Investigations into the nature of halogen- and hydrogen-bonding interactions of some heteroaromatic rings with dichlorine monoxide

We have studied the structures, properties, and nature of halogen- and hydrogen-bonding interactions between some heteroaromatic rings (C₅H₅N, C₄H₄O, and C₄H₄S) with Cl₂O at the MP2/aug-cc-pVTZ level. We also considered the solvent effect on the halogen bonds and hydrogen bonds in the C₅H₅N-Cl₂O complexes and found that the solvent has a weakening effect on the π-type halogen bond and hydrogen bond but a prominent enhancing effect on σ-type halogen bond. The complexes have also been analyzed with symmetry adapted perturbation theory method (SAPT).     

Interplay between halogen bonds and hydrogen bonds in OH/SH···HOX···HY (X = Cl, Br; Y = F, Cl, Br) complexes

The character of the cooperativity between the HOX···OH/SH halogen bond (XB) and the Y―H···(H)OX hydrogen bond (HB) in OH/SH···HOX···HY (X = Cl, Br; Y = F, Cl, Br) complexes has been investigated by means of second-order Møller?Plesset perturbation theory (MP2) calculations and “quantum theory of atoms in molecules” (QTAIM) studies. The geometries of the complexes have been determined from the most negative electrostatic potentials (V _S,min) and the most positive electrostatic potentials (V _S,max) on the electron density contours of the individual species. The greater the V _S,max values of HY, the larger the interaction energies of halogen-bonded HOX···OH/SH in the termolecular complexes, indicating that the ability of cooperative effect of hydrogen bond on halogen bond are determined by V _S,max of HY. The interaction energies, binding distances, infrared vibrational frequencies, and electron densities ρ at the BCPs of the hydrogen bonds and halogen bonds prove that there is positive cooperativity between these bonds. The potentiation of hydrogen bonds on halogen bonds is greater than that of halogen bonds on hydrogen bonds. QTAIM studies have shown that the halogen bonds and hydrogen bonds are closed-shell noncovalent interactions, and both have greater electrostatic character in the termolecular species compared with the bimolecular species.

Insights into the strength and nature of carbene···halogen bond interactions: a theoretical perspective

Halogen-bonding, a noncovalent interaction between a halogen atom X in one molecule and a negative site in another, plays critical roles in fields as diverse as molecular biology, drug design and material engineering. In this work, we have examined the strength and origin of halogen bonds between carbene CH₂ and XCCY molecules, where X?=?Cl, Br, I, and Y?=?H, F, COF, COOH, CF₃, NO₂, CN, NH₂, CH₃, OH. These calculations have been carried out using M06-2X, MP2 and CCSD(T) methods, through analyses of surface electrostatic potentials V _S(r) and intermolecular interaction energies. Not surprisingly, the strength of the halogen bonds in the CH₂···XCCY complexes depend on the polarizability of the halogen X and the electron-withdrawing power of the Y group. It is revealed that for a given carbene···X interaction, the electrostatic term is slightly larger (i.e., more negative) than the dispersion term. Comparing the data for the chlorine, bromine and iodine substituted CH₂···XCCY systems, it can be seen that both the polarization and dispersion components of the interaction energy increase with increasing halogen size. One can see that increasing the size and positive nature of a halogen’s σ-hole markedly enhances the electrostatic contribution of the halogen-bonding interaction.

Chalcogen- and halogen-bonds involving SX<Subscript>2</Subscript> (X = F,Cl, and Br) with formaldehyde

