NMR measurements and density functional calculations of the 199Hg-13C spin-spin coupling tensor in methylmercury halides

The isotropic average, JisoHgC, and the anisotropy, DeltaJHgC, of the 199Hg-13C spin-spin coupling tensor in methylmercury halides, CH3HgX (X=Cl, Br, I), were determined for the first time by utilizing the NMR spectra of these molecules dissolved in liquid crystals. Furthermore, density functional calculations were performed using the zeroth-order regular approximation, including also dimethylmercury. The temperature-dependence of the JisoHgC couplings in the isotropic phase was studied in each case in order to extrapolate their values into the liquid crystal state. Good agreement is found between the experimental and the calculated DeltaJHgC values as long as solvent effects are considered in the computations. Most of the magnitude of DeltaJ can be attributed to the spin mechanism of J-coupling, with additional sizable spin-orbital cross terms due to electronic spin-orbit coupling.     

Modeling of heavy-atom-ligand NMR spin-spin coupling in solution: molecular dynamics study and natural bond orbital analysis of Hg-C coupling constants

Ab initio molecular dynamics (MD) and relativistic density functional NMR methods were applied to calculate the one‐bond Hg? C NMR indirect nuclear spin–spin coupling constants (J) of [Hg(CN)₂] and [CH₃HgCl] in solution. The MD averages were obtained as J(¹⁹⁹Hg? ¹³C)=3200 and 1575 Hz, respectively. The experimental Hg? C spin–spin coupling constants of [Hg(CN)₂] in methanol and [CH₃HgCl] in DMSO are 3143 and 1674 Hz, respectively. To deal with solvent effects in the calculations, finite “droplet” models of the two systems were set up. Solvent effects in both systems lead to a strong increase of the Hg? C coupling constant. From a relativistic natural localized molecular orbital (NLMO) analysis, it was found that the degree of delocalization of the Hg 5d_σ nonbonding orbital and of the Hg? C bonding orbital between the two coupled atoms, the nature of the trans Hg? C/Cl bonding orbital, and the s character of these orbitals, exhibit trends upon solvation of the complexes that, when combined, lead to the strong increase of J(Hg? C).     

Ab initio study of the NMR shielding constants and spin-spin coupling constants in cyclopropene

Summary Ab initio calculations of parameters which characterize the NMR spectrum are presented for the cyclopropene molecule. The London orbitals CHF (or GIAO-CHF, Gauge-Independent Atomic Orbital Coupled Hartree-Fock) results for the shielding constants are in good agreement with the experimental data, accurately determined, and with otherab initio values. The calculations of the NMR spin-spin coupling constants have been performed using the Multiconfiguration Time-Dependent Hartree-Fock (MC TDHF) approach. Different basis sets and MC SCF wavefunctions were used to estimate the accuracy of the results. Good agreement is obtained with the coupling constants estimated using the available experimental data.Dedicated to Professor Werner Kutzelnigg on the occasion of his 60th birthday     

A theoretical study of the large Hg-Hg spin-spin coupling constants in Hg(2)(2+), Hg(3)(2+), and Hg(2)(2+)-crown ether complexes

Nuclear spin-spin coupling constants (1)J(Hg-Hg) in the systems Hg(2)(2+) and Hg(3)(2+) represent the largest coupling constants so far observed in NMR experiments. We have performed a computational study on these ions, on Hg(2)(2+) complexes with 18-crown-6 and 15-crown-5, and on Hg(3)(2+) with solvent molecules and counterions. The results obtained with our recently developed program for the density functional computation of heavy nucleus spin-spin coupling constants are in good agreement with experiments. The data reveal that the bare ions Hg(2)(2+) and Hg(3)(2+) would afford much larger coupling constants than those experimentally observed, with an upper limit of approximately 0.9 MHz for Hg(2)(2+). This limit is much larger than that previously estimated by Hückel theory. It is demonstrated that in solution or due to complexation the experimentally determined values are much smaller than the free ion's coupling constants. With the help of intuitive MO arguments, it is illustrated how the environment strongly reduces the coupling constants in Hg(2)(2+) and Hg(3)(2+). The two-bond coupling constant (2)J(Hg-Hg) in Hg(3)(2+) is also examined.     

