Nuclear magnetic shielding tensors for the carbon, nitrogen, and selenium nuclei of selenocyanates - a combined experimental and theoretical approach

2000 ◽  
Vol 78 (5) ◽  
pp. 614-625 ◽  
Author(s):  
Guy M Bernard ◽  
Klaus Eichele ◽  
Gang Wu ◽  
Christopher W Kirby ◽  
Roderick E Wasylishen

The principal components of the carbon, nitrogen, and selenium chemical shift (CS) tensors for several solid selenocyanate salts have been determined by NMR measurements on stationary or slow magic-angle-spinning powder samples. Within experimental error, all three CS tensors are axially symmetric, consistent with the expected linear geometry of these anions. The spans (Ω) of the carbon and selenium CS tensors for the selenocyanate anion (SeCN-) are approximately 300 and 800 ppm, respectively, much less than the corresponding values for carbon diselenide (CSe2). This difference is a consequence of the difference in the CS tensor components perpendicular to the C infiniti symmetry axes in these systems. Ab initio calculations show that the orbital symmetries of these compounds are a significant factor in the shielding. For CSe2, efficient mixing of the σ and π orbitals results in a large paramagnetic contribution to the total shielding of the chemical shielding tensor components perpendicular to the molecular axis. Such mixing is less efficient for the SeCN-, resulting in a smaller paramagnetic contribution and hence in greater shielding in directions perpendicular to the molecular axis.Key words: selenocyanates, solid-state NMR, carbon shielding tensors, nitrogen shielding tensors, selenium shielding tensors, ab initio calculations.

1992 ◽  
Vol 70 (4) ◽  
pp. 1229-1235 ◽  
Author(s):  
Gang Wu ◽  
Roderick E. Wasylishen ◽  
William P. Power ◽  
Graziano Baccolini

Phosphorus-31 NMR static powder spectra and high-resolution magic angle spinning spectra have been obtained for a new heterocyclic compound, cis-2,10-dimethyl[1,2,3]benzothiadiphospholo[2,3b][1,2,3]benzothiadiphosphole (1), which contains a P(III)—P(III) single bond. The homonuclear 31P–31P dipolar interaction manifests itself in both the magic angle spinning spectra and the non-spinning line shape. Under the AX spin pair approximation, analysis of the spinning sidebands in the MAS experiment yields a full characterization of the two 31P chemical shielding tensors. This approximation is confirmed by the exact powder line shape simulation for a homonuclear spin pair. Analysis of the dipolar subspectra also yields the absolute sign of 1J(P,P), which is found to be negative. Keywords: phosphorus–phosphorus single bond, chemical shielding tensors, dipolar NMR, MAS, static line shape.


1999 ◽  
Vol 77 (11) ◽  
pp. 1962-1972
Author(s):  
Scott Kroeker ◽  
Roderick E Wasylishen

Direct NMR observation of copper-63/65 nuclei in solid K3Cu(CN)4 provides the first experimental example of anisotropic copper chemical shielding. Axially symmetric by virtue of the space group symmetry, the shielding tensor spans 42 ppm, with the greatest shielding when the unique axis is perpendicular to the applied magnetic field. The nuclear quadrupole coupling constant is also appreciable, CQ(63Cu) = -1.125 MHz, reflecting a deviation of the Cu(CN)43- anion from pure tetrahedral symmetry. Spin-spin coupling to 13C nuclei in an isotopically enriched sample is quantified by line-shape simulations of both 13C and 63/65Cu magic-angle spinning (MAS) NMR spectra to be 300 Hz. It is shown that this information is also directly available by 63/65Cu triple-quantum (3Q) MAS NMR. The relative merits of these three approaches to characterizing spin-spin couplings involving half-integer quadrupolar nuclei are discussed. Chemical shielding tensors for nitrogen-15 and carbon-13 are obtained from NMR spectra of non-spinning samples, and are compared to those of tetrahedral group 12 tetracyanometallates. Finally, 2J(63/65Cu,15N) detected in 15N MAS experiments are found to be 19 and 20 Hz for the two crystallographically distinct cyanide ligands.Key words: NMR, quadrupolar nucleus, chemical shielding tensor, multiple-quantum magic-angle spinning, metal cyanide, spin-spin coupling.


RSC Advances ◽  
2014 ◽  
Vol 4 (99) ◽  
pp. 56248-56258 ◽  
Author(s):  
Diego Carnevale ◽  
Sharon E. Ashbrook ◽  
Geoffrey Bodenhausen

The magnetic shielding tensors of protons of water in barium chlorate monohydrate are investigated by means of solid-state NMR spectroscopy, both for static powders and under magic-angle spinning conditions.


2013 ◽  
Vol 2013 ◽  
pp. 1-10 ◽  
Author(s):  
Wei Li ◽  
Linxi Hou ◽  
Zhongren Chen

Novel exfoliated and interacted polyethylene (PE)/montmorillonite (MMT) nanocomposites prepared byin situpolymerization were characterized by solid-state nuclear magnetic resonance (NMR). The phase structure and molecular mobility were investigated by proton and carbon NMR under static and magic-angle spinning (MAS) conditions. The results showed that incorporation of MMT layer enhanced the polyethylene crystallinity behavior. The chain mobility of crystalline phase, interphase and amorphous phase was hindered in the nanocomposites. The phase structure and chain dynamics were also investigated upon changing the temperature. The orthorhombic and monoclinic phases were detected according to the13CP/MAS NMR. Quantitative characterization of the phase structure was also conducted by13C DP/MAS upon changing the temperature. Finally, the difference in the phase structure and chain dynamics in each phase of PE/nanocomposites was compared based on the NMR results when fiber filler was introduced.


The high-resolution solid-state 13 C NMR (nuclear magnetic resonance) spectra are reported of the iron carbonyl complexes Fe 3 (CO) 8 (PhCCPh) 2 (I) and Fe 3 (CO) 12 (II), 13 C-enriched at the carbonyl carbons. The spectra were recorded with slow magic-angle spinning, and the intensities of the spinning side bands analysed by a computerized adaptation of the method of Herzfeld & Berger to give values for the principal components of the carbonyl carbon shielding tensors. Complex (I) includes two asymmetric double-bridging carbonyl groups, and the 13 C shielding-tensor components assigned to the C—O bond axis (σ 33 ) are intermediate between the values obtained for symmetric double-bridging carbonyl groups and linear M—C≡0 terminal carbonyls. It is proposed that the σ 33 shielding component may therefore be used to monitor the degree of asymmetric bridging of a carbonyl group. All 13 C resonances of complex (II) exhibit a degree of asymmetry in the shielding tensor and possible reasons for this are discussed. Three methods of estimating errors in the derived shielding-tensor components are considered. One method use calculated variances based upon differences between the experimental and calculated side-band intensities; this gives unreasonably large errors in the cases of axial symmetry in the shielding tensor. A second method explores different shielding components for values of ɸ 2 (the sum of the squares of the differences between the experimental and calculated side-band intensity ratios) which exceed the best minimum by an arbitrary percentage. The third method considers errors due to the signal: noise ratios in the experimental spectra. The relative merits of these three approaches of error estimation are examined.


2020 ◽  
Vol 11 (14) ◽  
pp. 5655-5660 ◽  
Author(s):  
Frédéric A. Perras ◽  
Muralikrishna Raju ◽  
Scott L. Carnahan ◽  
Dooman Akbarian ◽  
Adri C. T. van Duin ◽  
...  

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