空调制冷专业实验室建设探索

结合高等职业教育空调制冷专业实验室建设的实际情况,阐述了建设制冷专业实验室的必要性;根据制冷专业的特点和人才培养目标,分析了现有制冷专业实验室存在的一些问题,提出了具有建设性的意见;并对实验室进一步建设提出了规划方案,同时对现有的专业实验室提出了改进措施。     

国际地下实验室发展综述

地下实验室是开展粒子物理学、天体物理学及宇宙学等领域一些重大基础性前沿课题的重要研究场所和良好的低本底环境,建设和发展地下实验室对于一个国家的基础科学研究具有重要科学意义.目前,国际上许多国家都已经建立起地下实验室,而中国一直没有很好的地下实验室,特别是极深地下实验室.2009年,清华大学与二滩水电开发有限责任公司开展战略合作,利用锦屏山隧道建立中国首个世界最深的地下实验室--中国锦屏地下实验室(China Jinping Underground Laboratory,CJPL),并于2010年12月12日正式启用.中国锦屏地下实验室的建成,标志着中国已经具备开展物理学重大基础前沿科学研究的自主地下实验平台,对于推动我国相关领域的重大基础前沿课题的自主研究意义重大.文章对国际上一些重要地下实验室的情况进行了介绍,并对中国锦屏地下实验室的基本情况进行了介绍.     

公共计算机实验室的组建与管理

计算机在各高校已相当普及,为了满足计算机实验教学的需要,各种类型的机房建设发展很快。根据计算机公共基础实验室的当前基本情况和需求,本文分析了在实验室的组建技术、日常管理与维护中常见问题,并给出解决办法。具体描述了实验室布局设置、设备需求、布线、软硬件安装等组建技术。科学地管理好高校计算机实验室,可以提高设备利用率和延长设备的使用寿命,分别从实验室制度、实验教师与管理人员的协调、应用实验室开放的管理系统软件等角度来提升日常管理水平,并通过网络还原卡的网络对拷来改善系统维护。     

注重特色与创新,建设具有海洋院校特色的物理实验室

实验室在建设与管理的过程中,仅注重设备的先进性和功能室的数量是不够的,还要注重建设与管理理念的准确定位。我校物理实验室以正确合理的理念为指导,注重特色,敢于创新,使实验室的建设与管理与我校具体实际情况相适应,取得了突出的成绩。     

轻量级光电实验室综合管理系统的设计与实现

针对当前光电实验室数据繁多且结构复杂的实际情况,本文利用数据库等技术设计了一套针对于大型光电实验室综合管理系统的框架和数据结构,并最终实现该系统。该系统能够对光电实验室的实验数据进行有效的组织、管理和应用,能够对实验设备进行管理和统计,该系统设计有完善的架构体系,并有预留接口,为系统的升级和功能的添加提供了便利。光电实验室综合管理系统可以使实验室人员科学合理地安排实验,减少实验次数、缩短实验周期,更好的利用现有实验数据,从而减少资源的浪费,实现实验室数据资源有效而经济的管理。同时,通过对设备信息的管理可以提高设备的利用率,进而优化实验室的资源配置。     

普通高中物理开放性实验室建设的思考

《普通高中物理课程标准》“实施建议”中,关于“建立开放性实验室”的内容中提到,学校和教师应根据课程标准的要求安排足够的学生实验和演示实验;应最大限度地利用实验室现有的器材,力求利用多年闲置的器材开发新的实验;充分地开发和利用实验室的丰富课程资源,尽快改变实验室的封闭式管理状态,实验室应该尽快向学生开放,鼓励学生主动做课外实验．课程标准颁布至今,而开放性实验室建设情况如何,值得我们思索．本文就普通高中物理开放性实验室建设谈几点看法．     

美国斯坦福大学和加州大学伯克利分校物理实验教学介绍

介绍了美国斯坦福大学和加州大学伯克利分校大学物理实验教学情况、实验特点、实验课程设置和实验室管理,讲述了访问学习后的收获和体会.     

