Infrared laser magnetic resonance spectroscopy of OD at 118.8, 96.5 and 215.4μ m

Zeeman spectral data are presented for the ²Π_3/2: J = _7/2 → J= _9/2,²Π_3/2: J= _7/2→²Π_1/2:J= _5/2 and²Π_3/2 J= _3/2→ J = _5/2 transitions in OD. Data for the ²Π_3/2. J=3/2→ J= 5/2 and ²Π_3/2 J= _5/2 → ²Π_l/2 : J= _3/2 transitions in OH, taken under similar conditions, are included.     

Fraction of excited-state oxygen formed as b Σg in solution-phase-photosensitized reactions II. Effects of sensitizer substituent

The fraction F_Σ of excited-state oxygen formed as b ¹Σ_g⁺ was determined for a series of triplet-state photosensitizers in CCl₄ solutions. F_Σ was determined by monitoring the intensities of (a) O₂(b ¹Σ_g⁺) fluorescence at 1926 nm (O₂(b ¹Σ_g⁺)→O₂(a ¹Δ_g) and (b) O₂(a ¹ Δ_g) phosphorescence at 1270 nm (O₂(a ¹Δ_g) → O₂(X³Σ_g⁻)). Oxygen excited states were formed by energy transfer from substituted benzophenones and acetophenones. The data indicate that F_Σ depends on several variables including the orbital configuration of the lowest triplet state and the triplet-state energy. The available data indicate that the sensitizer-oxygen charge transfer (CT) state is not likely to influence F_Σ strongly by CT-mediated mixing of various sensitizer-oxygen states.     

Ab initio CCSD(T) and MRD-CI study of excited states and the electronic spectrum of linear C5

Large-scale ab initio coupled cluster and multi-reference configuration interaction calculations (MRD-CI) are carried out to determine the equilibrium geometry and the vertical electronic spectrum of linear C₅⁺. Contrary to prior theoretical estimates we find three low-lying states within an energy range of 0.3 eV: ²Σ_u⁺, ²Σ_g⁺ and ²Π_g and a symmetric arrangement of nuclei. Transitions from ²Σ_u⁺ to these low-lying states are dipole-allowed; sizeable oscillator strengths are computed for the ²Π⁺_g←X²Σ_u⁺ transition at 2.62 eV and the ²Σ_g←X²Σ_u⁺ transition at 3.36 eV and should give a guide to spectroscopic identification of linear C₅⁺.     

THE DOSE RESPONSE CURVE IN PHYTOCHROME-MEDIATED ANTHOCYANIN SYNTHESIS IN THE MUSTARD SEEDLING

Abstract —The dose response curve for light (phytochrome)-induced anthocyanin synthesis was determined in the mustard seedling. The curve gives the amount of anthocyanin (A) synthesized within 24 h as a function of the amount of P_fr* produced by a brief light pulse. The [P_fr] response curve is composed of two linear parts with very different slopes ( a _1,2) connected by a relatively narrow transient range (curved segment). The [P_fr] response curve extrapolates precisely through zero [P_fr]. The reciprocity law is valid over the whole range investigated (up to 320 s of irradiation). It is concluded that the initial (or primary) reaction of P_fr (P_fr+ X → P_frX) does not involve any significant cooperativity in the case of phytochrome-mediated anthocyanin synthesis. It is speculated that the linear parts of the [P_fr] response curve truly reflect the mode of phytochrome action ( A = a _1,2 [P_fr]; X does not come into play since it is not rate limiting) whereas the curved segment represents a transition of the reaction matrix of P_fr. The large difference between a₁ and a₂ seems to indicate that the physiological effectiveness of a given amount of P_fr (or P_frX) is determined by [P_fr] through a P_fr-induced change in the reaction matrix.     

