Gas-phase infrared spectrum of the anionic GFP-chromophore

2012 ◽  
Vol 330-332 ◽  
pp. 118-123 ◽  
Author(s):  
Mitra Almasian ◽  
Josipa Grzetic ◽  
Giel Berden ◽  
Bert Bakker ◽  
Wybren Jan Buma ◽  
...  
1981 ◽  
Vol 59 (5) ◽  
pp. 663-672 ◽  
Author(s):  
K-E. J. Hallin ◽  
J. W. C. Johns ◽  
A. Trombetti

The gas phase spectrum of N2H2 has been investigated in the region of 7.6 μm at a resolution of about 0.06cm−1. Two bands have been identified; one, near 1288 cm−1, is a type C band and must correspond to ν4 (the hitherto unidentified Au torsional mode), and the other, near 1317 cm−1, is a type A–B hybrid and corresponds to ν6 (the Bu bending mode). Analysis of the spectrum is complicated by the simultaneous presence of strong A-type and B-type Coriolis interactions which couple the observed levels.


1972 ◽  
Vol 26 (5) ◽  
pp. 540-542 ◽  
Author(s):  
G. R. Burns ◽  
D. G. McGavin

Infrared and Raman spectra have been measured for spiropentane-H8. Raman spectra for the liquid have enabled the b1 species ring twist to be assigned. Previous assignments of this mode were based on calorimetric data and on the assignment of a band in the infrared spectrum to a combination band involving the ring twist mode. Infrared spectra of low temperature crystalline films have provided sufficient information that, when taken with the Raman data and gas phase infrared spectra, we have assignments for all of the fundamental modes.


1999 ◽  
Vol 110 (8) ◽  
pp. 3861-3869 ◽  
Author(s):  
Helga Körsgen ◽  
Wolfgang Urban ◽  
John M. Brown

1988 ◽  
Vol 145 (2) ◽  
pp. 143-145 ◽  
Author(s):  
Cornelis E. Blom ◽  
Hartmut G. Hedderich

2011 ◽  
Vol 308 (2-3) ◽  
pp. 175-180 ◽  
Author(s):  
Gary S. Groenewold ◽  
Michael J. van Stipdonk ◽  
Jos Oomens ◽  
Wibe A. de Jong ◽  
Michael E. McIlwain

2004 ◽  
Vol 108 (42) ◽  
pp. 9008-9010 ◽  
Author(s):  
Travis D. Fridgen ◽  
Terry B. McMahon ◽  
Luke MacAleese ◽  
Joel Lemaire ◽  
Philippe Maitre

1984 ◽  
Vol 39 (3) ◽  
pp. 314-316 ◽  
Author(s):  
Helge Willner

The new compound SFCl was obtained by UV photolysis of FC(O)SCl in rare gas matrix and by UV photolysis of Cl2/SF3SF in the gas phase. Isotopic substitution verifies the molecular identity. Eight frequencies from three isotropic molecules determine the force constants fSF = 4.30 and fscl = 2.90 102N/m.


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