Sensing behavior of Al-rich AlN nanotube toward hydrogen cyanide

In order to explore a sensor for detection of toxic hydrogen cyanide (HCN) molecules, interaction of pristine and defected Al-rich aluminum nitride nanotubes (AlNNT) with a HCN molecule has been investigated using density functional theory calculations in terms of energetic, geometric, and electronic properties. It has been found that unlike the pristine AlNNT, the Al-rich AlNNT can effectively interact with the HCN molecule so that its conductivity changes upon the exposure to this molecule. The adsorption energies of HCN on the pristine and defected AlNNTs have been calculated to be in the range of ?0.16 to ?0.62 eV and ?1.75 to ?2.21 eV, respectively. We believe that creating Al-rich defects may be a good strategy for improving the sensitivity of these tubes toward HCN molecules, which cannot be trapped and detected by the pristine AlNNT.     

Hydrogen dissociation on diene-functionalized carbon nanotubes

Chemical functionalization of a zigzag carbon nanotube (CNT) with 1, 3-cyclohexadiene (CHD), previously reported by experimentalists, has been investigated in the present study using density functional theory in terms of energetic, geometric, and electronic properties. Then, the thermodynamic and kinetic feasibility of H₂ dissociation on the pristine and functionalized CNTs have been compared. The dissociation energy of the H₂ molecule on the pristine and functionalized CNT has been calculated to be about ?1.00 and ?1.55 eV, while the barrier energy is found to be about 3.70 and 3.51 eV, respectively. Therefore, H₂ dissociation is thermodynamically more favorable on the CNT-CHD system than on the pristine tube, while the favorability of the dissociation on the pristine tube is higher in term of kinetics.     

A large gap opening of graphene induced by the adsorption of CO on the Al-doped site

We investigated CO adsorption on the pristine, Stone-Wales (SW) defected, Al- and Si- doped graphenes by using density functional calculations in terms of geometric, energetic and electronic properties. It was found that CO molecule is weakly adsorbed on the pristine and SW defected graphenes and their electronic properties were slightly changed. The Al- and Si- doped graphenes show high reactivity toward CO, so calculated adoption energies are about ?11.40 and ?13.75 kcal mol^?1 in the most favorable states. It was found that, among all the structures, the electronic properties of Al-doped graphene are strongly sensitive to the presence of CO molecule. We demonstrate the existence of a large E_g opening of 0.87 eV in graphene which is induced by Al-doping and CO adsorption.     

Si-doped graphene: an ideal sensor for NO- or NO<Subscript>2</Subscript>-detection and metal-free catalyst for N<Subscript>2</Subscript>O-reduction

Exploring and evaluating the potential applications of two-dimensional graphene is an increasingly hot topic in graphene research. In this paper, by studying the adsorption of NO, N₂O, and NO₂ on pristine and silicon (Si)-doped graphene with density functional theory methods, we evaluated the possibility of using Si-doped graphene as a candidate to detect or reduce harmful nitrogen oxides. The results indicate that, while adsorption of the three molecules on pristine graphene is very weak, Si-doping enhances the interaction of these molecules with graphene sheet in various ways: (1) two NO molecules can be adsorbed on Si-doped graphene in a paired arrangement, while up to four NO₂ molecules attach to the doped graphene with an average adsorption energy of −0.329 eV; (2) the N₂O molecule can be reduced easily to the N₂ molecule, leaving an O-atom on the Si-doped graphene. Moreover, we find that adsorption of NO and NO₂ leads to large changes in the electronic properties of Si-doped graphene. On the basis of these results, Si-doped graphene can be expected to be a good sensor for NO and NO₂ detection, as well as a metal-free catalyst for N₂O reduction.     

Nitrous oxide adsorption on pristine and Si-doped AlN nanotubes

Using density functional theory, we studied the adsorption of an N₂O molecule onto pristine and Si-doped AlN nanotubes in terms of energetic, geometric, and electronic properties. The N₂O is weakly adsorbed onto the pristine tube, releasing energies in the range of ?1.1 to ?5.7 kcal mol^-1. The electronic properties of the pristine tube are not influenced by the adsorption process. The N₂O molecule is predicted to strongly interact with the Si-doped tube in such a way that its oxygen atom diffuses into the tube wall, releasing an N₂ molecule. The energy of this reaction is calculated to be about ?103.6 kcal mol^-1, and the electronic properties of the Si-doped tube are slightly altered.     