Exploiting the complementary nature of LC/MALDI/MS/MS and LC/ESI/MS/MS for increased proteome coverage

The goal of this work was to evaluate the improvement in proteome coverage of complex protein mixtures gained by analyzing samples using both LC/ESI/MS/MS and LC/MALDI/MS/MS. Parallel analyses of a single sample were accomplished by interfacing a Probot fractionation system with a nanoscale LC system. The Probot was configured to perform a post-column split such that a fraction (20%) of the column effluent was sent for on-line LC/ESI/MS/MS data acquisition, and the majority of the sample (80%) was mixed with a matrix solution and deposited onto the MALDI target plate. The split-flow approach takes advantage of the concentration sensitive nature of ESI and provides sufficient quantity of sample for MALDI/MS/MS. Hybrid quadrupole time-of-flight mass spectrometers were used to acquire LC/ESI/MS/MS data and LC/MALDI/MS/MS data from a tryptic digest of a preparation of mammalian mitochondrial ribosomes. The mass spectrometers were configured to operate in a data dependent acquisition mode in which precursor ions observed in MS survey scans are automatically selected for interrogation by MS/MS. This type of acquisition scheme maximizes the number of peptide fragmentation spectra obtained and is commonly referred to as shotgun analysis. While a significant degree of overlap (63%) was observed between the proteins identified in the LC/ESI/MS/MS and LC/MALDI/MS/MS data sets, both unique peptides and unique proteins were observed by each method. These results demonstrate that improved proteome coverage can be obtained using a combination of these ionization techniques.     

鳞状BiOBr/Bi2WO6的合成及其吸附性能

采用一步水热法成功制备鳞状形貌的BiOBr/Bi₂WO₆复合物,通过X射线衍射（XRD）仪、扫描电子显微镜（SEM）、N2吸附/解吸附比表面测定仪（BET）、傅里叶变换红外（FT-IR）光谱等对复合物进行了表征。对比Bi₂WO₆与BiOBr的SEM照片,结合KBr的浓度实验,提出了BiOBr/Bi₂WO₆的鳞状形貌的形成机理。选取有机染料为吸附质,BiOBr/Bi₂WO₆为吸附剂进行了复合物吸附性能测试。结果表明,BiOBr/Bi₂WO₆对阳离子染料表现出优越的吸附性能,10 min对次甲基蓝（MB）的吸附率高达99%,优于常规的活性炭吸附剂。此外,BiOBr/Bi₂WO₆对有机染料的吸附行为符合准二级反应速率方程和Freundlich等温吸附模型。     

Testing the uncertainty principle using (n,γ) photon beams and pulsed neutron beams

Nuclear resonance scattering of a photon beam based on the (n,γ) reaction was used for measuring the mean square zero-point linear momenta p_a² and p_c² of the atoms of a metallic Zn single crystal. A similar measurement was carried out using a pulsed neutron source. These were combined with corresponding values of x_a² and x_c² obtained using the Mössbauer effect. In both the cases the measured values of p_a² and p_c² were found to conform to the requirements of the Uncertainty principle for a real solid to within 3%.     

Photochemical Reactions Involved in the Phototoxicity of the Anticonvulsant and Antidepressant Drug Lamotrigine (Lamictal®)

Lamotrigine (LTG) [3,5-diamino-6-(2,3-dichlorophenyl)-1,2,4-triazine], an anticonvulsant and antidepressant drug Lamictal^®, produces a (photo)toxic response in some patients. LTG absorbs UV light, generating singlet oxygen (¹O₂) with a quantum yield of 0.22 in CH₂Cl₂, 0.11 in MeCN and 0.01 in D₂O. A small production of superoxide radical anion was also detected in acetonitrile. Thus, LTG is a moderate photosensitizer producing phototoxicity and oxidizing linoleic acid. LTG is a weak ¹O₂ quencher ( k _q = 3.2 × 10⁵  m ⁻¹ s⁻¹ in MeCN), but its photodecomposition products in dimethyl sulfoxide (DMSO) quenched ¹O₂ very efficiently. Upon intense UV irradiation from a xenon lamp, LTG was photobleached rapidly in DMSO and slowly in acetonitrile, alcohol and water. The rate increased significantly when laser pulses at 266 nm were employed. The photobleaching products generated ¹O₂ twice as strongly as LTG. Photobleaching was usually accompanied by the release of chloride anions, which increased in the presence of ascorbic acid. This suggests the formation of aryl radicals via dechlorination, a process which may be responsible for the photoallergic response observed in some patients. Our results demonstrate that LTG is a moderate generator of ¹O₂ prone to photodechlorination, especially in a reducing environment, which can contribute to the reported phototoxicity of LTG.     

