117Sn and 119Sn hyperfine structure in the rotational spectrum of tin monosulfide recorded using laser ablation-source equipped, chirped-pulse Fourier transform microwave spectroscopy

2010 ◽  
Vol 259 (2) ◽  
pp. 120-122 ◽  
Author(s):  
G.S. Grubbs ◽  
S.A. Cooke
Keyword(s):  
Fourier Transform ◽  
Laser Ablation ◽  
Hyperfine Structure ◽  
Microwave Spectroscopy ◽  
Rotational Spectrum ◽  
Chirped Pulse ◽  
Fourier Transform Microwave Spectroscopy

scholarly journals Hydrogen bonding in the ethanol–water dimer

2015 ◽  
Vol 17 (37) ◽  
pp. 24210-24214 ◽  
Author(s):  
Ian A. Finneran ◽  
P. Brandon Carroll ◽  
Marco A. Allodi ◽  
Geoffrey A. Blake
Keyword(s):  
Hydrogen Bonding ◽  
Fourier Transform ◽  
Ground State ◽  
Microwave Spectroscopy ◽  
Water Dimer ◽  
Rotational Spectrum ◽  
Chirped Pulse ◽  
Fourier Transform Microwave Spectroscopy

We report the first rotational spectrum of the ground state of the isolated ethanol–water dimer using chirped-pulse Fourier transform microwave spectroscopy between 8–18 GHz.

The rotational spectrum of epifluorohydrin measured by chirped-pulse Fourier transform microwave spectroscopy

2006 ◽  
Vol 238 (2) ◽  
pp. 200-212 ◽  
Author(s):  
Gordon G. Brown ◽  
Brian C. Dian ◽  
Kevin O. Douglass ◽  
Scott M. Geyer ◽  
Brooks H. Pate
Keyword(s):  
Fourier Transform ◽  
Microwave Spectroscopy ◽  
Rotational Spectrum ◽  
Chirped Pulse ◽  
Fourier Transform Microwave Spectroscopy

33S Nuclear Hyperfine Structure in the Rotational Spectrum of Thiazole

1993 ◽  
Vol 48 (12) ◽  
pp. 1219-1222 ◽  
Author(s):  
U. Kretschmer ◽  
H. Dreizler
Keyword(s):  
Fourier Transform ◽  
Hyperfine Structure ◽  
Molecular Beam ◽  
Microwave Spectroscopy ◽  
Coupling Constants ◽  
Rotational Spectrum ◽  
Centrifugal Distortion ◽  
Quadrupole Coupling ◽  
Nuclear Quadrupole ◽  
Centrifugal Distortion Constants

Abstract We investigated the 33S nuclear quadrupole coupling of thiazole- 33S in natural abundance by molecular beam Fourier transform microwave spectroscopy. In addition the 14N nuclear quadrupole coupling could be analyzed with high precision. We derived the rotational constants A = 8529.29268 (70) MHz, B = 5427.47098 MHz, and C = 3315.21676 (26) MHz, quartic centrifugal distortion constants and the quadrupole coupling constants of 33S χaa = 7.1708 (61) MHz and χbb= -26.1749 (69) MHz and of 14N χ aa = -2.7411 (61) MHz and χbb = 0.0767 (69) MHz.

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