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1.
本文在束-气条件下研究了亚稳态原子He(2^3S)与CH2Cl2间的传能反应,测得了由该反应产生的CH(A^2△-X^2П),CH(B^2∑^-X^2П)CH(C^2∑^+-X^2П)和H原子(Balmer系)的化学发光光谱。通过对CH(A,B)的光谱进行计算机模拟,推测出初手的CH(A^2△,v^1=0-2)态振动分布为No:N1:N2=100:40±5:19±2,CH(A^2△,v^1=0-0  相似文献   

2.
采用光学双共振多光子电离技术在静态池条件下测量了CO A^1П(v=3)能级上的绝对(J→J')转动传能截面,其中在J=3 ̄16、(e,f)被选择研究了;碰撞拌分别为He、Ne、Ar、HCl、CO2。在以上传能过程中发现明显的宇称守恒的倾向性规则。用能隙规则能很好地拟合大部分实验数据,并且采用Alexander等人的非弹性散射理论来解释宇称守恒定则。但是,当ΔJ=0时,对于碰撞伴Ar、HCl、CO  相似文献   

3.
利用以前我们得到的双原分子的振转波函数,计算了BN分子A^3П-X^3П带系Franck-Condon因子。计算中拢转动量子数的值由J=0取至J=180,结果适用于低温,高温和强激波条件。  相似文献   

4.
在成功制备C60外延薄膜的基础上,我们又尝试了碱金属Rb对该膜的掺杂。结果表明,从室温至80K左右,Rb3C60薄膜的电阻温度系数大于0,并近似符合公式:ρ(T)=a+bT^2,与单晶样品一致。但是,当温度低于80K以后,出现了弱的对数局域。在5K、零场下,样品的Jc值一般为10^3-10^4A/cm^2,且有如下规律:Jc(T)=Jc(0)(1-T/Tc)^a,α=1.3-2.0。此外,我们还测  相似文献   

5.
测量了CCl_4,CH_2Cl_2和CHCl_3对生物膜中磷脂酰胆碱作用的紫外电子吸收光谱,实验结果表明,由于CCl_4,CH_2Cl_2和CHCl_3分子结构的差异,三种溶剂的极性依次递增,磷脂酰胆碱π-π ̄*电子跃迁的吸收峰红移。磷脂酰胆碱在CCl_4中光谱呈单吸收峰,在CH_2Cl_2和CHCl_3中光谱特征呈双蜂结构,存在聚集体的激子态跃迁,由此给出了脂质分子聚集状态的光谱依据。  相似文献   

6.
Nd(Pro)3(Phen)Cl3·2H2O三元固体配合物的FTIR光谱和Raman光谱   总被引:2,自引:0,他引:2  
合成了Nd(Pro)3(Phen)Cl3.2H2O三元固体配合物,测定了配合物的 红外光谱和Raman光谱,对配合物分子的振动频率作了归属。光谱数据表明,钕(Nd )屯脯食氨酸(Pro)的羧酸基形成四员螯环,与邻啡罗啉(Phen)的C=N基形成五员螯环。  相似文献   

7.
利用以前我们得到的双原分子的振转波函数,计算了BN分子A3Π-X3Π带系的Franck-Condon因子。计算中转动量子数的值由J=0取至J=180,结果适用于低温、高温和强激波条件。  相似文献   

8.
Ce3+,Tb3+氟化物磷光体的发光性质比较   总被引:3,自引:1,他引:2  
采用溶液反应和固相反应分别合成了K3AlF6基质化合物及KBF4:Ce,Tb和K3AlF6:Ce,Tb等磷光体,研究了它们的光谱特性,并与KAlF4:Ce,Tb、CaF2:Tb和AlF3:Ce,Tb等磷光体的发光特性进行了比较。结果发现,CaF2:Ce,Tb、AlF3:Ce,Tb、KBF4:Ce,Tb和K3AlF6:Ce,Tb等磷光体中Ce^3+对Tb^3+的能量传递不能有效进行,有时Tb^3+起  相似文献   

