Spin observables in small-angle elastic → d scattering with an L-type deuteron target at 800 MeV

We have measured spin correlation parameters that describe the elastic scattering of 800 MeV polarized protons from an L-type polarized deuteron target at laboratory angles below 20°. The measured parameters include the correlated analyzing powers A_SL, A_LL and A_NLL and the proton spin-transfer coefficients C_0L,S, C_0L,L, C_SL,N, C_NL,S, C_NL,L and C_LL,N. The results are compared with single-scattering predictions based on different phase-shift solutions for the nucleon-nucleon scattering matrix.     

Novel Peak Assignments of in VivoC MRS in Human Brain at 1.5 T

¹³C MRS studies at natural abundance and after intravenous 1-¹³C glucose infusion were performed on a 1.5-T clinical scanner in four subjects. Localization to the occipital cortex was achieved by a surface coil. In natural abundance spectra glucose C_3β,5β, myo-inositol, glutamate C_1,2,5, glutamine C_1,2,5, N-acetyl-aspartate C_1-4,C=O, creatine CH₂, CH₃, and C_C=N, taurine C_2,3, bicarbonate HCO⁻₃ were identified. After glucose infusion ¹³C enrichment of glucose C_1α,1β, glutamate C_1-4, glutamine C_1-4, aspartate C_2,3, N-acetyl-aspartate C_2,3, lactate C₃, alanine C₃, and HCO⁻₃ were observed. The observation of ¹³C enrichment of resonances resonating at >150 ppm is an extension of previously published studies and will provide a more precise determination of metabolic rates and substrate decarboxylation in human brain.     

First-principles study of structural and elastic properties of CrO2 at high pressure

The structural and elastic properties of CrO₂ in the rutile phase under high pressures have been investigated using pseudopotential plane-wave method based on density functional theory. The optimized lattice parameters and the bulk modulus at zero pressure agree well with available experimental and theoretical data. The elastic constants C ₁₁, C ₁₂, C ₄₄, C ₃₃, C ₁₃, and C ₆₆ at zero pressure are calculated to be 359.91, 264.69, 143.28, 309.45, 218.45, and 260.74 GPa, respectively. Elastic constants, bulk modulus, shear modulus, Young's modulus, and Poisson's ratio under pressures are obtained. Our results indicate that the rutile phase is mechanically stable below 11.99 GPa. The elastic anisotropy of rutile phase under pressures has also been predicted.     

A note on the elastic constants of sodium bromate from 350 K to 77 K

The elastic constantsC ₁₁,C ₁₂ andC ₄₄ of sodium bromate single crystals have been evaluated using 10 MHz ultrasonic pulse echo superposition technique. The values areC ₁₁=5.57₈,C ₁₂=1.07₅,C ₄₄=1.51₀ (×10¹⁰ N/m²) at 290 K and 6.35, 1.98 and 1.65 (×10¹⁰ N/m²) at 77 K. The present room temperature values agree closely with the recent values of Gluyaset al. but the other earlier measurements show some scatter. A comparison between the elastic constants of sodium bromate and sodium chlorate is also made.     

压力及杂质氢对金属锂弹性特性的影响

针对六角密堆金属锂16个原子超晶胞(supercell)、填隙一个氢原子的周期单元，采用基于密度泛函理论的平面波-赝势方法，研究了零温条件下压力及填隙氢掺杂对体系弹性性质的影响.结果表明氢掺杂导致体系的体模量增加.常压下掺杂体系的弹性常数C₁₁，C₃₃，C₆₆和C₁₂高于单质体系，剪切模量C₄₄有所下降，而C₁₃则与单质体系持平.压力作用下C₁₁，C₃₃和C₆₆一直大于单质体系，但C₁₂的值低于单质体系.在2GPa—4GPa压力区间内，弹性常数C₁₃呈反常变化，小于单质体系；在高压区掺杂体系的C₄₄和C₁₃则高于单质体系的相应量值，压力导致掺杂体系和单质体系之间剪切模的偏离加剧.掺杂体系在压力作用下依然保持压缩模的各向同性，具有和单质体系相似的特性. 关键词： 第一性原理 压力效应 弹性常数 金属锂     

A study of molecular reorientation in a series of liquid n-alkanes using light-scattering spectroscopy

The spectra of the depolarized (VH) light scattered from the n-alkanes C₆H₁₄, C₈H₁₈, C₁₀H₂₂, C₁₂H₂₆, C₁₄H₃₀, C₁₅H₃₂ and C₁₆H₃₄ have been measured using a high resolution piezo-electrically scanned Fabry-Perot interferometer. The values of the molecular relaxation times τ _s derived from the spectra are compared with relaxation times τ _f derived from flow birefringence. The experimental results are discussed in terms of a phenomenological activation energy and also in terms of the coupling between the molecular reorientation and the hydrodynamic shear modes, allowing estimates of the strength of the coupling between these modes to be made.     