物理实验大平台建设实践与思考

本文介绍了中国石油大学(华东)物理实验教学中心开展物理实验大平台建设与实践情况。物理实验大平台建设以"整体规划、统一建设、集中管理、资源共享、促进创新"为指导思想,构建"一个中心,两个平台、多个模块"实验室运行体系,提高了实验室建设和运行水平,促进了教学、科研和人才培养。     

大学物理演示实验室的建设与实践

本文以讨论物理演示实验室的建设和应用为线索,论证了演示实验在大学物理教学中的重要性,并就我校近年来演示实验的建设和实践情况作了简要介绍。     

中国科学院物理学方面的开放实验室介绍 中国科学院武汉物理研究所波谱与 原子、分子物理实验室简介

本刊１９８５年第９期《动态》栏中已简单报道了中国科学院物理学方面的开放研究所和实验室情况．从本期开始将陆续介绍各开放实验室的研究方向、研究内容及优先支持的研究课题以及实验室的现状等．     

Experimental and Theoretical Study of the Electronic States and Spectra of TeH and TeLi

Gas-phase emission spectra of the hitherto unknown free radical TeLi have been measured in the NIR range with a Fourier-transform spectrometer. The emissions were observed from a fast flow system in which tellurium vapor in argon carrier gas was passed through a microwave discharge and mixed with lithium vapor in an observation tube. Two systems of blue-degraded bands were measured at high spectral resolution in the ranges 8000-9000 and 5700-6700 cm(-1) and vibrational and rotational analyses were performed. In order to aid in the analysis of the experimental data, a series of relativistic configuration interaction calculations has been carried out to obtain potential curves for the low-lying states of TeLi and the isovalent TeH and also electric dipole transition moments connecting them. As in the TeH system, the ground state of TeLi is found to be X(2)Pi(i), but with a remarkably smaller spin-orbit splitting. The TeLi calculations indicate a strongly bound A(2)Sigma(+) state, while in TeH the analogous state is computed to lie significantly higher at approximately 32 000 cm(-1), and it is strongly predissociated. Based on the theoretical analysis, the observed TeLi band systems are assigned to the transitions A(2)Sigma(+)(A1/2)-->X(1)(2)Pi(3/2)(X(1)3/2) and A(2)Sigma(+)(A1/2)-->X(2)(2)Pi(1/2)(X(2)1/2). Analysis of the spectra has yielded the molecular constants (in cm(-1)) X(1)(2)Pi(3/2):omega(e)=457.49(3), omega(e)x(e)=2.482(9), B(0)=0.408908(8); X(2)(2)Pi(1/2): T(e)=2353.44(3), omega(e)=456.28(4), omega(e)x(e)=2.635(8), B(0)=0.414954(8), p(0)=1.00637(4); A(2)Sigma(+): T(e)=8574.64(2), omega(e)=437.81(3), omega(e)x(e)=2.581(8), B(0)=0.423903(8), p(0)=-0.19915(2), where the numbers in parentheses are the standard deviations of the parameters. Comparison of the isovalent TeLi and TeH systems emphasizes that the difference in bonding character (ionic in TeLi vs covalent in TeH) is responsible for qualitative differences in the electronic spectra of these two molecules. Copyright 2001 Academic Press.     

碳纳米管-硅纳米线复合结构的形成和热稳定性

通过分子动力学方法模拟了在碳纳米管内填充一定数目的半导体元素硅形成碳纳米管-硅纳米线复合结构的过程,并采用Lindemann指数研究了这种复合结构的热稳定性．计算结果表明,当考虑碳纳米管和硅纳米线轴向方向的周期性边界条件之后,在C（13,0）和C （14,0）碳纳米管内能够形成亚稳结构的硅纳米线Si₁₆NW和Si₂₀NW,从而获得一种碳纳米管-硅纳米线的新型复合结构．通过计算这种复合结构的Lindemann指数,可以看到由于碳纳米管的保护作用,碳纳米管包裹的硅纳 关键词： 复合结构 纳米线 碳纳米管 分子动力学     

