硼化合物研究(ⅩⅥ)——氢硼酸π-环戊二烯基双(三苯基膦)镍(Ⅱ)的合成

MCArdle和Akker等人分别合成了[π-C_5H_5Ni(PPh_3)_2)SnCl_3·S[S=CH_2Cl_2,(CH_3)_2O)租[π-C_5H_5Ni(PPh_3)_2]F等化合物.本文报告七个新的氢硼酸根(B_(12)H_(12)~(2-)、B_(10)H_(10)~(2-)、B_(11)H_(14)~-、B_3H_3~-、B_(10)Cl_(10)~(2-)B_(10)H_2Br_8~(2-)、B_(10)H_4I_6~(2-))的π-一环戊二烯基双(三苯基膦)镍(Ⅱ)的合成和性质研究。     

C_2B_(10)H_(12),NB_(11)H_(12)和C_2B_(10)H_(11)Cl振动光谱的从头计算研究

利用Gaussian 92从头算程序在6-3lG基组下对C_2B_(10)H_(12),NB_(11)H_(12)和C_2B_(10)H_(11)Cl进行几何优化和振动频率的理论计算,结果与实验基本符合.优化几何与振动光谱均表明,从B_(12)H_(12)~2到上述化合物的取代过程中,几何结构基本保持二十面体构型不变;振动模式表明C_2B_(10)H_(11)Cl的光谱中低频处有一个(C_2B_(10)H_(11))-Cl间的类似于双原子分子的振动,而无C-Cl伸缩振动,     

硼化合物研究(ⅩⅩⅢ)——硼氢化钾与二茂铁甲基三烃基氯化铵的反应

我们曾研究了硼氢化钾与四乙基氯化铵在一定量水存在下的热解反应,制得了B_(10)H_(10)~(2-)、B_(12)H_(12)~(2-)等多面体硼氢化合物,并提出了热解反应的历程。在少量水存在下,通过三烷基苄基氯化铵与硼氢化钾反应,合成了四氢硼酸三烷基苄基铵R_3(C_6H_5CH_2)NBH_4。但热解该类型四氢硼酸盐时,得不到B_(10)H_(10)~(2-)、B_(10)H_(12)~(2-)等多面体硼氢化合物,而是苄基与氮相连的C—N键断裂形成的R_3N·BH_3配合物和甲苯。本文研究C_5H_5FeC_5H_4CH_2NMe_2(R)Cl与KBH_4在水溶液中     

硼化合物的研究——Ⅴ.氢硼酸π-芳烃-π-环戊二烯基铁的合成和性质

本文研究了氢硼酸根(B_(12)H_(12)~(2-)、B_(10)H_(10)~(1-)、B_(11)H_(14)~-)和π-芳烃-π-环戊二烯基铁阳离子的反应,合成了36个氢硼酸π-芳烃-π-环戊二烯基铁化合物。通过元素分析和红外光谱测定确定了化合物的组成。部份化合物还作了~1H NMR鉴定。对化合物的性质,包括它们的热行为,进行了较详细的研究。DTA仪测得的结果表明,(1)当阳离子相同时,化合物的热稳定性的顺序为:[ArFeC_5H_5]_2B_(12)H_(12)>[ArFeC_5H_5]_2B_(10)H_(10)>[ArFeC_5H_5]B_(11)H_(14);(2)当氢硼酸根相同时,其热稳定性受芳环上取代基的影响。     

一种有机-无机复合的硼钒酸盐[enH_2]_4[V_6B_(20)O_(50)H_8(H_2O)]·en·8H_2O（英文）

借助水热合成技术获得了一种新的有机-无机复合的硼钒酸盐[H_2en]_4[V_6B_(20)O_(50)H_8(H_2O)]·en·8H_2O(1)(en=乙二胺),并对其进行了红外光谱、热重分析和单晶X射线衍射等表征.化合物1的分子结构包含1个[V_6B_(20)O_(50)H_8(H_2O)]8-多酸阴离子、4个质子化的[H_2en]~(2+)阳离子、1个游离的乙二胺分子和8个结晶水分子.化合物1最有趣的结构特点体现在:夹心型的[V_6B_(20)O_(50)H_8(H_2O)]8-多酸阴离子是由2个呈交错排列的三角形{B_(10)O_(26)}簇和1个六边形的{V_6O_(18)}簇通过12个三重桥氧原子连接而成的,其中两个三角形{B_(10)O_(26)}簇相互旋转的角度为45°.     