A DFT study on the sensing behavior of a BC2N nanotube toward formaldehyde

We investigated the viability of using a BC₂N nanotube to detect formaldehyde (H₂CO) molecule by means of B3LYP and M06 density functionals. The results indicate that the molecule is weakly adsorbed on the intrinsic BC₂N nanotube releasing energy of 0.8 kcal mol^-1 (at B3LYP/6-31G(d)) without significant effect on the HOMO-LUMO energy gap and electrical conductivity of the tube. Thus, H₂CO cannot be detected using this intrinsic nanotube. To overcome this problem, a carbon atom of the tube wall was substituted by a Si atom. It was demonstrated that the Si-doped tube cannot only strongly adsorb the H₂CO molecule, but also may effectively detect its presence because of the increase in the electric conductivity of the tube.     

Monte Carlo calculation of the primary radical and molecular yields of liquid water radiolysis in the linear energy transfer range 0.3-6.5 keV/micrometer: application to 137Cs gamma rays

Monte Carlo simulations of the radiolysis of neutral liquid water and 0.4 M H(2)SO(4) aqueous solutions at ambient temperature are used to calculate the variations of the primary radical and molecular yields (at 10(-6)s) as a function of linear energy transfer (LET) in the range approximately 0.3 to 6.5 keV/micrometer. The early energy deposition is approximated by considering short (approximately 20-100 micrometer) high-energy (approximately 300-6.6 MeV) proton track segments, over which the LET remains essentially constant. The subsequent nonhomogeneous chemical evolution of the reactive species formed in these tracks is simulated by using the independent reaction times approximation, which has previously been used successfully to model the radiolysis of water under various conditions. The results obtained are in good general agreement with available experimental data over the whole LET range studied. After normalization of our computed yields relative to the standard radical and molecular yields for (60)Co gamma radiation (average LET approximately 0.3 keV/micrometer), we obtain empirical relationships of the primary radiolytic yields as a function of LET over the LET range studied. Such relationships are of practical interest since they allow us to predict a priori values of the radical and molecular yields for any radiation from the knowledge of the average LET of this radiation only. As an application, we determine the corresponding yields for the case of (137)Cs gamma radiation. For this purpose, we use the value of approximately 0.91 keV/micrometer for the average LET of (137)Cs gamma rays, chosen so that our calculated yield G(Fe(3+)) for ferrous-ion oxidation in air-saturated 0.4 M sulfuric acid reproduces the value of 15.3 molecules/100 eV for this radiation recommended by the International Commission on Radiation Units and Measurements. The uncertainty range on those primary radical and molecular yields are also determined knowing the experimental error (approximately 2%) for the measured G(Fe(3+)) value. The following values (expressed in molecules/100 eV) are obtained: (1) for neutral water: G(e(-)(aq)) = 2.50 +/- 0.16, G(H(.)) = 0.621 +/- 0.019, G(H(2)) = 0.474 +/- 0.025, G((.)OH) = 2.67 +/- 0.14, G(H(2)O(2)) = 0.713 +/- 0.031, and G(-H(2)O) = 4.08 +/- 0.22; and (2) for 0.4 M H(2)SO(4) aqueous solutions: G(H(.)) = 3.61 +/- 0.09, G(H(2)) = 0.420 +/- 0.019, G((.)OH) = 2.78 +/- 0.12, G(H(2)O(2)) = 0.839 +/- 0.037, and G(-H(2)O) = 4.46 +/- 0.16. These computed values are found to differ from the standard yields for (60)Co gamma rays by up to approximately 6%.     