Hartree-fock and Hückel-like orbital energies: an elementary extension to Koopmans‘ theorem

For a closed-shell MO configuration with 2n electrons which occupy n non-degenerate canonical MOs, it is deduced that the RHF energy, Σⁿ_i=1[2H⁰_n+Σⁿ_j-1(2J_ij-K_ij)], may be expressed in Hückel-like form as 2Σⁿ_i-1ε, −Σⁿ_i-1[j_i(λ+1)+1,(λ+2)] with λ=2(n-i). The l_i(λ+1) and I_i(λ+2) are the ionization potentials for the HOMO ψ, which arises after λ and λ+1 electrons have been successively removed from the initial configuration.     

Synthesis and characterisation of [(C5Me4R)2NbS2]2M complexes (M = Fe, Co; R = Me, Et) : organometallic tetrathiometalates with niobocene ligands

Irradiation of Cp₂^* Nb(η²---S₂)H (Cp^* = C₅Me₅) 1a in the presence of Fe(CO)₅ gives the CO-free complex [Cp₂^*NbS₂]₂Fe 2a. The core of 2a contains an FeS₄ tetrahedron which is ligated by two niobocene ligands as shown by X-ray diffraction analysis. In the reaction of 1a or Cp₂^xNb(η²---S₂)H (CP^x = C₅Me₄Et) 1b with Co₂(CO)₈, compounds 3a and 3b of the same type are formed. Electrochemical studies of 2a and 3a,b show that they undergo three reversible 1e⁻ steps. The oxidation of 3b exerts a considerable influence on its absorption spectrum. A qualitative EHMO analysis is in agreement with a strong delocalisation of electron density over the whole NbS₂MS₂Nb system.     

Influence de la structure cristalline sur la décomposition thermique des hydroxynitrates de métaux bivalents: Exemple des hydroxynitrates de cadmium

The solid solid equilibria in the binary system Ca₃(PO₄)₂-CaNaPO₄ have been studied. Different diagrams have been proposed for this system. The differences relate to the limits of the field of existence of a non-stoichiometric phase (phase A) stable at high temperature and undergoing eutectoid decomposition during cooling; they can be explained by the existence of two metastable equilibria diagrams which are superposed in the stable diagram. These metastabilities depend on both the cooling rates and the maximum temperatures reached before this cooling.

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Zusammenfassung Fest fest Gleichgewichte des binären Systems Ca₃(PO₄)₂-CaNaPO₄ wurden untersucht. Verschiedene Diagramme wurden für dieses System vorgeschlagen. Diese Unterschiede beziehen sich auf die Grenzen des Existenzbereiches einer nichtstöchiometrischen, hochtemperaturstabilen Phase (Phase A), die sich beim Abkühlen nach einer eutektoiden Reaktion zersetzt; sie können durch die Existenz von zwei dem stabilen Diagramm überlagerten metastabilen Gleichgewichtsdiagrammen erklärt werden. Diese metastabilen Zustände hängen sowohl von der Abkühlungsgeschwindigkeit als auch von den vor dem Abkühlen erreichten maximalen Temperaturen ab.

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Ca₃(PO₄)₂-CaNaPO₄ — . . / A/, , - , , . , , .

     

A PHYTOCHROME STUDY USING TWO-LASER/TWO-COLOR FLASH PHOTOLYSIS: I700 IS A MANDATORY INTERMEDIATE IN THE PrPfr PHOTOTRANSFORMATION

Abstract— The phototransformation of native (124 kDa)oat phytochrome, P_r P_fr, Has been studied at 10C by two laser/ two-color flash photolysis. the overall P_rP_fr reaction yield did not vary with temperature within the range4–21C. Foloeing the excitation of P_r with a single 15 ns laser flash at 650nm, the formation of P_fr was quantitavely measured in a time-resolved experiment in the presence of a second 8 ns laser flash at 710 nm delayed from the initial flash. the second laser flash causes at 1.0 s after the initial laser flash a depletion of the uintermediate I₇₀₀ as welll as a reduction of the P_fr absorption at 730 nm. The depletion of I₇₀₀ correlates quantitavely with the reduction of P_fr formation. The absorpton spectra of I₇₀₀ and of the following intermendiate, I_bi, were calculated assuming that the amount of P_r, which is photoconverted by a single laser, equals the amount of P_fr formed.     

