Quantitative characterization of protein tertiary motifs

Dimerization of 2-naphthalenecarbonitrile (2-NpCN) mediated by cucurbit[8]uril (CB[8]) has been investigated employing the density functional theory. Different structures of 2-NpCN dimers were generated by combining monomers in anti-head-to-head (A), anti-head-to-tail (B) and syn-head-to-tail (C) fashion. All these dimeric structures possess rigid cube-like architecture. On confinement within the CB[8] dimer A turns out to be the lowest energy structure. Calculated ¹H NMR spectra revealed that the 2-NpCN dimer exhibits large shielding for aromatic protons consistent with the experiment. The protons attached to cubane moiety on the other hand, led to down-field signals. Dimerization mediated with CB[8] cavitand is further accompanied by the frequency up-shift (blue shift) of methylene stretching vibration in its infrared spectra.

DFT and docking studies of rhodostreptomycins A and B and their interactions with solvated/nonsolvated Mg2+ and Ca2+ ions

The interactions of L-aminoglucosidic stereoisomers such as rhodostreptomycins A (Rho A) and B (Rho B) with cations (Mg²⁺, Ca²⁺, and H⁺) were studied by a quantum mechanical method that utilized DFT with B3LYP/6-311G**. Docking studies were also carried out in order to explore the surface recognition properties of L-aminoglucoside with respect to Mg²⁺ and Ca²⁺ ions under solvated and nonsolvated conditions. Although both of the stereoisomers possess similar physicochemical/antibiotic properties against Helicobacter pylori, the thermochemical values for these complexes showed that its high affinity for Mg²⁺ cations caused the hydration of Rho B. According to the results of the calculations, for Rho A–Ca²⁺(H₂O)₆, ΔH = ?72.21 kcal?mol^?1; for Rho B–Ca²⁺(H₂O)₆, ΔH = ?72.53 kcal?mol^?1; for Rho A–Mg²⁺(H₂O)₆, ΔH = ?72.99  kcal?mol^?1 and for Rho B–Mg²⁺(H₂O)₆, ΔH = ?95.00  kcal?mol^?1, confirming that Rho B binds most strongly with hydrated Mg²⁺, considering the energy associated with this binding process. This result suggests that Rho B forms a more stable complex than its isomer does with magnesium ion. Docking results show that both of these rhodostreptomycin molecules bind to solvated Ca²⁺ or Mg²⁺ through hydrogen bonding. Finally, Rho B is more stable than Rho A when protonation occurs.

Theoretical description of the magnetic properties of μ3-hydroxo bridged trinuclear copper(II) complexes

A theoretical study of the magnetic properties, using density functional theory, of a family of trinuclear μ₃-OH copper(II) complexes reported in the literature is presented. The reported X-ray crystal structures of [Cu₃(μ₃-OH)(aat)₃(H₂O)₃](NO₃)₂·H₂O (HUKDUM), where aat: 3-acetylamine-1,2,4-triazole; [Cu₃(μ₃-OH)(aaat)₃(H₂SO₄)(HSO₄)(H₂O)] (HUKDOG), where aaat: 3-acetylamine-5-amine-1,2,4-triazole; [Cu₃(μ₃-OH)(PhPyCNO)₃(tchlphac)₂] (HOHQUR), where PhPyCNO: phenyl 2-pyridyl-ketoxime and tchlphac: acid 2,4,5-trichlorophenoxyacetic; [Cu₃(μ₃-OH)(PhPyCNO)₃(NO₃)₂(CH₃OH)] (ILEGEM); [Cu₃(μ₃-OH)(pz)₃(Hpz)₃(ClO₄)₂] (QOPJIP), where Hpz?=?pyrazole; [Cu₃(μ₃-OH)(pz)₃(Hpz)(Me₃CCOO)₂]?2Me₃CCOOH (DEFSEN) and [Cu₃(μ₃-OH)(8-amino-4-methyl-5-azaoct-3-en-2-one)₃][CuI₃] (RITXUO), were used in the calculations. The magnetic exchange constants were calculated using the broken-symmetry approach. The calculated J values are for HUKDUM J₁?=??68.6 cm^?1, J₂?=??69.9 cm^?1, J₃?=??70.4 cm^?1; for HUKDOG, J₁?=??73.5 cm^?1, J₂?=??58.9 cm^?1, J₃?=??62.1 cm^?1; for HOHQUR J₁?=??128.3 cm^?1, J₂?=??134.1 cm^?1, J₃?=??120.4 cm^?1; for ILEGEM J₁?=??151.6 cm^?1, J₂?=??173.9 cm^?1, J₃?=??186.9 cm^?1; for QOPJIP J₁?=??118.3 cm^?1, J₂?=??106.0 cm^?1, J₃?=??120.6 cm^?1; for DEFSEN J₁?=??74.9 cm^?1, J₂?=??64.0 cm^?1, J₃?=??57.7 cm^?1 and for RITXUO J₁?=??10.9 cm^?1, J₂?=?+14.3 cm^?1, J₃?=??35.4 cm^?1. The Kahn-Briat model was used to correlate the calculated magnetic properties with the overlap of the magnetic orbitals. Spin density surfaces show that the delocalization mechanism is predominant in all the studied compounds.