NMR study of conjugation effects 15.13C-13C spin-spin coupling constants in phenyl alkyl ether

Conclusions ¹³C-¹³C SSCC were measured for a series of phenyl alkyl ethers. The values through the bond between C² and C³ in mono substituted benzenes most clearly reflect the -electron interaction of the aromatic ring with the substituent, provided the latter contains no atoms from a period of the periodic table higher than the second.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya.No. 1, pp. 113–119, January, 1982.The authors thank N. M. Sergeev for useful discussions while the work was in progress, and V. N. Khlopkov for technical assistance in setting up the experiments.     

Crystal-chemical functions of [Hg2]2+ and [Hg3]4+ groups in inorganic structures

About 20 structures of natural and synthetic inorganic compounds containing a [H_g2] (dumbbell) pair (Hg-Hg = 2.47?2.56 å) or a [H_g3] triangle (Hg-Hg_av = 2.7 å) are analyzed. From crystal-chemical viewpoint, it is reasonable to consider these groups as a single cation with coordinates of its geometrical center. In all cases, the coordination polvhedra are convex polxhedra with 8–14 vertices and with distances from the center to the vertex of 3.00?3.91 å, which makes the [H_g2]²⁺ and [Hg3]⁴⁺ cations analogs of Cs. Examples are given to demonstrate the advantages of the suggested analysis of structures with a [Hg_n] group. This approach extends classical crystal chemistry to compounds with nonuniform chemical bonds, in particular, to compounds with pseudocluster and cluster groups inserted in the ionic structure; therefore, it is especially useful for comparison and classification purposes and for analysis of structure-foming factors.     

Probing the flexibility of internal rotation in silylated phenols with the NMR scalar spin-spin coupling constants

The rotation of a trimethylsiloxy (TMSO) group in three silylated phenols (with three different ortho substituents -H, -CH3, and -C(CH3)3) was studied with the NMR (n)J(Si,C), n = 2, 3, 4, 5, scalar spin-spin coupling between the (29)Si nucleus of the TMSO group and the (13)C nuclei of the phenyl ring. The internal rotation potential calculated with the B3LYP and MP2 calculation methods including the effect of a solvent environment (gas phase, chloroform, and water) was used for the calculation of the dynamical averages of the scalar coupling constants in the framework of the rigid-bender formalism. Solvent effects, the quality of the rotational potential, and the applicability of the classical molecular dynamic to the problem is discussed. Quantum effects have a sizable impact on scalar couplings, particularly for the internal rotational states well localized within the wells of the potential surfaces for the TMSO group. The overall difference between the experimental and theoretical scalar couplings calculated for the global energy-minima structures (static model) decreases substantially for both model potentials (B3LYP, MP2) when the molecular motion of the TMSO group is taken into account. The calculated data indicate that the inclusion of molecular motion is necessary for the accurate calculation of the scalar coupling constants and their reliable structural interpretation for any system which possesses a large-amplitude motion.     

A computational study of 2J(HH)(gem) indirect spin-spin coupling constants in simple hydrides of the second and third periods

Several theoretical methods have been used to compute (2)J(HH) in neutral, anionic and cationic HXH hydrides, X being the 14 nuclei from Li to Cl (28 molecules). Since the calculations also provide (1)J(XH) spin-spin coupling constants (SSCC), these have also been analyzed. The best results were obtained using Second-order polarization propagator approximation (SOPPA)/sadJ. The geminal coupling constants appear to be dependent on the electronegativity of the X-atom.     

Synthesis, 31P and 199Hg NMR spectroscopy of the cationic heterodimetallacycle [HgAg{μ-[bis(diphenylphosphino)methane]}2]3+

The complex [Hg(η¹-dppm)₂](O₃SCF₃)₂ [dppm = bis(diphenylphosphino)methane] reacts with AgO₃SCF₃ to give the new eight-mem     

An ab initio study of the nuclear spin-spin coupling constants in the second-row hydrides

Ab initio SCF perturbation theory calculations have been performed for the contact, orbital and dipolar contributions to the nuclear spin—spin coupling constants in A1H₃, SiH₄ PH₃, H₂S and HCl, using large, stable gaussian basis sets. The results for J(XH) are in reasonably good agreement with experiment, those for. J(HH) are rather less good.     

