator; LD, laser diode; MOD, optical modulator; DDU, direct-detection unit; OF, optical filter; PD, photodetector; EF, electrical filter; DSP, digital signal processing.

If the CEFA at the DDU input is εDD(ω), then the output voltage of the DDU can be evaluated as [10, 13]

yDD(t)=k8π2 dω dω' exp{j(ω'ω)t}εDD*(ω)K(ω,ω')εDD(ω')

The kernel is given by K(ω, ω') = H*o(ω)He(ω' − ω)Ho(ω'); it has the Hermitian property K(ω, ω') = K*(ω', ω). Ho(ω) is the transfer function of the OF between the CEFA input to the OF and the CEFA output from the OF, in the optical frequency domain. He(ω) is the transfer function of the EF between the current input to the EF and the voltage output from the EF, in the optical frequency domain. k is a proportionality constant. ϕn(ω) satisfies the following homogeneous Fredholm integral equation of the 2nd kind with real eigenvalue λn:

ϕn(ω)=λn dω'K(ω,ω')ϕn(ω')

Exact solutions of Eq. (5) are often not available, in which case ϕn(ω) and λn are found numerically [10]. The eigenvalues are positive in general, and increase indefinitely as n increases: λ0 ≤ λ1 ≤ λ2 ≤ ….

As for the CORi,m in Fig. 2, the LO’s output light is proportional to the mth ORM subcarrier having the same center wavelength as the ith optical channel. Only the in-phase detection part is shown, for brevity. The quadrature-phase detection part is hidden, and has the same structure except for the 90° phase shift for the LO [3]. For ease of explanation, we also assume that the received optical WDM channels and the LO have the same polarization.

The transmitted optical WDM channels are applied to the 3-dB coupler, along with the LO light. The two outputs of the 3-dB coupler are directed to the two DDU inputs. The two DDUs use the same kinds of devices and have the same ORM set. Let us assume that the CEFAs at the upper and the lower DDU inputs in the optical frequency domain are ε1(ω) + ε1(ω) and ε1(ω) − ε2(ω) respectively [3]. ε1(ω) is from the optical WDM channels and ε2(ω) is from the LO. If we denote the voltages at the upper and the lower DDU outputs as y+(t) and y(t) respectively, then using Eq. (4) we obtain

y±(t)=k8π2 dω dω' exp{j(ω'ω)t}{ε1*(ω)±ε2*(ω)}K(ω,ω'){ε1(ω')±ε2(ω')}

Then the differential output voltage y(t) = y+(t) − y(t) is

y(t)=k4π2 dω dω' ε1* (ω)K(ω,ω')ε 2 (ω')exp{j(ω'ω)t} +ε 2* (ω)K(ω,ω')ε1 (ω')exp{j(ω'ω)t}

We exchange the integration variables ω and ω' within the first term of Eq. (7) to find

y(t)=k2π2 dω dω'Re ε 2* (ω)K(ω,ω')ε1 (ω')exp{j(ω'ω)t}

where we have used the Hermitian property of K(ω', ω). Equation (8) is the result for the in-phase detection. Changing ε2(ω) to jε2(ω) in Eq. (8), we can also find the result for the quadrature-phase detection. With these two detection results, we can build a complex received signal for the CORi,m as follows:

Ym(t)=k2π2 dω dω'ε2*(ω)K(ω,ω')ε1(ω')exp{j(ω'ω)t}

Now, we assume that only a single ORM signal of the ith optical channel is received, and exclude any crosstalk for the reception of this ORM signal. We use n=0 M1anϕn(ω) as the signal part of ε1(ω). The ASE noise part of ε1(ω) can be expressed as n=0χnϕn(ω). Also, we use a single ORM waveform for the LO: ε2(ω) = cmϕm(ω), where cm is a complex constant. Then we obtain

Ym(t)=4cm* n=0 M1(an+χn)ymn(t)+ n=Mχnymn(t)

where ymn(t) is defined as [8, 9]

Ym(0)=kcm*(am+χm)/πλm

Since ymn(0) = δmnk / 4πλm, we have

Ym(0)=kcm*(am+χm)/πλm

which is our main result. It tells us that at t = 0 we can find the transmitted data of the mth ORM subchannel directly, without the heavy use of DSP circuits. Note that this property is unique to the CO-ORMDM, because of the kernel K(ω, ω') in Eq. (11). The t = 0 time point is equal to the origin of the ORM signal Eq. (1). If we regard the maximum point of the zeroth ORM waveform as the center of the ORM signal, each origin time in Fig. 1 has an offset from the center of the corresponding ORM signal, reflecting the delay of the DDU filters.

Let us decompose the mode coefficient am as am = γζmzm, where zm is the transmitted data. γ is a proportionality constant, and ζm is a dimensionless real constant related to the optical power of the ORM subchannel. The mode coefficient χm is decomposed as χm = γnm, where nm is a dimensionless zero-mean complex Gaussian random variable. All of the real and imaginary parts of {n0, n1, n2, ...} are mutually independent of each other, having identical variance [10]. With these decompositions we obtain

Y¯m(0)=zm+nm/ζm

where m(t) = Ym(t)πλm / c*mγζmk. Only the mth ORM contributions appear in Eq. (13), for both the signal and the ASE noise. In addition, we need to include the effects from other ORM signals in the same and adjacent optical channels, and we need to use the full subcarrier expression for the LO. These modifications will add crosstalk terms to the right-hand side of Eq. (13). The phase and the polarization diversities can be included as per [3].

