A measurement of the proton structure function F2(x,Q2)

A measurement of the proton structure function F₂(x, Q²) is reported for momentum transfers squared Q² between 4.5 GeV² and 1600 GeV² and for Bjorken x between 1.8 × 10⁻¹⁴ and 0.13 using data collected by the HERA experiment H1 in 1993. It is observed that F₂ increases significantly with decreasing x, confirming our previous measurement made with one tenth of the data available in this analysis. The Q² dependence is approximately logarithmic over the full kinematic range covered. The subsample of deep inelastic events with a large pseudo-rapidity gap in the hadronic energy flow close to the proton remnant is used to measure the “diffractive” contribution to F₂.     

Model for the nucleon structure function F2(x,Q2)

A particular j-plane singularity, leading to long-range effects in hadron scattering, is attributed to hard constituent quark interactions. A definite prediction for the nucleon structure function, including scaling violations consistent with QCD. is obtained, which is confronted with the available data.     

The longitudinal structure function F L(x, Q 2) and the gluon distribution G(x, Q 2) at low x

We obtain a relation between the longitudinal structure function F _L(x, Q ²), F ₂(x, Q ²) and G(x, Q ²) at small x, using the formalism recently reported by one of the authors [2]. We also obtain a relation between F _L(x, Q ²), F ₂(x, Q ²) and its slope (dF ₂(x, Q ²))/(dlnQ ²). This provides us with the determination of the longitudinal structure function F _L(x, Q ²) from F ₂(x, Q ²) data and hence extract the gluon distribution G(x, Q ²).     

Defect-induced magnetic structure in (Ga(1)-(x)Mn(x))As

We show that magnetic structures involving partial disorder of local magnetic moments on the Mn atoms in (Ga(1)-(x)Mn(x))As lower the total energy, compared to the case of perfect ferromagnetic ordering, when As defects on the Ga sublattice are present. Such magnetic structures are found to be stable for a range of concentrations of As antisites, and this result accounts for the observed magnetic moments and critical temperatures in (Ga(1)-(x)Mn(x))As. We propose an explanation for the stabilization of the partially disordered magnetic structures and conclude that the magnetization and critical temperatures should increase substantially by reducing the number of As antisite defects.     

Optical spectroscopy and electronic structure of the GdCu x compounds (x = 1, 2, 5)

Physics of the Solid State - Optical properties of the GdCu, GdCu2, and GdCu5 compounds with various crystal lattices have been investigated using ellipsometry in a spectral range of 0.22–16...     

Jacobi polynomials and non-singlet structure function F2(x,Q2)up to N3LO

In this paper we present the non-singlet QCD analysis to determine valence quark distribution up to four loop.We obtain the fractional difference between the 4-loop and the 1-,2-and 3-loop presentations of xuv(x,Q2)and xdv(x,Q2).     

AlxOy(x=1—2,y=1—3)分子几何结构与稳定性的DFT研究

用密度泛函理论(DFT)的B31yp方法在6-311++g^水平上对Al_xO_y(x=1—2,y=2—3)分子的几何构型、电子结构、振动频率等性质进行了理论研究. 通过对基态结构的几何参数分析发现，它们的基态结构趋于直线或平面结构. 对基态结构的绝热电离能讨论表明，金属铝原子数一定时，氧原子数从1增加到3，其气态分子越来越稳定，铝原子数少的分子体系更稳定. 系统给出了该系列分子基态的几何参数、电子结构、光谱性质. Al₂O₃的C_2V三重态是该分子的能量最低结构. 关键词： xO_y分子')" href="#">Al_xO_y分子 密度泛函理论 结构与稳定性     

Ba(1-x)K(x)Mn2As2: an antiferromagnetic local-moment metal

The compound BaMn2As2 with the tetragonal ThCr2Si2 structure is a local-moment antiferromagnetic insulator with a Néel temperature T(N)=625 K and a large ordered moment μ=3.9μ(B)/Mn. We demonstrate that this compound can be driven metallic by partial substitution of Ba by K while retaining the same crystal and antiferromagnetic structures together with nearly the same high T(N) and large μ. Ba(1-x)K(x)Mn2As2 is thus the first metallic ThCr2Si2-type MAs-based system containing local 3d transition metal M magnetic moments, with consequences for the ongoing debate about the local-moment versus itinerant pictures of the FeAs-based superconductors and parent compounds. The Ba(1-x)K(x)Mn2As2 class of compounds also forms a bridge between the layered iron pnictides and cuprates and may be useful to test theories of high T(c) superconductivity.     

