TY - JOUR
T1 - Torsional Structural Relaxation Caused by Pt-Pt Bond Formation in the Photoexcited Dimer of Pt(II) N̂ C ̂ N Complex in Solution
AU - Watanabe, Honoka
AU - Iwamura, Munetaka
AU - Nozaki, Koichi
AU - Takanashi, Tsukasa
AU - Kuramochi, Hikaru
AU - Tahara, Tahei
N1 - Publisher Copyright:
© 2024 American Chemical Society.
PY - 2025/1/9
Y1 - 2025/1/9
N2 - [Pt(NCN)MeCN]+ (NCN = 1,3-di(2-pyridyl)benzene, MeCN = acetonitrile) forms oligomers in the ground state due to metallophilic interactions, and a Pt-Pt bond is formed with photoexcitation. Ultrafast excited-state dynamics of the [Pt(NCN)MeCN]+ dimer in acetonitrile is investigated by femtosecond time-resolved absorption (TA) and picosecond emission spectroscopy. The femtosecond TA signals exhibit 60 cm-1 oscillations arising from the Pt-Pt stretching motion in the S1 dimer. The excited-state absorption in the 500-700 nm region increases with time constants of 0.3, 1.4, and 9.4 ps, which are assigned to contraction of the Pt-Pt distance, structural change in the S1 dimer, and S1 → T1 intersystem crossing, respectively. The 1.4 ps structural change is attributed to torsional structural relaxation proceeding in the S1 dimer based on the computation, which indicates that a torsional angle around the Pt-Pt bond in the S0 dimer is widely distributed around two potential minima, whereas that of the S1 dimer has much narrower distributions around noticeably different torsional angles.
AB - [Pt(NCN)MeCN]+ (NCN = 1,3-di(2-pyridyl)benzene, MeCN = acetonitrile) forms oligomers in the ground state due to metallophilic interactions, and a Pt-Pt bond is formed with photoexcitation. Ultrafast excited-state dynamics of the [Pt(NCN)MeCN]+ dimer in acetonitrile is investigated by femtosecond time-resolved absorption (TA) and picosecond emission spectroscopy. The femtosecond TA signals exhibit 60 cm-1 oscillations arising from the Pt-Pt stretching motion in the S1 dimer. The excited-state absorption in the 500-700 nm region increases with time constants of 0.3, 1.4, and 9.4 ps, which are assigned to contraction of the Pt-Pt distance, structural change in the S1 dimer, and S1 → T1 intersystem crossing, respectively. The 1.4 ps structural change is attributed to torsional structural relaxation proceeding in the S1 dimer based on the computation, which indicates that a torsional angle around the Pt-Pt bond in the S0 dimer is widely distributed around two potential minima, whereas that of the S1 dimer has much narrower distributions around noticeably different torsional angles.
UR - http://www.scopus.com/inward/record.url?scp=85214705981&partnerID=8YFLogxK
U2 - 10.1021/acs.jpclett.4c03170
DO - 10.1021/acs.jpclett.4c03170
M3 - 学術論文
C2 - 39737549
AN - SCOPUS:85214705981
SN - 1948-7185
VL - 16
SP - 406
EP - 414
JO - Journal of Physical Chemistry Letters
JF - Journal of Physical Chemistry Letters
IS - 1
ER -