𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Vacuum ultraviolet photoelectron spectroscopy of transient species. XVII. The SiH3(X 2A1) radical

✍ Scribed by J.M. Dyke; N. Jonathan; A. Morris; A. Ridha; M.J. Winter

Publisher
Elsevier Science
Year
1983
Tongue
English
Weight
636 KB
Volume
81
Category
Article
ISSN
0301-0104

No coin nor oath required. For personal study only.

πŸ“œ SIMILAR VOLUMES

Observation of the CH2 OH radical in the
Observation of the CH2 OH radical in the gas phase by vacuum ultraviolet photoelectron spectroscopy
✍ J.M. Dyke; A.R. Ellis; N. Jonathan; N. Keddar; A. Morris πŸ“‚ Article πŸ“… 1984 πŸ› Elsevier Science 🌐 English βš– 371 KB

The Iiis~ ptIoIoclccIron hnd of I~C Ct!2011 radiwl has been obscrvcd will1 a mulIidctccIor phoIoclccIron spccrromcrcr. It cxhibitcd clear vibrational sIrucIurc in IWO vibrdIiona1 modes which wcrc assigned IO cscirarion of the C-O stretch and Cl11 dcformaIion mode in Ihc ion. 'I'hc vcrticll and adiab

Laser Excitation Spectroscopy of theB̃2A
Laser Excitation Spectroscopy of theBΜƒ2A1–XΜƒ2A1Transition of the CaOCH3Radical
✍ C.J. Whitham; S.A. Beaton; Y. Ito; J.M. Brown πŸ“‚ Article πŸ“… 1998 πŸ› Elsevier Science 🌐 English βš– 237 KB

The (0 -0) band of the B ˜2A 1 -X ˜2A 1 transition of CaOCH 3 at 565 nm has been recorded and analyzed at Doppler limited resolution (FWHM Ο­ 0.005 cm Οͺ1 ). The molecule was generated using a laser ablation/molecular beam source in which a solid calcium rod was ablated and a mixture of argon seeded w

Stimulated Emission Pumping Spectroscopy
Stimulated Emission Pumping Spectroscopy of SiH2: First Observation of the Spin–Orbit Interaction between the XΜƒ1A1 and the Γ£3B1 States
✍ Haruki Ishikawa; Yasuhiko Muramoto; Naohiko Mikami πŸ“‚ Article πŸ“… 2002 πŸ› Elsevier Science 🌐 English βš– 203 KB

Stimulated emission pumping spectra of the Γƒ 1 B 1 -X 1 A 1 transition of the SiH 2 radical were observed in order to obtain information about the Γ£ 3 B 1 state through the spin-orbit interaction. The vibrational level structure of the X state, which is the basis for the present observation of the t