Magnetic ordering in FexMg1−xCl2, (x=0.55, x=0.45, x=0.30)

Mössbauer measurements on the diluted crystals Fe_xMg_1–xCl₂ show that fluctuating magnetic clusters are present. These can be related to the known spin-glass properties of these compounds. The fluctuating frequencies depend on temperature and the fluctuations can be suppressed by a sufficiently high external magnetic field     

Study of Disordered Fe2Cr(1−x)Mn x Al Alloys

Hyperfine Interactions - A series of ferromagnetic alloys Fe2Cr(1?x)Mn x Al were prepared by arc melting for x=0 to 0.05. The alloys are single phased, but disordered with B2 type structure....     

Thermodynamic properties of the mixed elpasolites Rb2KGaxSc1−x F6 (x=0.6–1.0)

Measurements of the heat capacity of the elpasolite Rb₂KGaF₆ and the solid solutions Rb₂KGa_xSc_1−x F₆ with a gallium content in the range x=0.6–0.95 are performed. The nature of the influence of the chemical composition of the compounds and the hydrostatic pressure on the temperature and entropy of the ferroelastic phase transitions is established. Fiz. Tverd. Tela (St. Petersburg) 39, 1844–1849 (October 1997)     

Nuclear structure of 18F: (V). A further study and summary of low-lying (2s, 1d)2 states

The 6164, 6284, 6310, 6383, 6480, 6777 and 6803 keV states have been studied via the capture reactions ¹⁴N(α, γ)¹⁸F and ¹⁷O(p, γ)¹⁸F. These studies yield respective assignments of J^πT = 3⁺(1), 2⁺(0+1), 3⁺(0), 2⁺(0+1), 3⁺(0), 4⁺(0) and 1⁺, 2 or 3⁺(0). Information on radiative widths, branching and multipole mixing ratios is reported. The 6164 and 6777 keV states are well described theoretically by simple $\text{(}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{s}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{)}{}_3{}^{\mathrm{+}}\text{and}\text{(}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{d}{}_{\mathrm{<mtext>3</mtext><mtext>2</mtext>}}{}_4{}^{\mathrm{+}}$ configurations, respectively. The 2⁺ states at 6284 and 6383 keV are mixed in isospin. A comparison of the observed properties with the available model calculations is presented for the above states as well as for some low-lying positive-parity states.     

La2/3Ca1/3Mn1-xCuxO3(x=4%)中的热弛豫现象

采用溶胶-凝胶法并经不同温度烧结而制备了名义组分为La2/3Ca1/3MnO3和La2/3Ca1/3Mn1-xCuxO3(x=4%)的系列样品,对它们进行了阻温关系测量.从试验结果观察到:在La2/3Ca1/3MnO3样品中,降温和升温测量的阻温曲线几乎完全重合,没有观察到明显的热弛豫现象.而在不同温度烧结的La2/3Ca1/3Mn1-xCuxO3(x=4%)样品中,阻温关系有明显的热弛豫现象.同时试验还观察到该热弛豫现象随样品烧结温度(颗粒尺寸)的增加逐渐消失.     

SiX2(X=H,F)分子的结构与势能函数

应用QCISD/6-311++G(3df,3pd)和B3P86/6-311++G(3d2f)对SiH2,SiF2的结构进行了优化,优化出SiH2分子的稳定构型为C2v,电子态为1A1,其平衡核间距Re=0.15149 nm、键角∠HSiH=92.5025°,离解能为3.7098 eV.SiF2分子的稳定构型为C2v,电子态为1A1,其平衡核间距Re=0.16014 nm、键角∠FSiF=100.7079°、离解能为14.1391eV.并对它们的力常数及谐振频率进行了进一步的计算.在推断出SiX2(X=H,F)的离解极限的基础上,应用多体展式理论方法,导出了基态SiX:(X=H,F)分子的解析势能函数,该势能表面准确地再现了SiX:(X=H,F)分子的结构特征和能量变化.分析讨论势能面的静态特征时得到SiH+H-SiH2反应中存在鞍点,活化能为192.971 kJ/mol,为有阈能的反应.而SiF+F→SiF2反应中没有鞍点,是无阈能的反应.     