The capacity of SX₂ (X = F, Cl, and Br) to engage in different kinds of noncovalent bonds was investigated by ab initio calculations. SCl₂ (SBr₂) has two σ-holes upon extension of Cl (Br)?S bonds, and two σ-holes upon extension of S?Cl (Br) bonds. SF₂ contains only two σ-holes upon extension of the F?S bond. Consequently, SCl₂ and SBr₂ form chalcogen and halogen bonds with the electron donor H₂CO while SF₂ forms only a chalcogen bond, i.e., no F···O halogen bond was found in the SF₂:H₂CO complex. The S···O chalcogen bond between SF₂ and H₂CO is the strongest, while the strongest halogen bond is Br···O between SBr₂ and H₂CO. The nature of these two types of noncovalent interaction was probed by a variety of methods, including molecular electrostatic potentials, QTAIM, energy decomposition, and electron density shift maps. Termolecular complexes X₂S···H₂CO···SX′₂ (X = F, Cl, Br, and X′ = Cl, Br) were constructed to study the interplay between chalcogen bonds and halogen bonds. All these complexes contained S···O and Cl (Br)···O bonds, with longer intermolecular distances, smaller values of electron density, and more positive three-body interaction energies, indicating negative cooperativity between the chalcogen bond and the halogen bond. In addition, for all complexes studied, interactions involving chalcogen bonds were more favorable than those involving halogen bonds.

Open image in new window

Graphical Abstract Molecular electrostatic potential and contour map of the Laplacian of the electron density in Cl₂S···H₂CO···SCl₂ complex

     

Theoretical studies on the structures,intra- and inter-molecular hydrogen bonding interactions in HNF and HNF–H2O clusters in the gaseous,aqueous and solid phases

Hydrazimium nitroformate ([N₂H₅]⁺[C(NO₂)₃]^? , HNF) is an ionic oxidiser used in solid propellants. Its properties are easily affected by H₂O because of its hygroscopicity. In this article, density functional theory (DFT) and molecular dynamics (MD) were employed to study the isolated HNF molecule and the HNF–H₂O cluster in gas phase and in the aqueous solution. Three stable conformations were obtained for HNF in the gas phase and in the aqueous solution, respectively, and each conformation can form several different HNF–H₂O clusters. Irrespective of whether it is in gas phase or in solution, intramolecular hydrogen bond interactions and other interactions (e.g. the binding energy, the dispersion energy, the second-order perturbation energy and the energy gap between frontier orbitals) of HNF are weaker in the clusters than in the isolated state. The initial decomposition energy of the cluster is lower than that of the isolated HNF molecule in both gaseous and aqueous phases, while the dissociation processes are the same. Molecular dynamic simulations showed that the clustered H₂O elongates and weakens the C–NO₂ bond in the solid HNF–H₂O cluster compared with that in the solid HNF. H₂O reduces and weakens intramolecular N–HΛO bonds too, and O–HΛN is the dominant intermolecular hydrogen bond between HNF and H₂O.     

Interaction of glucosamine with uracil and thymine: a computational study

Noncovalent interactions are ubiquitous and have been well recognized in chemistry, biology and material science. Yet, there are still recurring controversies over their natures, due to the wide range of noncovalent interaction terms. In this Essay, we employed the Valence Bond (VB) methods to address two types of interactions which recently have drawn intensive attention, i.e., the halogen bonding and the CH???HC dihydrogen bonding. The VB methods have the advantage of interpreting molecular structures and properties in the term of electron-localized Lewis (resonance) states (structures), which thereby shed specific light on the alteration of the bonding patterns. Due to the electron localization nature of Lewis states, it is possible to define individually and measure both polarization and charge transfer effects which have different physical origins. We demonstrated that both the ab initio VB method and the block-localized wavefunction (BLW) method can provide consistent pictures for halogen bonding systems, where strong Lewis bases NH₃, H₂O and NMe₃ partake as the halogen bond acceptors, and the halogen bond donors include dihalogen molecules and XNO₂ (X?=?Cl, Br, I). Based on the structural, spectral, and energetic changes, we confirm the remarkable roles of charge transfer in these halogen bonding complexes. Although the weak C-H???H-C interactions in alkane dimers and graphane sheets are thought to involve dispersion only, we show that this term embeds delicate yet important charge transfer, bond reorganization and polarization interactions.

