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Femtosecond X-ray solution scattering reveals that bond formation mechanism of a gold trimer complex is independent of excitation wavelength
Author(s) -
Kyung Hwan Kim,
Jong Goo Kim,
Key Young Oang,
Tae Wu Kim,
Hosung Ki,
Junbeom Jo,
Jeongho Kim,
Tokushi Sato,
Shunsuke Nozawa,
Shinichi Adachi,
Hyotcherl Ihee
Publication year - 2016
Publication title -
structural dynamics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.415
H-Index - 29
ISSN - 2329-7778
DOI - 10.1063/1.4948516
Subject(s) - trimer , femtosecond , excitation , excitation wavelength , scattering , wavelength , mechanism (biology) , materials science , molecular physics , chemical physics , optics , chemistry , physics , optoelectronics , dimer , laser , nuclear magnetic resonance , quantum mechanics
The [Au(CN) 2 − ] 3 trimer in water experiences a strong van der Waals interaction between the d 10 gold atoms due to large relativistic effect and can serve as an excellent model system to study the bond formation process in real time. The trimer in the ground state (S 0 ) exists as a bent structure without the covalent bond between the gold atoms, and upon the laser excitation, one electron in the antibonding orbital goes to the bonding orbital, thereby inducing the formation of a covalent bond between gold atoms. This process has been studied by various time-resolved techniques, and most of the interpretation on the structure and dynamics converge except that the structure of the first intermediate (S 1 ) has been debated due to different interpretations between femtosecond optical spectroscopy and femtosecond X-ray solution scattering. Recently, the excitation wavelength of 267 nm employed in our previous scattering experiment was suggested as the culprit for misinterpretation. Here, we revisited this issue by performing femtosecond X-ray solution scattering with 310 nm excitation and compared the results with our previous study employing 267 nm excitation. The data show that a linear S 1 structure is formed within 500 fs regardless of excitation wavelength and the structural dynamics observed at both excitation wavelengths are identical to each other within experimental errors.

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