Zeeman spectroscopy of the 4 Eu → 2 B 1g phosphorescence of copper porphin in an n-alkane single crystal

The phosphorescence spectrum of the metastable ⁴ E_u state of copper porphin in single crystals of n-octane (C₈) and n-decane (C₁₀) has been studied between 2·3 and 35 K, with and without a magnetic field B. The crystal field splitting between the orbital components observed at 35 K is δ = 30·3 ± 0·3 (C₈), 13·8 ± 0·2 cm^-1 (C₁₀). From the Zeeman shifts we derive the effective orbital angular momentum Λ′ = 0·8 ± 0·2 (C₁₀), the spin-orbit coupling parameter |Z′| = 1·5 ± 1·0 cm^-1 (C₁₀), the spin-spin dipolar interaction parameters D = -0·1 ± 0·2 cm^-1 (C₈, C₁₀) and |E| = 0·31 ± 0·03 cm^-1 (C₈, C₁₀), and the g-factors g _∥ = 2·14 ± 0·04 (C₈, C₁₀) and g _⊥ = 2·00 ± 0·03 (C₈, C₁₀).     

Relaxation intensity in some polyacrylates

Empirical formula suggested by Kita and Koizumi for evaluation of relaxation intensity in a limited range of frequency around the relaxation frequency for the Cole-Cole type distribution has been tested for poly butyl acrylate (PBA), Poly butyl methacrylate (PBMA) and poly isobutyl methacrylate (PiBMA). The relaxation intensity Δε is expressed in terms ofε″ _M , the dielectric loss maxima andW, the frequency separation for half, two thirds or three quarters ofε″ _M , in the form Δε=ε″ _M /[(C ₁/W)+C ₂+C ₃ W], where the numerical constantsC ₁,C ₂,C ₃ are given for the respective type of relaxation.     

Equilibrium composition and the effective adiabatic exponent of a clustering carbon plasma

The equilibrium composition and the effective adiabatic exponent of a low-temperature carbon plasma containing eight components (C, C₂, C₃, C₄, C₅, C⁺, C₂⁺, and e) are calculated. The temperature and pressure ranges are found in which polyatomic clusters form in a gas flow. It is shown that the effective adiabatic exponent of the carbon plasma is a nonmonotonic function of temperature. In the parameter range where the plasma consists largely of polyatomic clusters, the adiabatic exponent is close to unity. It is noted that anomalously low values of the effective adiabatic exponent indicate a considerable concentration of polyatomic molecules in the plasma jet. Such values can be observed in experiments with a low-temperature carbon plasma flowing about bodies.     

Dynamics of the first-order magnetostructural transition in Gd<Subscript>5</Subscript>(Si<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>Ge<Subscript>1-<Emphasis Type="Italic">x</Emphasis></Subscript>)<Subscript>4</Subscript>

For a given crystal structure, say body-centred-cubic, the many-body Hamiltonian H in which nuclear and electron motions are to be treated from the outset on the same footing, has parameters, for the elements, which can be classified as (i) atomic mass M, (ii) atomic number Z, characterizing the external potential in which electrons move, and (iii) bcc lattice spacing, or equivalently one can utilize atomic volume, . Since the thermodynamic quantities can be determined from H, we conclude that T _c , the superconducting transition temperature, when it is non-zero, may be formally expressed as T _c = . One piece of evidence in support is that, in an atomic number vs. atomic volume graph, the superconducting elements lie in a well defined region. Two other relevant points are that (a) T _c is related by BCS theory, though not simply, to the Debye temperature, which in turn is calculable from the elastic constants C ₁₁, C ₁₂, and C ₄₄, the atomic weight and the atomic volume, and (b) T _c for five bcc transition metals is linear in the Cauchy deviation C ^* = (C ₁₂ - C ₄₄ )/(C ₁₂ + C ₄₄ ). Finally, via elastic constants, mass density and atomic volume, a correlation between C ^* and the Debye temperature is established for the five bcc transition elements.Received: 13 May 2004, Published online: 23 July 2004PACS: 74.62.-c Transition temperature variations - 74.70.Ad Metals; alloys and binary compounds     

Coupled cluster calculations for the interstellar molecule HC3NH+

An accurate equilibrium structure has been established for the linear interstellar molecular cation HC₃NH⁺: r _1e(CH) = 1.0703Å, R _1e(C₍₁₎C₍₂₎) = 1.2097 Å, R _2e(C₍₂₎C₍₃₎) = 1.3509Å, R _3e(C₍₃₎N) = 1.1448 Å and r _2e(NH) = 1.0079Å. Ground-state rotational constants for less abundant isotopomers are predicted with an uncertainty of about 0.02 MHz. The equilibrium dipole moment of HC₃NH⁺ is calculated to be 1.61 D.     