Observation of textures of nematic polymers and estimation of the elastic constants

The texture of a copolyesteramide, Vectra® B950, has been studied by optical microscopy. At rest, the defects are typical of a biaxial nematic phase, but under the influence of a magnetic field or under shear, the nematic transforms into a uniaxial phase. The Freedericksz geometry yields a K₁ elastic constant of the order of 10^-8 N. The diffusivities K_III/_n and K_II/_n are obtained by measuring the light intensity transmitted through a sample during shear start-up and relaxation, and from this we estimate K_III ≅ 10 ^-9N and K_II ≅ 10 ^-10N. Since the biaxiality is small, these uniaxial constants adequately describe the phase at rest.     

一种新型比色荧光双通道水相检测氰根离子的化学传感器

合成了一种新型的,能在含水介质中比色荧光双通道单一选择性识别CN^-的传感器分子1-羟基萘甲叉酰肼乙基-3-羟基萘甲叉酰肼甲基苯并咪唑溴鎓盐(J1)。 在J1的DMSO/H₂O (体积比3:2)HEPES 的缓冲体系(pH=7.2)中分别加入F^-、Cl^-、Br^-、I^-、AcO^-、HSO₄^-、ClO₄^-、H₂PO₄^-、SCN^-和CN^-等阴离子后,只有CN^-的加入会使得溶液颜色发生明显的变化,由无色变为深黄色。 相应地在J1的DMSO/H₂O (体积比4:1)HEPES的缓冲体系(pH=7.2)中加入CN^-,溶液发出明亮的黄色荧光。 这一识别过程,不会受到其它阴离子的干扰。 紫外-可见光谱的最低检测限为1.57×10^-7 mol/L,检测线性范围为3.875×10^-4~2.15×10^-2 mol/L。 荧光光谱的最低检测限为4.63×10^-6 mol/L,检测线性范围为0.8×10^-4~1.60×10^-3 mol/L。 此结果表明,J1是一种良好的用于识别 CN^-的化学传感器,在含水介质中对CN^-具有选择性好、灵敏度高以及抗干扰性强的识别性能。 与此同时,基于J1对于CN^-的高选择性识别我们制备了CN^-的检测试纸,该试纸能够方便、快捷、准确地检测水中的CN^-。     

Induced smectic C* phases

Induced ferroelectric S*_C phases are formed by non-chiral S_C host phases doped with chiral dipolar guest molecules. In those mixtures the spontaneous polarization P_s and the tilt angle Θ has been investigated as a function of the mole fraction x_G of the chiral dopant. In most cases the reduced polarization P₀ = P_S/ sin Θ has been found to depend linearly on x_G. The polarization power which is defined by δ_P=(∂P₀/∂x_G)ΔT is discussed in terms of the molecular structure of the chiral dopants. There are systems in which P₀(x_G) deviates positively from linearity. This behaviour can be understood by considering a local field correction to P₀. By assuming a local field of Lorentz type a theoretical relation for P₀(x_G) has been derived which explains the experimental results. The effect of a local field is considerable if the transverse dipole moment and the polarizability of the chiral dopant are large.     

Self-termination rate of para-substituted benzyl radicals in aqueous solutions: a time-resolved study

The self-termination rates of the benzyl radical (C₆H₅---CH₂^√) and para-substituted benzyl radicals (X---C₆H₄---CH₂^√) were studied in aqueous solutions. The Arrhenius parameters and activation energies were determined in the temperature range 275.5–328 K. The kinetic activation energies of these radicals were close to the dynamic activation energy of the solvent, indicating that the termination rate is controlled by diffusion. The values for the rate constants (2k_t (10⁹ dm³ mol⁻¹ s⁻¹)) and the activation energies (E (kJ mol⁻¹)) were 5.94±0.52 and 14.69±0.61 for CH₃O---C₆H₄---CH₂^√, 4.52±0.2 and 17.65±1.16 for CH₃7z.sbnd;C₆H₄---CH₂^√, 3.07±0.45 and 17.58±0.97 for H---C₆H₄---CH₂^√, 4.13±0.81 and 19.10±1.20 for Cl---C₆H₄---CH₂^√ and 4.17±0.44 and 14.62±0.52 for NO₂---C₆H₄---CH₂^√.     