In this section we present the waveforms of Ym(t) for the foregoing case of single-ORM-signal input. We assume that Ho(ω) and He(ω) are Gaussian [13]. The eigenvalue of the mth ORM is λm = λ0 / qm , where q is a positive quantity smaller than 1. The expressions for λ0 and q are in [13]. From Eq. (12), Ym(0) is proportional to qm. To use higher-order ORMs, we need to use high q values, which can be done by decreasing the EF bandwidth compared to the OF bandwidth [13]. Thus we choose 3-dB bandwidths |Ho (ω)|2 and |He(ω)|2 as 100 GHz and 10 GHz respectively, which gives q = 0.754. For simplicity, we set ζm = 1 for all m. Neglecting the ASE, we have from Eq. (10)

Y¯m(t)= n=0 M1znymn(t)/qmyc

where yc = k / 4πλ0 [8]. We show the real and imaginary parts of m(t) in Fig. 3, denoted as Rm(t) and Im(t) respectively. We set M = 3 with z0 = 1 + j, z1 = −1 + 3j, and z2 = 3 + j. Note that m(0) = zm for m = 0, 1, 2, 3, where z3 = 0 naturally.

Figure 3.Real and imaginary parts of the waveforms of m(t), denoted as Rm(t) and Im(t) respectively. The three lowest-order optical receiver mode subchannels are transmitted (M = 3) with z0 = 1 + j, z1 = −1 + 3j, and z2 = 3 + j. (a) m = 0, (b) m = 1, (c) m = 2, (d) m = 3.

The proposed COR can be applied to conventional optical communication systems, to upgrade their SEs. From the ORMDM point of view, the optical signal of a conventional optical channel, excluding the OFDM, can be regarded as an ORM signal with an {n = 0, 1, 2, …} dependent on each other. If one of the ORMs (say the mth ORM) has an independent am, we have more freedom and can increase the SE. In this case we need two CORs. One uses the mth ORM subcarrier as its LO, while the other uses the sum of the rest of the ORM subcarriers as its LO. This procedure can be extended to other ORMs, until the ORMDM is fully utilized.

The COR can be used in multiple-access networks [16]. If only one ORM subchannel is to be dropped at an optical node, for example, we use one COR at that node.

If we detect multiple optical channels and ORM subchannels, we use a WDM demultiplexer (DMUX) and place optical splitters after the WDM DMUX, as shown in Fig. 4. We place one COR at the end of each optical-splitter arm. The optical splitters can be integrated [17], and their losses can be compensated by the optical amplifier (OA) before the WDM DMUX. We can also use gain materials for the optical splitter [18]. If we use the WDM DMUX as the DDU’s OF in Fig. 2, we may remove all OFs from within the CORs. Then the modulation signal to obtain the LO in Fig. 2 is modified to make the LO light seem as if it has passed the OF already.

Figure 4.Receiver side of a CO-ORMDM system to detect multiple optical channels and ORM subchannels. CO, coherent optical; ORM, optical receiver mode; ORMDM, ORM division multiplexing; OA, optical amplifier; WDM, wavelength division multiplexing; DMUX, demultiplexer; COR, coherent optical receiver.

We perform numerical simulations for the foregoing CO-ORMDM system. The 256-quadrature amplitude modulation (QAM) code is used for the modulation of the ORM subcarriers. The optical channel power is fixed here by allocating smaller optical power evenly to the ORM subchannels as M is increased from 1 to 12. Thus we set ζm=1/M in Eq. (13). For M = 1, we assume that the ASE noise term in Eq. (13) is below 5% of the minimum constellation distance (MCD). If we want to get error-free results in this case, the crosstalk fluctuations should be kept below 45% of the MCD. Under this condition, we have a SE of 6.0 bit s−1 Hz−1. For M = 6, the ASE noise term in Eq. (13) is below 8.7% of the MCD, and we have a SE of 9.8 bit s−1 Hz−1. Similarly, for M = 12 SE is 11.0 bit s−1 Hz−1 and exhibits saturation behavior. If the ORM subchannels have unequal optical powers and unequal QAM codes, we can further increase the SE. Also, with forward error-correction methods the SE can be increased even further [4, 19].

In contrast to CO-OFDM, real-time operation is possible in our CO-ORMDM system. The speed of the CORs in our CO-ORMDM system is not limited by the DSP circuits, as Eq. (12) shows. As for the transmitter of the CO-ORMDM system, we may use a single in-phase/quadrature optical modulator driven by two digital-to-analog converters (DACs) to produce one or a few subchannels. Then the DSP circuit limits can be avoided, and real-time operation can be attained. The digital inputs to the DACs can be modified to pre-compensate for the optical-fiber dispersion, etc. As a reference, a 100 GS/s DAC can generate electrical signals that are about 25 GHz in bandwidth [20].

To increase the channel bandwidth beyond the limit of the DACs, we can use optical arbitrary-waveform generators (OAWGs) to obtain ORM subcarriers from mode-locked laser diodes [2123]. Modulating the ORM subcarriers, we get ORM subchannels. Also, there is no limit from the DSP circuits in this case.

To make the proposed CO-ORMDM system more practical, we could integrate photonic devices. Similar works have been done for conventional COR [24, 25].