     

Syntheses and crystal structures of trimethyltin(IV) coordination polymers based on mixed ligands of 5-nitroisophthalate and 2,2′(4,4′)-bipy or phen

The trimethyltin(IV) polymer [(Me₃Sn)₂(nip) · EtOH]_n (1) of 5-nitroisophthalic acid (H₂nip) and its three derivatives with mixed organic N-donor ligands 2,2′-bipy [(Me₃Sn)₂(nip) · 2H₂O] · [(Me₃Sn)₂(nip) · H₂O] · 2(2,2′-bipy) (2) 4,4′-bipy {[(Me₃Sn)₂(nip)]₂(4,4′-bipy)}_n (3) or phen [(Me₃Sn)₂(nip) · H₂O] · (phen) (4) have been synthesized by the reaction of trimethyltin(IV) chloride and H₂nip when sodium ethoxide was added in the presence of 2,2′-bipy 4,4′-bipy or phen. All complexes 1–4 were characterized by elemental, IR, ¹H, ¹³C, and ¹¹⁹Sn NMR spectroscopy and X-ray crystallography analyses. Crystal, data collection and structure refinement parameters for complexes 1, 2, 3 and 4 are shown in Table 1, Table 2, respectively. The X-ray data showed the geometries of all the tin atoms in complexes 1–4 are trigonal bipyramidal. The X-ray analysis of 1 showed that the structure was a polymeric infinite chain with neighboring triorganotin centers being linked by dicarboxylate ligands and hydrogen bonds were found between adjacent chains. For 2, two different monomers were found, in one monomer, Me₃Sn were coordinated to both carboxyl groups of the ligand and water molecules were coordinated to the two Sn(IV) centers. In the other monomer, water molecules were coordinated to only one Sn center. Co-crystallized2,2′-bipy was found in 2 and a 2D supermolecular structure was formed via O–H⋯O and O–H⋯N (N atoms derived from 2,2′-bipy) hydrogen bonds. In 3 however, a 2D polymeric block was formed due to the inversion center of the 4,4′-bipy. For 4, due to the O–H⋯O and O–H⋯N (N atoms derived from phen) hydrogen bonds and intermolecular Sn⋯O bonds, a 2D polymeric structure was formed.     

Preparation and characterization of two supramolecular complexes with 5-amino-2,4,6-triiodoisophthalic acid under N-donor auxiliary ligand intervention

Assemblies of 5-amino-2,4,6-triiodoisophthalic acid (H₂ATIBDC) with Cd(II) and Zn(II) in the presence of N-donor auxiliary ligand, 1,4-bis(1,2,4-triazol-1-yl)butane (btb), at ambient conditions yield two new supramolecular complexes, [Cd(ATIBDC)(btb)(H₂O)₂]·3H₂O (1), and [Zn(ATIBDC)(btb)]·2H₂O (2). Generally, these two complexes display 1D ATIBDC²⁻-bridged coordination arrays. Distinct extended 3D network architectures are further constructed with the help of weak secondary interactions especially aromatic stacking, halogen bonding, and hydrogen bonding as supramolecular driving forces. It is worthy to mention that halogen bonds (C-I?π and C-I?N/O) play important roles in the supramolecular assembly. The pentameric cluster (H₂O)₅ in 1 assembles into highly ordered helical infinite chains. Complex 2 exhibits the fascinating single-walled tube-like chain structure. It loses crystallinity rapidly in the air and leads to the formation of [Zn(ATIBDC)(btb)]·H₂O (2A). Thermal stabilities and solid state fluorescent properties of complexes 1 and 2A have been studied.     

Relativistic theoretical studies on hydrogen bonds and the electronic structure of aqueous solvated bis(uranyl) complex: an insight into explicit and/or implicit solvent effects

To understand the chemical behavior of uranyl complexes in water, a bis-uranyl [(phen)(UO₂)(μ₂–F)(F)]₂ (A; phen?=?phenanthroline, μ₂?=?doubly bridged) and its hydrated form A?·?(H₂O)_n (n?=?2, 4 and 6) were examined using scalar relativistic density functional theory. The addition of water caused the phen ligands to deviate slightly from the U₂(μ₂–F)₂ plane, and red-shifts the U–F-terminal and U?=?O stretching vibrations. Four types of hydrogen bonds are present in the optimized hydrated A?·?(H₂O)_n complexes; their energies were calculated to fall within the range 4.37–6.77 kcal mol^-1, comparable to the typical values of 5.0 kcal mol^-1 reported for hydrogen bonds. An aqueous environment simulated by explicit and/or implicit models lowers and re-arranges the orbitals of the bis-uranyl complex.