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.

Microsolvation and hydration enthalpies of CaC2O4(H2O) n (n = 0-16) and C2O4 2-(H2O) n (n = 0-14): an ab initio study

We studied hydrated calcium oxalate and its ions at the restricted Hartree–Fock RHF/6-31G* level of theory. Performing a configurational search seems to improve the fit of the HF/6-31G* level to experimental data. The first solvation shell of calcium oxalate contains 13 water molecules, while the first solvation shell of oxalate ion is formed by 14 water molecules. The first solvation shell of Ca(II) is formed by six water molecules, while the second shell contains five. At 298.15 K, we estimate the asymptotic limits (infinite dilution) of the total standard enthalpies of hydration for Ca(II), oxalate ion and calcium oxalate as ?480.78, –302.78 and –312.73 kcal mol^?1, resp. The dissociation of hydrated calcium oxalate is an endothermic process with an asymptotic limit of +470.84 kcal mol^?1.

A UB3LYP and UMP2 theoretical investigation on unusual cation–π interaction between the triplet state HB=BH ( {}^3\Sigma_g^{-} ) and H+, Li+, Na+, Be2+ or Mg2+

The nature of the unusual cation–π interactions between cations (H⁺, Li⁺, Na⁺, Be²⁺ and Mg²⁺) and the electron-deficient B=B bond of the triplet state HB=BH ( $ {}^3\Sigma_g^{-} $ ) was investigated using UMP2(full) and UB3LYP methods at 6–311++G(2df,2p) and aug-cc-pVTZ levels, accompanied by a comparison with 1:1 and 2:1 σ-binding complexes between BH and the cations. The binding energies follow the order HB=BH...H⁺ > HB=BH...Be²⁺ > HB=BH...Mg²⁺ ? HB=BH...Li⁺ > HB=BH...Na⁺ and HB=BH (¹Δ_g)...M⁺/M²⁺ > H₂C=CH₂...M⁺/M²⁺ > HC≡CH...M⁺/M²⁺ > HB=BH ( $ {}^3\Sigma_g^{-} $ )...M⁺/M²⁺. Furthermore, except for HB...H⁺, the σ-binding interaction energy of the 1:1 complex HB...M⁺/M²⁺ is stronger than the cation–π interaction energy of the C₂H₂...M⁺/M²⁺, C₂H₄...M⁺/M²⁺, B₂H₂ (¹Δ_g)...M⁺/M²⁺ or B₂H₂ ( $ {}^3\Sigma_g^{-} $ )...M⁺/M²⁺ complex, and, for the 2:1 σ-binding complexes, except for HBBe²⁺...BH, they are less stable than the cation–π complexes of B₂H₂ (¹Δ_g) or B₂H₂ ( $ {}^3\Sigma_g^{-} $ ). The atoms in molecules (AIM) theory was also applied to verify covalent interactions in the H⁺ complexes and confirm that HB=BH ( $ {}^3\Sigma_g^{-} $ ) can be a weaker π-electron donor than HB=BH (¹Δ_g), H₂C=CH₂ or HC≡CH in the cation–π interaction. Analyses of natural bond orbital (NBO) and electron density shifts revealed that the origin of the cation–π interaction is mainly that many of the lost densities from the π-orbital of B=B and CC multiple bonds are shifted toward the cations.

