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The people involved: O. F. Mohammed, J. Dreyer, E. T. J. Nibbering, T.
Elsaesser Former team members: C. Chudoba, F. Tschirschwitz, M. Rini,
A. Kummrow, M. Pfeiffer, A. Usman
Excited
state intramolecular hydrogen transfer

1. Vibrational perspective of hydrogen/proton transfer: the idea
is to probe the hydrogen/proton transfer reaction by inspection of specific vibrational
marker modes of either the reactant or product states. In the case of Excited
State Hydrogen Transfer (ESIHT) in 2-(2'-hydroxyphenyl) benzothiazole (HBT) we
monitor the infrared active vibrations in the fingerprint region, in particular
the C=O stretching band of the keto*-state located at 1530 cm-1. |
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2. 2-(2'-hydroxyphenyl)benzothiazole
(HBT) exists in the enol form in the electronic ground
state. After electronic excitation to the S1 state a rapid hydrogen
transfer occurs towards the keto*-state. The latter product state can be probed
by inspection of the infrared active C=O stretching band. | | |

3. Typical features observed in spectrally resolved femtosecond UV
pump / IR probe spectroscopy. At negative delay times contributions occur due
to the perturbed free induction decay of vibrational bands in the electronic ground
state. Around zero delay solvent signals appear that are frequency independent
with comparable magnitudes as the solute bands. At postive delay times the bleach
signals of the reactant modes and absorbance signals due to product bands contribute
to the pump-probe results. | | | |
4. The C=O stretching band marking the
appearance of the keto*-state shows a delayed rise, indicating a delayed hydrogen
transfer process. Subsequent blue shifting of the C=O band is clearly seen in
the transient spectra. | | | |
5. After the hydrogen transfer process
the C=O band position is a) modulated by anharmonically coupled low frequency
modes that have been coherently excited by the UV pump pulse or by the hydrogen
transfer process. The blue-shifting behaviour with clear sub-picosecond and picosecond
components indicate the ongoing intramolecular vibrational redistribution and
vibrational cooling processes through which the excess energy of the hydrogen
transfer is channeled, thereby making the hydrogen transfer process ultrafast
and irreversible. | | | | infrared
active out-of-plane twisting mode | |

| | | | infrared-active
twisting mode | | 
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| | | Raman
active in-plane deformation mode | |
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| 6. The
coherent modulations with frequencies of 60 and 120 cm-1 are ascribed
to the infrared active out-of-plane twisting mode (top) and the Raman active in-plane
deformation mode (bottom) respectively. The latter is coherently excited by the
UV pump pulse, the other is impulsively excited before/during the hydrogen transfer
process, but not by the optical pump pulse. The twisting mode (middle) is assumed
not to contribute to the coherent oscillations in the pump-probe signals as it
does not significantly modulate the hydrogen bond distance.
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