First principle calculation of elastic and thermodynamic properties of stishovite

Using ab initio plane-wave pseudo-potential density functional theory method,the elastic constants and band structures of stishovite were calculated.The calculated elastic constants under ambient conditions agree well with previous experimental and theoretical data.C13,C33,C44,and C66 increase nearly linearly with pressure while C 11 and C 12 show irregularly changes with pressure over 20 GPa.The shear modulus(C11-C12)/2 was observed to decrease drastically between 40 GPa and 50 GPa,indicating acoustic mode softening in consistency with the phase transition to CaCl 2-type structure around 50 GPa.The calculated band structures show no obvious difference at 0 and 80 GPa,being consistent with the high incompressibility of stishovite.With a quasi-harmonic Debye model,thermodynamic properties of stishovite were also calculated and the results are in good agreement with available experimental data.     

Structures and stabilities of CBHz (z ≤ 8) and CxB3-xHz (x = 1, 2, z ≤ 14): prediction of novel organo-boron radicals

Hydrogenated boron-carbon clusters, i.e. organo-borons, have received considerable attention both theoretically and experimentally. Herein, using a topology searching strategy, we systematically explore the structures and stabilities of small organo-borons with CBH_z (z ≤ 8) and C_xB_3-xH_z (x = 1, 2,z≤ 14) stoichiometry, with particular interests in the intrinsic stabilities of the organo-boron radicals. At the CCSD(T)/aug-cc-pVQZ//B3LYP/aug-cc-pVTZ and CCSD(T)/aug-cc-pVQZ//MP2/aug-cc-pVTZ levels, the stabilities of these global minimum organo-boron species were evaluated by considering dissociation pathways and the binding energy per atom. Aside from the five already studied radicals (CBH₂, CBH₄, C₂BH₂, C₂BH₄ and CB₂H₃), we predict six novel radicals, i.e. CBH₆, C₂BH₆, C₂BH₈, CB₂H, CB₂H₅ and CB₂H₇, which could be detected under suitable circumstances. However, observation of the highly hydrogenated CB₂H₉ radical is much less likely due to its minute stability towards H-extrusion. The computationally determined stable/meta-stable maximum hydrogenation numbers for CB, C₂B and CB₂ (6, 8 and 8, respectively) are in excellent agreement with a simple electron-counting model for C_xB_y chains. The newly predicted organo-boron radicals await future laboratory verification.     

Ab initio prediction of the infrared absorption spectrum of the C2Br radical

The first three electronic states of the C₂Br radical, correlating at linear geometries with ²Σ⁺ and ²Π states, have been studied ab initio, using Multi Reference Configuration Interaction techniques. The electronic ground state is found to have a bent equilibrium geometry, RCC=1.2621Å, R _CBr=1.7967Å, ∠ CCBr=156.1°, with a very low barrier to linearity. Similarly to the valence isoelectronic radicals C₂F and C₂Cl, this anomalous behaviour is attributed to a strong three-state non-adiabatic electronic interaction. The Σ ,Π_1/2,Π_3/2 vibronic energy levels and their absolute infrared absorption intensities at a temperature of 5 K have been calculated for the ¹² C¹² C⁷⁹Br isotopomer, to an upper limit of 2000 cm^?1, using ab initio diabatic potential energy and dipole moment surfaces and a recently developed variational method.     

Long-range interaction between hydrogen atoms: estimate of third-order contributions

Third-order long-range coefficients C ₁₁, C ₁₃, C ₁₅ for two hydrogen atoms in their ground states are evaluated by perturbation-variation methods in terms of finite basis sets of Slater-type orbitals. Some tests for the accuracy of the variational solutions are proposed and discussed.     

One-dimensional Anderson model with dichotomic correlation in the presence of external electric field

A one-dimensional diagonal tight binding electronic system with dichotomic correlated disorder in the presence of external d.c field is investigated. It is found numerically that the conductance distribution obeys fairly well to log-normal distribution in weak disorder strength in localized regime, which indicates validity of single parameter scaling theory in this limit. Contrary to the universal cumulant relation C ₁ = 2C ₂ in the absence of d.c. field, we demonstrated numerically that C ₁ ≫ 2C ₂ in the presence of the field in localized regime. We interpret this result as suppression of the fluctuation effects by the external field. In addition, it is obtained that the quantity NF _c , here N is the system size and F _c is the crossover field, decreases as the as the system energy E increases. Moreover, we find numerically a simple linear relation between the average logarithm of the conductance 〈ln(g)〉 and the field strength as 〈ln(g)〉 = C(N, λ)F, here C(N, λ) is a constant for particular values of N and λ, which is the Poisson parameter of the dichotomic process.     

