2014
DOI: 10.1103/physreva.89.013813
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Static third-harmonic lines in widely variable fiber continuum generation

Abstract: An intriguing phenomenon of third-harmonic generation under fiber continuum generation is the emission of an anharmonic signal. One popular interpretation of this effect has developed into a general theory of fiber third-harmonic generation. Here we produce “static” third-harmonic Unes dictated fully by fiber properties independent of pump parameters, in contrast to the signals of all known phase-matched nonlinear optical processes that vary dynamically with these parameters. We argue that the anharmonic signa… Show more

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Cited by 4 publications
(5 citation statements)
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“…Following the same procedure for a jump process one can define a Laplace transform of the probability of current, analogous to equation (11) (with an integral instead of a sum). The time evolution of this Laplace transform follows equation (14). Hence, the SCGF λ(z) can be expressed in terms of the maximum eigenvalue ρ 1 (z) trough the formula (20).…”
Section: Appendix B Diusion Processesmentioning
confidence: 99%
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“…Following the same procedure for a jump process one can define a Laplace transform of the probability of current, analogous to equation (11) (with an integral instead of a sum). The time evolution of this Laplace transform follows equation (14). Hence, the SCGF λ(z) can be expressed in terms of the maximum eigenvalue ρ 1 (z) trough the formula (20).…”
Section: Appendix B Diusion Processesmentioning
confidence: 99%
“…Within this theory, periodically driven systems are modeled as Markov processes with time-dependent transition rates that are periodic. Such modeling has been used in several works that include: models for stochastic resonance [4], linear response theory for periodically driven systems [5][6][7][8][9][10][11], theoretical studies for small heat engines far from equilibrium [12][13][14][15], necessary conditions for the generation of a current in a molecular pump [16][17][18][19][20], a mapping relating periodically driven systems with systems driven by a fixed thermodynamic anity [21,22], and 2.5 large deviations for Markov process with time-periodic generators [23,24]. However, a generic formalism to evaluate the rate of large deviations of single currents is still not available.…”
Section: Introductionmentioning
confidence: 99%
“…must be fulfilled. The equality in equations ( 17) and ( 18) corresponds to the quasi-static case (16).…”
Section: Adiabatic Processesmentioning
confidence: 99%
“…We employ these finite-time adiabatic processes to build the corresponding adiabatic branches of the irreversible Carnot engine. Therefore, our approach differs from other recent attempts to construct an irreversible Carnot engine [14][15][16][17][18], the limitations of which are discussed in what follows. Specifically, we focus on the respective definitions of 'adiabaticity'.…”
Section: Introductionmentioning
confidence: 99%
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