Negative linear deuterium isotope shift for13C in iodoform

1988 ◽  
Vol 28 (6) ◽  
pp. 934-934 ◽  
Author(s):  
N. M. Sergeev ◽  
N. D. Sergeeva ◽  
L. F. Kobets





1972 ◽  
Vol 50 (6) ◽  
pp. 531-543 ◽  
Author(s):  
J. Billingsley

A new absorption spectrum in the region 4600–5600 Å has been discovered in the flash photolysis of silyl iodide, SiH3I. A rotational analysis, together with the observation of a deuterium isotope shift, has shown that the spectrum is due to the HSiI radical.The lower electronic state of HSiI is a 1A′ state with a bond angle of ~103°, and the upper state is 1A″ with angle ~116°. Axis-switching effects, due to the increase in bond angle, cause the appearance of ΔK = 0, ± 2 subbands, in addition to the ordinary ΔK = ± 1 subbands.



1994 ◽  
Vol 49 (4) ◽  
pp. 2255-2259 ◽  
Author(s):  
K. Pachucki ◽  
M. Weitz ◽  
T. W. Hänsch


1974 ◽  
Vol 52 (18) ◽  
pp. 3247-3250 ◽  
Author(s):  
Roderick E. Wasylishen ◽  
Ted Schaefer

The carbon-13 magnetic resonance spectra of propane and of propane-2,2-d2 are analyzed to give 1j(13C1,H) = 124.35, 1J(13C2,H) = 125.35, 2J(13C1,H) = −4.25, 2J(13C2,H) = −4.39, 3J(13C,H) = 5.80, 3J(H,H) = 7.375, 4j(H,H) < ± 0.18 Hz. The deuterium isotope shift at C2 is 0.72 ± 0.10 p.p.m. to high field.



2001 ◽  
Vol 16 (08) ◽  
pp. 507-511 ◽  
Author(s):  
R. N. FAUSTOV ◽  
A. P. MARTYNENKO

The correction to the hydrogen–deuterium isotope shift due to the proton and deuteron polarizability is evaluated on the basis of modern experimental data on the structure functions of inelastic lepton–nucleus scattering. The numerical value of this contribution is equal to 63 ± 12 Hz.



2011 ◽  
Vol 83 (4) ◽  
Author(s):  
U.D. Jentschura ◽  
A. Matveev ◽  
C.G. Parthey ◽  
J. Alnis ◽  
R. Pohl ◽  
...  






1969 ◽  
Vol 30 (C1) ◽  
pp. C1-41-C1-47 ◽  
Author(s):  
M. ELBEL ◽  
H. HÜHNERMANN


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