Building each optical channel as a linear sum of multiple ORM subchannels, CO-ORMDM systems can attain high SEs. To detect the ORM subchannels selectively, we have introduced a new COR that is fast and does not require heavy use of DSP circuits. Thus, in contrast to CO-OFDM, real-time operation is possible in our CO-ORMDM system. In addition, we can use OAWGs to increase the channel bandwidth beyond the limit of the DACs. With photonic integration, CO-ORMDM systems using the proposed CORs can be made simple and practical.

Data underlying the results presented in this paper are not publicly available at the time of publication, but may be obtained from the authors upon reasonable request.

The work reported in this paper was conducted during the sabbatical year of Kwangwoon University in 2019.

The author received no financial support for the research, authorship, or publication of this article.

  1. W. Klaus, P. J. Winzer, and K. Nakajima, “The role of parallelism in the evolution of optical fiber communication systems,” Proc. IEEE 110, 1619-1654 (2022).
    CrossRef
  2. B. J. Puttnam, R. S. Luís, G. Rademacher, M. Mendez-Astudillio, Y. Awaji, and H. Furukawa, “S, C- and L-band transmission over a 157 nm bandwidth using doped fiber and distributed Raman amplification,” Opt. Express 39, 10011-10018 (2022).
    Pubmed CrossRef
  3. K. Kikuchi, “Fundamentals of coherent optical fiber communications,” J. Light. Technol. 34, 157-179 (2016).
    CrossRef
  4. P. J. Winzer, “High-spectral-efficiency optical modulation formats,” J. Light. Technol. 30, 3824-3835 (2012).
    CrossRef
  5. I. B. Djordjevic and B. Vasic, “Orthogonal frequency division multiplexing for high-speed optical transmission,” Opt. Express 14, 3767-3775 (2006).
    Pubmed CrossRef
  6. D. Qian, M.-F. Huang, E. Ip, Y.-K. Huang, Y. Shao, J. Hu, and T. Wang, “101.7-Tb/s (370×294-Gb/s) PDM-128QAM-OFDM transmission over 3×55-km SSMF using pilot-based Phase noise mitigation,” in Optical Fiber Communication Conf. Technical Digest 2011 (Optical Society of America, 2011), Paper PDPB5.
    CrossRef
  7. T. Omiya, M. Yoshida, and M. Nakazawa, “400 Gbit/s 256 QAM-OFDM transmission over 720 km with a 14 bit/s/Hz spectral efficiency by using high-resolution FDE,” Opt. Express 21, 2632-2641 (2013).
    Pubmed CrossRef
  8. J. S. Lee, “Optical signals using superposition of optical receiver modes,” Curr. Opt. Photonics 1, 308-314 (2017).
  9. B. Batsuren, K. H. Seo, and J. S. Lee, “Optical communication using linear sums of optical receiver modes: proof of concept,” IEEE Photonics Technol. Lett. 30, 1707-1710 (2018).
    CrossRef
  10. J. S. Lee and C. S. Shim, “Bit-error-rate analysis of optically preamplified receivers using an eigenfunction expansion method in optical frequency domain,” J. Light. Technol. 12, 1224-1229 (1994).
    CrossRef
  11. E. Forestieri, “Evaluating the error probability in lightwave systems with chromatic dispersion, arbitrary pulse shape and pre- and postdetection filtering,” J. Light. Technol. 18, 1493-1503 (2000).
    CrossRef
  12. R. Holzlohner, V. S. Grigoryan, C. R. Menyuk, and W. L. Kath, “Accurate calculation of eye diagrams and bit error rates in optical transmission systems using linearization,” J. Light. Technol. 20, 389-400 (2002).
    CrossRef
  13. J. S. Lee and A. E. Willner, “Analysis of Gaussian optical receivers,” J. Light. Technol. 31, 2687-2693 (2013).
    CrossRef
  14. A. Li, W. Shieh, and R. Tucker, “Wavelet packet transform-based OFDM for optical communications,” J. Light. Technol. 28, 3519-3528 (2010).
  15. A. Güner and A. Özen, “Lifting wavelet transform based multicarrier modulation scheme for coherent optical communication systems,” J. Light. Technol. 39, 4255-4261 (2021).
    CrossRef
  16. E. Wong, “Next-generation broadband access networks and technologies,” J. Light. Technol. 30, 597-608 (2012).
    CrossRef
  17. K. Nara, N. Matsubara, and H. Kawashima, “Monolithically integrated 1×32 optical splitter/router using low loss ripple MZI-based WDM filter and low loss Y-branch circuit,” in Optical Fiber Communication Conference 2006 (Optical Society of America, 2006), paper OWO1.
    CrossRef
  18. J. D. B. Bradley, R. Stoffer, A. Bakker, L. Agazzi, F. Ay, K. Wörhoff, and M. Pollnau, “Integrated Al2O3:Er3+ zero-loss optical amplifier and power splitter with 40-nm bandwidth,” IEEE Photonics Technol. Lett. 22, 278-280 (2010).
    CrossRef
  19. S. Y. Kim, K. H. Seo, and J. S. Lee, “Spectral efficiencies of channel-interleaved bidirectional and unidirectional ultradense WDM for metro applications,” J. Light. Technol. 30, 229-233 (2012).
    CrossRef
  20. H. Huang, J. Heilmeyer, M. Grozing, M. Berroth, J. Leibrich, and W. Rosenkranz, “An 8-bit 100-GS/s Distributed DAC in 28-nm CMOS for optical communications,” IEEE Trans. Microw. Theory Tech. 63, 1211-1218 (2015).
    CrossRef
  21. S. T. Cundiff and A. M. Weiner, “Optical arbitrary waveform generation,” Nat. Photonics 4, 760-767 (2010).
    CrossRef
  22. J. Dunayevsky and D. M. Marom, “MEMS spatial light modulator for phase and amplitude modulation of spectrally dispersed light,” J. Microelectromech. Syst. 22, 1213-1221 (2013).
    CrossRef
  23. H. Tsuda, Y. Tanaka, T. Shioda, and T. Kurokawa, “Analog and digital optical pulse synthesizers using arrayed-waveguide gratings for high-speed optical signal processing,” J. Light. Technol. 26, 670-677 (2008).
    CrossRef
  24. Z. Xuan and F. Aflatouni, “Integrated coherent optical receiver with feed-forward carrier recovery,” Opt. Express 28, 16073-16088 (2020).
    Pubmed CrossRef
  25. Y. Wang, X. Li, Z. Jiang, L. Tong, W. Deng, X. Gao, X. Huang, H. Zhou, Y. Yu, L. Ye, X. Xiao, and X. Zhang, “Ultrahigh-speed graphene-based optical coherent receiver,” Nat. Commun. 12, 5076 (2021).
    Pubmed KoreaMed CrossRef

