Improved design and construction of an ionization chamber for the CSNS beam loss monitor (BLM)

Based on the first ionization chamber (IC) prototype, the structure, working gas component and electrode material of the IC are improved. The test of the improved IC shows that the plateau length is about 2000 V, the plateau slope is less than 0.2%/100 V, the sensitivity is 19.6 pA/rad·h^-1, the up-limitation of the linearity can be up to 3.6×10⁵ rad/h, and the applied voltage can be operated to 3500 V. The test results show that the performance of the improved IC meets the requirements of the beam loss monitor.     

Interference effects on the photoionization cross sections between two neighbouring atoms: nitrogen as an example

Interference effects on the photoionization cross sections between two neighbouring atoms are considered based on the coherent scattering of the ionized electrons by the two nuclei when their separation is less than or comparable to the de Broglie wave length of the ionized electrons. As an example, the single atomic nitrogen ionization cross section and the total cross sections of two nitrogen atoms with coherently added photoionization amplitudes are calculated from the threshold to about 60~\AA (1~\AA=0.1~nm) of the photon energy. The photoionization cross sections of atomic nitrogen are obtained by using the close-coupling R-matrix method. In the calculation 19 states are included. The ionization energy of the atomic nitrogen and the photoionization cross sections agree well with the experimental results. Based on the R-matrix results of atomic nitrogen, the interference effects between two neighbouring nitrogen atoms are obtained. It is shown that the interference effects are considerable when electrons are ionized just above the threshold, even for the separations between the two atoms are larger than two times of the bond length of N₂ molecules. Therefore, in hot and dense samples, effects caused by the coherent interference between the neighbours are expected to be observable for the total photoionization cross sections.     

体外预应力混凝土梁的受弯承载力研究

体外预应力混凝土结构的受弯承载力同多种因素有关,目前还没有较好的计算方法.本文在14根体外预应力混凝土梁模型试验研究基础上,对影响受弯承载力的主要因素进行了分析,并通过对国内外主要规范的比较研究,提出了具有较高精度的体外预应力梁受弯承载力计算公式.     

LUND面积定律产生子在R值测量中的应用

对Lund弦碎裂模型强子化面积定律严格求解,得到e⁺e^－湮没产生少体初始强子态的遍举分布.基于面积定律的新产生子LUARLW在2—5GeV能区的模拟结果与BES数据的多种谱分布符合很好,用于BES上强子产生总截面测量的强子探测效率的估计.     

Near threshold photodetachment cross section of negative atomic oxygen ions

A 40-target state close-coupling calculation for the photodetachment cross section of negative atomic oxygen near threshold is carried out with core－valence electron correlation by using the R-matrix method. It was shown that after considering the excitations of two electrons from the 2s shell, the electron affinity of O^- (2s^22p^5{}^2P°) agrees with the experimental result much better than that just considering the excitations of electrons only from the 2p shell as well as only one electron from the 2s shell. Total cross section as well as the main contribution of the ionization channels to the partial cross section are illustrated to show the structure near threshold clearly.     

一维链状冠醚配合物[K(B18-C-6)]_2[M(SCN)_4](M=Pd,Pt)的合成与结构

合成了苯并18-冠-6（B18-C-6）与K_2[Pd(SCN)_4]生成的配合物[K（B18-C-6 ）]_(12) [Pd(SCN)_4] (1), [K(B18-C-6)]_2[Pt(SCN)_4] (2)和[K(B18-C-6)]_2 [Pt(SCN)_4]·C_2H_4Cl_2 (3),并通过元素分析、红外光谱、单晶X射线衍射进行 了表征。1和2为单斜晶系,空间群P2_l/n,晶体学数据：1, a = 1.00970(17) nm, b = 1.3157(2) nm, c = 1.7303(3) nm, β = 94.841(2)°, V = 2.2852(7) nm~3, Z = 2, F(000) = 1136, R_1 = 0.0257。3为三斜晶系,空间群P1,晶体学 数据：a = 0.95914(18) nm, b = 1.2137(2) nm, c = 2313(2) nm, α = 63.693 (2)°, β = 76.293(2)°, γ-1.2406(4) n~3, Z = 1 F(000)618,R_1 = 0.0366 。在固态,三个配合物相邻的两个[K（B18-C-6）]~+基团通过冠醚氧化原子与钾的 子的相边接而形成一维链状结构。     

弱相互作用构筑的二维、三维冠醚配合物{[K(18-C-6)2(C2H4Cl2)}[Ni(dmit)2]2和[K(18-C-6)][Ni(dmit)2]的合成与结构