Uncoupled Hartree-Fock calculations of the 13C shielding by means of ab initio and NEMO-wavefunctions

¹³C shielding constants of some molecules are approximatively evaluated by decoupling the equations of the single excitation scheme of Caves and Karplus. The ab initio minimal basis wavefunctions of Palke and Lipscomb of CH₄, C₂H₂, C₂H₄, C₂H₆, HCN and NEMO-wavefunctions are used. It is shown that for the molecules under study these UPHF calculations reveal the same trends as the finite perturbation method by Ditchfield et al.     

13C-NMR Spectroscopy of para-Substituted Benzylideneacetones.: I. Long Distance Electronic Effects

para-benzylideneacetones present a characteristic long distance charge transfer pattern, where the olefinic bridge (CH=CH) and the aromatic ring (Ph) carbon centers are perturbed according to the nature of the para-substituent groups.

By means of ¹³C-NMR spectroscopy and AMl molecular orbital calculations we have found that in this molecular series the chemical shifts (Δ) and the charge densities (qAMI) corresponding to the C₃, C₁ and C_β centers follow a functional dependence of the type: Δ = a qAMl + Δ°, while C₂, C_α and C_CO are practically constants.

On the other hand, after a complete spectral assignment of the ¹³C-NMR signals, an analysis of the electron-donor substituent effect at the para-position of the aromatic carbonyl compounds on the C₄ center, has permitted us to find a good correlation between the C₄ spectral shift and the electronegativity of this vicinal center.     

富勒烯衍生物C60（CF3）n（n=2，4，6，10）几何结构和电子性质变化规律的密度泛函研究

采用密度泛函理论中的广义梯度近似对C₆₀（CF₃）_n （n=2,4,6,10）几何结构和电子性质的变化规律进行了计算研究.发现在C₆₀（CF₃）₄可能稳定存在的三种同分异构体中,具有p p p加成方式的衍生物热力学性质最为稳定;在C₆₀（CF₃）₆可能稳定存在的三种同分异构体中,具有p p p m p加成方式的衍生物热力学性质最为稳定.对C₆₀（CF₃）₂,C₆₀（CF₃）₄,C₆₀（CF₃）₆和C₆₀（CF₃）₁₀四种加成衍生物的几何结构分析可知：随着CF₃加成个数的增加,C₆₀中的C—C平均键长逐渐变大,笼子与CF₃之间连接键C_C60—C_CF3逐渐变大.对它们的电子结构分析可知,随着CF₃加成数目的增多,反应热几乎是线性增加.而C₆₀（CF₃）_n（n=2,4,6,10）分子的平均反应热在n=6处为极大值,说明C₆₀（CF₃）₆应该是最容易得到的加成产物.由Mulliken电荷可知,加成的CF₃个数越多,CF₃与笼子的相互作用也就越强,每个CF₃转移到笼子上电荷数也就越多.C₆₀（CF₃）_n的自旋聚居数分布表明它们均为闭壳层结构.最后,从CF₃对分子的前线轨道贡献可知,四种分子的得电子情况和失电子情况均发生在碳笼本身,并不随着CF₃个数的增加而发生明显的改变. 关键词： 60（CF₃）_n （n=2')" href="#">C₆₀（CF₃）_n （n=2 10） 几何结构和电子性质 密度泛函     

Fluorescence Spectrometric Studies on the Binding of an Amino-Functionalized Ionic Liquid to Cytochrome c

The interaction of an amino-functionalized ionic liquid, 1-(2-aminoethyl)-3-butylimidazolium bromide ([NH₂C₂C₄im]Br), with cytochrome c (cyt c) at pH 7.4 was investigated using fluorescence and UV-Vis absorption spectroscopic techniques. From the experimental results, it is found that cyt c has a strong ability to quench the intrinsic fluorescence of [NH₂C₂C₄im]Br and the quenching mechanism is considered as a static quenching process. The binding constants and the number of binding sites (n) were calculated at different temperatures. The thermodynamic parameters such as free energy change (ΔG), enthalpy change (ΔH), and entropy change (ΔS) were calculated by thermodynamic equations. According to the results, the values of ΔG, ΔH, and ΔS are all negative, suggesting that interaction between [NH₂C₂C₄im]Br and cyt c is spontaneous and mainly driven by hydrogen bonding and van der Waals forces.