Theoretical studies of the interaction between enflurane and water

Increase of the atmospheric concentration of halogenated organic compounds is partially responsible for a change of the global climate. In this work we have investigated the interaction between halogenated ether and water, which is one of the most important constituent of the atmosphere. The structures of the complexes formed by the two most stable conformers of enflurane (a volatile anaesthetic) with one and two water molecules were calculated by means of the counterpoise CP-corrected gradient optimization at the MP2/6–311++G(d,p) level. In these complexes the CH…O_w hydrogen bonds are formed, with the H…O_w distances varying between 2.23 and 2.32 Å. A small contraction of the CH bonds and the blue shifts of the ν(CH) stretching vibrations are predicted. There is also a weak interaction between one of the F atoms and the H atom of water, with the H_w…F distances between 2.41 and 2.87 Å. The CCSD(T)/CBS calculated stabilization energies in these complexes are between ?5.89 and ?4.66 kcal?mol^?1, while the enthalpies of formation are between ?4.35 and ?3.22 kcal?mol^?1. The Cl halogen bonding between enflurane and water has been found in two complexes. The intermolecular (Cl···O) distance is smaller than the sum of the corresponding van der Waals radii. The CCSD(T)/CBS stabilization energies for these complexes are about ?2 kcal?mol^?1.

Prediction of thermodynamically reversible hydrogen storage reactions utilizing Ca–M(M = Li, Na, K)–B–H systems: a first-principles study

Calcium borohydride is a potential candidate for onboard hydrogen storage because it has a high gravimetric capacity (11.5 wt.%) and a high volumetric hydrogen content (～130 kg m^?3). Unfortunately, calcium borohydride suffers from the drawback of having very strongly bound hydrogen. In this study, Ca(BH₄)₂ was predicted to form a destabilized system when it was mixed with LiBH₄, NaBH₄, or KBH₄. The release of hydrogen from Ca(BH₄)₂ was predicted to proceed via two competing reaction pathways (leading to CaB₆ and CaH₂ or CaB₁₂H₁₂ and CaH₂) that were found to have almost equal free energies. Using a set of recently developed theoretical methods derived from first principles, we predicted five new hydrogen storage reactions that are among the most attractive of those presently known. These combine high gravimetric densities (>6.0 wt.% H₂) with have low enthalpies [approximately 35 kJ/(mol^?1 H₂)] and are thermodynamically reversible at low pressure within the target window for onboard storage that is actively being considered for hydrogen storage applications. Thus, the first-principles theoretical design of new materials for energy storage in future research appears to be possible.

Effects of negative air ions on oxygen uptake kinetics,recovery and performance in exercise: a randomized,double-blinded study