E. COLI RNASE HI AND THE PHOSPHONATE-DNA/RNA HYBRID: MOLECULAR DYNAMICS SIMULATIONS

A model for the complex between E. coli RNase HI and the DNA/RNA hybrid (previously refined by molecular dynamics simulations) was used to determine the impact of the internucleotide linkage modifications (either 3′–O–CH₂–P–O–5′ or 3′–O–P–CH₂–O–5′) on the ability of the modified-DNA/RNA hybrid to create a complex with the protein. Modified internucleotide linkages were incorporated systematically at different positions close to the 3′-end of the DNA strand to interfere with the DNA binding site of RNase H. Altogether, six trajectories were produced (length 1.5). Mutual hydrogen bonds connecting both strands of the nucleic acids hybrid, DNA with RNase H, RNA with RNase H, and the scissile bond with the Mg⁺⁺ · 4H₂O chelate complex (bound in the active site) were analyzed in detail. Many residues were involved in binding of the DNA (Arg88, Asn84, Trp85, Trp104, Tyr73, Lys99, Asn100, Thr43, and Asn16) and RNA (Gln76, Gln72, Tyr73, Lys122, Glu48, Asn44, and Cys13) strand to the substrate-binding site of the RNase H enzyme. The most remarkable disturbance of the hydrogen bonding net was observed for structures with modified internucleotide linkages positioned in a way to interact with the Trp104, Tyr73, Lys99, and Asn100 residues (situated in the middle of the DNA binding site, where a cluster of Trp residues forms a rigid core of the protein structure).     

Proton polarizability of poly(L-tyrosine)–hydrogen phosphate hydrogen bonds as a function of alkali cations

We studied films of poly(L -tyrosine) with hydrogen phosphate (residue/phosphate, 1:1) by ir spectroscopy. The influences of the alkali cations (Li⁺, Na⁺, K⁺) and of the degree of hydration were clarified. If Li⁺ ions are present, the OH ?^?OP hydrogen bonds formed in the dried films between the tyrosine OH groups and hydrogen phosphate are asymmetrical. The formation of hydrogen phosphate–hydrogen phosphate hydrogen bonds is prevented by the presence of the Li⁺ ions. With an increase in the degree of hydration, the tyrosine–phosphate bonds are not broken but become slightly stronger. Completely different behaviour is found if K⁺ ions are present. In dry films, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed between tyrosine and hydrogen phosphate show large proton polarizability. The tyrosine proton has a noticeable residence time at the acceptor O atom of the phosphate. The difference in the behaviour of the system with K⁺ ions when compared to the system with Li⁺ ions can be explained, since the hydrogen acceptor O atom of phosphate ions is more negatively charged due to the weaker influence of the K⁺ ions. Furthermore, POH ?^?OP hydrogen bonds between hydrogen phosphate molecules are formed. With an increase in the degree of hydration, the tyrosine–hydrogen phosphate hydrogen bonds are broken, all tyrosine protons are found at the tyrosine residues, and the -PO₃^? groupings are in a symmetrical environment, indicating that the K⁺ ions are removed from these groupings. If the degree of hydration increases further, hydrogen-bonded systems such as hydrogen phosphate–water–hydrogen phosphate are formed that show large proton polarizability due to collective proton motion. When Na⁺ ions are present, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed in dry films still show proton polarizability, but the residence time of the tyrosine proton at the phosphate is very short.     