Article

Article

Curr. Opt. Photon. 2023; 7(1): 15-20

Published online February 25, 2023 https://doi.org/10.3807/COPP.2023.7.1.15

Copyright © Optical Society of Korea.

Coherent Optical Receiver for Real-time CO-ORMDM Systems

Jae Seung Lee

Department of Electronic Engineering, Kwangwoon University, Seoul 01897, Korea

Correspondence to:*jslee@kw.ac.kr, ORCID 0000-0002-3927-9200

Received: August 19, 2022; Revised: November 22, 2022; Accepted: November 29, 2022

This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/4.0/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

We propose a new coherent optical receiver (COR) to detect optical receiver mode (ORM) subchannels selectively in coherent optical (CO) ORM division multiplexing (ORMDM) systems. In the COORMDM systems, each optical channel is a linear sum of ORM subchannels, to obtain high spectral efficiencies (SEs). The COR uses an ORM subcarrier as its local oscillator (LO) and reads the transmitted data at the origin times of ORM signals. For example, if the mth ORM subcarrier is used as the LO, then the COR reads the data of the mth ORM subchannel. The proposed COR is fast and can make COORMDM systems useful for real-time optical communication with high SE.

Keywords: Coherent optical communication, Optical fiber communication, Optical receivers, Wavelength division multiplexing (WDM)

I. INTRODUCTION

As data-traffic demands grow in areas such as the Internet of Things and artificial intelligence, it is important to increase the spectral efficiencies (SEs) of optical-fiber transmission systems [1, 2]. With the advent of coherent optical (CO) communication systems [3, 4], the SEs of optical communication systems have grown remarkably, greater than 10 bit s−1 Hz−1. The CO communication systems can discriminate the differences in polarizations, amplitudes, frequencies, and phases of received optical signals.

The SE can be enhanced when CO communication systems use the orthogonal frequency-division multiplexing (OFDM) technique [5]; these are called CO-OFDM systems. OFDM uses many closely spaced subcarriers that are modulated independently. CO-OFDM systems have produced high SE records [6, 7], because the CO-OFDM subcarriers are orthogonal to each other and form a complete set. Usually the modulation speed for subcarriers is low, which helps to overcome the optical fiber’s dispersion. However, CO-OFDM suffers from a high peak-to-average power ratio (PAPR) and is sensitive to the phase noises of laser diodes. Most of all, it requires heavy use of digital signal processing (DSP) circuits, which makes its real-time operation difficult [6, 7].

Recently it has been suggested to use a linear sum of optical receiver modes (ORMs) as an optical signal, called an ORM signal [8, 9]. We refer to this kind of multiplexing as ORM division multiplexing (ORMDM). Let’s assume that ORMDM is used in CO-ORMDM systems. Then, the ORMs are inherent modes of the coherent optical receiver (COR) in the CO-ORMDM system [1013]. They are orthogonal to each other and form a complete set as well. Thus the CO-ORMDM can yield high SE values.

In a CO-ORMDM system the optical channel is a linear sum of ORM subchannels, as will be explained in Section II. The ORM subchannels have wider spectra and higher baud rates than those of CO-OFDM systems. Thus the foregoing PAPR and phase noise problems can be mitigated, as in wavelet OFDM [14, 15]. In this case, how is one to detect each ORM subchannel separately, in real time? To this end, we propose a new COR that uses an ORM subcarrier as its local oscillator (LO).

II. ORMDM

Let us consider the ith optical channel in a CO-ORMDM system. The electric field of this optical channel can be written as e(t) = Re{E(t)exp( it)}, where ωi is the center angular frequency of the ith optical channel, and E(t) is the complex electric field amplitude (CEFA). For a single ORM signal localized at t = 0, E(t) is a linear sum of ORM mode functions ψn(t){n = 0, 1, 2, …} [8]

E(t)=n=0M1anψn(t)

where M is the number of ORMs used for the ORMDM. The complex mode coefficient an includes the data to be transmitted. We call the t = 0 time the origin of this ORM signal [8, 9]. The mode functions are real and complete, satisfying the orthogonality relation [8]

dtψm(t)ψn(t)=δmn

where δmn is the Kronecker delta function.

