Indirect nuclear spin–spin coupling in InP studied by CP/MAS NMR

2004 ◽  
Vol 346-347 ◽  
pp. 476-478
Author(s):  
Takahiro Iijima ◽  
Kenjiro Hashi ◽  
Atsushi Goto ◽  
Tadashi Shimizu ◽  
Shinobu Ohki
1997 ◽  
Vol 91 (5) ◽  
pp. 897-907 ◽  
Author(s):  
SHEELA KIRPEKAR ◽  
THOMAS ENEVOLDSEN ◽  
JENS ODDERSHEDE ◽  
WILLIAM RAYNES

1965 ◽  
Vol 139 (6A) ◽  
pp. A1880-A1882
Author(s):  
D. Beeman ◽  
P. Pincus ◽  
F. Hartmann-Boutron

1994 ◽  
Vol 98 (36) ◽  
pp. 8858-8861 ◽  
Author(s):  
C. Vizioli ◽  
M. C. Ruiz de Azua ◽  
C. G. Giribet ◽  
R. H. Contreras ◽  
L. Turi ◽  
...  

1992 ◽  
Vol 57 (1) ◽  
pp. 366-370 ◽  
Author(s):  
Frank B. Mallory ◽  
Eddie D. Luzik ◽  
Clelia W. Mallory ◽  
Patrick J. Carroll

2009 ◽  
Vol 87 (7) ◽  
pp. 1090-1101 ◽  
Author(s):  
Fu Chen ◽  
Se-Woung Oh ◽  
Roderick E. Wasylishen

High-resolution solid-state 31P NMR spectroscopy was used to investigate a series of 1:1 silver–triphenylphosphine complexes, [Ph3PAgX]n, where X is a monovalent anion and n = 1, 2, 3, 4, or ∞. The 31P CP MAS NMR spectra reveal the number of distinct phosphorus sites in these complexes as well as the |1J(109Ag,31P)| values, which range from 401 ± 10 Hz (X = N3–) to 869 ± 10 Hz (X = SO3CF3–). The data obtained here and in earlier investigations indicate that |1J(109Ag,31P)| values for silver–tertiary phosphine complexes decrease as Ag–P bond lengths increase. This experimental conclusion is supported by DFT calculations, which also indicate that the Fermi-contact mechanism is the only important spin–spin coupling mechanism for 1J(109Ag,31P) in these complexes. In addition, the crystal structure of a silver–triphenylphosphine trifluoroacetate tetramer was determined using X-ray crystallography, and the structure of a silver–triphenylphosphine chloride tetramer was reinvestigated.


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