This document describes a proposed system for using dark soliton arrays (DSA) for secure optical communication. The system consists of multiple micro ring resonators (MRRs) that generate an array of dark solitons. Dark solitons with different center wavelengths are input into the MRR system. The radii and coupling coefficients of the MRRs are configured to produce filtering of the input signals. This results in a DSA containing multiplexed dark soliton pulses that could be used for communication security applications. Simulation results show that a DSA is generated with center wavelengths ranging from 1513nm to 1517nm. The DSA could allow for secure transmission over long distance optical links.
Integrated ring resonator system analysis to Optimize the soliton transmissionPremier Publishers
The chaotic signals can be generated within the microring resonator (MRR) system when the Gaussian pulse with input power of 120 mW is inserted into the system. Generation of chaotic signals respect to the ring's radius has been studied. The coupling coefficient affects the output power significantly, thus in order to generate signals with higher output power, the smaller coupling coefficient can be used. Here the output power of the system is characterized with respect to the different coupling coefficients of the system.A series of MRRs connected to an add/drop filter system in order to anaylize the soliton signals. The nonlinear refractive index of the MRR is n2=2.2 x 10-17 m2/W. The capacity of the output signals can be increased through generation of peaks with smaller full width at half maximum (FWHM). Here, we generate and characterize the ultra-short optical soliton pulses respect to the ring's radius and coupling coefficients variation of the system. As result, soliton pulses with FWHM and free spectral range (FSR) of 50 pm and 1440 pm are generated.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
Integrated ring resonator system analysis to Optimize the soliton transmissionPremier Publishers
The chaotic signals can be generated within the microring resonator (MRR) system when the Gaussian pulse with input power of 120 mW is inserted into the system. Generation of chaotic signals respect to the ring's radius has been studied. The coupling coefficient affects the output power significantly, thus in order to generate signals with higher output power, the smaller coupling coefficient can be used. Here the output power of the system is characterized with respect to the different coupling coefficients of the system.A series of MRRs connected to an add/drop filter system in order to anaylize the soliton signals. The nonlinear refractive index of the MRR is n2=2.2 x 10-17 m2/W. The capacity of the output signals can be increased through generation of peaks with smaller full width at half maximum (FWHM). Here, we generate and characterize the ultra-short optical soliton pulses respect to the ring's radius and coupling coefficients variation of the system. As result, soliton pulses with FWHM and free spectral range (FSR) of 50 pm and 1440 pm are generated.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
Generation of Nanometer Optical Tweezers Used for Optical Communication Netw...University of Malaya (UM)
A system of Half-Panda microring resonator (MRR) is proposed to generate ultra-short nanometer (nm)
optical tweezers. The dark soliton propagates inside nonlinear MRR. Molecules or photons transport within the system when the dark soliton is used as input pulse. Nano optical tweezers can be generated and used to many applications in optical communication networks. Here the smallest nano optical tweezers signals with full width at half maximum (FWHM) of 9 nm is obtained where the free spectrum range (FSR) of 50 nm is simulated.
Soliton comb generation using add-drop ring resonatorsPremier Publishers
Add-drop ring resonator system is the fundamental building block of the optical transmission and communication systems. The microring resonator (MRR) made of semiconductor with a length of 750 μm, K1=k2= 0.02, is used to filter the input spectrum of Gaussian laser beam and generate the comb frequency of soliton pulses, where the transmission characteristics and group delay profile of the through and drop port output signals are presented. The semiconductor material (InGaAsP/InP) is used to generate the add-drop ring resonator. The operating wavelength is 1550 nm andthe iterative method is used to generate the results based on practical parameters of the system.
B.tech Major Project: In this project I have simulated the illuminance distribution, optical power distribution on received optical plane for Line of Sight(LOS) condition as well as Diffuse link, SNR distribution and graph showing the variation of RMS Delay Spread for different sample receiver positions using MATLAB.
Reduction of Frequency offset Using Joint Clock for OFDM Based Cellular Syste...IJRST Journal
This project addresses the problem of clock synchronization between a base station (BS) and a mobile station (MS). A conventional technique for clock synchronization is that the MS clock is derived from the downlink signal originated from a base station. In cellular systems, a base station and mobile stations need to be synchronized before data exchange. Since the base station clock reference is more accurate, a mobile station typically derives its clock reference from the base station. But the carrier frequency offset due to Doppler shift may have harmful effects on the local clock derivation. This project proposes a joint clock and frequency synchronization technique between a base station and a mobile station, which is effective even with Doppler shift. We derive the joint estimation algorithm by analyzing the phase and the amplitude distortion caused by the sampling frequency offset and the carrier frequency offset. Simulation results showing the effectiveness of the proposed algorithm will also be presented.
ACCURATE NUMERICAL SIMULATION OF HIGHER ORDER SOLITON DECOMPOSITION IN PRESEN...IAEME Publication
Generally, one considers only the groupvelocity dispersion (GVD) and self-phase modulation (SPM) induced solitons inoptical communication while other higher order effects such as the third-orderdispersion (TOD), self-steepening, and stimulated Raman scattering are wellthought-out only perturbatively . In this article, we study the existence ofthe TOD and self-steepening induced soliton solutions. The results haveshown that, the combination of the linear with nonlinear effects escort to newqualitative feature as a shifting and the center-shift beside the deformationin the shape of the soliton. To accomplish this purpose we used, the split-stepFourier Method, in our simulations, that is broadly used to simulate numerical solutionsof the nonlinear Schrodinger equation.
