关于K+介子和核子的弹性散射

本文用塔姆-唐可夫近似解K⁺介子和核子的弹性散射问题,得到了K介子实验室动能400Mev以下的相移截面和能量的关系,并和实验及前人的理论结果作了比较。计算中较严格考虑了核子反冲效应,指出了在考虑了反冲效应后能使理论曲线在高能端更与实验曲线接近。同时就Λ-K和∑-K的各种可能的宇称情况进行了分析,排斥了相对宇称皆正的可能,并指出Λ-K和∑-K的相对宇称选取不同的符号和二者皆取负号一样,能符合K⁺-p散射实验,但在分析K⁺-n散射时仍遇到困难。     

论反常作用、轻子结构和μ-e质量差

本文提出了反常作用的μ荷观点,μ荷不仅是一种反映μ-e禁戒性的量子数,而且是反常作用的承担者。在此观点下,讨论了轻子结构和μ-e质量差,得到了关于轻子结构的一些普遍定理。例如,证明了电子的反常作用和电磁作用形状因子相同等。在讨论轻子结构的基础上,得到了将μ-e质量差和轻子的电磁结构相联系的公式,证明了主要由于电磁作用干涉产生的μ荷-μ矩作用是反常作用自能的主要部分,它是负值,故是电子参与反常作用。利用电子的电磁结构数据能合理地解释μ-e质量差,而后者也提供了有关电子电磁结构的进一步知识。     

中间玻色子理论Ⅱ.超子的非轻子衰变

本文用中间玻色子理论,讨论了超子的非轻子衰变,考虑了各种衰变机构,解释了FMS极点,建立了李氏和则的更广泛的动力学基础,并求得了和实验大致相符的衰变率和不对称系数。     

MEASUREMENTS OF NUMBER OF RADIOACTIVE ATOMS AND HALF-LIFE(Ⅲ)

The present paper examines theoretically the way of reducing tha errors introducedby the inaccuracy of the decay constant and measuring statistics in the determinationof the number of the radioactive atoms. It was discovered that the "front-back sym-metrical measurements with life-time as center" (FBSLC) may fulfil this reguirement.Even if the error of the decay constant reaches ±10%, the error introdnced by theinaccuracy of decay constant of the number of the radioactive atoms at zero time cal-culated from the radioactivities measured at zero time and two life-times by takingaverage will still be smaller than 0.1%. Experimental data of ^99mTc radioactive decaywithin measuring statistics verified the above theoretical prediction. Therefore, by FBSLC with measuring time as early as possible, it is possible toreduce the errors introduced by inaccuracy of the decay constant and measuring sta-tistics, so that the results of the absolute measurements may be more accurate.     

高层建筑火灾安全评价的模糊最优归类模型

将模糊数学中的综合评判模型、最优归类模型与高层建筑中对火灾风险有影响的因子相结合，建立了高层建筑火灾风险评价的模糊最优归类模型。并对高层建筑火灾风险评价进行了实例分析。     

The Shallow Arch—General Buckling,Postbuckling, and Imperfection Analysis∗

A general discussion of the behavior of the shallow circular arch is presented. It is shown that, irrespective of specific loading or boundary conditions, it is possible to arrive at general conclusions regarding buckling, postbuckling, and imperfection sensitivity. General methods of analysis are established which lead to the determination of points of bifurcation and of postbuckling paths under symmetric loads. Modifications accounting for antisymmetric load components are introduced, with special emphasis on their asymptotic and limit load effect.

A typical numerical example is carried through in detail. The solution is “exact” in the sense of shallow arch theory. Its asymptotic behavior conforms to the asymptotic theory of Koiter.     

稀土对水泥熟料烧成的矿化作用机理

利用SEM—EDS分析了稀土氧化物在熟料中的分布并结合熟料的岩相分析初步探讨了稀土对水泥熟料烧成的矿化作用机理。研究结果表明,稀土元素La和Y在熟料煅烧过程中更多地分布在硅酸盐相中,同时增加了溶剂型氧化物（Al2O3、Fe2O3）在A矿中的固溶量;稀土离子的掺杂引起微观介质应力场发生畸变,增加结构中的空位缺陷,降低扩散活化能,从而提高质点的扩散速度,促进了C3S矿物的形成。     

