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Volumn 77, Issue 6, 2008, Pages

Monte Carlo simulations of pulse propagation in massive multichannel optical fiber communication systems

Author keywords

[No Author keywords available]

Indexed keywords

BIT ERROR RATE; COMMUNICATION; COMMUNICATION SYSTEMS; COMPUTER SIMULATION; COSMIC RAY DETECTORS; CRACK PROPAGATION; ERROR ANALYSIS; FIBER OPTICS; FIBERS; MODAL ANALYSIS; MONTE CARLO METHODS; NONLINEAR EQUATIONS; OPTICAL COMMUNICATION; OPTICAL FIBERS; OPTICAL MATERIALS; OPTICAL SYSTEMS;

EID: 46149103675     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.77.063835     Document Type: Article
Times cited : (22)

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    • The dimensionless z in Eq. 1 is z= (| β2 | X) / (2 τ0), where X is the actual position, τ0 is the soliton width, and β2 is the second order dispersion coefficient. The dimensionless retarded time is t=τ/ τ0, where τ is the retarded time. The spectral width is ν0 =1/ (π2 τ0) and the frequency difference is Δν= (πΔβ ν0) /2. ψ=E/ P0, where E is proportional to the electric field and P0 is the peak power. The dimensionless second order dispersion coefficient is d=-1= β2 / (γ P0 τ02), where γ is the Kerr nonlinearity coefficient. The coefficient R is given by R =0.006/ τ0, where τ0 is in picoseconds.
    • The dimensionless z in Eq. 1 is z= (| β2 | X) / (2 τ0), where X is the actual position, τ0 is the soliton width, and β2 is the second order dispersion coefficient. The dimensionless retarded time is t=τ/ τ0, where τ is the retarded time. The spectral width is ν0 =1/ (π2 τ0) and the frequency difference is Δν= (πΔβ ν0) /2. ψ=E/ P0, where E is proportional to the electric field and P0 is the peak power. The dimensionless second order dispersion coefficient is d=-1= β2 / (γ P0 τ02), where γ is the Kerr nonlinearity coefficient. The coefficient R is given by R =0.006/ τ0, where τ0 is in picoseconds.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.