Stereospecificity of the 3JCH spin-spin coupling constants in bicyclic cis-diaziridines. Stereochemistry of 2,4,6-trialkyl-1,3,5-triazabicyclo[3.1.0]-hexanes

Stereospecificity of the ³J_C,N,C,H spin-spin coupling constants (³J^trans > J^gauche) in the ¹³C NMR spectra of 1,5-diaza- and 1,3,5-triazabicyclo[3.1.0]hexanes was observed. Proceeding from this, the preferred conformations of the d, Z and meso isomers of 2,4,6-trialkyl-1,3,5-triazabicyclo[3.1.0]hexanes were established, and a mechanism for the interconversion of these isomers via openings of the five-membered ring and an imino-enamine equilibrium was proposed. It is also shown that the stereochemical result of the Schmitz reaction is determined in the step involving cyclization of the iminium intermediate.Communication 42 from the series Asymmetric unbridged nitrogen. See [1] for communication 41.Translated from Khimiya Geterotsiklicheskikh Soedinenii, No. 10, pp. 1348–1354, October, 1985.The authors thank N. L. Zaichenko for his assistance in measuring the NMR spectra.     

The solvation of the mercury(II) ion-a 199Hg NMR study

The solvation of the mercury(II) ion in solvents with different solvation properties, water, dimethylsulfoxide, N,N-dimethylthioformamide, and liquid ammonia, has been studied by means of (199)Hg NMR. The (199)Hg chemical shift shows a pronounced dependence on the coordination number of the mercury(II) ion in the solvates resulting in a difference of over 1200 ppm between basically tetrahedral and octahedral complexes. The chemical shifts can furthermore be associated with electron-pair donor properties of the solvents. The spin-lattice relaxation times of the (199)Hg nucleus in the solvates have been measured at different applied magnetic fields, concentrations, temperatures, and isotope substitutions. Possible mechanisms for the (199)Hg relaxation were proposed and the chemical shielding anisotropy in the solvates has been estimated. The (199)Hg relaxation rates and the anisotropy are correlated with the structure of the solvate complexes in solution obtained from recent LAXS and EXAFS studies.     

2 + 4] and [4 + 2] cycloadditions of o-thioquinones with 1,3-dienes: a computational study

Cycloadditions of o-thioquinones (o-TQs) with 1,3-dienes could proceed via either a [2 + 4] or a [4 + 2] mechanism. Under kinetic control and with acyclic dienes the reaction affords the spiro cycloadducts 5deriving from the [2 + 4] path as the main products. Under thermodynamic control, or with cyclic dienes, the o-TQs behave as heterodienes to give the benzoxathiin derivatives 4, in most cases with complete regioselectivity. In the present computational study, DFT calculations were performed in order to achieve a deep understanding of both [2 + 4] and [4 + 2] paths. The reactions of three o-TQs with six 1,3-dienes were thoroughly investigated at the B3LYP/TZVP//B3LYP6-31G level, and the two reaction mechanisms were then compared, evidencing that [2 + 4] cycloadditions are kinetically favored, strongly asynchronous, or even unconcerted, while [4 + 2] reactions are thermodynamically favored, quite asynchronous, but undoubtedly concerted. Moreover, the observed regioselectivity was rationalized by mean of the FMO theory and by comparison of the activation energies for different pathways.     

Crystal Structure Formation in Compounds with [Hg2]2+ Dimers

This paper describes the arrangement of cations in the structures of inorganic compounds HgVO₃, HgReO₄, Hg₂MoO₄ ( and , Hg₂Mo₂O₇, Hg₂Mo₅O₁₆, Hg₅Re₂O₁₀ (two modifications), Hg₂ReO₅, and Hg₂VO₄. To isolate crystal-forming planes and cation sublattices, it is preferable to consider the [Hg₂]²⁺ dumbbell pair as a single cation. Two types of mutual orientation of close-packed cation planes intersecting at an angle of 60° or 90° (45°) have been found. Details of three-dimensional ordering of cations and possible methods of structure modification in polymorphous transformations are discussed.