Webphase can describe the pulse behavior satisfactorily. If they do, the theoretical description of pulse propagation and interaction with matter can be greatly simpli-fied by applying the slowly varying envelope approximation (SVEA), as will be evident later in this chapter. Note that even for pulses consisting of a few optical WebFor sech 2-shaped pulses, the pulse duration is ≈ 0.65 times the width of the autocorrelation signal, but this conversion factor depends on the pulse shape. A rough evaluation is often …
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Web1 Jan 2009 · Amplitude modulation (AM), frequency modulation (FM), and time-dependent longitudinal magnetization of the HS pulse (sech/tanh). The HS pulse shown has T p = 2 ms and BW/2π = 10 kHz. (a) AM functions (ω 1 (t)/2π) are shown for π/2 excitation and π inversion (ω 1 max /2π = 1.35 and 4 kHz, respectively). Web28 Feb 2024 · Here, we assume input vector solitons in our simulation have sech pulse profiles in orthogonal directions. After modulation of the amplitude ratio, time delay, pulse chirp and phase difference, the electric fields in orthogonal directions after Col and before PBS are expressed as: A0 1 (t) = A1sech 1.763(t DT/2) T0 exp (iC1 1.763(t DT/2) 0 2 ... black duck integration with jenkins
Operating Vector Solitons with Chirped Sech Pulse Shapes
WebAn interesting question is whether soliton-like solutions exist near the zero-dispersion wavelength of an optical fiber. In the case of β 2 = 0, numerical solutions show [148] that a sech-shape pulse evolves over a length ξ ′ ∼ 10 / N ˜ 2 into a soliton that contains about half of the pulse energy. The remaining energy is carried by an ... Web1 Apr 2024 · The soliton with super-sech pulse shape has also been theoretically analyzed, but the generation of super-sech optical soliton in fiber laser has seldom been reported. … WebTRANSFORM-LIMITED PULSE A. Analysis of the spectrum of a Gaussian pulse 1. Analysis In order to introduce the basis of our discussion, we first consider the case of the widely used Fourier-transform-limited Gaussian pulse with the temporal intensity profile: I(t) = G(t) = exp(−(t/T 0)2), where T 0 is the half-width at 1/e intensity point ... gamecocks bonn