Proton polarizability and proton transfer in histidine-phosphate hydrogen bonds as a function of cations present: ir investigations

(L -His)_n- dihydrogen phosphate systems are studied by ir spectroscopy in the presence of various cations and as a function of the degree of hydration. Ir continua indicate that (I) OH … N ? O^?…H⁺N (IIR) hydrogen bonds are formed and that these bonds show high proton polarizability, which increases from the Li⁺ to the K⁺ system. In the K⁺?system, His-P_i-P_i chains are formed, showing particularly high proton polarizability due to collective proton motion within both hydrogen bonds. The OH N ? O^?…H^?N equilibria are determined from ir bands. With the Li⁺ system, 55% of the protons are present at the histidine residues; this percentage is smaller with the Na⁺ system (41%), and amounts to only 32% with the K⁺ system. With the increasing degree of hydration the removal of the degeneracy of ν_as?PO^2?₃ vanishes, indicating loosening of the cations from the phosphates. Nevertheless, the hydrogen bond acceptor O atom becomes more negative; a shift of the equilibrium to the right is observed in the OH… N ? O^?…H⁺N bond. This is explained by the strong interaction of the dipole of the hydrogen bonds with the water molecules. All these results show that protons can be shifted easily in these hydrogen bonds due to their high proton polarizability. The transfer equilibria can be controlled easily by local electrical fields. In addition, these results may be of significance when phosphates interact with proteins.     

Role of Li+ ions on the surface morphology and thermoluminescence properties of Y2O3:Tm3+ nanophosphor

Y₂O₃:Tm³⁺ and Li⁺ co‐doped Y₂O₃:Tm³⁺ nanopowders were synthesized using the solution combustion method for possible application in ultraviolet (UV) light dosimetry. X‐ray diffraction revealed the crystallite sizes to be in the range 21–44 nm and 30–121 nm using the Scherrer equation and the W‐H plot relationship, respectively. Field emission scanning electron microscopy confirmed that, after co‐doping with 4 mol% concentration of Li⁺, the particles were spherical in nature with an average size of ~30 nm. Fourier transformed infrared spectroscopy results showed bands at wavenumbers of 556, 1499, 1704, 2342, 2358, 2973, 3433, and 3610 cm^?1 that corresponded to the stretching and bending vibrations of Y–O, C=O and O–H. Thermoluminescence (TL) glow peaks for Y₂O₃:Tm³⁺ nanophosphors observed at 399 and 590 K were attributed to oxygen defects caused using UV irradiation. These oxygen defects firstly resulted in an increased prominent peak TL intensity for up to 270 min of irradiation and then a decrease. This was attributed to the presence of oxygen defect clusters that caused a reduction in recombination centres. The Li⁺ co‐doped sample showed peaks at 356, 430, and 583 K and its intensity sublinearly increased up to 90 min and then thereafter decreased. The TL trapping parameters were calculated using computerized glow curve deconvolution methods. The Li⁺ co‐doped sample exhibited less fading and high trap density under the UV radiation.     

Discovery of σ-hole interactions involving ylides

The positive electrostatic potentials (σ-hole) have been found in ylides CH₂XH₃ (X = P, As, Sb) and CH₂YH₂ (Y = S, Se, Te), on the outer surfaces of group VA and VIA atoms, approximately along the extensions of the C–X and C–Y bonds, respectively. These electrostatic potentials suggest that the above ylides can interact with nucleophiles to form weak, directional noncovalent interactions similar to halogen bonding interactions. MP2 calculations have confirmed the formation of CH₂XH₃···HM complexes (X = P, As, Sb; M = BeH, ZnH, MgH, Li, Na). The interaction energies, interaction distances, topological properties (electron density and its Laplacian), and energy properties (kinetic electron energy density and potential electron energy density) at the X(1)···H(10) bond critical points are all correlated with the most negative electrostatic potential value of HM, indicating that electrostatic interactions play an important role in these weak X···H interactions. Similar to the halogen bonding interactions, weak interactions involving ylides may be significant in several areas such as organic synthesis, crystal engineering, and design of new materials.     

The unrestricted local properties: application in nanoelectronics and for predicting radicals reactivity

I have performed quantum chemical calculations for the CF₃X (X = Cl, Br) ???Au_n (n?=?2, 3, and 4) complexes at M05-2X/aug-cc-pVDZ(PP) level. Two types of optimized structures were obtained. Type I complexes are stabilized by the coordination force between the negative electrostatic potential of halogen atom and the gold atom, and type II complexes contain halogen bonds formed between the σ-hole of the halogen atoms and the negative electrostatic potential of Au_n. Results of the interaction energy indicate that type I complexes are more stable than type II complexes. AIM analysis reveals that type II complexes are a closed shell interaction and there is a partially covalent nature for type I complexes.     