Taking the Fourier transform of both sides of Eq. (1), we have an alternative form of the ORM signal that is more convenient than Eq. (1) in many cases: ε(ω)= n=0 M1anϕn(ω), where ε(ω) and ϕn(ω) are the CEFA and the nth ORM mode function in the optical frequency domain respectively [8]. The mode functions ϕn(ω){n = 0, 1, 2, …} are also complete and satisfy the orthogonality relation dωϕm*(ω)ϕn(ω)=2πδmn−∞ dωϕ*m(ω)ϕn(ω) = 2πδmn.

With all ORM signals present, the full expression for E(t) can be written as

E(t)= n=0 M1l=a n,lψn(tlT)

where T is the period of the ORM signal, and we use the simplification an,0 = an. The optical channel is a linear sum of ORM subchannels. The CEFA of the mth ORM subchannel is l=am,lψm(tlT). The mth ORM subchannel before its modulation is the mth ORM subcarrier, the CEFA of which is given by l=ψm(tlT). The CEFA of the ORM subcarriers and the origin times are shown in Fig. 1, for the three lowest-order ORMs.

Figure 1. Complex electric field amplitudes of the three lowest-order optical receiver mode subcarriers.

III. PROPOSED COR

In Fig. 2, we illustrate the proposed COR that detects the mth ORM subchannel of the ith optical channel. This COR will be denoted as CORi,m. Let us first discuss the characteristics of the direct-detection unit (DDU) within the dotted box in Fig. 2. The DDU defines the ORM set, and is the key element of the COR. The optical filter (OF) demultiplexes the received optical wavelength division multiplexing (WDM) channels. The photodetector (PD) is an ideal one, and its frequency response is absorbed by the electrical filter (EF). The EF filters out beat noises generated by the amplified spontaneous emission (ASE) optical noise. The ORMs and related quantities are dependent on the optical channel index i, but we will not use the optical channel index here explicitly, except in CORi,m.

Figure 2. The CORi,m that detects the mth ORM subchannel within the ith optical channel. COR, coherent optical receiver; ORM, optical receiver mode; WDM, wavelength division multiplexing; LO, local oscillator; LD, laser diode; MOD, optical modulator; DDU, direct-detection unit; OF, optical filter; PD, photodetector; EF, electrical filter; DSP, digital signal processing.

If the CEFA at the DDU input is εDD(ω), then the output voltage of the DDU can be evaluated as [10, 13]

yDD(t)=k8π2 dω dω' exp{j(ω'ω)t}εDD*(ω)K(ω,ω')εDD(ω')

The kernel is given by K(ω, ω') = H*o(ω)He(ω' − ω)Ho(ω'); it has the Hermitian property K(ω, ω') = K*(ω', ω). Ho(ω) is the transfer function of the OF between the CEFA input to the OF and the CEFA output from the OF, in the optical frequency domain. He(ω) is the transfer function of the EF between the current input to the EF and the voltage output from the EF, in the optical frequency domain. k is a proportionality constant. ϕn(ω) satisfies the following homogeneous Fredholm integral equation of the 2nd kind with real eigenvalue λn:

ϕn(ω)=λn dω'K(ω,ω')ϕn(ω')

Exact solutions of Eq. (5) are often not available, in which case ϕn(ω) and λn are found numerically [10]. The eigenvalues are positive in general, and increase indefinitely as n increases: λ0 ≤ λ1 ≤ λ2 ≤ ….

As for the CORi,m in Fig. 2, the LO’s output light is proportional to the mth ORM subcarrier having the same center wavelength as the ith optical channel. Only the in-phase detection part is shown, for brevity. The quadrature-phase detection part is hidden, and has the same structure except for the 90° phase shift for the LO [3]. For ease of explanation, we also assume that the received optical WDM channels and the LO have the same polarization.

The transmitted optical WDM channels are applied to the 3-dB coupler, along with the LO light. The two outputs of the 3-dB coupler are directed to the two DDU inputs. The two DDUs use the same kinds of devices and have the same ORM set. Let us assume that the CEFAs at the upper and the lower DDU inputs in the optical frequency domain are ε1(ω) + ε1(ω) and ε1(ω) − ε2(ω) respectively [3]. ε1(ω) is from the optical WDM channels and ε2(ω) is from the LO. If we denote the voltages at the upper and the lower DDU outputs as y+(t) and y(t) respectively, then using Eq. (4) we obtain

y±(t)=k8π2 dω dω' exp{j(ω'ω)t}{ε1*(ω)±ε2*(ω)}K(ω,ω'){ε1(ω')±ε2(ω')}

Then the differential output voltage y(t) = y+(t) − y(t) is

y(t)=k4π2 dω dω' ε1* (ω)K(ω,ω')ε 2 (ω')exp{j(ω'ω)t} +ε 2* (ω)K(ω,ω')ε1 (ω')exp{j(ω'ω)t}

We exchange the integration variables ω and ω' within the first term of Eq. (7) to find

y(t)=k2π2 dω dω'Re ε 2* (ω)K(ω,ω')ε1 (ω')exp{j(ω'ω)t}

where we have used the Hermitian property of K(ω', ω). Equation (8) is the result for the in-phase detection. Changing ε2(ω) to jε2(ω) in Eq. (8), we can also find the result for the quadrature-phase detection. With these two detection results, we can build a complex received signal for the CORi,m as follows:

Ym(t)=k2π2 dω dω'ε2*(ω)K(ω,ω')ε1(ω')exp{j(ω'ω)t}

Now, we assume that only a single ORM signal of the ith optical channel is received, and exclude any crosstalk for the reception of this ORM signal. We use n=0 M1anϕn(ω) as the signal part of ε1(ω). The ASE noise part of ε1(ω) can be expressed as n=0χnϕn(ω). Also, we use a single ORM waveform for the LO: ε2(ω) = cmϕm(ω), where cm is a complex constant. Then we obtain

Ym(t)=4cm* n=0 M1(an+χn)ymn(t)+ n=Mχnymn(t)

where ymn(t) is defined as [8, 9]

Ym(0)=kcm*(am+χm)/πλm

Since ymn(0) = δmnk / 4πλm, we have

Ym(0)=kcm*(am+χm)/πλm

which is our main result. It tells us that at t = 0 we can find the transmitted data of the mth ORM subchannel directly, without the heavy use of DSP circuits. Note that this property is unique to the CO-ORMDM, because of the kernel K(ω, ω') in Eq. (11). The t = 0 time point is equal to the origin of the ORM signal Eq. (1). If we regard the maximum point of the zeroth ORM waveform as the center of the ORM signal, each origin time in Fig. 1 has an offset from the center of the corresponding ORM signal, reflecting the delay of the DDU filters.

Let us decompose the mode coefficient am as am = γζmzm, where zm is the transmitted data. γ is a proportionality constant, and ζm is a dimensionless real constant related to the optical power of the ORM subchannel. The mode coefficient χm is decomposed as χm = γnm, where nm is a dimensionless zero-mean complex Gaussian random variable. All of the real and imaginary parts of {n0, n1, n2, ...} are mutually independent of each other, having identical variance [10]. With these decompositions we obtain

Y¯m(0)=zm+nm/ζm

where m(t) = Ym(t)πλm / c*mγζmk. Only the mth ORM contributions appear in Eq. (13), for both the signal and the ASE noise. In addition, we need to include the effects from other ORM signals in the same and adjacent optical channels, and we need to use the full subcarrier expression for the LO. These modifications will add crosstalk terms to the right-hand side of Eq. (13). The phase and the polarization diversities can be included as per [3].

IV. RECEIVED WAVEFORMS

In this section we present the waveforms of Ym(t) for the foregoing case of single-ORM-signal input. We assume that Ho(ω) and He(ω) are Gaussian [13]. The eigenvalue of the mth ORM is λm = λ0 / qm , where q is a positive quantity smaller than 1. The expressions for λ0 and q are in [13]. From Eq. (12), Ym(0) is proportional to qm. To use higher-order ORMs, we need to use high q values, which can be done by decreasing the EF bandwidth compared to the OF bandwidth [13]. Thus we choose 3-dB bandwidths |Ho (ω)|2 and |He(ω)|2 as 100 GHz and 10 GHz respectively, which gives q = 0.754. For simplicity, we set ζm = 1 for all m. Neglecting the ASE, we have from Eq. (10)

Y¯m(t)= n=0 M1znymn(t)/qmyc

where yc = k / 4πλ0 [8]. We show the real and imaginary parts of m(t) in Fig. 3, denoted as Rm(t) and Im(t) respectively. We set M = 3 with z0 = 1 + j, z1 = −1 + 3j, and z2 = 3 + j. Note that m(0) = zm for m = 0, 1, 2, 3, where z3 = 0 naturally.

Figure 3. Real and imaginary parts of the waveforms of m(t), denoted as Rm(t) and Im(t) respectively. The three lowest-order optical receiver mode subchannels are transmitted (M = 3) with z0 = 1 + j, z1 = −1 + 3j, and z2 = 3 + j. (a) m = 0, (b) m = 1, (c) m = 2, (d) m = 3.

V. DISCUSSION

The proposed COR can be applied to conventional optical communication systems, to upgrade their SEs. From the ORMDM point of view, the optical signal of a conventional optical channel, excluding the OFDM, can be regarded as an ORM signal with an {n = 0, 1, 2, …} dependent on each other. If one of the ORMs (say the mth ORM) has an independent am, we have more freedom and can increase the SE. In this case we need two CORs. One uses the mth ORM subcarrier as its LO, while the other uses the sum of the rest of the ORM subcarriers as its LO. This procedure can be extended to other ORMs, until the ORMDM is fully utilized.

The COR can be used in multiple-access networks [16]. If only one ORM subchannel is to be dropped at an optical node, for example, we use one COR at that node.

If we detect multiple optical channels and ORM subchannels, we use a WDM demultiplexer (DMUX) and place optical splitters after the WDM DMUX, as shown in Fig. 4. We place one COR at the end of each optical-splitter arm. The optical splitters can be integrated [17], and their losses can be compensated by the optical amplifier (OA) before the WDM DMUX. We can also use gain materials for the optical splitter [18]. If we use the WDM DMUX as the DDU’s OF in Fig. 2, we may remove all OFs from within the CORs. Then the modulation signal to obtain the LO in Fig. 2 is modified to make the LO light seem as if it has passed the OF already.

Figure 4. Receiver side of a CO-ORMDM system to detect multiple optical channels and ORM subchannels. CO, coherent optical; ORM, optical receiver mode; ORMDM, ORM division multiplexing; OA, optical amplifier; WDM, wavelength division multiplexing; DMUX, demultiplexer; COR, coherent optical receiver.

