2009
DOI: 10.1021/jp8056064
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Relaxation Dynamics of Naphthalene and 1-Aminonaphthalene in Superexcited States

Abstract: The relaxation dynamics of naphthalene (NPH) and 1-aminonaphthalene (AMN) in superexcited (SE) states has been investigated by pump-probe femtosecond ionization. SE states were produced by two-photon resonant absorption via S1 and S2 states and their time evolution probed by ionization with 800 nm light pulses. A fine-tuning of the pump and probe laser intensities permits us to separate the dynamics of the SE states from that of the S1/S2 intermediate states. SE state relaxation pathways were investigated in t… Show more

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Cited by 13 publications
(24 citation statements)
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“…Clearly, it cannot be attributed to background signal produced by two pump‐photon absorption, because in this case, it would also be observed at positive delay times. A signal at negative delay times has been reported for several aromatic molecules, for which two possible explanations were given: 1) dynamics of states excited by the probe beam (inverse pump‐probe process) and 2) two‐photon absorption by the pump beam; this causes excitation at superexcited neutral states and/or ionization, with subsequent dissociation caused by the probe beam, which thus leads to depletion of the baseline. The latter case would contaminate the processes under investigation, whereas the former would not affect them significantly, as the decay would occur towards the negative delay times.…”
Section: Resultsmentioning
confidence: 99%
“…Clearly, it cannot be attributed to background signal produced by two pump‐photon absorption, because in this case, it would also be observed at positive delay times. A signal at negative delay times has been reported for several aromatic molecules, for which two possible explanations were given: 1) dynamics of states excited by the probe beam (inverse pump‐probe process) and 2) two‐photon absorption by the pump beam; this causes excitation at superexcited neutral states and/or ionization, with subsequent dissociation caused by the probe beam, which thus leads to depletion of the baseline. The latter case would contaminate the processes under investigation, whereas the former would not affect them significantly, as the decay would occur towards the negative delay times.…”
Section: Resultsmentioning
confidence: 99%
“…The intensities of pump pulses at the ionization region were optimized to avoid saturation effects and contributions from higher excited states. 43 The probe beams intensities were estimated to be, (1.4-2) × 10 10 , (0.7-1) × 10 11 , and (3.5-6) × 10 11 W/cm 2 for the 400, 800, and 1305 nm probe beams. The relative polarization was set at magic angle, except for the polarization anisotropy measurements.…”
Section: Methodsmentioning
confidence: 95%
“…The experimental method and apparatus have already been described elsewhere 33 and only a brief description is included in this section.…”
Section: Experimental Methodsmentioning
confidence: 99%