2012
DOI: 10.9790/4861-0214348
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Dark-Bright Solitons Conversion System for Secured and Long Distance Optical Communication

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Cited by 14 publications
(7 citation statements)
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References 25 publications
(23 reference statements)
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“…By using the bright soliton input signal, the operation can be successfully achieved by dark-bright soliton conversion within microring resonator, which can be used to represent optical logic NOT gate (optical switching). This dark-bright soliton conversion can be controlled, where the high-security communication in long distance using such concept has been reported and confirmed [29,30]. The simulation shows that the ultrafast-optical switching time of ( =0.14 ps), an on-off ratio of ~47.99 and propagation time of ~0.30 ps are obtained.…”
Section: Resultssupporting
confidence: 62%
“…By using the bright soliton input signal, the operation can be successfully achieved by dark-bright soliton conversion within microring resonator, which can be used to represent optical logic NOT gate (optical switching). This dark-bright soliton conversion can be controlled, where the high-security communication in long distance using such concept has been reported and confirmed [29,30]. The simulation shows that the ultrafast-optical switching time of ( =0.14 ps), an on-off ratio of ~47.99 and propagation time of ~0.30 ps are obtained.…”
Section: Resultssupporting
confidence: 62%
“…For the soliton pulse in the micro ring device, a balance should be achieved between the dispersion length (L D ) and the nonlinear length (L NL = (1/ NL ) [46], where  = n 2 ×k 0 , is the length scale over which disperse or nonlinear effects makes the beam becomes wider or narrower [47][48][49][50]. For a soliton pulse, there is a balance between dispersion and nonlinear lengths, hence L D =L NL [51][52][53].…”
Section: Theoretical Modelingmentioning
confidence: 99%
“…is given [61], then o T is known [62]. For the soliton pulse in the micro ring device, a balance should be achieved between the dispersion length (L D ) [63][64][65] and the nonlinear length (L NL = (1/ NL ) [66][67][68] , where  = n 2 ×k 0 [69], is the length scale over which disperse or nonlinear effects makes the beam becomes wider or narrower [70][71].…”
Section: Entangled Photon Encoding Using Trapping Of Picoseconds Solimentioning
confidence: 99%