在TiO2纳米阵列上电沉积RuO2用于CO2电还原

传统上,RuO₂/TiO₂复合电极制备是通过在TiO₂/Ti基体上多次涂覆含Ru前驱体溶液和随后热分解（TD）来实现的. 为克服上述方法中Ru用量大和利用率低之不足, 本工作主要基于循环伏安法（CV）在TiO₂纳米管阵列（TNA）上电沉积RuO₂制备RuO₂^CV/TNA复合电极. SEM、GIXRD和CV结果表明, 电沉积的RuO₂为无定型结构, 所制备电极中的Ru用量约为传统的RuO₂^TD/TNA电极中Ru用量的1/30. 尽管两电极催化CO₂还原产物的法拉第效率接近, 但是RuO₂^CV/TNA电极比RuO₂^TD/TNA电极展示了更高的还原电流, 较正的初始还原电位和更好的稳定性. 与磷酸盐缓冲溶液中电还原CO₂相比,RuO₂^CV/TNA电极在0.1 mol•L^-1 KHCO₃中电还原CO₂除生成更高法拉第效率的甲酸根和甲烷外,还检测到CO的生成.     

Synthesis and thermal properties of mesomorphic 1,1'-bis[ω-(4'-cyano-4-biphenyloxy)alkyl] ferrocenes

A new series of 1,1'-disubstituted ferrocene compounds of the type [(η⁵-C₅H₄(CH₂)_nOC₆H₄C₆H₄CN]₂Fe (3a-d, n = 5, 6, 8, 11) incorporating a variable length alkyloxy cyanobiphenyl unit has been prepared and their mesomorphic properties have been investigated. Compounds 3b, c and d exhibit a thermotropic smectic C phase and 3c also exhibits a monotropic smectic A phase over a fairly wide range near ambient temperature.     

EFFECTS OF INTENSITY AND FLUENCE UPON DNA SINGLE-STRAND BREAKS INDUCED BY EXCIMER LASER RADIATION

Abstract— A Xenon-chloride excimer laser emitting energy at 308 nm was used to induce single-strand breaks (SSBs, frank breaks plus alkali-labile lesions as assayed by alkaline sucrose sedimentation techniques) in purified DNA from Bacillus subtilis . A fluence response study and a peak pulse intensity study were performed. At a pulse energy of 0.1 mJ/pulse, the radiation induced SSBs in a linear fashion (91 SSB/10⁸ Da per MJ/m²) to a maximum exprimental fluence of 1.28 MJ/m². The pulse intensity study showed that there were no significant changes in DNA breakage (105 SSB/10⁸ Da) between 2.93 times 10⁹ and 5.86 times 10¹¹ W/m² (0.11 and 22.0 mJ/pulse) at a constant total fluence of 1.1 MJ/m² (27000 mJ dose). This study has verified and extended previous work by quantifying the yield of SSBs induced in DNA by this laser radiation.     

Flow injection analysis methods for determination of diffusion coefficients

Two flow injection analyses (FIA) methods for the determination of diffusion coefficients in a straight single tube FIA system were developed. Based on the analytical solution of the convection-diffusion equation, linear relationships of the logarithmic values of the dispersion coefficient (D) and the half-peak width (W_1/2) with the diffusion coefficient (D_m) were obtained. Experiments were designed to verify these methods. For example, for potassium hexacyanoferrate (III) a D_m value of 0.72 × 10⁵ cm² s⁻¹ was found versus a literature value of 0.76 × 10⁵ cm² s⁻¹ (error, 5%). For potassium hexacyanoferrate (II) a D_m value of 0.67 × 10⁵ cm² s⁻¹ was obtained versus a literature value of 0.63 × 10⁵ cm² s⁻¹ (error, 6%). The diffusion coefficients of some important biomedical compounds, such as dopamine, epinephrine, norepinephrine and ascorbic acid, were then determined. The values of 10⁵ D_m/cm² s⁻¹ are 0.60 ± 0.03, 0.44 ± 0.02, 0.60 ± 0.01 and 0.68 ± 0.06, respectively.