2 0 1 6年高考四川物理压轴题的多种解法

通过对2 0 1 6年高考四川物理压轴题多种解法的讨论, 希望与广大同行进行交流. 在高中物理教学中, 培养学生勤于思考、 善于思考的习惯, 而一题多解不仅可以开拓学生的思维, 还可以提高学习物理的兴趣, 有利于 培养高素质人才     

对2 0 1 6年高考四川卷物理压轴题的研究

结合在学生犯错案例, 就2 0 1 6年高考四川卷物理压轴题进行了探讨, 为以后物理教学的改进找准了方 向, 进一步分析了该题所给参考答案的一些瑕疵     

对2 0 1 6年高考江苏卷力学实验题的评析

2 0 1 6年江苏高考卷力学实验题的命题方式体现了创新理念, 从试题设置和提问中得到两点启示. 结合 高中物理实验室装备的仪器, 对题中所给数据进行深入分析, 发现在部分数据设置、 实验的可操作性、 精确性、 系统 误差上存在一些疑惑和不足     

Saturation effects on Ba 6phi （l=0, 2） and 6pnk （｜M｜= 0, 1） autoionization spectra

Using a three-step laser saturation excitation technique, the saturation effects on the Ba 6pns （J = 1） and 6pad （J = 1, 3） autoionization spectra are observed systemically in zero field. These saturation spectra are introduced to determine the high n members of 6pnl （l = 0, 2） autoionizing series and are used to analyse the channel interactions among the autoionizing series in zero field. Furthermore, the saturation excitation technique is applied to the electric field case, in which the saturation spectra of Ba 6pnk （｜M｜= 0, 1） autoionizing Stark states are measured. Most of these saturation spectra are observed for the first time so far as we know, which indicate the mixing of the autoionizing states in the electric fields.     

从核心素养的视角观2 0 1 6年中考实验探究题

以2 0 1 6年全国中考物理实验探究题为切入点, 从物理观念、 科学思维、 科学态度与责任、 科学应用4个 方面, 通过典型试题分析, 对实验教学提出建议, 以培养学生的核心素养     

ThTiO_4~(-/0),Th_2TiO_6~(-/0)和ThTi_2O_6~(-/0)的电子结构和化学成键的密度泛函理论研究

本文采用B3LYP密度泛函理论方法,探究双核、三核掺杂钍氧簇体系ThTiO_4~(-/0)、Th_2TiO_6~(-/0)和ThTi_2O_6~(-/0)的几何构型、电子结构和化学成键等规律,并与等价电子体(TiO_2)-/0n(n=2,3)进行对比,研究掺杂效应对于掺杂体系的结构和成键等性质的影响.结果表明:掺杂钍氧簇与其等价电子体(TiO_2)-/0n(n=2,3)具有类似的键连方式.ThTiO_4~-中单电子占据的位置与Ti2O-4中单电子的所处位置类似,都是被两个金属原子共用,而Th_2 TiO_6~-,Th Ti_2O_6~-以及Ti_3O_6~-中的单电子均处于那个不含端氧的金属原子上.     

High resolution photoassociation spectra of an ultracold Cs2 long-range 0u＋ （6S1/2 ＋ 6P1/2） state＊

In this paper, ultracold cesium molecules are formed through photoassociation technology, which is carried out in a magneto-optical trap. High resolution photoassociaion spectra with the rotational progressions up to J = 7 are obtained. Three rovibrational levels of the long-range 0＋ state of Cs2 below the （6S1/2 ＋ 6P1/2） dissociation limit are specifically investigated. By fitting their binding energy intervals to the non-rigid rotational model, the rotational constant of the long- range 0u＋ state is determined. A proportional dependence of the value of the rotational constant on the vibrational quantum number is demonstrated.     

CHINESE JOURNAL OF LOW TEMPERATURE PHYSICS Vol.2 3 2 0 0 1 CONTENTS

Ｎｏ .1Ｔｈｅｉｎｓｕｌａｔｏｒ ｍｅｔａｌｔｒａｎｓｉｔｉｏｎａｎｄＣＭＲｅｆｆｅｃｔｉｎＬａ2 / 3 Ｃａ1/ 3 ＭｎＯ3 ＬｉｕＮｉｎｇ ,　ＳｕｎＹｏｎｇ ,　ＴｏｎｇＷｅｉ,　ＺｈｅｎｇＹｕ ｈｅｎｇ (5 )…Ｔｈｅｎｏｎｌｉｎｅａｒｒｅｓｐｏｎｓｅｆｕｎｃｔｉｏｎｉｎｈｉｇｈ ｓｕｐｅｒｃｏｎｄｕｃｔｏｒｓａｎｄｔｈｅｖｏｒｔｅｘｐｈａｓｅｔｒａｎｓｉｔｉｏｎＱｉＺｈｉ,　ＹｉｎＤａｏ ｌｅ (13)………………ＡｒｅｖｉｅｗｏｆｓｔｕｄｙｏｎＭＴＧＹＢＣＯｂｕｌｋａｎｄＢｉ 2 2 2 3/Ａｇｔａｐｅｓｂｙｍａｇｎ…     

氨分子在0_0~0和2_0~1带的选择光离解

本文利用脉冲紫外激光(UV)选择激发氨分子到A~1A″_2电子激发态的两个最低振动能级υ′_2=0和υ′_2=1(ν_2振动),然后检测新生态H原子的飞行谱(TOF),研究了氨分子的光碎片动力学。光谱证实了最近所测的离解能D_0~0(H-NH_2)=4.645eV;绝大多数生成的NH_2(X~2B_1)基处于非振动激发,但是具有围绕a惯性轴的高度转动激发。通过NH_3(A)的υ′_2=1光离解产生的NH_2(X)基具有较高的内部激发,并且显示了在N=K_a转动能级上的反转布居。     