Predicting CO2 adsorption and reactivity on transition metal surfaces using popular density functional theory methods

ABSTRACT

In this work, with Ni (110) as a model catalyst surface and CO₂ as an adsorbate, a performance study of Density Functional Theory methods (functionals) is performed. CO being a possible intermediate in CO₂ conversion reactions, binding energies of both, CO₂ and CO, are calculated on the Ni surface and are compared with experimental data. OptPBE-vdW functional correctly predicts CO₂ binding energy on Ni (?62?kJ/mol), whereas CO binding energy is correctly predicted by the rPBE-vdW functional (?138?kJ/mol). The difference in computed adsorption energies by different functionals is attributed to the calculation of gas phase CO₂. Three alternate reaction systems based on a different number of C=O double bonds present in the gas phase molecule are considered to replace CO₂. The error in computed adsorption energy is directly proportional to the number of C=O double bonds present in the gas phase molecule. Additionally, both functionals predict similar carbon–oxygen activation barrier (40?kJ/mol) and equivalent C1s shifts for probe species (?2.6?eV for CCH₃ and +1.5?eV CO₃^?), with respect to adsorbed CO₂. Thus, by including a correction factor of 28?kJ/mol for the computed CO₂ gas phase energy, we suggest using rPBE-vdW functional to investigate CO₂ conversion reactions on different metals.     

Theoretical study of chemisorption of cyanuric fluoride and S-triazine on the surface of Al-doped graphene

We studied the adsorption of cyanuric fluoride (CF) and s-triazine (ST) molecules on the surface of pristine as well as Al-doped graphenes using density functional theory calculations. Our results reveal low adsorption on the surface of pristine graphene; but by modification of surface using aluminium, resulted Al-doped graphene becomes more reactive towards both CF and ST molecules. We aimed to focus on the adsorption energy, electronic structure, charge analysis, density of state and global indices of each system upon adsorption of CF and ST molecules on the above-mentioned surfaces. Our calculated adsorption energies for the most stable position configurations of CF and ST on Al-doped graphene were ?76.53 kJ mol^?1 (?57.45 kJ mol^?1 BSSE corrected energy) and ?115.55 kJ mol^?1 (?86.87 kJ mol^?1 BSSE corrected energy), respectively, which point to the chemisorption process. For each CF and ST molecule, upon adsorption on the surface of Al-doped graphene, the band gap of HOMO-LUMO was reduced considerably and it becomes a p-type semiconductor, whereas there is no hybridisation between the above-mentioned molecules and pristine graphene.     

Effect of multiple ionization on the yield of H2O2 produced in the radiolysis of aqueous 0.4 M H2SO4 solutions by high-LET 12C6+ and 20Ne9+ ions

Monte Carlo track structure simulations were performed to investigate the effect of multiple ionization of water on the primary (or "escape") (at approximately 10(-6) s) yield of hydrogen peroxide (G(H2O2)) produced in the radiolysis of deaerated 0.4 M H2SO4 solutions by 12C6+ and 20Ne9+ ions at high linear energy transfer (LET) up to approximately 900 keV/microm. It was found that, upon incorporating the mechanisms of double, triple and quadruple ionizations of water in the calculations, a quantitative agreement between theory and experiment can be obtained. The curve for G(H2O2) as a function of LET reaches a well-defined maximum of approximately 1.4 molecules/100 eV at approximately 180-200 keV/microm, in very good accord with the available experimental data. Our results also show that, for the highest LET values considered in this study, the H2O2 escape yields obtained in 0.4 M sulfuric acid solutions are about 45% greater in magnitude than those found in neutral water. Contrary to a recent assumption suggesting that the limiting value of G(H2O2) at infinite LET should be approximately 1 molecule/100 eV, somewhat similar for neutral and acidic water, our simulations show a clear decrease in the primary H2O2 yields with increasing LET at high LET, indicating that the question of the limiting value of G(H2O2) at very high LET for both neutral and acidic liquid water is still open.     

