Characteristic Study on Conventional and Soliton Based Transmission System
Here, we study the characteristic feature of
conventional (ON-OFF keying) and soliton based transmission
system. We consider 20Gbps transmission system implemented with
Conventional Single Mode Fiber (C-SMF) to examine the role of
Gaussian pulse which is the characteristic of conventional
propagation and Hyperbolic-secant pulse which is the characteristic
of soliton propagation in it. We note the influence of these pulses
with respect to different dispersion lengths and soliton period in
conventional and soliton system respectively and evaluate the system
performance in terms of Quality factor. From the analysis, we could
prove that the soliton pulse has the consistent performance even for
long distance without dispersion compensation than the conventional
system as it is robust to dispersion. For the length of transmission of
200Km, soliton system yielded Q of 33.958 while the conventional
system totally exhausted with Q=0.
[1] Stegeman, G.I., Segev, M.: Optical spatial solitons and their interactions:
universality and diversity. Science 286, 1518–1523 (1999).
[2] N.J. Zabusky and M.D. Kruskal, Interaction of solitons in a collisionless
plasma and recurrence of initial state, Phy. Rev Lett., 15 (6), 1965, 240-
243.
[3] Masataka Nakazawa, Soliton transmission in Telecommunication
Networks, IEEE Communication Magazine, 1994
[4] A. Hasegawa and F. Tappert. Transmission of stationary nonlinear
optical pulse in dispersive dielectric fibers I. Anomalous dispersion,
Applied Phy. Lett. 23 (3), 1976, 142-144.
[5] Mollenauer, L.F., Smith, K.: Demonstration of soliton transmission over
more than 4000 km in fiber with loss periodically compensated by
Raman Gain. Opt. Lett. 13, 1988, 675–677.
[6] Haus, H.A., Wong, W.S.: Solitons in optical communication. Rev. Mod.
Phys. 68(2), 1996, 423–444.
[7] M. Nakazawa, Kimura, and K. Suzuki, Efficient Er3+ doped optical fiber
amplifier pumped by a 1.48μm in InGaAsP laser diode, App. Phy Rev
Lett., 13, 1988, 675-677
[8] Li, T., The impact of optical amplifiers on long-distance lightwave
telecommunications, Proc. IEEE 81, 1568–1579.
[9] Desurvire, E., J. R. Simpson, and P. C. Pecker, 1987, ‘‘High gain
erbium-doped traveling-wave fiber amplifier,’’ Opt. Lett.12, 1987, 888–
890.
[10] Mears, R. J., L. Reekie, I. M. Jauncey, and D. N. Payne, Low-noise
erbium-doped fibre amplifier operating at 1.54 μm, Electron. Lett. 23,
1987, 1026–1028.
[11] Chernikov, S. V., D. J. Richardson, R. I. Laming, E. M. Dianov, and D.
N. Payne, 1992, ‘‘70 Gbit/s fibre based source of fundamental solitons at
1550 nm,’’ Electron. Lett. 28, 1989, 1210–1212.
[12] Desurvire, E., J. W. Sulhoff, J. L. Zyskind, and J. R. Simpson, 1990,
‘‘Spectral dependence of gain saturation and effect of inhomogeneous
broadening in erbium-doped aluminosilicate fiber amplifiers,’’ in
Optical Amplifiers and their Applications, 1990 Technical Digest Series,
Vol. 13 (Optical Society of America, Washington, D.C.), 1989, p. PdP9.
[13] Tachibana, M., R. I. Laming, P. R. Morkel, and D. N. Payne, 1991,
Erbium-doped fiber amplifier with flattened gain spectrum, IEEE
Photonics Technol. Lett. 3, 1991, 118–120.
[14] Runge, P. K., ‘Undersea lightwave systems, AT&T Tech. J. 71, 1992, 5–
13.