Limited research has suggested that acute exposure to negatively charged ions may enhance cardio-respiratory function, aerobic metabolism and recovery following exercise. To test the physiological effects of negatively charged air ions, 14 trained males (age: 32?±?7 years; \( \overset{\cdotp }{V}{\mathrm{O}}_{2 \max } \) : 57?±?7 mL min^?1 kg^?1) were exposed for 20 min to either a high-concentration of air ions (ION: 220?±?30?×?10³ ions cm^?3) or normal room conditions (PLA: 0.1?±?0.06?×?10³ ions cm^?3) in an ionization chamber in a double-blinded, randomized order, prior to performing: (1) a bout of severe-intensity cycling exercise for determining the time constant of the phase II \( \overset{\cdotp }{V}{\mathrm{O}}_2 \) response (τ) and the magnitude of the \( \overset{\cdotp }{V}{\mathrm{O}}_2 \) slow component (SC); and (2) a 30-s Wingate test that was preceded by three 30-s Wingate tests to measure plasma [adrenaline] (ADR), [nor-adrenaline] (N-ADR) and blood [lactate] (B_Lac) over 20 min during recovery in the ionization chamber. There was no difference between ION and PLA for the phase II \( \overset{\cdotp }{V}{\mathrm{O}}_2 \) τ (32?±?14 s vs. 32?±?14 s; P?=?0.7) or \( \overset{\cdotp }{V}{\mathrm{O}}_2 \) SC (404?±?214 mL vs 482?±?217 mL; P?=?0.17). No differences between ION and PLA were observed at any time-point for ADR, N-ADR and B_Lac as well as on peak and mean power output during the Wingate tests (all P?>?0.05). A high-concentration of negatively charged air ions had no effect on aerobic metabolism during severe-intensity exercise or on performance or the recovery of the adrenergic and metabolic responses after repeated-sprint exercise in trained athletes.     

[(B3O3H3)nM]+(n = 1, 2;M = Cu, Ag, Au): a new class of metal-cation complexes

A density functional theory (DFT) investigation into the structures and bonding characteristics of [(B₃O₃H₃)_nM]⁺(n?=?1, 2;M?=?Cu, Ag, Au) complexes was performed. DFT calculations and natural bond orbital (NBO) analyses indicate that the ΙB metal complexes of boroxine exhibit intriguing bonding characteristics, different from the typical cation–π interactions between ΙB metal-cations and benzene. The complexes of [B₃O₃H₃M]⁺ and [(B₃O₃H₃)₂?M]⁺ (M?=?Cu, Ag, and Au) favor the conformation of perfectly planar structures with the C_2v and D_2h symmetry along one of the threefold molecular axes of boroxine, respectively. Detailed natural resonance theory (NRT) and canonical molecular orbitals (CMOs) analyses show that interaction between the metal cation and the boroxine in [B₃O₃H₃M]⁺ (M?=?Cu, Ag, and Au) is mainly ionic, while the ΙB metal-cations←π donation effect is responsible for the binding site. In these complexes, boroxine serves as terminals η¹-B₃O₃H₃ with one O atom of the B₃O₃ ring. The infra-red (IR) spectra of [B₃O₃H₃M]⁺ were simulated to facilitate their future experimental characterization. The complexes all give two IR active modes at about 1,300 and 2,700 cm^?1, which are inactive in pure boroxine. Simultaneously, the B–H stretching modes of the complexes are red-shifted due to the interaction between the metal-cation and boroxine. To explore the possibility of the structural pattern developed in this work forming mesoporous materials, complexes [(B₃O₃H₃M)₆]⁶⁺ (M?=?Cu, Ag, and Au) were also studied, which appear to be unique and particular interesting: they are all true minima with D_6h symmetries and pore sizes ranging from 12.04 Å to 13.65 Å.

Calixarene building block bis(2-hydroxyphenyl)methane (2HDPM) and hydrogen-bonded 2HDPM-H2O complex in electronic excited state

Intramolecular and intermolecular hydrogen bonding in electronic excited states of calixarene building blocks bis(2-hydroxyphenyl)methane (2HDPM) monomer and hydrogen-bonded 2HDPM-H₂O complex were studied theoretically using the time-dependent density functional theory (TDDFT). Twenty-four stable conformations (12 pairs of enantiomers) of 2HDPM monomer have been found in the ground state. From the calculation results, the conformations 1a and 1b which both have an intramolecular hydrogen bond are the most stable ones. The infrared spectra of 2HDPM monomer and 2HDPM-H₂O complex in ground state and S₁ state were calculated. The stretching vibrational absorption band of O₂???H₃ group in the monomer and complex disappeared in the S₁ state. At the same time, a new strong absorption band appeared at the C=O stretching region. From the calculation of bond lengths, it indicates that the O₂???H₃ bond is significantly lengthened in the S₁ state. However, the C₁???O₂ bond is drastically shortened upon electronic excitation to the S₁ state and has the characteristics of C=O band. Furthermore, the intramolecular hydrogen bond O₂???H₃?·?·?·?O₄ of the 2HDPM monomer and the intermolecular hydrogen bonds O₂???H₃?·?·?·?O₇ and O₇???H₉?·?·?·?O₄ of 2HDPM-H₂O complex are all shortened and strengthened in the S₁ state.