Digital signal processing techniques for lti fiber impairment compensationeSAT Journals
Abstract Coherent detection is one of the active research areas for the development of high speed, high spectral efficient optical communication network. Digital signal processing is the important technique for compensating the fiber transmission impairments because of number of advantages such as signal can be amplified, delayed, splitted and manipulated without degrading the signal quality. This paper presents DSP compensation algorithms for linear time invariant (LTI) impairment such as chromatic dispersion (CD) and polarization mode dispersion (PMD) in optical fiber communication. We presented a mathematical framework for compensation of LTI fiber impairments. This paper also focuses the different compensation methods both in time and frequency domain for chromatic dispersion compensation. These DSP techniques confirm that coherent detection with high data rates will become feasible in future for compensating transmission impairments. Keywords: Coherent Detection, Chromatic Dispersion, Polarization Mode Dispersion
IJRET : International Journal of Research in Engineering and Technology is an international peer reviewed, online journal published by eSAT Publishing House for the enhancement of research in various disciplines of Engineering and Technology. The aim and scope of the journal is to provide an academic medium and an important reference for the advancement and dissemination of research results that support high-level learning, teaching and research in the fields of Engineering and Technology. We bring together Scientists, Academician, Field Engineers, Scholars and Students of related fields of Engineering and Technology.
IOSR Journal of Applied Physics (IOSR-JAP) is an open access international journal that provides rapid publication (within a month) of articles in all areas of physics and its applications. The journal welcomes publications of high quality papers on theoretical developments and practical applications in applied physics. Original research papers, state-of-the-art reviews, and high quality technical notes are invited for publications.
Generation of Nanometer Optical Tweezers Used for Optical Communication Netw...University of Malaya (UM)
A system of Half-Panda microring resonator (MRR) is proposed to generate ultra-short nanometer (nm)
optical tweezers. The dark soliton propagates inside nonlinear MRR. Molecules or photons transport within the system when the dark soliton is used as input pulse. Nano optical tweezers can be generated and used to many applications in optical communication networks. Here the smallest nano optical tweezers signals with full width at half maximum (FWHM) of 9 nm is obtained where the free spectrum range (FSR) of 50 nm is simulated.
Soliton comb generation using add-drop ring resonatorsPremier Publishers
Add-drop ring resonator system is the fundamental building block of the optical transmission and communication systems. The microring resonator (MRR) made of semiconductor with a length of 750 μm, K1=k2= 0.02, is used to filter the input spectrum of Gaussian laser beam and generate the comb frequency of soliton pulses, where the transmission characteristics and group delay profile of the through and drop port output signals are presented. The semiconductor material (InGaAsP/InP) is used to generate the add-drop ring resonator. The operating wavelength is 1550 nm andthe iterative method is used to generate the results based on practical parameters of the system.
B.tech Major Project: In this project I have simulated the illuminance distribution, optical power distribution on received optical plane for Line of Sight(LOS) condition as well as Diffuse link, SNR distribution and graph showing the variation of RMS Delay Spread for different sample receiver positions using MATLAB.
Reduction of Frequency offset Using Joint Clock for OFDM Based Cellular Syste...IJRST Journal
This project addresses the problem of clock synchronization between a base station (BS) and a mobile station (MS). A conventional technique for clock synchronization is that the MS clock is derived from the downlink signal originated from a base station. In cellular systems, a base station and mobile stations need to be synchronized before data exchange. Since the base station clock reference is more accurate, a mobile station typically derives its clock reference from the base station. But the carrier frequency offset due to Doppler shift may have harmful effects on the local clock derivation. This project proposes a joint clock and frequency synchronization technique between a base station and a mobile station, which is effective even with Doppler shift. We derive the joint estimation algorithm by analyzing the phase and the amplitude distortion caused by the sampling frequency offset and the carrier frequency offset. Simulation results showing the effectiveness of the proposed algorithm will also be presented.
ACCURATE NUMERICAL SIMULATION OF HIGHER ORDER SOLITON DECOMPOSITION IN PRESEN...IAEME Publication
Generally, one considers only the groupvelocity dispersion (GVD) and self-phase modulation (SPM) induced solitons inoptical communication while other higher order effects such as the third-orderdispersion (TOD), self-steepening, and stimulated Raman scattering are wellthought-out only perturbatively . In this article, we study the existence ofthe TOD and self-steepening induced soliton solutions. The results haveshown that, the combination of the linear with nonlinear effects escort to newqualitative feature as a shifting and the center-shift beside the deformationin the shape of the soliton. To accomplish this purpose we used, the split-stepFourier Method, in our simulations, that is broadly used to simulate numerical solutionsof the nonlinear Schrodinger equation.
Digital signal processing techniques for lti fiber impairment compensationeSAT Journals
Abstract Coherent detection is one of the active research areas for the development of high speed, high spectral efficient optical communication network. Digital signal processing is the important technique for compensating the fiber transmission impairments because of number of advantages such as signal can be amplified, delayed, splitted and manipulated without degrading the signal quality. This paper presents DSP compensation algorithms for linear time invariant (LTI) impairment such as chromatic dispersion (CD) and polarization mode dispersion (PMD) in optical fiber communication. We presented a mathematical framework for compensation of LTI fiber impairments. This paper also focuses the different compensation methods both in time and frequency domain for chromatic dispersion compensation. These DSP techniques confirm that coherent detection with high data rates will become feasible in future for compensating transmission impairments. Keywords: Coherent Detection, Chromatic Dispersion, Polarization Mode Dispersion
IJRET : International Journal of Research in Engineering and Technology is an international peer reviewed, online journal published by eSAT Publishing House for the enhancement of research in various disciplines of Engineering and Technology. The aim and scope of the journal is to provide an academic medium and an important reference for the advancement and dissemination of research results that support high-level learning, teaching and research in the fields of Engineering and Technology. We bring together Scientists, Academician, Field Engineers, Scholars and Students of related fields of Engineering and Technology.
Dark-Bright Solitons Conversion System for Secured and Long Distance Optical ...University of Malaya (UM)
We suggest a new purpose of a security scheme by employing the nonlinear behaviors of temporal dark and bright solitons amongst a micro-ring resonator system for signal security application. The chaotic signal is generated, where the required bright soliton pulse can be recovered and discovered by an add/drop filtering device. By using the reserve ring parameters, simulation results obtained have demonstrated that the soliton conversion can be performed. In application, the chaotic signal is generated and formed by the dark soliton inside a nonlinear micro-ring device. The different temporal soliton response time can be seen, the response times of 169 and 84 ns are mentioned for temporal dark and bright solitons, respectively, which can also be used to figure the security key. The technique of optical conversion can be use to improve the optical communication network systems.