研究了18－冠－6与NiCl·6H2O,K2dmit(dmit=4,5-dimercapto-1,3-dithiole- 2-thione,C3S5^2－）在不同溶剂中反应生成的两个标题配合物{[K(18-C-6)]2 (C2H4Cl2)}[Ni(dmit)2]2（1）和[K(18-C-6)][Ni(dmit)2](2)。通过元素分析、红 外光谱、单晶X射线衍射进行了表征。1和2均属三斜晶系,空间群P1^-.1的晶体学 数据：a=1.0272(2)nm,b=1.2282(3)nm,c=1.4205(3)nm,α=113.473(3)°,β=90. 609(3)°,γ=91.439(3)°,V=1.6430(6)nm^3,Z=2,F（000)=876,R1=0.0503。2的 晶体学数据：a=0.8502(2)nm,b=1.2178(4)nm,c=1.5118(4)nm,α=86.454(5)°,β =77.734(5)°,γ=85.364(5)°,V=1.5228(8)nm^3,Z=2,F(000)=774,R1=0.0565。配 合物1,2分别通过K…S,K…Cl,S…S和K…S,S…S弱相互作用形成二维、三维网状 结构。     

Molecular and Crystal Structure of 4-Amino-4'-Nitrodiphenyl Ether

1　ＩＮＴＲＯＤＵＣＴＩＯＮＴｈｅｏｒｇａｎｉｃｓｅｃｏｎｄｏｒｄｅｒｎｏｎｌｉｎｅａｒｏｐｔｉｃａｌ(ＮＬＯ)ｍａｔｅｒｉａｌｓｈａｖｅｂｅｅｎｐａｉｄｍｏｒｅａｎｄｍｏｒｅａｔｔｅｎｔｉｏｎｓｂｅｃａｕｓｅｏｆｔｈｅｉｒｉｍｐｏｒｔａｎｔａｐｐｌｉｃａｔｉｏｎｓｉｎｏｐｔｏｅｌｅｃｔｒｏｎｉｃｓｔｅｃｈｎｏｌｏｇｙｆｉｅｌｄｓ.[1～3]Ｔｈｅｉｒｓｅｃｏｎｄｈａｒｍｏｎｉｃｇｅｎｅｒａｔｉｏｎ(ＳＨＧ)ｅｆｆｉｃｉｅｎｃｉｅｓｕｓｕａｌｌｙｅｘｃｅｅｄｔｈｏｓｅｏｆｃｏｍｍｏｎｌｙｕｓｅｄｉｎｏｒｇ…     

阳离子- π相互作用————————[K(DI18C6)]2[M(SCN)4] (M=Pd,Pt)的合成与结构 研究

合成了二苯并18冠6与Pd,Pt生成的新颖配合物：[K(DI18C6)]2[Pd(SCN)4](1),(K(DB18C6)]2[Pt(SCN)4](2),并通过元素分析、红外光谱、单晶X射线衍射进行了表征,两个配合物均为三斜晶系,空间群P-1.1的晶体学数据：a=087375(17)nm,b=1.1990(2)nm,C=1.3180(3)nm,α=73.56(3)°,β=99.90(3)°,γ=82.34(3)°,V=1.2986(4)nm^3,Z=1,F(000)=584,R1=0.0752ωR2=0.1660.2的晶体学数据：a=0.8553(5)nm,b=1.3127(3)nm,c=1.1819(3)nm,α=106.21(2)°,β=82.77(3)°,γ=99.72(3)°V=1.2516(8)nm^3,Z=1,F(000)=818,R1=0.0254,ωR2=0.0682.1,2均由两个[K(DB18C6)^+配离子和一个[M(SCN)4]^2+配阴离子组成。在固态、配合物两个分子的[K(DB18C6)]^+和[M(SCN)4]^2-通过K^+-π相互作用形成假一维无限链状结构。     

18-冠-6与Na2[M(mnt)2](M=Cu,Ni)配合物的合成与结构

研究了18-冠-6分别与Na2[M(mnt)2][M=Cu,Ni;mnt=丁二腈烯二硫醇阴离子,C2S2(CN)^2^-~2]的反应,得到的配合物{[Na(18-C-6)][Na(18-C-6)(H2O)]}[Cu(mnt)2](1),[Na(18-C-6)(H2O)]2[Ni(mnt)2].(18-C-6)(2)通过元素分析、红外光谱、X射线单晶衍射进行了表征。两个配合物均为三斜晶系,空间群P1。1的晶体学结构数据：a=1.22697(19)nm,b=1.22780(19)nm,c=1.5665(3)nm,α=95.083(3)°,β=101.534(3)°,Υ=91.007(3)°,V=2.3016(6)nm^3,Z=2,Dcalcd=1.350g/cm^3,F(000)=976,R1=0.0726,wR2=0.1843.2的晶体学结构数据：a=1.11620(17)nm,b=1.22054(18)nm,c=1.27939(18)nm,α=111.647(2)°,β=29.792(3)°,Υ=103.201(2)°,V=2.5461(4)nm^3,Z=1,Dcalcd=1.304g/cm^3,F(000)=642,R1=0.0459,wR2=0.1003.1中的[Cu(mnt)2]^2^-通过mnt的氮原子与[Na(18-C-6)]^+中的钠原子成键,形成了一维链状结构;[Na(18-C-6)(H2O)]^+只起平衡电荷的作用。2中的[Ni(mnt)2]^2^-也通过配体的mnt氮原子与两个[Na(18-C-6)(H2O)]^+中的钠原子成键,形成稳定的中性配合物。