Transport of l-proline by the proton-coupled amino acid transporter PAT2 in differentiated 3T3-L1 cells

Mechanism and substrate specificity of the proton-coupled amino acid transporter 2 (PAT2, SLC36A2) have been studied so far only in heterologous expression systems such as HeLa cells and Xenopus laevis oocytes. In this study, we describe the identification of the first cell line that expresses PAT2. We cultured 3T3-L1 cells for up to 2 weeks and differentiated the cells into adipocytes in supplemented media containing 2 μM rosiglitazone. During the 14 day differentiation period the uptake of the prototype PAT2 substrate l-[³H]proline increased ~5-fold. The macro- and microscopically apparent differentiation of 3T3-L1 cells coincided with their H⁺ gradient-stimulated uptake of l-[³H]proline. Uptake was rapid, independent of a Na⁺ gradient but stimulated by an inwardly directed H⁺ gradient with maximal uptake occurring at pH 6.0. l-Proline uptake was found to be mediated by a transport system with a Michaelis constant (K_t) of 130 ± 10 μM and a maximal transport velocity of 4.9 ± 0.2 nmol × 5 min^?1 mg of protein^?1. Glycine, l-alanine, and l-tryptophan strongly inhibited l-proline uptake indicating that these amino acids also interact with the transport system. It is concluded that 3T3-L1 adipocytes express the H⁺-amino acid cotransport system PAT2.     

Microsolvation of Mg2+, Ca2+: strong influence of formal charges in hydrogen bond networks

A stochastic exploration of the quantum conformational spaces in the microsolvation of divalent cations with explicit consideration of up to six solvent molecules [Mg (H ₂ O) _n )]²⁺, (n?=?3, 4, 5, 6) at the B3LYP, MP2, CCSD(T) levels is presented. We find several cases in which the formal charge in Mg²⁺ causes dissociation of water molecules in the first solvation shell, leaving a hydroxide ion available to interact with the central cation, the released proton being transferred to outer solvation shells in a Grotthus type mechanism; this particular finding sheds light on the capacity of Mg²⁺ to promote formation of hydroxide anions, a process necessary to regulate proton transfer in enzymes with exonuclease activity. Two distinct types of hydrogen bonds, scattered over a wide range of distances (1.35–2.15 Å) were identified. We find that in inner solvation shells, where hydrogen bond networks are severely disturbed, most of the interaction energies come from electrostatic and polarization+charge transfer, while in outer solvation shells the situation approximates that of pure water clusters.

Theoretical study of the interaction between molecular oxygen and tetraaza macrocyclic manganese complexes

Theoretical chemistry calculations using the Density Functional Theory (DFT) were carried out to understand the interaction between oxygen (O₂) and MnN₄ type manganese-based complexes during the formation of MnN₄-O₂ adducts. In order to understand how this interaction is affected by different macrocyclic ligands, O₂ was bonded to manganese-porphyrin (MnP), manganese-octamethylporphyrin (MnOMP), manganese-tetraaza[14]annulene (MnTAA), manganese-dibenzo [b,i] [1, 4, 8, 11]-tetraaza [14] annulene (MnDBTAA), manganese-2,3,9,10-tetramethyl-1,4,8,11-tetraazacyclotetradeca-1,3,8,10-tetraene ([(tim)Mn]²⁺), and manganese-2,3,9,10-tetraphenyl-1,4,8,11-tetraazacyclotetradeca-1,3,8,10-tetraene ([(ph-tim)Mn]²⁺). The binding and activation of the oxygen molecule was facilitated by an increasing trend in the O-O bond lengths and a decreasing one in the O-O vibrational frequency, with preference for the O₂ side-on interaction among MnN₄ macrocycles. The catalytic activities of the MnN₄ complexes toward the O₂ binding process increased in the following order: [(ph-tim)Mn]²⁺?<?MnP?<?MnOMP?<?MnDBTAA?<?MnTAA?<?[(tim)Mn]²⁺. Therefore, it was concluded that the [(tim)Mn]²⁺complex was the most active for the binding and activation of molecular oxygen.     