Experimental and Theoretical Study of the Electronic States and Spectra of BiNa

Gas-phase emission spectra of the hitherto unknown free radical BiNa have been measured in the NIR range with a Fourier transform spectrometer. The emissions were observed from a fast-flow system in which bismuth vapor in argon carrier gas was passed through a microwave discharge and mixed with sodium vapor in an observation tube. Two systems of blue-degraded bands observed in the ranges 8900-9800 and 7200-7800 cm(-1) were measured at high spectral resolution and vibrational and rotational analyses were performed. To aid in the analysis of the experimental data, a series of relativistic configuration interaction calculations has been carried out to obtain potential curves for the low-lying states of BiNa and also electric dipole transition moments connecting them. As in the isovalent BiH system, the ground state of BiNa is found to be X(3)Sigma(-) with a spin splitting of about 1769 cm(-1). The first excited state is A(3)Pi, and the observed band systems are assigned to the transitions A(3)Pi(A(2)0(+)) --> X(3)Sigma(-)(X(1)0(+), X(2)1). Comparison with earlier work on the isovalent BiH system emphasizes that the relative weakness of the varsigma MO in BiNa is responsible for qualitative differences in the electronic spectra of these two systems. Copyright 2000 Academic Press.     

Production and decay of Omegac0

We present an analysis of inclusive Omega(c)(0) baryon production and decays in 230.5 fb(-1) of data recorded with the BABAR detector. Omega(c)(0) baryons are reconstructed in four final states (Omega(-)pi(+), Omega(-)pi(+)pi(0), Omega(-)pi(+)pi(+)pi(-), Xi(-)K(-)pi(+)pi(+)) and the corresponding ratios of branching fractions are measured. We also measure the momentum spectrum in the e(+)e(-) center-of-mass frame. From the spectrum, we observe Omega(c)(0) production from B decays and in cc events, and extract the two rates of production.     

Structure and properties of some chiralanes and chirolanes

The molecular structures, spectra and properties of six chiralanes and chirolanes (approximately spheroidal, saturated, cage hydrocarbons) have been determined by density functional theory (DFT) quantum chemistry calculations. The main features determined are: molecular geometry, partial atomic charges, standard enthalpy of formation, IR, nuclear magnetic resonance (NMR) and circular dichroism (CD) spectra. On the basis of the calculated standard enthalpies of formation and highest occupied molecular orbital (HOMO)–lowest unoccupied molecular orbital (LUMO) gaps, we suggest that chiralanes/chirolanes are potential synthetic targets. We have calculated the anomalously large downfield ¹³C-NMR shifts for endohedral carbons in the spectra of [5.5] and [5.7]chiralanes.     

Characterization of Electronic Spectra of Rhodium Monohydride and Monodeuteride

Emission spectra of two new electronic transitions of Pb(2) have been measured with a Fourier transform spectrometer in the 5200-8500 cm(-1) range. The emissions were observed from the afterglow of a microwave discharge in a mixture of Pb(x) vapor with hydrogen and argon carrier gas. By comparison with the results of ab initio calculations, the spectra are assigned to transitions from the lowest 1(g) and 1(u) states to the X(1)0(+)(g) ground state. The X(2)1(g) --> X(1)0(+)(g) transition between the fine-structure components of the X(3)Sigma(-)(g) ground state must be magnetic dipole in nature and thus is the first purely magnetic dipole fine-structure transition observed in the optical region. The 1(u) state is mostly a component of the low-lying inverted A(3)Pi(u) state and so is denoted A(2)1(u). Vibrational analyses have yielded the following electronic energies and vibrational constants for (208)Pb(2) (in cm(-1)): X(1)0(+)(g): omega(e) = 110.20(2), omega(e)x(e) = 0.341(2); X(2)1(g): T(e) = 5304.9(1), omega(e) = 120.57(7), omega(e)x(e) = 0.254(14); A(2)1(u): T(e) = 7817.5(2), omega(e) = 126.45(6), omega(e)x(e) = 0.399(11), where the numbers in parentheses are the standard deviations of the parameters. Copyright 2000 Academic Press.     

金属-糖胺配合物的合成,光谱表征及催化酯类水解的动力学研究

合成了4种新的糖胺 金属配合物,分别为[Ni(HL) (H2 O) 2 ]2 Cl2 ·CH3OH·2H2 O ,[Cu(HL) ]2 Cl2 ·CH3CH2 OH·3H2 O ,[Zn(HL) ]2 Cl2 ·H2 O ,[Co(HL) (H2 O) (OH) ]2 Cl2 ·CH3OH·2H2 O (HLN ,N′ 二βD 葡萄糖基乙二胺) ,并用元素分析、红外、紫外、核磁共振氢谱对其结构进行了表征。结果表明,Ni(Ⅱ) ,Co(Ⅲ)配合物为八面体构型,而Cu(Ⅱ) ,Zn(Ⅱ)配合物为四面体构型。最后研究了其对对硝基苯吡啶甲酸酯(PNPP)催化水解的催化速率常数。     