无机化学试题

一、填充 1.命名下列离子:MoO_4~(2-)____;Mo_7O_(24)~(6-)____;H_2W_(12)O_(40)~(6-)____。 2.B_(12)H_(12)~(2-)离子的构型是____体,构成这骨架的成键电子数共有____个。 3.络合物(C_5H_5)V(CO)_4在液氨中能被金属钠还原产生负离子[(C_5H_5)V(CO)_3]~(n-),n的值等于____;CO的伸缩频率在(C_5H_5)V(CO)_4比在[(C_5H_5)V(CO)_3]~(2-)____。     

硼化合物的研究——Ⅹ。B_(10)H_(10)~(2-)、B_(10)H_(12)~(2-)及B_3H_8~-双二茂铁季铵盐及环状二茂铁季铵盐的合成

众所周知,二茂铁类和硼氢类化合物都具有特殊的化学结构,并且有可能作为高能材料得到应用。作者通过B_(10)H_(10)~(2-)、B_(12)H_(12)~(2-)及B_3H_8~-与(N,N-二甲基胺甲基)二茂铁和1,1’-双(N,N-二甲基胺甲基)二茂铁卤化铵反应,曾合成了一系列新的化合物并研究了它们的反应性能和晶体结构。     

硼化合物的研究——Ⅺ.氢硼酸π-环戊二烯基-烷撑双(二苯基膦)合镍(Ⅱ)的合成和性质

本文以C_5H_5NiPPh_3Cl与Ph_2P(CH_2)_nPPh_2为起始物合成了C_5H_5NiPh_2P(CH_2)nPPh_2Cl·C_6H_6,再进一步与氢硼酸季铵盐反应,合成了12个氢硼酸π-环戊二烯基-烷撑双(二苯基膦)合镍(Ⅱ)化合物。对这些化合物进行了元素分析、红外光谱鉴定,并测定了氯化物的~1H NMR谱。所有含硼化合物于室温下对空气是稳定的,而它们的热稳定性与阳离子中螯合环的大小和氢硼酸根结构有关,即氢硼酸根相同的化合物,热稳定性随着螯合环的增大而降低;阳离子相同时,热稳定性次序是:[C_5H_5NiPh_2P(CH_2)_nPPh_2]_2B_(12)H_(12)>[C_5H_5NiPh_2P(CH_2)_nPPh_2]_2B_(10)H_(10)>C_5H_5NiPh_2P(CH_2)_nPPh_2B_(11)H_(14)>C_5H_5NiPh_2P(CH_2)_nPPh_2B_3H_8。     

已烯自由基阳离子的密度泛函理论研究

使用密度泛函理论B3LYP方法和6-31G(d,p),6-31+G(d,p),6-311G(d,p)及6- 311+G(d,p)基组,分别对1-C_6H_(12)~+,2-C_6H_(12)~+和3-C_6H_(12)~+的各种构 象进行了几何构型优化,并在B3LYP/6-311G(d,p)水平上进行了频率分析计算,在 各优化构型上,使用B3LYP和MP2(full)方法进行了超精细结构的计算。计算的3- C_6H_(12)~+的超精细偶合常数比以往的计算结果更好;1-C_6H_(12)~+和2-C_6H_ (12)~+的超精细偶合常数目前尚无实验数据报道,本计算预言了它们的超精细偶合 常数和最稳定构型。     

