2015
DOI: 10.1021/acs.jpclett.5b00528
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Identification of the Excited-State C═C and C═O Modes of trans-β-Apo-8′-carotenal with Transient 2D-IR-EXSY and Femtosecond Stimulated Raman Spectroscopy

Abstract: Assigning the vibrational modes of molecules in the electronic excited state is often a difficult task. Here we show that combining two nonlinear spectroscopic techniques, transient 2D exchange infrared spectroscopy (T2D-IR-EXSY) and femtosecond stimulated Raman spectroscopy (FSRS), the contribution of the C═C and C═O modes in the excited-state vibrational spectra of trans-β-apo-8'-carotenal can be unambiguously identified. The experimental results reported in this work confirm a previously proposed assignment… Show more

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Cited by 7 publications
(15 citation statements)
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“…This compensates for the probe fluctuations on a shot‐to‐shot basis but requires the simultaneous detection of two pulses at a repetition rate of 1 kHz. Therefore, this scheme is most common in connection with photodiode array detectors but is also used with CCD cameras albeit at lower readout rates . Jin et al .…”
Section: Methodsmentioning
confidence: 99%
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“…This compensates for the probe fluctuations on a shot‐to‐shot basis but requires the simultaneous detection of two pulses at a repetition rate of 1 kHz. Therefore, this scheme is most common in connection with photodiode array detectors but is also used with CCD cameras albeit at lower readout rates . Jin et al .…”
Section: Methodsmentioning
confidence: 99%
“…Therefore, the most common approach is direct supercontinuum generation in transparent dielectrics based on the Kerr effect. Examples include solids like sapphire,, CaF2 and YAG crystals for Yb‐based laser systems, as well as liquids in flow cells, like water and CCl 4 . Liquids, in principle, allow higher fluences, but solids are much easier to use and produce more stable continua.…”
Section: Methodsmentioning
confidence: 99%
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“…The initial ultrafast component may indicate a conical intersection in the vertical Franck−Condon region, directly funneling molecules back to S 0 , or to a lower lying dark state. An alternative explanation is the infrared transition dipole (Table 2), centered roughly at 1590 cm −1 , and from transient 2DIR exchange spectroscopy measurements in cyclohexane, 34 we can assign this to the excited state CO symmetric stretch. The large change in fundamental frequency associated with the C O bond on the excited state (the frequency is reduced by ∼70 cm −1 ), likely reflects a weaker C−O bond on the excited state.…”
Section: Resultsmentioning
confidence: 92%