DFT study of geometrical and vibrational features of a 3′,5′-deoxydisugar-monophosphate (dDSMP) DNA model in the presence of counterions and solvent

The B3LYP/6–31++G* theoretical level was used to study the influence of various hexahydrated monovalent (Li⁺, Na⁺, K⁺) and divalent (Mg²⁺) metal counterions in interaction with the charged PO₂^? group, on the geometrical and vibrational characteristics of the DNA fragments of 3′,5′-dDSMP, represented by four conformers (g⁺g⁺, g⁺t, g^?g^? and g^?t). All complexes were optimized through two solvation models [the explicit model (6H₂O) and the hybrid model (6H₂O/Continuum)]. The results obtained established that, in the hybrid model, counterions (Li⁺, Na⁺, K⁺, Mg²⁺) always remain in the bisector plane of the O1–P–O2 angle. When these counterions are explicitly hydrated, the smallest counterions (Li⁺, Na⁺) deviate from the bisector plane, while the largest counterions (K⁺ and Mg²⁺) always remain in the same plane. On the other hand, the present calculations reveal that the g⁺g⁺ conformer is the most stable in the presence of monovalent counterions, while conformers g⁺t and g^?t are the most stable in the presence of the divalent counterion Mg²⁺. Finally, the hybrid solvation model seems to be in better agreement with the available crystallographic and spectroscopic (Raman) experiments than the explicit model. Indeed, the six conformational torsions of the C4′-C3′-O3′-PO^?₂-O5′-C5′-C4′ segment of all complexes of the g^?g^? conformer in 6H₂O/Continuum remain similar to the available experimental data of A- and B-DNA forms. The calculated wavenumbers of the g⁺g⁺ conformer in the presence of the monovalent counterion and of g^?t conformer in presence of the divalent counterion in the hybrid model are in good agreement with the Raman experimental data of A- and B-DNA forms. In addition, the maximum deviation between the calculated wavenumbers in the 6H₂O/Continuum for the g⁺g⁺ conformer and experimental value measured in an aqueous solution of the DMP-Na⁺ complex, is <1.07% for the PO₂^? (asymmetric and symmetric) stretching modes and <2.03% for the O5′-C5′ and O3′-C3′ stretching modes.

Open image in new window

Graphical abstract dDSMP-(OO)^? Mg²⁺/6W/Continuum

     

Theoretical study of the triangular bonding complex formed by carbon tetrabromide, a halide, and a solvent molecule in the gas phase

MP2(full)/aug-cc-pVDZ(-PP) computations predict that new triangular bonding complexes (where X^? is a halide and H–C refers to a protic solvent molecule) consist of one halogen bond and two hydrogen bonds in the gas phase. Carbon tetrabromide acts as the donor in the halogen bond, while it acts as an acceptor in the hydrogen bond. The halide (which commonly acts as an acceptor) can interact with both carbon tetrabromide and solvent molecule (CH₃CN, CH₂Cl₂, CHCl₃) to form a halogen bond and a hydrogen bond, respectively. The strength of the halogen bond obeys the order CBr₄???Cl^? > CBr₄???Br^? > CBr₄???I^?. For the hydrogen bonds formed between various halides and the same solvent molecule, the strength of the hydrogen bond obeys the order C-H???Cl^? > C-H???Br^? > C-H???I^?. For the hydrogen bonds formed between the same halide and various solvent molecules, the interaction strength is proportional to the acidity of the hydrogen in the solvent molecule. The diminutive effect is present between the hydrogen bonds and the halogen bond in chlorine and bromine triangular bonding complexes. Complexes containing iodide ion show weak cooperative effects.