Theoretical study about the 5-azido-1H-tetrazole and its ion salts

Periodic DFT method has been firstly used to calculate the bulk structure, electronic structure, electrical transferring and thermodynamic properties of crystalline 5-azido-1H-tetrazole (HCN₇) and its four different salts. The anion CN₇ ^? was included in all of the salts such as ammonium 5-azidotetrazolate ([NH₄]⁺[CN₇]^?), hydrazinium 5-azidotetrazolate ([N₂H₅]⁺[CN₇]^?), guanidinium 5-azidotetrazolate ([CH₆N₃]⁺[CN₇]^??·?H₂O) and 1-aminoguanidinium 5- azidotetrazolate ([CH₇N₄]⁺[CN₇]^?). The simulation is in reasonable agreement with the experimental results. It is found the salts of HCN₇ are more stable than itself because the band gap of the salts is larger. The density of state shows the p states of them (including HCN₇ and its four salts) have played a very significant role in the reaction.

Simulations on the possibility of formation of complexes between fluorouracil drug and cucurbit[n]urils: ab initio van der Waals DFT study

The binding geometry of fluorouracil/cucurbit[n]urils (CB[n]s) complexes with n?=?5–8 is investigated using the first-principles van der Waals density functional (vdW-DF) method, involving full geometry optimization. Such host-guest complexes are typically calculated using conventional DFT method, which significantly underestimates non-local dispersion forces (or vdW contributions) and therefore affects interactions between respected entities. We address here the role of vdW forces for the fluorouracil and CB[n]s molecules which can form directional hydrogen bonds with each other. It was found that the inclusion of dispersion interactions significantly affects the host-guest binding properties and the hydrogen bonding between the molecules provides the main binding mechanism, while results in the same geometries for the considered complexes. The 0.84 eV binding energy, for the thermodynamically favorable state, reveals that the interaction of fluorouracil with CB[n]s is an exothermic interaction and typical for strong hydrogen bonding. Furthermore, we have investigated the binding nature of these host-guest systems in aqueous solution with ab initio MD simulations adopting vdW-DF method. These findings afford evidence for the applicability of the vdW-DF approach and provide a realistic benchmark for the investigation of the host-guest complexes.

Biological evaluation of a cytotoxic 2-substituted benzimidazole copper(II) complex: DNA damage,antiproliferation and apoptotic induction activity in human cervical cancer cells

Exploring novel chemotherapeutic agents is a great challenge in cancer medicine. To that end, 2-substituted benzimidazole copper(II) complex, [Cu(BMA)Cl₂]·(CH₃OH) (1) [BMA = N,N′-bis(benzimidazol-2-yl-methyl)amine], was synthesized and its cytotoxicity was characterized. The interaction between complex 1 and calf thymus DNA was detected by spectroscopy methods. The binding constant (K _b = 1.24 × 10⁴ M^?1) and the apparent binding constant (K _app = 6.67 × 10⁶ M^?1) of 1 indicated its moderate DNA affinity. Complex 1 induced single strand breaks of pUC19 plasmid DNA in the presence of H₂O₂ through an oxidative pathway. Cytotoxicity studies proved that complex 1 could inhibit the proliferation of human cervical carcinoma cell line HeLa in both time- and dose-dependent manners. The results of nuclei staining by Hoechst 33342 and alkaline single-cell gel electrophoresis proved that complex 1 caused cellular DNA damage in HeLa cells. Furthermore, treatment of HeLa cells with 1 resulted in S-phase arrest, loss of mitochondrial potential, and up-regulation of caspase-3 and -9 in HeLa cells, suggesting that complex 1 was capable of inducing apoptosis in cancer cells through the intrinsic mitochondrial pathway.     