Decimal Convertor Application for Optical Wireless Communication by Generatin...University of Malaya (UM)
Two systems consist of microring resonators (MRRs) and an add/drop filter are used to generate signals as localized multi wavelengths. Quantum dense encoding
can be performed by output signals of selected wavelengths incorporated to a polarization control system. Therefore dark and bright optical soliton pulses
with different time slot are generated. They can be converted into digital logic quantum codes using a decimal convertor system propagating along a wireless networks. Results show that multi soliton wavelength, ranged from 1.55 m to 1.56 m with FWHM and FSR of 10 pm and 600 pm can be generated respectively. Keywords- Micro Ring Resonator, Quantum Dense Coding (QDC), Wireless network communication system.
We propose a novel system of the dynamic optical tweezers generated by a dark soliton in the fiber optic loop. A dark soliton known as an optical tweezer is amplified and tuned within the microring resonator (MRR) system. The required tunable tweezers with different widthsand powers can be controlled. The analysis of dark-bright soliton conversion using a dark soliton pulse propagating within a MRR is analyzed. The control dark soliton is input into the system via the add port of the add/drop filter. The dynamic behavior of the dark-brightsoliton conversion is observed. The required stable signal is obtained via a drop and throughput ports of the add/drop filter with some suitable parameters. In application, generation of optical tweezers and transportation can be realized by using the proposed system, where the communication network is performed.
Generation of Quantum Photon Information Using Extremely Narrow Optical Tweez...University of Malaya (UM)
A system of microring resonator (MRR) is presented to generate extremely narrow optical tweezers. An add/drop filter system consisting of one centered ring and one smaller ring on the left side can be used to generate extremely narrow pulse of optical tweezers. Optical tweezers generated by the dark-Gaussian behavior propagate via the MRRs system, where the input Gaussian pulse controls the output signal at the drop port of the system. Here the output optical tweezers can be connected to a quantum signal processing system (receiver), where it can be used to generate high capacity quantum codes within series of MRR’s and an add/drop filter. Detection of the encoded signals known as quantum bits can be done by the receiver unit system. Generated entangled photon pair propagates via an optical communication link. Here, the result of optical tweezers with full width at half maximum (FWHM) of 0.3 nm, 0.8 nm and 1.6 nm, 1.3 nm are obtained at the through and drop ports of the system respectively. These results used to be transmitted through a quantum signal processor via an optical computer network communication link.
Long Distance Communication Using Localized Optical Soliton via Entangled Ph...University of Malaya (UM)
A system of microring resonators (MRRs) is presented to generation entangled photon. Different time slot for continuous variable quantum key distribution (CVQKD) use is applicable in optical wireless link. Chaotic behavior of a soliton pulse within the device can be presented respect to the Kerr nonlinear type of light in the MRR devices. Continuous spatial and temporal signals are generated spreading over the spectrum. The CVQKD is formed using the localized spatial soliton pulse. Here localized temporal soliton with FWHM and FSR of 0.2 ps and 0.58 ns is obtained respectively. The spatial soliton pulse has a FWHM of 80 pm. Transmission of soliton pulse with FWHM of 1.5 ps is simulated along the long distance fiber optics where the polarized photons are formed incorporating with the polarization control unit into the MRRs, which allows different time slot entangled photons to be randomly formed.
The microring resonator (MRR) system can be used to trap optical solitons. These types of pulses are used to generate entangled photon required for quantum keys. The required information can be provided via the quantum keys. We simulate localized spatial and temporal soliton pulses to form an optical communication used in wireless systems. The input soliton pulses with peak power of 500 and 550 mW are used to generate a spectrum of chaotic signals within the nonlinear medium, where the nonlinear refractive index is selected to n2=2.2 x 10-17m2/W. The ultra-short soliton pulse can be trapped within the 3.52 GHz frequency, where the temporal soliton pulse with FWHM of 25 ps could be simulated and used to generate entangled photon pair. The generated entangled photons are input into a wireless router system which is used to transfer them within a network communication system. The router system is used to receive the information and convert it to analog signals at the end of the transmission link, thus data can be sent to the users via a secured optical communication system using MRRs.
Secured Transportation of Quantum Codes Using Integrated PANDA-Add/drop and T...University of Malaya (UM)
New system of quantum cryptography for communication networks is proposed. Multi optical Soliton can be generated and propagated via an add/drop interferometer system incorporated with a time division multiple access (TDMA) system. Here the transportation of quantum codes is performed. Chaotic output signals from the PANDA ring resonator are inserted into the add/drop filter system. Using the add/drop filter system multi dark and bright solitons can be obtained and used to generate entangled quantum codes for internet security. In this research soliton pulses with FWHM and FSR of 325 pm and 880 nm are generated, respectively.
Cryptography Scheme of an Optical Switching System Using Pico/Femto Second So...University of Malaya (UM)
We propose a system of microring resonators (MRRs) incorporating with an add/drop filter system. Optical soliton can be simulated and used to generate entangled photon, applicable in single and multiple optical switching. Chaotic signals can be generated via the MRRs system. Therefore continuous spatial and temporal signals are generated spreading over the spectrum. Polarized photons are formed incorporating the
polarization control unit into the MRRs, which allows different time slot entangled photons to be randomly formed. Results show the single soliton pulse of 0.7 ps where the multi soliton pulse with FSR and FWHM of 0.6 ns and 20 ps are generated using the add/drop filter system. Here Ultra-short single soliton pulse with FWHM=42 fs can be simulated. These pulses are providing required communication signals to generate pair of polarization entangled photons among different time frame where the polarization control unit and polarizer beam splitter (PBS) are connected to the ring resonator system.