[15] Bergano, N. S., and C. R. Davidson, Circulating loop transmission
experiments for the study of long-haul transmission systems using
erbium-doped fiber amplifiers, J. Lightwave Technol. 13, 1995, 879–
888.
[16] Forghieri, F., R. W. Tkach, and A. R. Chraplyvy, WDM systems with
unequally spaced channels, J. Lightwave Technol.13, 1995, 889–897
[17] Hansen, P. B., 2.488 Gbit/s unrepeatered transmission over 423 km
employing remotely pumped post- and preamplifiers, Electron. Lett. 31,
1995, 466–467.
[18] Masatoshi Suzuki, Noboru Edagawa, Hidenori Taga, Hideaki Tanaka,
Shu Yamamoto, and Shigeyuki Akiba, 10 Gb/s, Over 12200 km Soliton
Data Transmission with Alternating-Amplitude Solitons, IEEE Photonic
Tech. Lett. 6 (6), 1994, 757-759.
[19] R.-M. Mu and C. R. Menyuk, Convergence of the Chirped Return-to-
Zero and Dispersion Managed Soliton Modulation Formats in WDM
Systems, Journal of Lightwave Tech. 20 (4), 608,617, 2002.
[20] O. V. Sinkin, J. Zweck, and C. R. Menyuk, Comparative study of pulse
interactions in optical fiber transmission systems with different
modulation formats, Optics Express 9 (7), 2001, 339-352.
[21] P. Shum & H. Ghafouri-Shiraz, Effects of gordon-haus jitter on soliton
transmission, Fiber and Integrated Optics, 16(3), 1997, 303-319.
[22] Segev, M., Stegeman, G.: Self trapping of optical beams, spatial
solitons. Phys. Today. 51, 1998, 42–48.
[23] Aitchison, J.S., Weiner, A.M., Silberberg, Y., Leaird, D.E., Oliver,
M.K., Jackel, J.L., Smith, P.W.E.: Experimental observation of spatial
soliton interactions. Opt. Lett. 16(1), 1991, 15–17.
[24] Konar, S., Biswas, A.: Intra-channel collision of Kerr law optical
solitons. Progr. Electromagn. Res. PIER 53, 2005, 55–67.
[25] Nakazawa, M., Kubota, H., Suzuki, K., Yamada, E., Sahara, A.: Recent
progress in soliton transmission technology. Chaos 10, 2000, 486–514.
[26] Bhupeshwaran Mani · K. Chitra · A. Sivasubramanian, Realization of
soliton interaction in 100 Gbps, uncompensated single channel
telecommunication system implemented with various telecom fibers, J.
of optical and Quantum Electronics, Published September 25, (2014).
[27] H. S. Chung, S. K. Shin, D. W. Lee, D. W. Kim and Y.C Chung, 640
Gbit/s (32x20Gbit/s) WDM transmission with 0.4 (bit/s)/Hz spectral
efficiency using short-period dispersion-managed fibre, Elect. Lett 37
(10), 618-620, 2001.
[28] M. Nakazawa, E. Yoshida, E. Yamada, K. Suzuki, T. Kitoh and M.
Kawachi, “I 6OGbitk soliton data transmission over 200km”, Elect.
Lett., 31(7),1995. 565-566.
[29] Leonard D. Coelho, Camelo J. A. Bastos-Filho and Joaquim F. Martins-
Filho, 160 Gbit/s Soliton Transmission in the S and C Bands,
Proceedings of SBMO/IEEE MTT-S IMOC 2003, 245-249
[30] Jing Huang, Jianquan Yao, Performance comparison between 160 Gb/s
WDM and TDM systems, Optik 123 , 2012 2254– 2259.
[31] Agrawal, G.P.: Nonlinear Fiber Optics, 4th edn. Academic Press, USA
(2008)
[1] Stegeman, G.I., Segev, M.: Optical spatial solitons and their interactions:
universality and diversity. Science 286, 1518–1523 (1999).
