1999
DOI: 10.1016/s0030-4018(99)00297-7
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Intensity threshold in the conversion from reverse saturable absorption to saturable absorption and its application in optical limiting

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Cited by 41 publications
(25 citation statements)
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“…Hence, the RSA type of nonlinearity observed here in semiconducting TBO-PVA nanocomposite films at 632.8 nm excitation may primarily be attributed to an ESA process actuated by the population build up in the triplet state [11]. However, the SA type of nonlinearity observed at high intensity (around focus), which occurs after the observation of RSA, may be assigned to the saturation of RSA, as has been reported earlier [22,42]. Herein, the fall of β with I 0 may be the consequence of an ESA assisted RSA process.…”
Section: Resultssupporting
confidence: 74%
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“…Hence, the RSA type of nonlinearity observed here in semiconducting TBO-PVA nanocomposite films at 632.8 nm excitation may primarily be attributed to an ESA process actuated by the population build up in the triplet state [11]. However, the SA type of nonlinearity observed at high intensity (around focus), which occurs after the observation of RSA, may be assigned to the saturation of RSA, as has been reported earlier [22,42]. Herein, the fall of β with I 0 may be the consequence of an ESA assisted RSA process.…”
Section: Resultssupporting
confidence: 74%
“…This flip-flop can be explained on the basis of triplet state excitation in detailed using a four-level model (see Fig. 8) [42,43]. The unfilled PVA film yielded no Z-scan signals (see Fig.…”
Section: Resultsmentioning
confidence: 99%
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“…influence of different parameters on the RSA/SA conversion intensity based on a three-level manifold with three consecutive one-photon absorption processes. 18 They demonstrated that, for an RSA/SA switch to occur, the cross-section of the higher lying excited state must be lower than that of the lower lying excited 25 state, which in turn must be larger than that of the ground state absorption cross-section. The switch occurs only when the intensity threshold is reached.…”
Section: Impact Of the Four-level Model Fitting Parameters On The Nonmentioning
confidence: 99%
“…RSA in porphyrin materials is usually induced by two photon absorption or excited-state absorption [31][32][33][34]. Saturable absorption (SA) as well as switch between SA and RSA are also observed in porphyrins [35,36], which is useful for mode locking, laser pulse compression, and laser amplification [37]. In this article, cyano (CN) and methoxy (OMe) substitutes as the typical acceptor and donor groups are introduced into TPP to synthesize the meso-tetrakis(4-cyano phenyl)porphyrin [TPP(CN) 4 ], and meso-tetrakis(4-methoxyphe nyl)porphyrin [TPP(OMe) 4 ], respectively.…”
Section: Introductionmentioning
confidence: 99%