All-optical logic XOR/XNOR gate operation using microring and nanoring reson...University of Malaya (UM)
In this paper, a novel system of simultaneous optical logic AND and OR gates using dark -bright soliton conversion within the add/drop optical filter system is proposed. The input logic „0‟ and control logic „0‟ are formed by using the dark soliton pulse (D) trains. By using the dark-bright soliton conversion behavior within the π/2 phase shift device, we found that the simultaneous optical logic AND and OR gates at the drop and through ports can be randomly formed, respectively.
All-Optical OFDM Generation for IEEE802.11a Based on Soliton Carriers Using M...University of Malaya (UM)
The optical carrier generation is the basic building block to implement all-optical
orthogonal frequency-division multiplexing (OFDM) transmission. One method to optically
generate single and multicarriers is to use the microring resonator (MRR). The MRRs can be
used as filter devices, where generation of high-frequency (GHz) soliton signals as single
and multicarriers can be performed using suitable system parameters. Here, the optical
soliton in a nonlinear fiber MRR system is analyzed, using a modified add/drop system
known as a Panda ring resonator connected to an add/drop system. In order to set up a
transmission system, i.e., IEEE802.11a, first, 64 uniform optical carriers were generated and
separated by a splitter and modulated; afterward, the spectra of the modulated optical
subcarriers are overlapped, which results one optical OFDM channel band. The quadrature
amplitude modulation (QAM) and 16-QAM are used for modulating the subcarriers. The
generated OFDM signal is multiplexed with a single-carrier soliton and transmitted through
the single-mode fiber (SMF). After photodetection, the radio frequency (RF) signal was
propagated. On the receiver side, the RF signal was optically modulated and processed.
The results show the generation of 64 multicarriers evenly spaced in the range from 54.09 to
55.01 GHz, where demodulation of these signals is performed, and the performance of the
system is analyzed.
Ultra-short Multi Soliton Generation for Application in Long Distance Commun...University of Malaya (UM)
Generation of picometer optical soliton pulses is investigated using a nonlinear PANDA ring resonator system connecting to an add/drop filter system. The objectives of the research are to employ systems of microring resonator (MRR) to generate binary signals to be carried out along fiber optic communication. Effective parameters such as refractive indices of a silicon waveguide, coupling coefficients (), coupling loss, radius of the ring (R) and the input power can be selected properly to operate the nonlinear behavior. The input Gaussian laser pulses with power of 600 mW are inserted into the system. The central wavelength of the input power has been selected to λ0=1.55 µm where the nonlinear refractive index of the medium is n2=2.6×10−17 m2 W−1. Therefore binary signals generated by the add/drop filter system can be converted to secure codes where the decoding process of the transmitted codes can be obtained at the final step. Here, multi soliton pulses with full width at half maximum (FWHM) of 325 could be generated, converted to secure codes and finally detected over 70 km optical fiber communication link.
Frequency-Wavelength Trapping by Integrated Ring Resonators For Secured Netwo...University of Malaya (UM)
Optical pulse trapping via a series of microring resonator (MRR) is presented. Large bandwidth of optical soliton is generated by input pulse propagating within the MRRs. Distinguished discrete wavelength or frequency pulses can be generated by using localized spatial pulses via a networks communication system. Quantum codes can be generated by using a polarization control unit and a beam splitter, incorporating to the MRRs. Here frequency band of 10.7 MHz and 16 MHz and wavelengths of 206.9 nm, 1448 nm, 2169 nm and 2489 nm are localized and obtained and used for quantum codes generation applicable for secured networks communication.
Similar to Dark soliton array for communication security (20)
Tunable and Storage Potential Wells using Microring Resonator System for Bioc...University of Malaya (UM)
In this work, we propose the technique that can be used to trap/delivery bio-cell by using the concept of dark solitons and potential well, in which the trapping force is formed by using the intense optical vortices generated within the series ring and the PANDA ring resonator, the microscopic bio-cell can be trapped and moved dynamically, in which the valley of the dark soliton is generated and controlled within the PANDA ring resonator by the control port signals.
ASK-to-PSK Generation based on Nonlinear Microring Resonators Coupled to One ...University of Malaya (UM)
We present a new concept of ASK-to-PSK generation based on nonlinear microring resonators coupled to one MZI arm by using OptiWave FDTD method. By microring resonator increase from one to three microring (SR to TR), we found that the amplitude shift keying (ASK) are increase exactly and the phase shift keying (PSK) is equal to π.
Simulation and Analysis of Multisoliton Generation Using a PANDA Ring Resonat...University of Malaya (UM)
A novel system of multisoliton generation using nonlinear equations of the propagating signals is presented. This system uses a PANDA ring resonator incorporated with an add/drop filter system. Using resonant conditions, the intense optical fields known as multisolitons can be generated and propagated within a Kerr-type nonlinear medium. The present simulation results show that multisolitons can be controlled by using additional Gaussian pulses input into the add port of the PANDA system. For the soliton pulse in the microring device, a balance should be achieved between dispersion and nonlinear lengths. Chaotic output signals from the PANDA ring resonator are input into the add/drop filter system. Chaotic signals can be filtered by using the add/drop filter system, in which multi dark and bright solitons can be generated. In this work multi dark and bright solitons with an FWHM and an FSR of 425pm and 1.145 nm are generated, respectively, where the Gaussian pulse with a central wavelength of 1.55 μm and power of 600 mW is input into the system.
In this study an interesting system in which a bright and dark soliton pulse can be stopped inside a nonlinear waveguide is presented. Here, we propose a system consisting of a series of ring resonators for optical trapping within a nonlinear waveguide. The bright and dark solitons can be controlled and slowed down within the waveguide. The FWHM for the output signals are calculated and used as an optical memory. Bright and dark soliton behaviors within a micro and nano ring resonator are also investigated and described. The required pulse is filtered and amplified, can be controlled and localized within the system. The localized bright and dark solitons are stopped by controlling the input power,which means that the photon stopping can be controlled by light in a ring resonator.