[2] N.J. Zabusky and M.D. Kruskal, Interaction of solitons in a collisionless
plasma and recurrence of initial state, Phy. Rev Lett., 15 (6), 1965, 240-
243.
[3] Masataka Nakazawa, Soliton transmission in Telecommunication
Networks, IEEE Communication Magazine, 1994
[4] A. Hasegawa and F. Tappert. Transmission of stationary nonlinear
optical pulse in dispersive dielectric fibers I. Anomalous dispersion,
Applied Phy. Lett. 23 (3), 1976, 142-144.
[5] Mollenauer, L.F., Smith, K.: Demonstration of soliton transmission over
more than 4000 km in fiber with loss periodically compensated by
Raman Gain. Opt. Lett. 13, 1988, 675–677.
[6] Haus, H.A., Wong, W.S.: Solitons in optical communication. Rev. Mod.
Phys. 68(2), 1996, 423–444.
[7] M. Nakazawa, Kimura, and K. Suzuki, Efficient Er3+ doped optical fiber
amplifier pumped by a 1.48μm in InGaAsP laser diode, App. Phy Rev
Lett., 13, 1988, 675-677
[8] Li, T., The impact of optical amplifiers on long-distance lightwave
telecommunications, Proc. IEEE 81, 1568–1579.
[9] Desurvire, E., J. R. Simpson, and P. C. Pecker, 1987, ‘‘High gain
erbium-doped traveling-wave fiber amplifier,’’ Opt. Lett.12, 1987, 888–
890.
[10] Mears, R. J., L. Reekie, I. M. Jauncey, and D. N. Payne, Low-noise
erbium-doped fibre amplifier operating at 1.54 μm, Electron. Lett. 23,
1987, 1026–1028.
[11] Chernikov, S. V., D. J. Richardson, R. I. Laming, E. M. Dianov, and D.
N. Payne, 1992, ‘‘70 Gbit/s fibre based source of fundamental solitons at
1550 nm,’’ Electron. Lett. 28, 1989, 1210–1212.
[12] Desurvire, E., J. W. Sulhoff, J. L. Zyskind, and J. R. Simpson, 1990,
‘‘Spectral dependence of gain saturation and effect of inhomogeneous
broadening in erbium-doped aluminosilicate fiber amplifiers,’’ in
Optical Amplifiers and their Applications, 1990 Technical Digest Series,
Vol. 13 (Optical Society of America, Washington, D.C.), 1989, p. PdP9.
[13] Tachibana, M., R. I. Laming, P. R. Morkel, and D. N. Payne, 1991,
Erbium-doped fiber amplifier with flattened gain spectrum, IEEE
Photonics Technol. Lett. 3, 1991, 118–120.
[14] Runge, P. K., ‘Undersea lightwave systems, AT&T Tech. J. 71, 1992, 5–
13.
[15] Bergano, N. S., and C. R. Davidson, Circulating loop transmission
experiments for the study of long-haul transmission systems using
erbium-doped fiber amplifiers, J. Lightwave Technol. 13, 1995, 879–
888.
[16] Forghieri, F., R. W. Tkach, and A. R. Chraplyvy, WDM systems with
unequally spaced channels, J. Lightwave Technol.13, 1995, 889–897
[17] Hansen, P. B., 2.488 Gbit/s unrepeatered transmission over 423 km
employing remotely pumped post- and preamplifiers, Electron. Lett. 31,
1995, 466–467.
[18] Masatoshi Suzuki, Noboru Edagawa, Hidenori Taga, Hideaki Tanaka,
Shu Yamamoto, and Shigeyuki Akiba, 10 Gb/s, Over 12200 km Soliton
Data Transmission with Alternating-Amplitude Solitons, IEEE Photonic
Tech. Lett. 6 (6), 1994, 757-759.