已烯自由基阳离子的密度泛函理论研究

使用密度泛函理论B3LYP方法和6-31G(d,p),6-31+G(d,p),6-311G(d,p)及6- 311+G(d,p)基组，分别对1-C_6H_(12)~+,2-C_6H_(12)~+和3-C_6H_(12)~+的各种构 象进行了几何构型优化，并在B3LYP/6-311G(d,p)水平上进行了频率分析计算，在 各优化构型上，使用B3LYP和MP2(full)方法进行了超精细结构的计算。计算的3- C_6H_(12)~+的超精细偶合常数比以往的计算结果更好；1-C_6H_(12)~+和2-C_6H_ (12)~+的超精细偶合常数目前尚无实验数据报道，本计算预言了它们的超精细偶合 常数和最稳定构型。     

Separation of the vibrational,rotational, and translational motions of polyatomic molecules using curvilinear vibrational coordinates

A new method is suggested for separating the vibrational, rotational, and translational motions of polyatomic molecules using curvilinear vibrational coordinates that are linear with respect to the natural vibrational coordinates. It is shown that, in this case, Coriolis interactions between the vibrational and rotational motions are absent. The solutions of the anharmonic vibrational-rotational problems in the curvilinear and linear vibrational coordinates are compared. The absence of Coriolis interactions between the vibrational and rotational motions in the curvilinear vibrational coordinates is proved numerically. The same conclusion is additionally supported by calculations of the anharmonic vibrational energy levels for the H₂O, H₂S, NO₂, SO₂, and ClO₂ molecules in the linear and curvilinear vibrational coordinates using the Hamiltonian designed in the curvilinear vibrational coordinates with and without Coriolis vibrational-rotational interactions. Volgograd Pedagogical University. Translated fromZhurnal Strukturnoi Khimii, Vol. 36, No. 2, pp. 239–254, March–April, 1995. Translated by I. Izvekova     

Doppler-free two-photon excitation spectroscopy and the Zeeman effects. Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6

Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u <-- S0 1A1g transition in gaseous benzene-d6 were measured. Although the spectral lines were strongly perturbed, almost all of the lines near the band origin could be assigned. From a deperturbation analysis, the perturbation near the band origin was identified as originating from an anharmonic resonance interaction. Perturbation centered at K = 28-29 in the 14(0)1 band was analyzed, and it was identified as originating from a perpendicular Coriolis interaction. The symmetry and the assignment of the perturbing state proposed by Schubert et al. (Schubert, U.; Riedle, E.; Neusser, H. J. J. Chem. Phys. 1989, 90, 5994.) were confirmed. No perturbation originating from an interaction with a triplet state was observed in both bands. From the Zeeman spectra and the analysis, it is demonstrated that rotationally resolved levels are not mixed with a triplet state. The intersystem mixing is not likely to occur at levels of low excess energy in the S1 state of an isolated benzene. Nonradiative decay of an isolated benzene in the low vibronic levels of the S1 state will occur through the internal mixing followed by the rotational and vibrational relaxation in the S0 state.     

On the contribution of vibrational anharmonicity to the binding energies of water clusters

The second-order vibrational perturbation theory method has been used together with the B3LYP and MP2 electronic structure methods to investigate the effects of anharmonicity on the vibrational zero-point energy (ZPE) contributions to the binding energies of (H2O)n, n = 2-6, clusters. For the low-lying isomers of (H2O)6, the anharmonicity correction to the binding energy is calculated to range from -248 to -355 cm(-1). It is also demonstrated that although high-order electron correlation effects are important for the individual vibrational frequencies, they are relatively unimportant for the net ZPE contributions to the binding energies of water clusters.     

A stimulated emission pumping study of the first excited singlet state of germylidene (H2C=Ge)

The A (1)A(2) states of H(2)CGe and D(2)CGe have been explored for the first time by A-X laser-induced fluorescence (LIF) spectroscopy of the orbitally forbidden S(1)-S(0) transition and stimulated emission pumping (SEP) and wavelength resolved fluorescence studies of the allowed B-A electronic transition. Medium-resolution SEP studies gave the excited A state nu(2), nu(3), nu(4), and nu(6) vibrational frequencies for H(2)C(74)Ge and D(2)C(74)Ge. The 4(1) and 6(1) levels and higher combination and overtone states are strongly Coriolis coupled, which perturbs the rotational subband structure, limiting the accuracy of the determination of the vibrational frequencies. High-resolution SEP studies of the B-A 0(0) (0) band have allowed us to determine the rotational constants of the A state of H(2)C(74)Ge, from which we were able to calculate an approximate r(0) structure with the CH bond length constrained to the ground state value. The zero-point level of D(2)C(74)Ge is substantially perturbed, most plausibly by interaction with an excited vibrational level of the nearby triplet (a (3)A(2)) state.     