A molecular cryptography technique using optical tweezers, is proposed. The optical tweezer transports the molecules in the communication system. The optical tweezer generated by the dark soliton is in the form of a potential well. The dark soliton propagates inside nonlinear microring resonator (NMRR). Transportation of molecules is implemented when the dark soliton is used as input pulse. The input bright soliton control the output signal at the drop port of the system. Output optical tweezers can be connected to the quantum signal processing system consisting of transmitter and the receiver. The transmitter is used to generate the high capacity quantum codes within the series of MRR’s and anadd/drop filter. The receiver will detect the encoded signals known as quantum bits. The transmitter will generate the entangled photon pair which propagates via an optical communication link. Here the smallest optical tweezer with respect to the full width at half maximum FWHM is 17.6 nm in the formof potential well is obtained and transmitted through quantum signal processor via an optical link.
This research is used to control the nonlinear behavior of silicon microring resonators, MRR’s such as chaos and bifurcation. Increasing of nonlinear refractive indices, coupling coefficients and radius of the SMRR leads to descend input power and round trips wherein the bifurcation occurs. As result, bifurcation or chaos behaviors are seen at lower input power of 44 W, where the nonlinear refractive index is n2=3.2×10−20 m2/W. Smallest round trips can be seen for the R=40 µm and 0.1 respectively. Signals from the SMRR are passing through a polarizer beam splitter to generate quantum
binary codes which are used in wireless network communication.
The aim of this study is to generate nano optical tweezers to be connected to an optical quantum signal processing system in order to transmit quantum photon via an optical communication link. A system of microring resonator (MRR) known as Half-Panda is proposed to generate nano optical tweezers. Optical tweezers can be used to transport molecules in a communication link. The dark soliton propagates inside nonlinear MRR. Transportation of molecules or photons is implemented when the dark soliton is used as input pulse. The input Gaussian soliton is used to control the output signal at the through and drop ports of the system. Output nano optical tweezers can be connected to the quantum signal processing system consisting of a receiver and transmitter. The receiver will detect the signals of optical tweezers and transmit them via wired/wireless as quantum bits. The transmitter will generate the entangled photon pair which propagates via an optical communication link. Here the smallest nano optical tweezers signals with width at half maximum (FWHM) of 4.2 nm is obtained where the free spectrum range (FSR) of 50 nm is simulated.
Single Soliton Bandwidth Generation and Manipulation by Microring ResonatorUniversity of Malaya (UM)
In this paper, we propose a system for chaotic signal generation using a microring resonator (MRR) fiber optic system. This system uses a regular laserdiode as input power and can be incorporated with an optical add/drop filter system. When light from the laser diode feedbacks to the fiber ring resonator, the actual chaotic signal is produced by using the appropriate fiber ring resonator parameters and also the laser diode input power. The filtering process of the chaotic signals occurs during the round-trip of the pulse within the ring resonators. The single soliton pulses generation and bandwidth manipulation of the pulse can be performed using the add/drop system. Results obtained have established particular possibilities from the application. The obtained results show the effects of coupling coefficients on the bandwidth of the single soliton pulse, where the chaotic behaviors of the input pulses are presented.
NEW SYSTEM OF CHAOTIC SIGNAL GENERATION BASED ON COUPLING COEFFICIENTS APPLI...University of Malaya (UM)
The nonlinear behavior (chaotic) of light traveling in an optical fiber ring resonator such as an add/drop system
is presented. The chaotic behavior is considered to be a beneficial effect that can be used in the communication
system. Such a system can be used to secure the information signals, therefore, the ability of chaotic carriers to synchronize in a communication system is performed. The used optical material is InGaAsP/InP regarding to suitable parameters of the system. The nonlinear refractive index is fixed to n2 = 3.8 × 10−20 m2
/W, and the 20,000 iterations of round-trip within the system is simulated. The input powers are selected at 1 W, where the coupling coefficient of the system varies according to two critical cases, where 0 0.1
and 0.1 1. As a results, larger coupler coefficient corresponds to lower input power for the case of
0 0.1 and smaller coupling coefficient of the system is corresponds to lower input power when
0.1 1. To optimize the microring systems, Lower input power is recommended in many applications in optical optical communication systems.
Chaotic soliton can be generated using a nonlinear PANDA system. The research uses microring resonator
(MRR) to generate and trap chaotic signals along fiber optic communication. The parameters such as refractive
indices of a silicon waveguide, coupling coefficients ( ), coupling loss, radius of the ring (R) and the input power can be selected properly to operate the nonlinear behavior. The input Gaussian laser pulses with power of 0.45 W are inserted into the system. The central wavelength of the input power has been selected to λ0=1.55 µm where the nonlinear refractive index of the medium is n2=1.3×10−17 m2 W−1
. The generated chaotic signals with Full at Half
Maximum of 24 pm can be transmitted along the fiber optic with length of 195 km. The trapping of chaotic signals can be obtained at the end of the transmission link. Here signals with 600 fm bandwidth could be trapped within the system.
Nonlinear behaviors of light such as chaos can be observed during propagation of a Gaussian laser beam inside a single ring resonator system. Chaotic signals can be employed to generate data of logic codes to be transmitted along the fiber optic communication. Controlling of the chaotic signals can be implemented by the parameter of the system such as coupling coefficient, the ring’s radius, coupling loss and input power. The central wavelength of the input Gaussian laser pulse has been selected to λ0=1550 nm where the nonlinear refractive index of the medium is n2=1.4×10−13 m2 W−1. Therefore the data of logic codes generated by the single ring resonator system can be converted to transmitting secured codes where the decoding process of the transmitted codes can be obtained at the end of the transmission link. Here generation of logic code of “101010101011010101011101011110101101010101010110101” is performed, encoded and decoded over 50 km fiber optics. Thus secured transmitting of signals can be obtained along the long distance fiber
communication.