NH3 on a BC3 nanotube: effect of doping and decoration of aluminum

The adsorption of the NH₃ molecule was investigated on pristine, Al-doped and Al-decorated BC₃ nanotubes (BC₃NT) using density functional theory calculations. It was found that NH₃ prefers to be adsorbed on a B atom of the tube wall, releasing energy of 1.02 eV. Al-doping increases the acidity of the tube surface and, therefore, its reactivity toward NH₃ so that the released energy in this case is about 1.62 eV, while decorating the BC₃NT with Al atom decreases the acidity and reactivity. Although Al-doping has no significant effect on the electronic properties of the BC₃NT, Al-decoration significantly reduces its HOMO/LUMO energy gap from 2.37 to 1.16 eV so that the tube becomes an n-type semiconductor. However, we believe that the acidity of the BC₃NTs may be controlled by doping or decoration of Al atoms.     

Interaction of a Ti-doped semi-fullerene (TiC<Subscript>30</Subscript>) with molecules of CO and CO<Subscript>2</Subscript>

Using density functional theory (DFT) and molecular dynamics (MD), we studied the interaction of a titanium atom with a half of a C₆₀ fullerene (i.e., C₃₀), formed from the corannulene structure with a pentagonal base. We considered atmospheric pressure and 300 K. We found that the most stable adsorption of the titanium atom on C₃₀ occurs in the concave surface of the molecule. Afterward, we investigated the interaction of the system C₃₀-titanium with carbon monoxide and carbon dioxide molecules, respectively. We found that each of these molecules is chemisorbed, with no dissociation. The value of the adsorption energy for the carbon monoxide molecule varies from ?0.897 to ?1.673 eV, and for the carbon dioxide molecule, it is between ?1.065 and ?1.274 eV. These values depend on the initial orientation of these molecules with respect to TiC₃₀.

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Graphical Abstract The TiC₃₀ system chemisorbs CO or CO₂?with no dissociation at atmospheric pressure and 300K

     

A Detailed Study of the Amino Acids Produced from the Vacuum UV Irradiation of Interstellar Ice Analogs

We present a detailed analysis of the variety, quantity and distribution of the amino acids detected in organic residues after acid hydrolysis. Such organic residues are produced in the laboratory after the vacuum ultraviolet (VUV) irradiation of several astrophysically relevant ice mixtures containing H(2)O, CO, CO(2), CH(3)OH, CH(4) and NH(3) at low temperature (10-80 K), and subsequent warm-up to room temperature. We explore five experimental parameters: the irradiation time, the temperature, the ice mixture composition, the photon dose per molecule and the substrate for the ice deposition. The amino acids were detected and identified by ex-situ liquid chromatography analysis of the organic residues formed after warming the photolysed ices up to room temperature. This study shows that in all experiments amino acids are formed. Their total quantities and distribution depend slightly on the experimental parameters explored in the present work, the important requirement to form such molecules being that the starting ice mixtures must contain the four elements C, H, O and N. We also discuss the effects of the chemical treatment needed to detect and identify the amino acids in the organic residues. Finally, these results are compared with meteoritic amino acid data from the carbonaceous chondrite Murchison, and the formation processes of such compounds under astrophysical conditions are discussed.     

HEHEHE-tagged affibody molecule may be purified by IMAC, is conveniently labeled with [⁹⁹(m)Tc(CO)₃](+), and shows improved biodistribution with reduced hepatic radioactivity accumulation

Affibody molecules are a class of small (ca. 7 kDa) robust scaffold proteins suitable for radionuclide molecular imaging of therapeutic targets in vivo. A hexahistidine tag at the N-terminus streamlines development of new imaging probes by enabling facile purification using immobilized metal ion affinity chromatography (IMAC), as well as convenient [??(m)Tc(CO)?](+)-labeling. However, previous studies in mice have demonstrated that Affibody molecules labeled by this method yield higher liver accumulation of radioactivity, compared to the same tracer lacking the hexahistidine tag and labeled by an alternative method. Two variants of the HER2-binding Affibody molecule Z(HER)?(:)??? were made in an attempt to create a tagged tracer that could be purified by immobilized metal affinity chromatography, yet would not result in anomalous hepatic radioactivity accumulation following labeling with [??(m)Tc(CO)?](+). In one construct, the hexahistidine tag was moved to the C-terminus. In the other construct, every second histidine residue in the hexahistidine tag was replaced by the more hydrophilic glutamate, resulting in a HEHEHE-tag. Both variants, denoted Z(HER)?(:)???-H? and (HE)?-Z(HER)?(:)???, respectively, could be efficiently purified using IMAC and stably labeled with [??(m)Tc(CO)?](+) and were subsequently compared with the parental H?-Z(HER)?(:)??? having an N-terminal hexahistidine tag. All three variants were demonstrated to specifically bind to HER2-expressing cells in vitro. The hepatic accumulation of radioactivity in a murine model was 2-fold lower with [??(m)Tc(CO)?](+)-Z(HER2:342)-H? compared to [??(m)Tc(CO)?](+)-H?-Z(HER)?(:)???, and more than 10-fold lower with [??(m)Tc(CO)?](+)-(HE)?-Z(HER)?(:)???. These differences translated into appreciably superior tumor-to-liver ratio for [??(m)Tc(CO)?](+)-(HE)?-Z(HER)?(:)??? compared to the alternative conjugates. This information might be useful for development of other scaffold-based molecular imaging probes.     

