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Femtosecond X-ray solution scattering reveals that bond formation mechanism of a gold trimer complex is independent of excitation wavelength

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 struc...

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Detalles Bibliográficos
Autores principales: Kim, Kyung Hwan, Kim, Jong Goo, Oang, Key Young, Kim, Tae Wu, Ki, Hosung, Jo, Junbeom, Kim, Jeongho, Sato, Tokushi, Nozawa, Shunsuke, Adachi, Shin-ichi, Ihee, Hyotcherl
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Crystallographic Association 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4851617/
https://www.ncbi.nlm.nih.gov/pubmed/27191012
http://dx.doi.org/10.1063/1.4948516
Descripción
Sumario: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.