9.
高温下CF4在H2中解离的反应动力学研究   总被引:2,自引:1,他引:1  
用单脉冲激波管研究了有少量CF3Cl参予下的CF4与H2的混合在高温下的反应动力学,发现主要产物为C2F4和CF3H。对实验结果的分析表明,反应过程为一个双中心链反应。始发反应为CF3Cl的C-Cl键的断裂,继之以由H2和CF4为媒介的双中心链传递,最后测得温度由1000至1080K,压力为0.1MPa下的CF4表观分解速率常数为keff=10^13.7exp(-55000/RT)l^1/2mol  相似文献   

10.
P538萃取锰(Ⅱ)的研究   总被引:1,自引:0,他引:1  
在25±0.5℃,用P538的环己烷溶液从NaClO4-HClO4介质中萃取Mn(Ⅱ)的反应机理为离子交换机理,萃取焓△H=-196kJ.mol^-1并用Cl^-离子水合作用和Mn^2+与Cl^-形成配合物的竞争解释了萃取分配比与水相中NaCl浓度的关系。  相似文献   

11.
A high-resolution analysis of the {nu(2), nu(3)} and {nu(4), nu(6)} bands of the two isotopomers of chloryl fluoride F(35)ClO(2) and F(37)ClO(2) has been carried out for the first time using simultaneously infrared spectra recorded around 16&mgr;m and 26&mgr;m with a resolution of ca. 0.003 cm(-1) and microwave and submillimeter-wave transitions occurring within the vibrational states 2(1), 3(1), 4(1), and 6(1). Taking into account the Coriolis resonances which link the rotational levels of the {2(1), 3(1)} and the {4(1), 6(1)} interacting states, it was possible to reproduce very satisfactorily the observed transitions and to determine accurate vibrational energies and rotational constants for the upper states 2(1), 3(1), 4(1), and 6(1) of both the (35)Cl and (37)Cl isotopic species. Copyright 2001 Academic Press.  相似文献   

12.
Rotational spectra have been recorded for both the 35Cl and 37Cl isotopic forms of two structural conformations of 2-chloroethyl ethyl sulfide (CEES). The rotational constants of the 35Cl and 37Cl isotopomers were used to identify the conformational isomers. A total of 236 hyperfine transitions have been assigned for 47 rotational transitions of the 35Cl isotope of a GGT conformer, and 146 hyperfine have been assigned for 37 rotational transitions of the 37Cl isotopomer. For the second conformer, a total of 128 (110) hyperfine and 30 (28) rotational transitions have also been assigned to the 35Cl (37Cl) isotopes of a TGT conformation. The extensive hyperfine splitting data, measured to high resolution with a compact Fourier transform microwave spectrometer, were used to determine both the diagonal and off-diagonal elements of the 35Cl and 37Cl nuclear quadrupole coupling tensors in the inertial tensor principal axis system. The experimental rotational constant data, as well as the 35Cl and 37Cl nuclear quadrupole coupling tensors, were compared to the results from 27 optimized ab initio (HF/6-311++G∗∗ and MP2/6-311++G∗∗) model structures.  相似文献   

13.
The microwave spectrum of 2-chloropyridine, C5H4NCl, has been studied in the frequency range from 26.5–40.0 GHz. The spectrum is characterized by strong parallel type transitions of a near-prolate asymmetric top. The assigned transitions have been used to evaluate the ground state rotational constants of the two chlorine isotopes. The rotational constants are (in MHz): A = 5872.52, B = 1637.83, C = 1280.48 for the 35Cl isotopic species and A = 5872.16, B = 1591.76, C = 1252.17 for the 37Cl isotopic species. The small inertial defect indicates the molecule is planar. In addition an excited vibrational state of C5H4N35Cl has been observed and analyzed. The chlorine quadrupolar coupling constants were determined for the ground state and are: χaa = ?71.9 MHz for 35Cl and χaa = ?54.9 MHz for 37Cl. By assuming the pyridine ring structure the CCl bond length is found to be 1.72 Å.  相似文献   