Calculating intensities using effective Hamiltonians in terms of Coriolis-adapted normal modes

The calculation of rovibrational transition energies and intensities is often hampered by the fact that vibrational states are strongly coupled by Coriolis terms. Because it invalidates the use of perturbation theory for the purpose of decoupling these states, the coupling makes it difficult to analyze spectra and to extract information from them. One either ignores the problem and hopes that the effect of the coupling is minimal or one is forced to diagonalize effective rovibrational matrices (rather than diagonalizing effective rotational matrices). In this paper we apply a procedure, based on a quantum mechanical canonical transformation for deriving decoupled effective rotational Hamiltonians. In previous papers we have used this technique to compute energy levels. In this paper we show that it can also be applied to determine intensities. The ideas are applied to the ethylene molecule.     

Ab initio and electron propagator theory study of boron hydrides

Boron hydrides (BH3, B2H6, B3H7, B4H10, B5H9, and B5H11) and their cations are studied by the coupled cluster CCSD(T) theory, the second-order Mller-Plesset (MP2) perturbation method, and the electron propagator theory in the partial third-order quasi-particle approximation, using the 6-311G(d,p) basis set. The vertical ionization potential energies are calculated, indicating an excellent agreement with the experimental data from photoelectron spectroscopy. Assignments to the experimental spectra are made on the basis of the present computational analyses. A significant Jahn-Teller effect on BH3+ leads to two states, 2A1 and 2B2, with the split energy of 0.14 eV. The triple and double B-H-B bridges are formed in B2H6+ and b-B3H7+, respectively. A new B-H-B bridge is formed while two B-B bonds are broken in B5H11+. The Jahn-Teller effect lowers the symmetry of B5H9 (C4v) to B5H9+ (C2) but slightly influences the structure of ara-B4H10 (C2v). The calculated properties of geometries, vibrational frequencies, and energies are compared with the experimental data available in the literatures.     

Ab initio calculation of the rotational spectrum of methane vibrational ground state

In a previous article we have introduced an alternative perturbation scheme to the traditional one starting from the harmonic oscillator, rigid rotator Hamiltonian, to find approximate solutions of the spectral problem for rotation-vibration molecular Hamiltonians. The convergence of our method for the methane vibrational ground state rotational energy levels was quicker than that of the traditional method, as expected, and our predictions were quantitative. In this second article, we study the convergence of the ab initio calculation of effective dipole moments for methane within the same theoretical frame. The first order of perturbation when applied to the electric dipole moment operator of a spherical top gives the expression used in previous spectroscopic studies. Higher orders of perturbation give corrections corresponding to higher centrifugal distortion contributions and are calculated accurately for the first time. Two potential energy surfaces of the literature have been used for solving the anharmonic vibrational problem by means of the vibrational mean field configuration interaction approach. Two corresponding dipole moment surfaces were calculated in this work at a high level of theory. The predicted intensities agree better with recent experimental values than their empirical fit. This suggests that our ab initio dipole moment surface and effective dipole moment operator are both highly accurate.     