陶瓷材料三点及四点弯曲断裂强度关系之讨论

利用Katayama在一种Si断裂强度; 弯曲试验; 加载因子; Weibull模量fracture strength, bending test, load factor, Weibull modulus2002年6月25日2003-12-10 利用Katayama在一种Si断裂强度; 弯曲试验; 加载因子; Weibull模量fracture strength, bending test, load factor, Weibull modulus2002年6月25日2003-12-10利用Katayama在一种Si3N4陶瓷得到的实验数据,考察了一条关联陶瓷材料三点及四点弯曲断裂强度的式子,其准确度较好,简要地导出了一般教材上较少提及其推导的四点弯曲加载因子。     

1H NMR Detection of superparamagnetic nanoparticles at 1T using a microcoil and novel tuning circuit

Magnetic beads containing superparamagnetic iron oxide nanoparticles (SPIONs) have been shown to measurably change the nuclear magnetic resonance (NMR) relaxation properties of nearby protons in aqueous solution at distances up to approximately 50 microm. Therefore, the NMR sensitivity for the in vitro detection of single cells or biomolecules labeled with magnetic beads will be maximized with microcoils of this dimension. We have constructed a prototype 550 microm diameter solenoidal microcoil using focused gallium ion milling of a gold/chromium layer. The NMR coil was brought to resonance by means of a novel auxiliary tuning circuit, and used to detect water with a spectral resolution of 2.5 Hz in a 1.04 T (44.2MHz) permanent magnet. The single-scan SNR for water was 137, for a 200 micros pi/2 pulse produced with an RF power of 0.25 mW. The nutation performance of the microcoil was sufficiently good so that the effects of magnetic beads on the relaxation characteristics of the surrounding water could be accurately measured. A solution of magnetic beads (Dynabeads MyOne Streptavidin) in deionized water at a concentration of 1000 beads per nL lowered the T(1) from 1.0 to 0.64 s and the T2 * from 110 to 0.91 ms. Lower concentrations (100 and 10 beads/nL) also resulted in measurable reductions in T2 *, suggesting that low-field, microcoil NMR detection using permanent magnets can serve as a high-sensitivity, miniaturizable detection mechanism for very low concentrations of magnetic beads in biological fluids.     

Temperature Dependence Kinetic Studies of the Reaction of O(3P) with CHI3 and C2H5I and the 298 K Reaction of OH(X2Π) with CHI3

A flash photolysis–resonance fluorescence technique was used to investigate the kinetics of the OH(X²Π) radical and O(³P) atom‐initiated reactions with CHI₃ and the kinetics of the O(³P) atom‐initiated reaction with C₂H₅I. The reactions of the O(³P) atom with CHI₃ and C₂H₅I were studied over the temperature range of 296 to 373 K in 14 Torr of helium, and the reaction of the OH (X²Π) radical with CHI₃ was studied at T = 298 K in 186 Torr of helium. The experiments involved time‐resolved resonance fluorescence detection of OH (A²Σ⁺ → X²Π transition at λ = 308 nm) and of O(³P) (λ = 130.2, 130.5, and 130.6 nm) following flash photolysis of the H₂O/He, H₂O/CHI₃/He, O₃/He, and O₃/C₂H₅I/He mixtures. A xenon vacuum UV (VUV) flash lamp (λ > 120 nm) served as a photolysis light source. The OH radicals were produced by the VUV flash photolysis of water, and the O(³P) atoms were produced by the VUV flash photolysis of ozone. Decays of OH radicals and O(³P) atoms in the presence of CHI₃ and C₂H₅I were observed to be exponential, and the decay rates were found to be linearly dependent on the CHI₃ and C₂H₅I concentrations. Measured rate coefficients for the reaction of O(³P) atoms with CHI₃ and C₂H₅I are described by the following Arrhenius expressions (units are cm³ s^?1): k_O+C2H5I(T) = (17.2 ± 7.4) × 10^?12 exp[?(190 ± 140)K/T] and k_O+CHI3(T) = (1.80 ± 2.70) × 10^?12 exp[?(440 ± 500)K/T]; the 298 K rate coefficient for the reaction of the OH radical with CHI₃ is k_OH+CHI3(298 K) = (1.65 ± 0.06) × 10^?11 cm³ s^?1. The listed uncertainty values of the Arrhenius parameters are 2σ‐standard errors of the calculated slopes by linear regression.