2019
DOI: 10.1016/j.chemphys.2019.02.023
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Time-resolved two-photon spectroscopy of carotenoids

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Cited by 3 publications
(5 citation statements)
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“…A brand-new challenge for the theoretical approaches was set by the femtosecond time-resolved two-photon excitation (2PE) experiments. Due to its multielectron character, the S 0 -S 1 transition is one-photon forbidden, but two-photon allowed. Considering that two-photon excitation does not populate the S 2 , the 2PE transient absorption spectra can be viewed as the “pure” S 1 state, minimizing artifacts arising from the depopulation of the higher lying energy levels.…”
Section: Perspective: Vera On Two-photon Initiated Ultrafast Dynamicsmentioning
confidence: 99%
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“…A brand-new challenge for the theoretical approaches was set by the femtosecond time-resolved two-photon excitation (2PE) experiments. Due to its multielectron character, the S 0 -S 1 transition is one-photon forbidden, but two-photon allowed. Considering that two-photon excitation does not populate the S 2 , the 2PE transient absorption spectra can be viewed as the “pure” S 1 state, minimizing artifacts arising from the depopulation of the higher lying energy levels.…”
Section: Perspective: Vera On Two-photon Initiated Ultrafast Dynamicsmentioning
confidence: 99%
“…(The transient absorption spectra at earlier times are contaminated by the strong coherent artifact.) The experimental setup for 2PE transient absorption spectroscopy was described in detail previously . Briefly, a Spitfire Ace regenerative amplifier system (Spectra Physics), seeded with a Ti:sapphire oscillator (MaiTai SP, Spectra Physics) and pumped by a Nd:YLF laser (Empower 30, Spectra Physics), was used for generating excitation (pump) and probe pulses.…”
Section: Perspective: Vera On Two-photon Initiated Ultrafast Dynamicsmentioning
confidence: 99%
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“…In the lutein/ Chl a mixture, the kinetics decay with a 14 ps lifetime, proving that the signal indeed is due to the S 1 state of lutein, in agreement with recent 2PE transient absorption data on carotenoids in solution. 25 The 540 nm band in LHCII decays much faster, and to exclude the possibility that the fast component is due to carotenoid−Chl EET, we add data showing the carotenoid S 1 decay after 1PE of LHCII at 490 nm. These data represent the selective 1PE of carotenoid in LHCII, thus the kinetics reflect the decay of the carotenoid S 1 state in LHCII.…”
mentioning
confidence: 99%
“…However, the mechanisms of the quenching process are not yet fully investigated and various different models have been proposed that are either based on distinct chlorophyll (Chl)–carotenoid (Car) interactions or on Chl–Chl interactions, only . Here, we study the potential role of energy transfer between optically forbidden states of Cars and the Chls which can be assessed by two‐photon excitation (TPE) . It has been suggested that these forbidden states comprise more than one state – typically termed Car S 1 , Car S x , or Car S* – but for the sake of simplicity, we will name the forbidden states by Car S 1 in the following.…”
mentioning
confidence: 99%