[19] R.-M. Mu and C. R. Menyuk, Convergence of the Chirped Return-to-
Zero and Dispersion Managed Soliton Modulation Formats in WDM
Systems, Journal of Lightwave Tech. 20 (4), 608,617, 2002.
[20] O. V. Sinkin, J. Zweck, and C. R. Menyuk, Comparative study of pulse
interactions in optical fiber transmission systems with different
modulation formats, Optics Express 9 (7), 2001, 339-352.
[21] P. Shum & H. Ghafouri-Shiraz, Effects of gordon-haus jitter on soliton
transmission, Fiber and Integrated Optics, 16(3), 1997, 303-319.
[22] Segev, M., Stegeman, G.: Self trapping of optical beams, spatial
solitons. Phys. Today. 51, 1998, 42–48.
[23] Aitchison, J.S., Weiner, A.M., Silberberg, Y., Leaird, D.E., Oliver,
M.K., Jackel, J.L., Smith, P.W.E.: Experimental observation of spatial
soliton interactions. Opt. Lett. 16(1), 1991, 15–17.
[24] Konar, S., Biswas, A.: Intra-channel collision of Kerr law optical
solitons. Progr. Electromagn. Res. PIER 53, 2005, 55–67.
[25] Nakazawa, M., Kubota, H., Suzuki, K., Yamada, E., Sahara, A.: Recent
progress in soliton transmission technology. Chaos 10, 2000, 486–514.
[26] Bhupeshwaran Mani · K. Chitra · A. Sivasubramanian, Realization of
soliton interaction in 100 Gbps, uncompensated single channel
telecommunication system implemented with various telecom fibers, J.
of optical and Quantum Electronics, Published September 25, (2014).
[27] H. S. Chung, S. K. Shin, D. W. Lee, D. W. Kim and Y.C Chung, 640
Gbit/s (32x20Gbit/s) WDM transmission with 0.4 (bit/s)/Hz spectral
efficiency using short-period dispersion-managed fibre, Elect. Lett 37
(10), 618-620, 2001.
[28] M. Nakazawa, E. Yoshida, E. Yamada, K. Suzuki, T. Kitoh and M.
Kawachi, “I 6OGbitk soliton data transmission over 200km”, Elect.
Lett., 31(7),1995. 565-566.
[29] Leonard D. Coelho, Camelo J. A. Bastos-Filho and Joaquim F. Martins-
Filho, 160 Gbit/s Soliton Transmission in the S and C Bands,
Proceedings of SBMO/IEEE MTT-S IMOC 2003, 245-249
[30] Jing Huang, Jianquan Yao, Performance comparison between 160 Gb/s
WDM and TDM systems, Optik 123 , 2012 2254– 2259.
[31] Agrawal, G.P.: Nonlinear Fiber Optics, 4th edn. Academic Press, USA
(2008)
@article{"International Journal of Information, Control and Computer Sciences:70053", author = "Bhupeshwaran Mani and S. Radha and A. Jawahar and A. Sivasubramanian", title = "Characteristic Study on Conventional and Soliton Based Transmission System", abstract = "Here, we study the characteristic feature of
conventional (ON-OFF keying) and soliton based transmission
system. We consider 20Gbps transmission system implemented with
Conventional Single Mode Fiber (C-SMF) to examine the role of
Gaussian pulse which is the characteristic of conventional
propagation and Hyperbolic-secant pulse which is the characteristic
of soliton propagation in it. We note the influence of these pulses
with respect to different dispersion lengths and soliton period in
conventional and soliton system respectively and evaluate the system
performance in terms of Quality factor. From the analysis, we could
prove that the soliton pulse has the consistent performance even for
long distance without dispersion compensation than the conventional
system as it is robust to dispersion. For the length of transmission of
200Km, soliton system yielded Q of 33.958 while the conventional
system totally exhausted with Q=0.", keywords = "Soliton, dispersion length, Soliton period, Return-tozero
(RZ), Q-factor.", volume = "9", number = "6", pages = "1417-10", }