We perform numerical simulations for the foregoing CO-ORMDM system. The 256-quadrature amplitude modulation (QAM) code is used for the modulation of the ORM subcarriers. The optical channel power is fixed here by allocating smaller optical power evenly to the ORM subchannels as M is increased from 1 to 12. Thus we set ζm=1/M in Eq. (13). For M = 1, we assume that the ASE noise term in Eq. (13) is below 5% of the minimum constellation distance (MCD). If we want to get error-free results in this case, the crosstalk fluctuations should be kept below 45% of the MCD. Under this condition, we have a SE of 6.0 bit s−1 Hz−1. For M = 6, the ASE noise term in Eq. (13) is below 8.7% of the MCD, and we have a SE of 9.8 bit s−1 Hz−1. Similarly, for M = 12 SE is 11.0 bit s−1 Hz−1 and exhibits saturation behavior. If the ORM subchannels have unequal optical powers and unequal QAM codes, we can further increase the SE. Also, with forward error-correction methods the SE can be increased even further [4, 19].

In contrast to CO-OFDM, real-time operation is possible in our CO-ORMDM system. The speed of the CORs in our CO-ORMDM system is not limited by the DSP circuits, as Eq. (12) shows. As for the transmitter of the CO-ORMDM system, we may use a single in-phase/quadrature optical modulator driven by two digital-to-analog converters (DACs) to produce one or a few subchannels. Then the DSP circuit limits can be avoided, and real-time operation can be attained. The digital inputs to the DACs can be modified to pre-compensate for the optical-fiber dispersion, etc. As a reference, a 100 GS/s DAC can generate electrical signals that are about 25 GHz in bandwidth [20].

To increase the channel bandwidth beyond the limit of the DACs, we can use optical arbitrary-waveform generators (OAWGs) to obtain ORM subcarriers from mode-locked laser diodes [2123]. Modulating the ORM subcarriers, we get ORM subchannels. Also, there is no limit from the DSP circuits in this case.

To make the proposed CO-ORMDM system more practical, we could integrate photonic devices. Similar works have been done for conventional COR [24, 25].

VI. CONCLUSION

Building each optical channel as a linear sum of multiple ORM subchannels, CO-ORMDM systems can attain high SEs. To detect the ORM subchannels selectively, we have introduced a new COR that is fast and does not require heavy use of DSP circuits. Thus, in contrast to CO-OFDM, real-time operation is possible in our CO-ORMDM system. In addition, we can use OAWGs to increase the channel bandwidth beyond the limit of the DACs. With photonic integration, CO-ORMDM systems using the proposed CORs can be made simple and practical.

DISCLOSURES

The author declares no conflicts of interest.

DATA AVAILABILITY

Data underlying the results presented in this paper are not publicly available at the time of publication, but may be obtained from the authors upon reasonable request.

ACKNOWLEDGMENT

The work reported in this paper was conducted during the sabbatical year of Kwangwoon University in 2019.

FUNDING

The author received no financial support for the research, authorship, or publication of this article.

Fig 1.

Figure 1.Complex electric field amplitudes of the three lowest-order optical receiver mode subcarriers.
Current Optics and Photonics 2023; 7: 15-20https://doi.org/10.3807/COPP.2023.7.1.15

Fig 2.

Figure 2.The CORi,m that detects the mth ORM subchannel within the ith optical channel. COR, coherent optical receiver; ORM, optical receiver mode; WDM, wavelength division multiplexing; LO, local oscillator; LD, laser diode; MOD, optical modulator; DDU, direct-detection unit; OF, optical filter; PD, photodetector; EF, electrical filter; DSP, digital signal processing.
Current Optics and Photonics 2023; 7: 15-20https://doi.org/10.3807/COPP.2023.7.1.15

Fig 3.

Figure 3.Real and imaginary parts of the waveforms of m(t), denoted as Rm(t) and Im(t) respectively. The three lowest-order optical receiver mode subchannels are transmitted (M = 3) with z0 = 1 + j, z1 = −1 + 3j, and z2 = 3 + j. (a) m = 0, (b) m = 1, (c) m = 2, (d) m = 3.
Current Optics and Photonics 2023; 7: 15-20https://doi.org/10.3807/COPP.2023.7.1.15

Fig 4.

Figure 4.Receiver side of a CO-ORMDM system to detect multiple optical channels and ORM subchannels. CO, coherent optical; ORM, optical receiver mode; ORMDM, ORM division multiplexing; OA, optical amplifier; WDM, wavelength division multiplexing; DMUX, demultiplexer; COR, coherent optical receiver.
Current Optics and Photonics 2023; 7: 15-20https://doi.org/10.3807/COPP.2023.7.1.15

