scholarly journals Control of Vibrational State of a Robot Interacting with a Rough Free-formed Surface

2017 ◽  
Vol 252 (4) ◽  
pp. 43-52 ◽  
Author(s):  
S.F. Burdakov ◽  
T.A. Baydina ◽  
O.B. Shagniev
Keyword(s):  
Vibrational State

Determination of O2 and N2 vibrational state distributions in CO laser-sustained plasmas

1999 ◽  
Author(s):  
Wonchul Lee ◽  
Matthew Chidley ◽  
Robert Leiweke ◽  
Walter Lempert ◽  
Igor Adamovich
Keyword(s):  
Vibrational State ◽  
Co Laser

Radiofrequency, Microwave, Submillimeter-Wave, and High-Resolution Infrared Spectra of thev6= 1 Vibrational State of CDF3

1997 ◽  
Vol 182 (1) ◽  
pp. 34-49 ◽  
Author(s):  
H. Bürger ◽  
J. Cosléou ◽  
J. Demaison ◽  
C. Gerke ◽  
H. Harder ◽  
...  
Keyword(s):  
High Resolution ◽  
Infrared Spectra ◽  
Vibrational State ◽  
Submillimeter Wave

Magnetic susceptibility of the BH molecule as a function of its vibrational state

1983 ◽  
Vol 19 (2) ◽  
pp. 115-119
Author(s):  
P. A. Braun ◽  
T. K. Rebane ◽  
O. I. Semakova
Keyword(s):  
Magnetic Susceptibility ◽  
Vibrational State

Nuclear Quadrupole Hyperfine Structure of the Direct /-Type Transitions of the Fulminic Acid Isotopomers H12C14N16O and H13C14N16O

1996 ◽  
Vol 51 (3) ◽  
pp. 207-214
Author(s):  
Jürgen Preusser ◽  
Manfred Winnewisser
Keyword(s):  
Hyperfine Structure ◽  
Vibrational State ◽  
Line Broadening ◽  
Frequency Range ◽  
Vibrational States ◽  
Contour Fitting ◽  
Splitting Parameter ◽  
Nuclear Quadrupole ◽  
Significant Line ◽  
Large Amplitude Motion

The direct I- type transitions of H133C14N16O in the vibrational states (υ4,υ5) = (01) and (03) were measured in the frequency range from 18 to 40 GHz. These transitions show a nuclear quadrupole hyperfine structure caused by the 14N nucleus, which could partially be resolved at Doppler-limited resolution. The analogous transitions of the parent species. H12C14N16O, were remeasured. They displayed a very similar hyperfine structure, also partially resolved. The hyperfine patterns of both H12C14N16O and H13C14N16O were analysed by means of contour fitting s to the absorption profiles. The parameter ηseQq, which is responsible for the splittings, is determined to be 645(20) kHz for the vibrational state (01) and 890(44) kHz for the vibrational state (03) for H12C14N16O and 642(32) kHz for (01) and 898(22) kHz for (03) for H13C14N16O. This unexpectedly large splitting parameter for states involving the large amplitude motion υ5 (HCN bending) is discussed as another consequence of the quasilinearity of fulminic acid, in view of the fact that the analogous transitions for the vibrational state (10) (NCO bending) do not split or even show a significant line broadening at the resolution used for the present measurements

scholarly journals Vibrational-state-dependent decay of the CO C(1s) excitation

1995 ◽  
Vol 51 (6) ◽  
pp. R4313-R4316 ◽  
Author(s):  
N. Saito ◽  
F. Heiser ◽  
O. Hemmers ◽  
A. Hempelmann ◽  
K. Wieliczek ◽  
...  
Keyword(s):  
Vibrational State ◽  
State Dependent
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