Quantum Transmission of Optical Tweezers Via Fiber Optic Using Half-Panda Sys...University of Malaya (UM)
: The aim of this study is to generate nano optical tweezers to be connected to an optical transmission link in order to transmit tweezers via an optical fiber. A system of microring resonator (MRR) known as Half-Panda is proposed to generate nano optical tweezers. Optical tweezers can be used to transport molecules in a communication link. The dark soliton propagates inside nonlinear MRR. The input bright soliton is used to control the output signal at the through and drop ports of the system. Throughput nano optical tweezers can be connected to the fiber optic with a length of 100 km, where transmission of tweezers can be performed. The optical receiver will detect the signals of optical tweezers. A transmitter system can be used to transmit the tweezers via wired/wireless link to the users in a short communication link. Here the nano optical tweezers signals with width at half maximum (FWHM) of 33 nm are obtained and transmitted, where the free spectrum range (FSR) of the pulses is 50 nm.
Nonlinear Chaotic Signals Generation and Transmission within an Optical Fiber...University of Malaya (UM)
The nonlinear behavior of light such as chaos traveling in an optical fiber ring resonator as a single
ring resonator is presented. This phenomenon can be used to generate secret codes or arbitrary digital codes of "0" and "1" applicable in the communication system such as time division multiple access (TDMA) system. Such a system can be used to secure the information signals therefore, the ability of chaotic carriers to synchronize in a communication system is performed. The used optical material is InGaAsP/InP regarding to suitable parameters of the system. The nonlinear refractive index is fixed to n2=3.8 × 10−20 m2
/W. The input power is selected at 1 W, where the coupling coefficient of the system varies as
0 0.1. As a result, train of logic
codes could be generated and transmitted via a fiber communication link using the chaotic signals. To optimize the microring systems, Lower input power is recommended in many applications in optical optical
communication systems.
IEEE 802.15.3c WPAN Standard Using Millimeter Optical Soliton Pulse Generated...University of Malaya (UM)
A system of microring resonators (MRRs) connected to an optical modified add/drop filter system known as a Panda ring resonator is presented. The optical soliton pulse of 60 GHz frequency band can be generated and used for Wireless Personal Area Network (WPAN) applications such as IEEE 802.15.3c. The system uses chaotic signals generated by a Gaussian laser pulse propagating within a nonlinear MRRs system. The chaotic signals can be generated via a series of microring resonators, where the filtering process is performed via the Panda ring resonator system wherein ultrashort single and multiple optical soliton pulses of 60 GHz are generated and seen at the through and drop ports, respectively. The IEEE 802.15.3c standard operates at the 60 GHz frequency band, and it is applicable for a short distance optical communication such as indoor systems, where the higher transmission data rate can be performed using a high frequency band of the output optical soliton pulses. The single and multi-soliton pulses could be generated and converted to logic codes, where the bandwidths of these pulses are 5 and 20 MHz, respectively. Thus, these types of signals can be used in optical indoor systems and transmission link using appropriate components such as transmitter, fiber optics, amplifier, and receiver.
Generation and wired/wireless transmission of IEEE802.16m signal using solito...University of Malaya (UM)
Multi-carrier generation is the main building block for generating WiMax signal. In order to use WiMax signal in radio over fiber applications the use of all
optical generation of RF signals is required. To generate multi carriers optically, the system consisting ofseries of microring resonators (MRRs)
incorporating with an add/drop filter system are used. Thus the high frequency (THz) solitons range of 193.29–193.35 THz at frequencies of 193.333,
193.3355 and 193.3388 THz with the free spectralrange of 2.5 and 5.8 GHz could be performed using MRRs, providing required WiMax signal used in
wired/wireless communication. The generated multi carriers are multiplexed with the single carrier soliton and transmitted through single mode fiber (SMF)
after being beaten to photodiode, a WiMax signal is propagated wirelessly in transmitter antenna base station and is received by the second antenna located
in the receiver.
Transmission of data with orthogonal frequency division multiplexing techniqu...University of Malaya (UM)
Microring resonators (MRRs) can be used to generate optical millimetre-wave solitons with a broadband frequency of
40–60 GHz. Non-linear light behaviours within MRRs, such as chaotic signals, can be used to generate logic codes (digital
codes). The soliton signals can be multiplexed and modulated with the logic codes using an orthogonal frequency division
multiplexing (OFDM) technique to transmit the data via a network system. OFDM uses overlapping subcarriers without
causing inter-carrier interference. It provides both a high data rate and symbol duration using frequency division multiplexing
over multiple subcarriers within one channel. The results show that MRRs support both single-carrier and multi-carrier optical
soliton pulses, which can be used in an OFDM based on whether fast Fourier transform or discrete wavelet transform
transmission/receiver system. Localised ultra-short soliton pulses within frequencies of 50 and 52 GHz can be seen at the
throughput port of the panda system with respect to full-width at half-maximum (FWHM) and free spectrum range of 5 MHz
and 2 GHz, respectively. The soliton pulses with FWHMs of 10 MHz could be generated at the drop port. Therefore,
transmission of data information can be performed via a communication network using soliton pulse carriers and an OFDM
technique.
A system of microring resonator (MRR) conected to an optical panda ring
resonator is presented. The optical soliton pulse of 57-61 GHz frequency band can be
generated and used for aplications in optical communications. The system uses a Gausian
laser pulse propagating within a nonlinear MRRs system. The ultra short single and multi
optical soliton pulses within the range of 57-61 GHz can be generated and sen at he through
and drop ports of the system. This range is aplicable for a short distance optical
communication such as indor systems. The generated optical soliton pulses have the
bandwidth of 5 and 20 MHz.
2. 418 I.S. Amiri et al. / Procedia Engineering 8 (2011) 417–422
[7]. The transmission signals can be transmitted in the form of dark solitons. The specific end user that is connected
to the link via the specific add/drop filter can recover the signals. Dark soliton applications have been widely
investigated in various applications [8–9]. In this study, the DSA which consists of an array of micro rings will be
used for generation of array dark soliton in communication security.