矿物药炉甘石煅制前后锌、铅元素的赋存形态及分布特征研究

采用X射线衍射(XRD)技术和电子探针微区分析(EPMA)技术针对中药炉甘石煅制前后锌、铅元素的赋存形态及分布特征进行了研究,探明了煅制对炉甘石中锌、铅元素赋存状态及分布的改变,为后续水飞减除铅元素的机理研究提供了理论依据。测试结果显示：21批次炉甘石(生品)中的锌元素以主矿物水锌矿[Zn₅(CO₃)₂(OH)₆]和杂质矿物异极矿[Zn₄(OH)₂(H₂O)(Si₂O₇)]为主要赋存形态,偶见菱锌矿(ZnCO₃);炉甘石(生品)的背散射电子图谱及元素分布数据显示：Zn和Pb元素同时分布的区域为水锌矿,Zn和Si元素同时分布的区域为异极矿,Ca和Mg元素同时分布的区域为白云石,Ca元素单独分布区域为方解石。在炉甘石(生品)中,Pb主要分布于水锌矿中且分布相对均匀,Pb元素的分布与水锌矿中的Zn元素密切相关。大量水锌矿的微区点位的电子探针定量分析结果显示：各不同点位中的ZnO/PbO含量的比值趋于定值,Pb在水锌矿中呈统计式均匀分布,说明Pb在水锌矿中主要以类质同象混入物的形式存在。但是炉甘石(生品)中的异极矿、方解石及白云石等杂质矿物中铅元素含量极低甚至检测不到。炉甘石煅烧后水锌矿晶格中的Zn和Pb分别生成了ZnO和PbO。Zn元素在炉甘石煅制品中主要以氧化锌(ZnO)形式存在,少部分以杂质矿物硅酸锌(Zn₂SiO₄)形式存在,呈较连续状态分布。Pb元素在炉甘石煅制品中主要以氧化铅(PbO)的形式存在,呈星点状分布,与Zn元素的分布未呈现相关性,说明Pb在炉甘石煅制品中是以独立矿物形式存在的。煅烧破坏了水锌矿的晶格结构,在改变锌、铅化合物形态的同时,更改变了锌、铅的分布特征,打破了炉甘石中锌、铅的共生状态,使水飞减除铅元素成为可能。     

Optical and defect properties of S-doped and Al-doped GaSe crystals

S-doped and Al-doped GaSe crystals are promising materials for their applications in nonlinear frequency conversion devices. The optical and defect properties of pure, S-doped, and Al-doped GaSe crystals were studied by using photoluminescence(PL) and Fourier transform infrared spectroscopy(FT-IR). The micro-topography of(0001) face of these samples was observed by using scanning electron microscope(SEM) to investigate the influence of the doped defects on the intralayer and interlayer chemical bondings. The doped S or Al atoms form the S_(Se)~0 or Al_(Ga)~(+1) substitutional defects in the layer GaSe structure, and the positive center of Al_(Ga)~(+1) could induce defect complexes. The incorporations of S and Al atoms can change the optical and mechanical properties of the GaSe crystal by influencing the chemical bonding of the layer structure. The study results may provide guidance for the crystal growth and further applications of S-doped and Al-doped GaSe crystals.     

The Millimeter- and Submillimeter-Wave Spectrum and the Dipole Moment of Ethylenimine

The 0(0)(0) bands of the ?(2)B(2)-&Xtilde;(2)A(1) and &Btilde;(2)B(1)-&Xtilde;(2)A(1) systems of SrNH(2) were observed at Doppler-limited resolution using a Broida oven source and laser-induced fluorescence detection. A full rotational analysis of both transitions was performed including K(a) levels up to 5 and J levels up to 55. The &Btilde;(2)B(1) state was found to be extensively perturbed and only some of the subbands could be analyzed. The ?(2)B(2) and &Btilde;(2)B(1) states undergo a strong Coriolis-type interaction which results in extremely large spin-rotation splittings in both states, effectively splitting all levels with K(a)(') not equal 0 into two well-separated spin components. Copyright 2000 Academic Press.