Vibrational Relaxation Dynamics of an Azido–Cobalt(II) Complex from Femtosecond UV-Pump/MIR-Probe Spectroscopy and Model Simulations with Ab Initio Anharmonic Couplings

2020 ◽  
Vol 59 (20) ◽  
pp. 14629-14642
Author(s):  
Steffen Straub ◽  
Jessica Stubbe ◽  
Jörg Lindner ◽  
Biprajit Sarkar ◽  
Peter Vöhringer
2011 ◽  
Vol 115 (13) ◽  
pp. 2892-2899 ◽  
Author(s):  
Pedro Pajón-Suárez ◽  
Jesús Rubayo-Soneira ◽  
Ramón Hernández-Lamoneda

2015 ◽  
Vol 177 ◽  
pp. 65-75 ◽  
Author(s):  
Yuki Fukui ◽  
Kaoru Ohta ◽  
Keisuke Tominaga

We studied the effects of hydrogen bonds on the vibrational structures and vibrational dynamics of the CO stretching mode of 9-fluorenone (FL) in the electronically excited state in aprotic and protic solvents using sub-picosecond visible-pump and IR-probe spectroscopy. The transient IR spectrum of the CO stretching band in methanol-d4 has two bands at 1529.9 cm−1 and 1543.4 cm−1, which are assigned to an FL-solvent complex and free FL, respectively. In the aprotic solvents, the CO stretching bands show blue-shifts in time. This shift is due to vibrational cooling, which is derived from anharmonic couplings with some low-frequency modes. Interestingly, a red-shift is observed at later delay time for the band at 1529.9 cm−1 in methanol-d4. A possible mechanism of this spectral shift is related to the hydrogen bond dynamics between the solute and solvent.


CLEO: 2015 ◽  
2015 ◽  
Author(s):  
Daniel Hutzler ◽  
Jasper C. Werhahn ◽  
Rupert Heider ◽  
Maximilian Bradler ◽  
Reinhard Kienberger ◽  
...  

2011 ◽  
Vol 84 (17) ◽  
Author(s):  
Y. Toda ◽  
T. Mertelj ◽  
P. Kusar ◽  
T. Kurosawa ◽  
M. Oda ◽  
...  

2001 ◽  
Vol 15 (28n30) ◽  
pp. 3965-3968
Author(s):  
ATSUSHI SUGITA ◽  
TAKASHI SAITO ◽  
TAKAYOSHI KOBAYASHI ◽  
MASAHIRO YAMASHITA

A quasi-one-dimensional halogen-bridged mixed-valence metal complex is studied by time-resolved pump and probe spectroscopy with sub-5 fs time resolution. Two kinds of oscillatory signals are observed, which are attributed to the wave packet motions both in an electronic ground state and in a self-trapped exciton (STE) state. The onset of the wave packet motion is found to be delayed by about 50 fs, comparing with the ideal wave packet in the electronic excited state. The delay reflects the thermalization process in a free exciton (FE) state and a lattice relaxation process from FE to STE states.


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