Surface structure of TiO2(011)-(2x1)

A combined experimental and first principles study of the (2x1)-reconstructed rutile TiO2(011) surface is presented. Our results provide evidence that the surface structure is described by a model that includes onefold coordinated (titanyl) oxygen atoms giving rise to double bonded Ti=O species. These species should play a special role in the enhanced photocatalytic activity of the TiO2(011) surface.     

基态BBrx(x=0,-1,+1)分子离子的势能函数与稳定性

用原子分子反应静力学原理推导出了BBrx(x=0,-1,+1)分子离子的基态电子状态及其离解极限.在CC-PVDZ水平基础上,用B3LYP方法计算了BBrx(x=0,- 1,+1)分子离子的基态电子状态的平衡几何Re和离解能De分别为BBr+:0.176 6 nm、3.530 7 eV; BBr-:0.221 7 nm、1.500 0 eV,并在计算出来的一系列单点势能基础上,用正规方程组拟合Murrell-Sorbie(M-S)势能函数,得到相应态的解析势能函数,由此计算对应的光谱参数(Be、αe、ωe、ωeχe),计算结果分别为:BBr+:0.577cm -1、0.004 8 cm-1、932.513 0 cm-1和6.506 5 cm-1;BBr-:0. 360 2 cm-1、0.005 5 cm-1、348.428 3 cm-1和3.541 7 cm-1, 计算值与实验和文献值基本一致,计算表明BBrx(x=0,-1,+1)分子离子是可稳定存在的,其稳定性次序为BBr>BBr+>BBr-.     

A comparative study of magnetic and dielectric behaviors for La(1-x)Bi(x)Mn(1-y)Fe(y)O3 series (with x = 0.5, 0.7 and y = 0.3, 0.7)

We have carried out an extensive investigation into the effect of doping on both the A- and B-sites for the multiferroic La(0.5)Bi(0.5)Mn(0.5)Fe(0.5)O(3) in relation to its physical properties. The temperature dependent magnetization and dielectric response are determined for different percentages of Bi- and Fe-substitutions. For La(0.5)Bi(0.5)Mn(0.7)Fe(0.3)O(3), there is a prominent ferromagnetic transition T(C) around 110 K, whereas the other La(0.5)Bi(0.5)Mn(0.3)Fe(0.7)O(3) and La(0.3)Bi(0.7)Mn(0.3)Fe(0.7)O(3) phases fail to exhibit any clear transition. On the other hand, for the Fe-rich phases, the coercive field increases to 2450 Oe compared to 1720 Oe (for the Mn-rich phase). All the compositions exhibit coexistence of ferromagnetic and antiferromagnetic phases at low temperatures. The temperature dependent dielectric constant of the investigated samples varies from 32,000 to 500 at room temperature and the data has been analyzed using the universal dielectric response model.     

Local atomic structure of Cu(In x Ga1−x )Se2 (x = 0.25, 0.5, and 0.75) systems for solar cells

The local atomic structure of thin surface layers of crystalline quasi-binary Cu(In _x Ga_1?x )Se₂ solid solutions was studied by SIMS and EXAFS techniques. The SIMS method showed that the elemental composition of the sample changes most significantly in thin layers at a depth of 5–10 nm; in deeper layers, the component concentrations correspond to the bulk values. The EXAFS method in the x-ray fluorescence mode showed that the results obtained are in agreement with the assumption that quaternary crystalline quasi-binary Cu(In _x Ga_1?x )Se₂ solid solutions exhibit local disorder while average long-range order is detected from x-ray diffraction data.     

Al2Hx(x=1～3)分子团簇结构与光谱研究

用密度泛函理论(DFT)的B3LYP方法在6-311 g(d,p)水平上对Al2Hx(x=1~3)分子团簇的几何构型、电子结构、振动频率、垂直电离能和垂直电子亲和能等性质进行了理论研究.通过对基态结构的几何参数分析发现,它们的基态结构趋于对称性较高的构型.它们的基态结构为:Al2H(2A1)C2V,Al2H2(1Ag)D2h和Al2H3(2A′1)D3h.对基态结构的垂直电离能讨论表明,氢原子数从1增加到3,其气态分子越来越稳定.