Interaction of H2S with α-Fe2O3(0 0 0 1) surface

The atomic-scale structural changes in an α-Fe₂O₃ (hematite) (0 0 0 1) surface induced by sulfidation and subsequent oxidation processes were studied by X-ray photoemission spectroscopy, LEED, and X-ray standing wave (XSW) measurements. Annealing the α-Fe₂O₃(0 0 0 1) with a H₂S partial pressure of 1 × 10⁻⁷ Torr produced iron sulfides on the surface as the sulfur atoms reacted with the substrate Fe ions. The oxidation state of the substrate Fe changed from 3+ to 2+ as a result of the sulfidation. The XSW measured distance of the sulfur atomic-layer from the unrelaxed substrate oxygen layer was 3.16 Å. The sulfide phase consisted of three surface domains identified by LEED. Formation of the two-dimensional FeS₂ phase with structural parameters consistent with an outermost layer of (1 1 1) pyrite has been proposed. Atomic oxygen exposure oxidized the surface sulfide to a sulfate () and regenerated the α-Fe₂O₃(0 0 0 1) substrate, which was indicated by a (1 × 1) LEED pattern and the re-oxidization of Fe to 3+.     

从2 0 1 6年高考新课标 Ⅰ 第1 6题谈“ 等效电阻法”的应用

针对考生在解答2 0 1 6年高考全国新课标Ⅰ卷第1 6题时, 常规的解法存在着推导繁琐和计算量大等困 难, 通过介绍变压器的“ 等效变阻法”并尝试应用该方法解题, 化繁为简, 起到事半功倍的效果     

2 0 1 5年高考浙江理综卷第1 6题与静电力演示仪

0 1 5年高考浙江理综卷第1 6题中提到的“ 静电力演示仪” , 在课堂教学中运用的并不广泛, 原因在于镀 膜乒乓球制备的复杂性以及安全性. 笔者在课堂教学中, 应用简单的设备和材料, 制作静电力演示仪, 能够产生相同 的实验现象, 并对实验进行了改良和变式, 获得了较好的教学效果     

Bi_（1．6）Pb_（0．4）Sr_2Ca_（2－x）（Nd_（0．75）Ce

本文通过Ｘ射线衍射、差热分析和超导电性测量等手段对Ｂｉ１．６Ｐｂ０．４Ｓｒ２Ｃａ２－ｘ（Ｎｄ０．７５Ｃｅ０．２５）ｘＣｕ３Ｏｙ体系的相结构和超导电性进行了研究．该体系中，在８１０—８４０℃空气中烧结４０小时样品的Ｔｅ随着ｘ增加而降低．研究了在７５０－８２０℃烧结样品的超导电性与组成的关系．ｘ＝１．６—２．０，在７５０—８２０℃空气中烧结４０小时样品的超导转变温度为１９—２１Ｋ．这种超导电性可能是由于部分被稳定的Ｂｉ－２２２２相所致．     

The laser-intensity dependence of the photoassociation spectrum of the ultracold Cs2（6S1/2 ＋ 6P1/2） 0＋ long-range molecular state

The high-resolution photoassociation spectrum of the ultracold cesium molecular 0＋ state below the 6S1/2 ＋ 6PI/2 limit is presented in this paper. The saturation of the photoassociation scattering probability is observed from the depen dence of the trap-loss probability on the photoassociation laser intensity. The corresponding resonant line width is also demonstrated to increase linearly with increasing photoassociation laser intensity. Our experimental data have good con sistency with the theoretical saturation model of Bohn and Julienne [Bohn J L and Julienne P S 1999 Phys. Rev. A 60 1].     

NiI［14. 6］2Δ5/2-X 2Δ5/2（9，0）带的超精细结构

在可见光范围内 ,用激光蒸发 /反应、超声射流和激光诱导荧光光谱方法 ,对NiI[14 .6 ]2 △5/ 2 -X2 △5/ 2跃迁的 (9,0 )带进行了高分辨研究 .80MHz分辨的光谱显示超精细结构是由于激发态中未成对电子与碘 (I=5 /2 )核大磁矩相互作用引起的 .在v =9能级上低J谱线的超精细线宽快速下降 ,表明在 [14 .6 ]2 △5/ 2 态中超精细耦合适合Hundaβ 耦合情况 .[14 .6 ]2 △5/ 2 态的精确转动参数和超精细参数已得到 ,而且显示v =9能级被微扰了 .     

Vibrational-electronic coupling in IrF6, OsCl6 2− and IrCl6 2−

The results obtained in a previous paper [1] for an unsymmetric regular model are applied to solid hydrogen at low temperatures when the lattice structure and the quadrupole-quadrupole interaction make the interaction energies non-isotropic. It is shown that, as for the lattice structures with isotropic interactions, no second-order transition is likely to occur through a cooperative rotational effect. The possible occurrence of spatial ordering on sub-lattices is discussed. It is found that such ordering is unlikely to occur at low temperatures on the face-centred cubic lattice, but that on the hexagonal close-packed lattice (which is the probable crystal structure) there is a second-order transition to an ordered state. Using a zeroth-order approximation the temperature at which this transition occurs in pure ortho-hydrogen is found to be 5·8°k.