A versatile method for preparation of hydrated microbial–latex biocatalytic coatings for gas absorption and gas evolution

We describe a latex wet coalescence method for gas-phase immobilization of microorganisms on paper which does not require drying for adhesion. This method reduces drying stresses to the microbes. It is applicable for microorganisms that do not tolerate desiccation stress during latex drying even in the presence of carbohydrates. Small surface area, 10-65?μm thick coatings were generated on chromatography paper strips and placed in the head-space of vertical sealed tubes containing liquid to hydrate the paper. These gas-phase microbial coatings hydrated by liquid in the paper pore space demonstrated absorption or evolution of H(2), CO, CO(2) or O(2). The microbial products produced, ethanol and acetate, diffuse into the hydrated paper pores and accumulate in the liquid at the bottom of the tube. The paper provides hydration to the back side of the coating and also separates the biocatalyst from the products. Coating reactivity was demonstrated for Chlamydomonas reinhardtii CC124, which consumed CO(2) and produced 10.2?±?0.2?mmol?O(2)?m(-2)?h(-1), Rhodopseudomonas palustris CGA009, which consumed acetate and produced 0.47?±?0.04?mmol?H(2)?m(-2)?h(-1), Clostridium ljungdahlii OTA1, which consumed 6?mmol CO?m(-2)?h(-1), and Synechococcus sp. PCC7002, which consumed CO(2) and produced 5.00?±?0.25?mmol O(2)?m(-2)?h(-1). Coating thickness and microstructure were related to microbe size as determined by digital micrometry, profilometry, and confocal microscopy. The immobilization of different microorganisms in thin adhesive films in the gas phase demonstrates the utility of this method for evaluating genetically optimized microorganisms for gas absorption and gas evolution.     

Dynamics of carbon monoxide recombination to fully reduced cytochrome c oxidase in plant mitochondria after low-temperature flash photolysis.

Rebinding of CO to reduced cytochrome c oxidase in plant mitochondria has been monitored optically at 590-630 nm after flash photolysis at low temperature from 160 to 200 K. (1) Under 100%-CO saturation, CO rebinding exhibits a four-step mechanism. The thermodynamic parameters of the first phase have been determined; its activation energy, Ea1, is 38.9 kJ.mol-1 and its enthalpy, delta H+/-1, and entropy, delta S+/-1, of activation are respectively 37.5 kJ.mol-1 and -75.8J.mol-1.K-1. (2) When the CO concentration is decreased to 0.2%, rebinding still occurs according to a four-step mechanism. The rate constant of the first phase is CO-concentration-independent. Under non-saturating conditions there is only one CO molecule per occupied site. The rebinding mechanism does not require additional CO molecules to be present in the haem pocket. (3) Dual-wavelength scanning experiments failed to detect optical forms correlated with the resolved phases. (4) Results are discussed with respect to previous work related to CO rebinding to mammalian cytochrome c oxidase and myoglobin.     

