Ultrashort soliton propagation in multi-clad optical fibers with per channel data rate of 1Tb/s

Salimullah, Shah Md.; Faisal, Mohammad

doi:10.1109/ictp.2015.7427921

Cited by 5 publications

(4 citation statements)

References 13 publications

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“…

S_{D} = \frac{italicdD}{italicdλ} = {[\frac{2 italicπc}{λ^{2}}]}^{2} β_{3} + ([], \frac{4 πc}{λ^{3}}) β_{2},

where S D is dispersion slope, β 3 and β 2 are 3OD and 2OD and c is the speed of light. The nonlinear span is manifested below,

{NL}_{s} = \frac{1}{((), γ) ((), P_{italicpi})},

where P pi is peak power of fractional‐order OBSs envelope, the below equation supports the computation of initial peak power

P_{pi} = \frac{∣ β_{2} ∣}{γ {T_{i}}^{2}} .

…”

Section: Governing Model and Equationssupporting

confidence: 66%

“…The given relation assists in the creation of fractional‐order OBSs envelope. The 2OD dispersive span D s is computed as,

D_{s} = \frac{{T_{i}}^{2}}{∣ β_{2} ∣},

where β 2 is 2OD, which is −20.4 ps 2 /km. The relation between 3OD dispersive span and β 3,

{D_{s}}^{'} = \frac{{T_{i}}^{3}}{∣ β_{3} ∣},

where β 3 is taken as 2 ps 3 /km.…”

Section: Governing Model and Equationsmentioning

confidence: 99%

“…The 2OD dispersive span D s is computed as,

D_{s} = \frac{{T_{i}}^{2}}{∣ β_{2} ∣},

where β 2 is 2OD, which is −20.4 ps 2 /km. The relation between 3OD dispersive span and β 3,

{D_{s}}^{'} = \frac{{T_{i}}^{3}}{∣ β_{3} ∣},

where β 3 is taken as 2 ps 3 /km. The nonlinearity parameter γ relation with effective area A eff is given below,

γ = \frac{2 italicπN}{normalλ A_{eff}},

where N shows nonlinear refractive index which is 2.6 e − 20 m 2 W −1 , λ is wavelength which 1550 nm and A eff is effective area of core of nonlinear dispersive (NLDF) Span which varies from 8 to 17 μm 2 .…”

Section: Governing Model and Equationsmentioning

confidence: 99%

“…The propagation of optical solitons through optical fiber is an extensive area of research with its valuable performance in all optical communication framework. The nonlinear Schrodinger equation (NLSE) is vastly utilized to display models in several areas such as nonlinear optics, optoelectronics, nonlinear sciences, mathematical biosciences, plasma physics, theoretical physics, nuclear physics, physical science and many more . The features of NLSE are contributed in text books on nonlinear optics .…”

Section: Introductionmentioning

confidence: 99%

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Generation and transmission of fractional‐order optical bright solitons in single mode fiber

Mehboob

Usman

Hussain

2019

Micro & Optical Tech Letters

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This article addresses the generation and transmission of fractional-order optical bright solitons (OBSs) in silica based single mode fiber. We take into account secondorder dispersion effect in the presence of anomalous dispersion and self-phase modulation together with third-order dispersion. Fractional-order OBS have been extracted using nonlinear Schrodinger equation. We consider dispersion dominant case with variation of data rates from 10 to 60 Gbps covering ultralong distance of 9040 km. The transmission link is composed of optical amplifier with gain of 20 dB and a noise figure of 4 dB. The analytical computations are carried out to calculate the nonlinear dispersive effects and a comparison is made between the analytical and simulated results. Erbiumdoped fiber amplifier and dispersion compensated fiber have been used to overcome fluctuations and to maintain the fractional-order OBS pulse profile. In the end, the outcomes are probed and compared on the basis of Q-factor and bit error rate (BER). It is observed that best OBS transmission result is achieved at 40 Gbps, where Q-factor is 9.85 with a corresponding BER of 2.91e −23 . K E Y W O R D S nonlinear Schrodinger equation, optical bright solitons, second-order dispersion, self-phase modulation, third-order dispersion

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“…

S_{D} = \frac{italicdD}{italicdλ} = {[\frac{2 italicπc}{λ^{2}}]}^{2} β_{3} + ([], \frac{4 πc}{λ^{3}}) β_{2},

where S D is dispersion slope, β 3 and β 2 are 3OD and 2OD and c is the speed of light. The nonlinear span is manifested below,

{NL}_{s} = \frac{1}{((), γ) ((), P_{italicpi})},

where P pi is peak power of fractional‐order OBSs envelope, the below equation supports the computation of initial peak power

P_{pi} = \frac{∣ β_{2} ∣}{γ {T_{i}}^{2}} .

…”

Section: Governing Model and Equationssupporting

confidence: 66%

“…The given relation assists in the creation of fractional‐order OBSs envelope. The 2OD dispersive span D s is computed as,

D_{s} = \frac{{T_{i}}^{2}}{∣ β_{2} ∣},

where β 2 is 2OD, which is −20.4 ps 2 /km. The relation between 3OD dispersive span and β 3,

{D_{s}}^{'} = \frac{{T_{i}}^{3}}{∣ β_{3} ∣},

where β 3 is taken as 2 ps 3 /km.…”

Section: Governing Model and Equationsmentioning

confidence: 99%

“…The 2OD dispersive span D s is computed as,

D_{s} = \frac{{T_{i}}^{2}}{∣ β_{2} ∣},

where β 2 is 2OD, which is −20.4 ps 2 /km. The relation between 3OD dispersive span and β 3,

{D_{s}}^{'} = \frac{{T_{i}}^{3}}{∣ β_{3} ∣},

where β 3 is taken as 2 ps 3 /km. The nonlinearity parameter γ relation with effective area A eff is given below,

γ = \frac{2 italicπN}{normalλ A_{eff}},

Section: Governing Model and Equationsmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

Generation and transmission of fractional‐order optical bright solitons in single mode fiber

Mehboob

Usman

Hussain

2019

Micro & Optical Tech Letters

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show abstract

Extremely Low and Compressed Soliton Generation in Hyperbolic Decreasing Dispersion Fiber

Salimullah

Faisal

2019

2019 International Conference on Electrical, Computer and Communication Engineering (ECCE)

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Optimization of Fiber Profile Based on Ultrashort Fundamental Soliton Compression

Salimullah¹,

Faisal

Muhaimin

et al. 2018

2018 International Conference on Computer, Communication, Chemical, Material and Electronic Engineering (IC4ME2)

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Ultrashort soliton propagation in multi-clad optical fibers with per channel data rate of 1Tb/s

Cited by 5 publications

References 13 publications

Generation and transmission of fractional‐order optical bright solitons in single mode fiber

Generation and transmission of fractional‐order optical bright solitons in single mode fiber

Extremely Low and Compressed Soliton Generation in Hyperbolic Decreasing Dispersion Fiber

Optimization of Fiber Profile Based on Ultrashort Fundamental Soliton Compression

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