2. Theoretical Simulation
The dark soliton array can be obtained using dark soliton pulses input to a series of micro ring resonator (MRR)
in single system. The stationary multiple dark soliton pulses are introduced into the MRR system, as shown in
Figure 1. Each input optical field (Ein) of the dark soliton pulses input is given by [3].
0
0
tanh exp
2
in
D
T z
E A i t
T L
ω
⎡ ⎤⎡ ⎤ ⎛ ⎞
= −⎢ ⎥⎜ ⎟⎢ ⎥
⎝ ⎠⎣ ⎦ ⎣ ⎦
(1)
where A and z are the optical field amplitude and propagation distance, respectively. T is the soliton pulse
propagation time in the frame moving at the group velocity, T = t-β1*z, where β1and β2 are the coefficient of the
linear and the second order terms of Taylor expansion of the propagation constant. 2
2
0 βTLD = is the dispersion
length of the soliton pulse. To in the equation is a soliton pulse propagation time at initial input (or collision pulse
width), where t is the soliton phase shift time, and the frequency shift of the soliton is ω0. Equation (1) describes a
pulse that keeps its temporal width invariance as it propagates and, thus, is called a temporal soliton [10]. When a
soliton peak intensity (( )2
02 / TΓβ ) is given, then T0 is known. When a soliton pulse is propagated within nonlinear
micro ring device, a balance should be achieved between the dispersion length (LD) and the nonlinear length (LNL=
1/ ΓφNL), where Γ = n2*k0 is the length scale over which dispersive or nonlinear effects make the beam wider or
narrower. For a soliton pulse, there is a balance between dispersion and nonlinear lengths, hence, NLD LL = . When
light propagates within the nonlinear material (medium), the refractive index (n) of light within the medium is given
by
P
A
n
nInnn
eff
)( 2
020 +=+= (2)
where 0n and 2n are the linear and nonlinear refractive indexes, respectively. I and P are the optical intensity and
optical power, respectively. The effective mode core area of the device is given by effA .
Fig. 1. Schematic of dark soliton array generation. Ein, soliton inputs; R, ring radii; κ, coupling coefficients;
MUX, optical multiplexer; Rd, add/drop radius; MRR, micro ring resonator.
3. I.S. Amiri et al. / Procedia Engineering 8 (2011) 417–422 419
2
2
2 2
( ) (1 (1 ) )
(1 ) 1
( ) (1 1 (1 ) 4 1 1 sin ( )
2
out
in
E t x
E t x x
γ κ
γ
φ
γ κ γ κ
⎡ ⎤
⎢ ⎥− −
= − −⎢ ⎥
⎢ ⎥− − − + − −
⎣ ⎦
(3)
Equation (3) indicates that a ring resonator in this particular case is very similar to a Fabry-Perot cavity, which
has an input and output mirror with a field reflectivity, (1-κ ), and a fully reflecting mirror. κ is the coupling
coefficient, and ( )2/exp Lx α−= represents a roundtrip loss coefficient, 00 = kLnφ and 2
2 inNL EkLn=φ are the
linear and nonlinear phase shifts, λπ /2=k is the wave propagation number in a vacuum. Where L and α are a
waveguide length and linear absorption coefficient, respectively. In this work, the iterative method is used to obtain
the results as shown in equation (3), similarly, when the output field is connected and input into the other ring
resonators. The optical field of dark soliton pulse is input into a nonlinear series MRR. By using the appropriate
parameters, we propose to use the add/drop device. This is given in detail as follows. The optical outputs of a ring
resonator add/drop filter can be given by [13].
( ) ( ) ( )
( )( ) ( )Lkee
eLke
E
E
n
L
L
L
n
L
in
t
cos)1()1(2111
1cos)1()1(21
2
2121
2
2
211
2
α
α
α
α
κκκκ
κκκκ
−
−
−
−
−⋅−−−−+
−+−⋅−−−
=
(4)
and
( )( ) ( )Lkee
e
E
E
n
L
L
L
in
d
cos)1()1(2111 2
2121
2
21
2
α
α
α
κκκκ
κκ
−
−
−
−⋅−−−−+
=
(5)
where Et and Ed represents the optical fields of the throughput and drop ports respectively. effknβ = is the
propagation constant, effn is the effective refractive index of the waveguide and the circumference of the ring is
2=L Rπ , here R is the radius of the ring. In the following, new parameters will be used for simplification: = Lφ β
is the phase constant. The chaotic noise cancellation can be managed by using the specific parameters of the add/drop
device, which the required signals can be retrieved by the specific users. κ1 and κ2 are coupling coefficient of add/drop
filters, λπ /2=nk is the wave propagation number for in a vacuum, and where the waveguide (ring resonator) loss is
α = 0.5 dBmm-1
. The fractional coupler intensity loss is γ = 0.1. In the case of add/drop device, the nonlinear
refractive index is neglected.
3. Result and Discussion
Generated dark soliton pulse for pulse with 50 ns pulse width and a maximum power of 0.65 W is input into each
ring resonator system with different center wavelengths is shown in Figure 1. Suitable ring parameters are used, such
as ring radii and ring coupling coefficients, where R1 =7 μm and R2 =5 μm. To make the system match to the practical
device [14], n0 = 3.34 (In-GaAsP/InP).
The effective core areas are Aeff = 0.50 μm2
and 0.25 μm2
for MRRs. The waveguide and coupling losses are α =
0.5 dBmm−1
and γ = 0.1, respectively, and the coupling coefficients κ of the MRRs range from 0.03 to 0.1. The
nonlinear refractive index is n2 = 2.2 × 10−13
m2
/W. In this case, the waveguide loss used is α = 0.5 dBmm−1
. However,
more parameters are used, as shown in Figure 1.