体外~(14)C-尿素呼气试验检测胃内幽门螺杆菌感染研究

目的　建立诊断胃内幽门螺杆菌感染 (Hp)的体外 1 4 C-尿素呼气试验 (1 4 C- U BT)。方法　 47例 Hp阳性和 32例 Hp阴性患者接受测试 ,用口服微量胃液采集胶囊的办法收集胃液标本于一 10 m l无菌试管内 ,加入生理盐水 0 .5 m l和 18.5 k Bq1 4 C-尿素后立即加橡皮塞密封试管 ,室温放置反应 3h,注射器经橡皮塞注入 2 M H2 SO41.0 ml,使 1 4 CO2 释出。同一注射器回抽气体并立即注入装有 6 .5 ml的 1 4 CO2 搜集闪烁剂液闪瓶内搜集 1 4 CO2 ,最后在液体闪烁计数仪上作 1 4 C放射性测定。结果　 47例 Hp阳性病人 1 4 C放射性几何均数为 5 30 dpm,而 32例 Hp阴性者结果为 2 1dpm,二者相差 2 3倍 (Wilcoxon秩和检验 ,u=5 .5 976 ,P<0 .0 1)。以受试者工作特征曲线分析法得出判别阈值为 75 dpm ,对 Hp诊断的敏感性和特异性为 92 %(4 3/ 47)和 91% (2 9/ 32 )。结论　体外 1 4 C- UBT诊断 Hp感染具有高度的准确性 ,无放射性损伤之虞 ,可适用于临床诊断。     

Specific binding of CO to tetraheme cytochrome c3

Carbon monoxide (CO) has been identified as another bioactive molecule like NO. Binding of CO to a tetraheme cytochrome c(3) (cyt c(3)) was investigated using visible absorption spectroscopy, circular dichroism (CD), and NMR. CO was found to bind to the four hemes in different manners. CD spectra, however, indicated that only single-site CO binding can keep the protein intact. The K(d) for the single-site binding was 8.0 microM, which is a typical value for a CO sensor protein. Furthermore, NMR spectra of uniformly (15)N-labeled and specifically [(15)N]His-labeled proteins have provided evidence that CO specifically binds to the sixth coordination site of heme 2 via single-site binding. The CO-bound cyt c(3) could conduct redox reactions. In light of triheme cytochrome c(7), the CO-bound cyt c(3) may work as an electron transporter. It was reported for sulfate-reducing bacteria that CO can be used as an energy source and CO cycling is operating like H(2) cycling. Therefore, the CO-bound cyt c(3) may play a role in maintaining electron transport pathways on accumulation of toxic CO for its utilization.     

Gas exchange in the filamentous cyanobacterium Nostoc punctiforme strain ATCC 29133 and Its hydrogenase-deficient mutant strain NHM5

Nostoc punctiforme ATCC 29133 is a nitrogen-fixing, heterocystous cyanobacterium of symbiotic origin. During nitrogen fixation, it produces molecular hydrogen (H(2)), which is recaptured by an uptake hydrogenase. Gas exchange in cultures of N. punctiforme ATCC 29133 and its hydrogenase-free mutant strain NHM5 was studied. Exchange of O(2), CO(2), N(2), and H(2) was followed simultaneously with a mass spectrometer in cultures grown under nitrogen-fixing conditions. Isotopic tracing was used to separate evolution and uptake of CO(2) and O(2). The amount of H(2) produced per molecule of N(2) fixed was found to vary with light conditions, high light giving a greater increase in H(2) production than N(2) fixation. The ratio under low light and high light was approximately 1.4 and 6.1 molecules of H(2) produced per molecule of N(2) fixed, respectively. Incubation under high light for a longer time, until the culture was depleted of CO(2), caused a decrease in the nitrogen fixation rate. At the same time, hydrogen production in the hydrogenase-deficient strain was increased from an initial rate of approximately 6 micro mol (mg of chlorophyll a)(-1) h(-1) to 9 micro mol (mg of chlorophyll a)(-1) h(-1) after about 50 min. A light-stimulated hydrogen-deuterium exchange activity stemming from the nitrogenase was observed in the two strains. The present findings are important for understanding this nitrogenase-based system, aiming at photobiological hydrogen production, as we have identified the conditions under which the energy flow through the nitrogenase can be directed towards hydrogen production rather than nitrogen fixation.