References

  1. W. Klaus, P. J. Winzer, and K. Nakajima, “The role of parallelism in the evolution of optical fiber communication systems,” Proc. IEEE 110, 1619-1654 (2022).
    CrossRef
  2. B. J. Puttnam, R. S. Luís, G. Rademacher, M. Mendez-Astudillio, Y. Awaji, and H. Furukawa, “S, C- and L-band transmission over a 157 nm bandwidth using doped fiber and distributed Raman amplification,” Opt. Express 39, 10011-10018 (2022).
    Pubmed CrossRef
  3. K. Kikuchi, “Fundamentals of coherent optical fiber communications,” J. Light. Technol. 34, 157-179 (2016).
    CrossRef
  4. P. J. Winzer, “High-spectral-efficiency optical modulation formats,” J. Light. Technol. 30, 3824-3835 (2012).
    CrossRef
  5. I. B. Djordjevic and B. Vasic, “Orthogonal frequency division multiplexing for high-speed optical transmission,” Opt. Express 14, 3767-3775 (2006).
    Pubmed CrossRef
  6. D. Qian, M.-F. Huang, E. Ip, Y.-K. Huang, Y. Shao, J. Hu, and T. Wang, “101.7-Tb/s (370×294-Gb/s) PDM-128QAM-OFDM transmission over 3×55-km SSMF using pilot-based Phase noise mitigation,” in Optical Fiber Communication Conf. Technical Digest 2011 (Optical Society of America, 2011), Paper PDPB5.
    CrossRef
  7. T. Omiya, M. Yoshida, and M. Nakazawa, “400 Gbit/s 256 QAM-OFDM transmission over 720 km with a 14 bit/s/Hz spectral efficiency by using high-resolution FDE,” Opt. Express 21, 2632-2641 (2013).
    Pubmed CrossRef
  8. J. S. Lee, “Optical signals using superposition of optical receiver modes,” Curr. Opt. Photonics 1, 308-314 (2017).
  9. B. Batsuren, K. H. Seo, and J. S. Lee, “Optical communication using linear sums of optical receiver modes: proof of concept,” IEEE Photonics Technol. Lett. 30, 1707-1710 (2018).
    CrossRef
  10. J. S. Lee and C. S. Shim, “Bit-error-rate analysis of optically preamplified receivers using an eigenfunction expansion method in optical frequency domain,” J. Light. Technol. 12, 1224-1229 (1994).
    CrossRef
  11. E. Forestieri, “Evaluating the error probability in lightwave systems with chromatic dispersion, arbitrary pulse shape and pre- and postdetection filtering,” J. Light. Technol. 18, 1493-1503 (2000).
    CrossRef
  12. R. Holzlohner, V. S. Grigoryan, C. R. Menyuk, and W. L. Kath, “Accurate calculation of eye diagrams and bit error rates in optical transmission systems using linearization,” J. Light. Technol. 20, 389-400 (2002).
    CrossRef
  13. J. S. Lee and A. E. Willner, “Analysis of Gaussian optical receivers,” J. Light. Technol. 31, 2687-2693 (2013).
    CrossRef
  14. A. Li, W. Shieh, and R. Tucker, “Wavelet packet transform-based OFDM for optical communications,” J. Light. Technol. 28, 3519-3528 (2010).
  15. A. Güner and A. Özen, “Lifting wavelet transform based multicarrier modulation scheme for coherent optical communication systems,” J. Light. Technol. 39, 4255-4261 (2021).
    CrossRef
  16. E. Wong, “Next-generation broadband access networks and technologies,” J. Light. Technol. 30, 597-608 (2012).
    CrossRef
  17. K. Nara, N. Matsubara, and H. Kawashima, “Monolithically integrated 1×32 optical splitter/router using low loss ripple MZI-based WDM filter and low loss Y-branch circuit,” in Optical Fiber Communication Conference 2006 (Optical Society of America, 2006), paper OWO1.
    CrossRef
  18. J. D. B. Bradley, R. Stoffer, A. Bakker, L. Agazzi, F. Ay, K. Wörhoff, and M. Pollnau, “Integrated Al2O3:Er3+ zero-loss optical amplifier and power splitter with 40-nm bandwidth,” IEEE Photonics Technol. Lett. 22, 278-280 (2010).
    CrossRef
  19. S. Y. Kim, K. H. Seo, and J. S. Lee, “Spectral efficiencies of channel-interleaved bidirectional and unidirectional ultradense WDM for metro applications,” J. Light. Technol. 30, 229-233 (2012).
    CrossRef
  20. H. Huang, J. Heilmeyer, M. Grozing, M. Berroth, J. Leibrich, and W. Rosenkranz, “An 8-bit 100-GS/s Distributed DAC in 28-nm CMOS for optical communications,” IEEE Trans. Microw. Theory Tech. 63, 1211-1218 (2015).
    CrossRef
  21. S. T. Cundiff and A. M. Weiner, “Optical arbitrary waveform generation,” Nat. Photonics 4, 760-767 (2010).
    CrossRef
  22. J. Dunayevsky and D. M. Marom, “MEMS spatial light modulator for phase and amplitude modulation of spectrally dispersed light,” J. Microelectromech. Syst. 22, 1213-1221 (2013).
    CrossRef
  23. H. Tsuda, Y. Tanaka, T. Shioda, and T. Kurokawa, “Analog and digital optical pulse synthesizers using arrayed-waveguide gratings for high-speed optical signal processing,” J. Light. Technol. 26, 670-677 (2008).
    CrossRef
  24. Z. Xuan and F. Aflatouni, “Integrated coherent optical receiver with feed-forward carrier recovery,” Opt. Express 28, 16073-16088 (2020).
    Pubmed CrossRef
  25. Y. Wang, X. Li, Z. Jiang, L. Tong, W. Deng, X. Gao, X. Huang, H. Zhou, Y. Yu, L. Ye, X. Xiao, and X. Zhang, “Ultrahigh-speed graphene-based optical coherent receiver,” Nat. Commun. 12, 5076 (2021).
    Pubmed KoreaMed CrossRef