Rotationally Resolved Vacuum Ultraviolet Pulsed Field Ionization-Photoelectron Vibrational Bands for H2+(X2§+g,v+=0-18)

We have obtained a rotationally resolved vacuum ultraviolet pulsed ˉeld ionization-photoelectron (VUV-PFI-PE) spectrum of H2 in the energy range of 15.30-18.09 eV, covering the ionization transitions H2+(X2§+g ,v+=0-18, N+=0-5)?H2(X1§+g , v00=0, J00=0-4). The assignment of the rotational transitions resolved inthe VUV-PFI-PE vibrational bands for H2+(X2§+g , v+=0-18) and their simulation using the Buckingham-Orr-Sichel (BOS) model are presented. Only the ￠N=N+?J00=0 and §2 rotational branches are observed in the VUV-PFI-PE spectrum of H2. However, the vibrational band is increasingly dominated by the 4N=0 rotational branch as v+ is increased. The BOS simulation reveals that the perturbation of VUV-PFI-PE rotational line intensities by near-resonance autoionizing Rydberg states is minor at v+?6 and decreases as v+ is increased. Thus, the rotationally resolved PFI-PE bands for H2+(v+?6) presented here providereliable estimates of state-to-state cross sections for direct photoionization of H2, while the rotationally resolved PFI-PE bands for H2+(v+·5) are useful data for fundamental understanding of the near resonance autoionizing mechanism. On the basis of the rovibrational assignment of the VUV-PFI-PE spectrum of H2, the ionization energies for the formation of H2+(X2§+g , v+=0-18, N+=0-5) from H2+(X1§+g , v00=0,J00=0-4), the vibrational constants (!e, !e?e, !eye, and !eze), the rotational constants (Bv+, Dv+, Be,and ?e), and the vibrational energy spacings ￠G(v++1/2) for H2+(X2§+g , v+=0-18) are determined. With a signiˉcantly higher photoelectron energy resolution achieved in the present study, the precisions of these spectroscopic values are higher than those obtained in the previous photoelectron studies. As expected, the spectroscopic results for H2+(X2§+g , v+=0-18) derived from this VUV-PFI-PE study are in excellent agreement with high-level theoretical predictions.     

Ro-vibrational Spectra of the Simplest Deuterated Criegee Intermediate CD2OO

Criegee intermediates are of significance in the atmospheric chemistry. In this work, the ro-vibrational spectra of the simplest deuterated Criegee intermediate, CD\begin{document}$ _2 $\end{document}OO, were studied by a vibrational self-consistent field/virtual configuration interaction (VSCF/VCI) method based on a nine-dimensional accurate potential energy surface and dipole surface for its ground electronic state. The calculated fundamental vibrational frequencies and rotational constants are in excellent agreement with the available experimental results. These data are useful for further spectroscopic studies of CD\begin{document}$ _2 $\end{document}OO. Especially, the rotational constants for excited vibrational levels are essential for experimental spectral assignments. However, the infrared intensities from different resources, including the current computation, the experiment, and previous calculations at the NEVPT2 and B3LYP levels, deviate significantly.     

Dark state vibronic coupling in the Ã(2Π) ← ͠X(2Σ+) band of ethynyl radical via high resolution infrared absorption spectroscopy

The high resolution infrared spectrum for the ? ((2)Π) ← ?X ((2)Σ(+)) origin band of jet-cooled ethynyl radical (C(2)H) in the gas phase is reported, which exhibits a strong, parity-specific local perturbation in the upper (2)Π(1/2) state. Based on revised parity assignments of the levels, the perturbing state is unambiguously determined to be (2)Σ(+) symmetry, and thus coupled to the ? ((2)Π) state by ΔK = ±1 Coriolis interactions. By incorporating Σ-Π Coriolis coupling into the unperturbed Hamiltonian (containing only rotational, spin-rotational, spin-orbit, and lambda-doubling contributions), we are now able to fit the observed (2)Π-(2)Σ(+) origin band to a sub Doppler experimental uncertainty of 15 MHz (0.0005 cm(-1)). In addition, the observation of pairs of transitions to mixed states permits determination of the band origin (ν(pert)) and rotational constant (B(pert)) for the "dark"(2)Σ(+) state, which prove to be in remarkably quantitative agreement with full vibronic predictions of Tarroni and Carter as well as UV dispersed fluorescence studies of Hsu et al. This represents an important benchmark in mapping out non-Born-Oppenheimer vibronic interactions and energy level structure in a polyatomic combustion radical system, an understanding of which will be key to modeling chemical reactions in both terrestrial and astronomical environments.