Design of Lewis acid–base complex: enhancing the stability and first hyperpolarizability of large excess electron compound

In the present paper, a new type of Lewis acid–base complex BX₃???Li@Calix[4]pyrrole (X = H and F) was designed and assembled based on electride molecule Li@calix[4]pyrrole (as a Lewis base) and the electron deficient molecule BX₃ (as a Lewis acid) by employing quantum mechanical calculation. The new Lewis acid–base complex offers an interesting push-excess electron-pull (P-e-P) framework to enhance the stability and nonlinear optical (NLO) response. To measure the nonlinear optical response, static first hyperpolarizabilities (β ₀) are exhibited. Significantly, point-face assembled Lewis acid–base complex BF₃???Li@Calix[4]pyrrole (II) has considerable first hyperpolarizabilities (β ₀) value (1.4?×?10⁶ a.u.), which is about 117 times larger than reported 11,721 a.u. of electride Li@Calix[4]pyrrole. Further investigations show that, in BX₃???Li@Calix[4]pyrrole with P-e-P framework, a strong charge-transfer transition from the ground state to the excited state contributes to the enhancement of first hyperpolarizability. Theory calculation of enthalpies of reaction (Δ_rH⁰) at 298 K demonstrates that it is feasible to synthetize the complexes BX₃???Li@Calix[4]pyrrole. In addition, compared with Li@Calix[4]pyrrole, the vertical ionization potential (VIP) and HOMO–LUMO gap of BX₃???Li@Calix[4]pyrrole have obviously increased, due to the introduction of the Lewis acid molecule BX₃. The novel Lewis acid–base NLO complex possesses not only a large nonlinear optical response but also higher stability.

A theoretical investigation on the proton transfer tautomerization mechanisms of 2-thioxanthine within microsolvent and long range solvent

A relative complete study on the mechanisms of the proton transfer reactions of 2-thioxanthine was carried out with density functional theory. The models were designed with monohydrated and dihydrated microsolvent catalyses either with or without the presence of water solvent considered with the polarized continuum model (PCM). A total number of 114 complexes and 67 transition states were found with the B3LYP/6-311+G** calculations. The energies were refined with both B3LYP/aug-cc-pVTZ and PCM-B3LYP/aug-cc-pVTZ methods. The activation energies were reported with respect to the Gibbs free energies obtained in conjunction with the standard statistical thermodynamics. Possible reaction pathways were confirmed with the intrinsic reaction coordinates. Pathways via C8 atom on the imidazole ring, via the bridged C4 and C5 atoms between pyrimidine and imidazole rings and via N, O and S atom on the pyrimidine ring were examined. The results show that the most feasible pathway is the proton transfers within the long range solvent surrounding via the N, O and S atoms in the pyrimidine ring with di-hydrated catalysis: N(7)H?+?2H₂O?→?IM89?→?IM90?→?P13?+?2H₂O?→?IM91?→?IM92?→?P6?+?2H₂O?→?IM71?→?IM72?→?P7?+?2H₂O?→?IM107?→?IM108?→?P18?+?2H₂O?→?IM111?→?IM112?→?P19?+?2H₂O?→?IM113?→?IM114?→?P17?+?2H₂O?→?IM105?→?IM106?→?N(9)H?+?2H₂O that has the highest energy barrier of 44.0 kJ mol^?1 in the transition of IM89 to IM90 via TS54. The small energy barrier is in good agreement with the experimental observation that 2-TX tautomerizes at room temperature in water. In the aqueous phase, the most stable intermediate is found to be IM21 [N(7)H?+?2H₂O] and the possible co-existing species are the monohydrated IM1, IM9, IM39 and IM46, and the di-hydrated IM5, IM8, IM13, IM16, IM81, IM89, IM90, IM91 and IM106 complexes that have a relative concentration larger than 10^?6 (1 ppm) with respect to IM21.