NMR study on the hydroxy protons of the Lewis X and Lewis Y oligosaccharides

The ¹H NMR chemical shifts and NOEs of hydroxy protons in Lewis X trisaccharide, β-d-Galp-(1 → 4)[α-l-Fucp-(1 → 3)]-β-d-GlcpNAc, and Lewis Y tetrasaccharide, α-l-Fucp-(1 → 2)-β-d-Galp-(1 → 4)[α-l-Fucp-(1 → 3)]-β-d-GlcpNAc, were obtained for 85% H₂O/15% (CD₃)₂CO solutions. The OH-4 signal of Galp in Lewis X and OH-3, OH-4 signals of Galp, and OH-2 signal of Fucp linked to Galp in Lewis Y had chemical shifts which indicate reduced hydration due to their proximity to the hydrophobic face of the Fucp unit linked to GlcpNAc. The inter-residue NOEs involving the exchangeable NH and OH protons confirmed the stacking interaction between the Fucp linked to the GlcpNAc and the Galp residues in Lewis X and Lewis Y.     

Theoretical description of halogen bonding – an insight based on the natural orbitals for chemical valence combined with the extended-transition-state method (ETS-NOCV)

In the present study we have characterized the halogen bonding in selected molecules H₃N–ICF₃ (1-NH ₃ ), (PH₃)₂C–ICF₃ (1-CPH ₃ ), C₃H₇Br–(IN₂H₂C₃)₂C₆H₄ (2-Br), H₂–(IN₂H₂C₃)₂C₆H₄ (2-H ₂ ) and Cl–(IC₆F₅)₂C₇H₁₀N₂O₅ (3-Cl), containing from one halogen bond (1-NH ₃ , 1-CPH ₃ ) up to four connections in 3-Cl (the two Cl–HN and two Cl–I), based on recently proposed ETS-NOCV analysis. It was found based on the NOCV-deformation density components that the halogen bonding C–X ^… B (X-halogen atom, B-Lewis base), contains a large degree of covalent contribution (the charge transfer to X ^… B inter-atomic region) supported further by the electron donation from base atom B to the empty σ*(C–X) orbital. Such charge transfers can be of similar importance compared to the electrostatic stabilization. Further, the covalent part of halogen bonding is due to the presence of σ-hole at outer part of halogen atom (X). ETS-NOCV approach allowed to visualize formation of the σ-hole at iodine atom of CF₃I molecule. It has also been demonstrated that strongly electrophilic halogen bond donor, [C₆H₄(C₃H₂N₂I)₂][OTf]₂, can activate chemically inert isopropyl bromide (2-Br) moiety via formation of Br–I bonding and bind the hydrogen molecule (2-H ₂ ). Finally, ETS-NOCV analysis performed for 3-Cl leads to the conclusion that, in terms of the orbital-interaction component, the strength of halogen (Cl–I) bond is roughly three times more important than the hydrogen bonding (Cl–HN).

Host-guest properties of the trinuclear arene-ruthenium cluster cation [H3Ru3(C6H6)(C6Me6)2(O)]

The trinuclear arene-ruthenium cluster cation [H₃Ru₃(C₆H₆)(C₆Me₆)₂(O)]⁺, containing a μ₃-oxo cap and three arene ligands that span a hydrophobic pocket above the metal skeleton, has been crystallised as tetrafluoroborate salt in the presence of various guest molecules. The host-guest complexes have been characterised by single-crystal X-ray structure analysis. With chloroform as the guest molecule, a CHCl₃ molecule sits perfectly in the hydrophobic pocket, the hydrogen atom being encapsulated inside the cavity. When dioxane is added during the crystallisation process, the cluster forms infinite chains which are connected by a complex network of hydrogen bonds involving the μ₃-oxo ligand, water and dioxane molecules. Interestingly, in the presence of phenol, a water molecule is hydrogen-bonded between the μ₃-oxo ligand and the phenol molecule, forming a one-dimensional μ₃-O ? H₂O ? HO hydrogen-bonded chain. Finally, with benzoic acid, a head-to-tail host-guest chain is obtained, the phenyl ring being incorporated in the hydrophobic pocket, while the acid group is hydrogen-bonded to the μ₃-oxo ligand.