Generic placeholder image

Micro and Nanosystems

Editor-in-Chief

ISSN (Print): 1876-4029
ISSN (Online): 1876-4037

Research Article

Implementation of Orthogonal Codes Using MZI

Author(s): Supriti Samanta, Goutam K. Maity* and Subhadipta Mukhopadhyay

Volume 12, Issue 3, 2020

Page: [159 - 167] Pages: 9

DOI: 10.2174/1876402912666200211121624

Abstract

Background: In Code Division Multiple Access (CDMA)/Multi-Carrier CDMA (MCCDMA), Walsh-Hadamard codes are widely used for its orthogonal characteristics, and hence, it leads to good contextual connection property. These orthogonal codes are important because of their various significant applications.

Objective: To use the Mach–Zehnder Interferometer (MZI) for all-optical Walsh-Hadamard codes is implemented in this present paper.

Method: The Mach–Zehnder Interferometer (MZI) is considered for the Tree architecture of Semiconductor Optical Amplifier (SOA). The second-ordered Hadamard and the inverse Hadamard matrix are constructed using SOA-MZIs. Higher-order Hadamard matrix (H4) formed by the process of Kronecker product with lower-order Hadamard matrix (H2) is also analyzed and constructed.

Results: To experimentally get the result from these schemes, some design issues e,g Time delay, nonlinear phase modulation, extinction ratio, and synchronization of signals are the important issues. Lasers of wavelength 1552 nm and 1534 nm can be used as input and control signals, respectively. As the whole system is digital, intensity losses due to couplers in the interconnecting stage may not create many problems in producing the desired optical bits at the output. The simulation results were obtained by Matlab-9. Here, Hadamard H2 (2×2) matrix output beam intensity (I ≈ 108 w.m-2) for different values of inputs.

Conclusion: Implementation of Walsh-Hadamard codes using MZI is explored in this paper, and experimental results show the better performance of the proposed scheme compared to recently reported methods using electronic circuits regarding the issues of versatility, reconfigurability, and compactness. The design can be used and extended for diverse applications for which Walsh-Hadamard codes are required.

Keywords: Orthogonal codes, semiconductor optical amplifier, Mach–Zehnder interferometer, walsh-hadamard code, MZI, time delay.

Graphical Abstract

[1]
Popovic, B.M. Spreading sequences for multicarrier CDMA systems. IEEE Trans. Commun., 1999, 47(5), 918.
[http://dx.doi.org/10.1109/26.771348]
[2]
Caulfield, H. J.; Dolev, S.; Green, W. M. Optical high-performance computing: Introduction to the JOSA A and applied optics feature. J. Appl. Opt , 2009; 48, . (22) OHPC1-OHPC3..
[3]
Chattopadhyay, T.; Maity, G.K.; Roy, J.N. Designing of the all-optical tri-state logic system with the help of optically nonlinear material. J. Nonlinear Opt. Phys. Mater., 2008, 17(3), 315-328.
[http://dx.doi.org/10.1142/S0218863508004159]
[4]
Mandal, A.K. Full-Optical TOAD based Walsh-Hadamard code generation. Opt. Quantum Electron., 2017, 49(9), 290.
[http://dx.doi.org/10.1007/s11082-017-1130-4]
[5]
Roy, J.N. Mach-Zehnder interferometer based tree architecture for all-optical logic and arithmetic operations. Optik (Stuttg.), 2009, 120(7), 318-324.
[http://dx.doi.org/10.1016/j.ijleo.2007.09.004]
[6]
Maity, G.K.; Maity, S.P.; Chattopadhyay, T.; Roy, J.N. Mach-Zehnder interferometer based all-optical fredkin gate. Proceedings of Trends in Optics and Photonics, Kolkata, India,, 2009, 234-239.
[7]
Maity, G.K.; Maity, S.P.; Roy, J.N. Mach-Zehnder interferometer based all-optical peres gate. Proceedings of Advances in Computing and Communications, Kochi, India,; , 2011, pp. 122-127.
[http://dx.doi.org/10.1007/978-3-642-22720-2_25]
[8]
Maity, G.K.; Maity, S.P.; Roy, J.N. MZI based modified trinary number system. Proceedings of Computer; Communication, Control and Information Technology, 2012, pp. 327-331.
[9]
Mandal, A.K.; Samanta, S.; Maity, G.K.; Manik, N.B. Implementation of Reed-Muller expansion technique using Mach-Zehnder in-terferometer based all-optical reversible gate. Advan. Optic. Sci. Eng., 2015, 166(1), 497-505.
[http://dx.doi.org/10.1007/978-81-322-2367-2_61]
[10]
Nath, D.; Dey, P.; Deb, D.; Rakshit, J.K.; Roy, J.N. Fabrication and characterization of organic semiconductor based photodetector for optical communication. CSI Trans. ICT, 2017, 5(2), 149-160.
[http://dx.doi.org/10.1007/s40012-016-0150-8]
[11]
Eiselt, M.; Pieper, W.; Weber, H.G. SLALOM: Semiconductor Laser Amplifier in a Loop Mirror. J. Lightwave Technol., 1995, 13(10), 2099-2112.
[http://dx.doi.org/10.1109/50.469721]
[12]
Li, W.; Zhang, M.; Ye, P. Simulation of an all-optical XOR gate with a semiconductor optical amplifier Mach-Zehnder Interferometer sped up by a continuous-wave assistant light. J. Optic. Netw., 2005, 4(8), 524-530.
[13]
Chattopadhyaya, T.; Gayen, D.K. Simultaneous all-optical multi logic operation using 3 × 3 interconnecting switch. Opt. Fiber Technol., 2019, 51(1), 41-47.
[http://dx.doi.org/10.1016/j.yofte.2019.05.002]

© 2024 Bentham Science Publishers | Privacy Policy