摘要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 425 pm 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.
Abstract：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 425 pm 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.
I. S. Amiri*;A. Afroozeh;M. Bahadoran
. Simulation and Analysis of Multisoliton Generation Using a PANDA Ring Resonator System[J]. 中国物理快报, 2011, 28(10): 104205-104205.
I. S. Amiri*, A. Afroozeh, M. Bahadoran
. Simulation and Analysis of Multisoliton Generation Using a PANDA Ring Resonator System. Chin. Phys. Lett., 2011, 28(10): 104205-104205.
[1] Jukgoljun B, Pipatsart S, Jalil M A, Yupapin P P and Ali J 2011 Optik 122 1492
[2] Yuan Y, Cai Y, Qu J, Eyyuboğu H T, Baykal Y and Korotkova O 2009 Opt. Express 17 17344
[3] Pornsuwancharoen N, Fujii Y, Srinuanjan K and Yupapin P P 2010 Optik 121 1863
[4] Jiang H B 1991 Appl. Phys. B Photophys. Laser Chem. 53 (5-6) 347
[5] Deng D and Guo Q 2007 Opt. Lett. 32 3206
[6] Liaw S K, Hsieh Y S, Cheng W L, Chang C L and Ting H F 2008 J. Opt. Network. 7 662
[7] Yupapin P P and Vanishkorn B 2011 Appl. Math. Model. 35 1729
[8] Mitatha S, Piyatamrong B, Yupapin P P, Knobnob B and Chaiyasoonthorn S 2011 J. Nonlin. Opt. Phys. Mater. 20 85
[9] Su Y, Liu F and Li Q 2007 Proc. SPIE 6783 68732P
[10] Fietz C and Shvets G 2007 Opt Lett. 32 1683
[11] Kokubun Y, Hatakeyama Y, Ogata M, Suzuki S and Zaizen N 2007 IEEE J. Sel. Top. Quantum Electron. 11 4
[12] Jukgoljun B, Suwanpayak N, Teeka C and Yupapin P P 2010 Opt. Engin. 49 12
[13] Agarwal G P 2007 Nonlinear Fiber Optics 4th edn (New York: Academic)
[14] Tasakorn M, Teeka C, Jomtarak R and Yupapin P P 2010 Opt. Engin. 49 075002
[15] Uomwech K, Sarapat K and Yupapin P P 2010 Microwave Opt. Technol. Lett. 52 1818
[16] Phatharaworamet T, Teeka C, Jomtarak R, Mitatha S and Yupapin P P 2010 J. Lightwave Technol. 28 2804
[17] Phattaraworamet T, Jomtarak R, Mitatha S and Yupapin P P 2011 Microwave Opt. Technol. Lett. 53 516
[18] Srinuanjan K, Kamoldilok S, Tipaphong W and Yupapin P P 2011 Optik (in press)
2011, Vol. 28 