The input dark soliton pulse is chopped (sliced) into the smaller signals R1 and R2, and the filtering signals within
add/drop ring Rd are seen. We find that the output signal from R2 is larger than that from R1 due to the different core
effective areas of the rings in the system. However, the effective areas can be transferred from 0.50 μm² and 0.25 μm²
with some losses. The soliton signals in Rd enter the add/drop filter, where the dark soliton conversion can be
performed by using Equation (4) and (5). Here, a different dark soliton wavelength is input into the MRR system and
4. 420 I.S. Amiri et al. / Procedia Engineering 8 (2011) 417–422
the parameters of the system are set as the same. For instance, the dark solitons are input into the system at the center
wavelengths λ1 = 1501 nm, λ2 = 1503 nm, and λ3 = 1505 nm.
When a dark soliton propagates into the MRR system, the dark soliton collision (modulation) in the MUX system
and the filtering signals within the add/drop ring (Rd) occur as shown in Figure 1. The dark soliton is generated by
multilight sources at the center wavelength λ1 = 1503 nm and the filtering signals are as shown in Figure 2. The free
spectral range (FSR) and the amplified power of 2.15 nm and 80W of the dark soliton are obtained when, in this case,
the spectral width or called it full width at half-maximum (FWHM) of 0.073 nm is achieved. Different center
wavelength are input to the micro rings system and filtered by the second ring resonator in each line of the proposed
system as shown in Figure 3. The multiplexed output signals from the system is shown in Figure 3(g)
Fig. 2: Simulation result of the dark solitons within the series MRRs when the dark soliton input wavelength is 1503 nm: (a) dark soliton input,
(b) and (c) dark solitons in rings R1 and R2, and (d) the drop port signals
5. I.S. Amiri et al. / Procedia Engineering 8 (2011) 417–422 421
Fig. 3: Simulation result of the dark soliton array when the dark soliton input wavelengths are 1513 nm, 1515 nm, and 1517 nm: (a), (b), and (c)
are the output signals R2, and (d), (e), and (f) are the drop port signals; (g) dark soliton array
6. 422 I.S. Amiri et al. / Procedia Engineering 8 (2011) 417–422
In Figure 3, the dark soliton array generated by multilight sources at center wavelengths of λ1 = 1513 nm, λ2 =
1515 nm, and λ3 = 1517 nm is presented.
͵Ǥ ‘…Ž—•‹‘
We have presented the use of ring resonators to generate dark soliton arrays is which the multiplexed dark
soliton pulses can be seen by using a light pulse in fiber optic loop or MRR systems. First, the multiple dark solitons
are input into the series MRRs, through which multiplexed dark solitons with different center wavelengths, i.e., dark
soliton arrays, can be obtained. In this study, dark soliton with FSR and amplified power respectively of 2.15 nm
and 80 W can be obtained at the center wavelength of 1503 nm.
4. Acknowledgement
We would like to thank the Institute of Advanced Photonics Science, Nanotechnology Research Alliance,
Universiti Teknologi Malaysia (UTM) and King Mongkut’s Institute of Technology (KMITL), Thailand for the
support in research facilities. This research work has been supported by the Ministry of Higher Education (MOHE),
FRGS-grant 78452.
‡ˆ‡”‡…‡•
[1] M. Ballav and A. R. Chowdhury, “On a study of diffraction and dispersion managed soliton in a cylindrical media,” Prog. Electromagn.
Res. (PIER), vol. 63, pp. 33–50, 2006.
[2] R. Gangwar, S. P. Singh, and N. Singh, “Soliton based optical communication,” Prog. Electromagn. Res. (PIER), vol. 74, pp. 157–166,
2007.
[3] F. G. Gharakhili, M. Shahabadi, and M. Hakkak, “Bright and dark soliton generation in a left-handed nonlinear transmission line with series
nonlinear capacitors,” Prog. Electromagn. Res. (PIER), vol. 96, pp. 237–249, 2009.
[4] A. D. Kim, W. L. Kath, and C. G. Goedde, “Stabilizing dark solitons by periodic phase-sensitive amplification,” Opt. Lett., vol. 21, pp.
465–467, 1996.
[5] K. Sarapat, N. Sangwara, K. Srinuanjan, P. P. Yupapin, and N. Pornsuwancharoen, “Novel dark-bright optical soliton conversion system
and power amplification,” Opt. Eng., vol. 48, pp. 45-49, 2009.
[6] B. A. Malomed, A. Mostofi, and P. L. Chu, “Transformation of a dark soliton into a bright pulse,” J. Opt. Soc. Am. B, vol. 17, pp. 507–513,
2000.
[7] S. Mithata, N. Pornsuwancharoen, and P. P. Yupapin, “A simultaneous short wave and millimeter wave generation using a soliton pulse
within a nano-waveguide,” IEEE Photonics Technol. Lett., vol. 21, pp. 932–934, 2009.
[8] S. Mitatha, “Dark soliton behaviors within the nonlinear micro and nanoring resonators and applications,” Prog. Electromagn. Res. (PIER),
vol. 99, pp. 383–404, 2009.
[9] C. Finot, J. M. Dudley, and G. Millot, “Generation of dark solitons by interaction between similaritons in Raman fiber amplifiers,” Opt.
Fiber Technol., vol. 12, pp. 217–226, 2006.
[10] G. P. Agarawal, Nonlinear Fiber Optics, 4th ed. (Academic, 2007).
[11] P. P. Yupapin, N. Pornsuwanchroen, and S. Chaiyasoonthorn, “Attosecond pulse generation using nonlinear microring resonators,”
Microwave Opt. Technol. Lett., vol. 50, pp. 3108–3110, 2008.
[12] P. P. Yupapin and W. Suwancharoen, “Chaotic signal generation and cancellation using a micro ring resonator incorporating an optical
add/drop multiplexer,” Opt. Commun., vol. 280, pp. 343–350, 2007.
[13] P. P. Yupapin, P. Saeung, and C. Li, “Characteristics of complementary ring-resonator add/drop filters modeling by using graphical
approach,” Opt. Commun., vol. 272, pp. 81–86, 2007.
[14] P. P. Yupapin and N. Pornsuwanchroen, “Proposed nonlinear microring resonator arrangement for stopping and storing light,” IEEE
Photonics Technol. Lett., vol. 21, pp. 404–406, 2009.