14.
The nuclear quadrupole hyperfine structure in rotational transitions of cis-1-chloro-2-fluoroethylene was measured for both (35)Cl and (37)Cl containing isotopomers in the millimeter-wave region. Near degeneracies of the 9(3,7) and 10(2,9) levels of (35)ClHC&dbond;CFH and of the 19(9,10/11) and 17(10,7/8) levels of (37)ClHC&dbond;CFH cause strong perturbations of the hyperfine patterns and give rise to perturbation-allowed DeltaJ = 2 and DeltaJ = 3 transitions. Lamb-dip measurements of such perturbed hyperfine patterns and of forbidden DeltaJ = +2 and perturbation-enhanced DeltaJ = 0 transitions of (35)ClHC&dbond;CFH provided an accurate determination of chi(ab), the off-diagonal element of the inertial nuclear quadrupole tensor. For (37)ClHC&dbond;CFH, chi(ab) was determined for the first time thanks to the observation of perturbed hyperfine patterns and of forbidden DeltaJ = +3 and DeltaJ = -2 transitions. Additional measurements of hyperfine structures led to improved values for the diagonal elements of the chi tensor of both (35)Cl and (37)Cl. Moreover, the complete inertial nuclear quadrupole tensor was evaluated from the field gradient at the chlorine nucleus computed by using the Multi-Configuration Self-Consistent Field (MCSCF) approach and employing basis sets of triple-zeta quality: very good agreement with the experiment was obtained. Copyright 2000 Academic Press.  相似文献   

15.
基于描述双核分子体系包含转动光谱常数Lv所在高阶项在内的跃迁能谱的经典表达式,采用差分收敛法(DCM)的物理思想,推导获得了求解双核分子体系P支跃迁谱线的另一解析表达形式。对于某一双核分子体系的P支跃迁带,新的谱线表达式仅需要11条精确的实验跃迁谱线就可以正确预言高激发振转态的谱线结构,同时,利用谱线展开系数C还可以进一步给出计算谱线的不确定度以更可靠地预言高激发振转态的跃迁谱线。推导获得了相应的计算公式以正确获得对应跃迁带的转动光谱常数(B_(v′),B_(v″),D_(v′),D_(v″),H_(v′),H_(v″),L_(v′),L_(v″))。应用新的谱线表达式,对~(35) Cl_2~+和~(35) Cl ~(37) Cl~+离子电子态A~2Π_u-X~2Π_g(Ω=1/2)跃迁体系(3,7)跃迁带的P支跃迁谱线进行了详细研究,获得的计算结果不但能完全重复已知的实验数据,还获得了实验上未能获得的包含高激发振转态在内的跃迁谱线。另外,通过计算同时也得到了各跃迁带的高阶转动光谱常数。该研究方法和计算结果为人们进一步正确认识Cl_2~+离子电子态的内部能级结构及物理化学的相关性质提供了更完整的参考数据。  相似文献   

16.
The rotational constants and quartic centrifugal distortion constants for NO235Cl and NO237Cl have been determined from an analysis of rotational transitions in the microwave and millimeter wave regions between 8.2–40 and 90–120 GHz, respectively.The values of the in-plane force constants in the general harmonic potential field have been obtained by combination of infrared and microwave data. Vibrational frequencies of 14NO2Cl and 15NO2Cl, inertia defects of NO235Cl in the excited vibrational states v3 = 1 and v5 = 1, and first-order centrifugal distortion constants of NO237Cl are the experimental data used in the least-squares fitting determination of force constants.  相似文献   

17.
The gas-phase infrared spectrum of the nu(4) fundamental band of CH(2)(79)BrF was recorded in the 1010-1116 cm(-1) wavenumber region using a TDL spectrometer. In this first high-resolution investigation of the synthesized (79)Br isotopic form, more than 10 200 transitions of this a/b-hybrid band centered at 1068.5385 cm(-1) were assigned and, using the Watson's A-reduced Hamiltonian in the I(r)-representation, a reliable set of molecular constants for the excited state v(4) = 1 was determined. From ground state combination differences having rotational quantum numbers J and K(a) up to 97 and 21, respectively, improved and extended ground state rotational and centrifugal distortion constants were calculated as well. Comparison between the observed and calculated band intensities in appropriate regions of the spectrum gave an estimate of the transition dipole-moment ratio along the a and b axes as ||Deltaμ(a)/Deltaμ(b) || = 2.0 +/- 0.2, in agreement with the predicted theoretical value of 1.99. Copyright 2000 Academic Press.  相似文献   

18.
The FTIR spectrum of chloro(sulphido)boron, Cl-B&bond;S, has been recorded at 0.0035 cm(-1) resolution. The nu(3) bands of the isotopomers (35)Cl(11)B(32)S, (37)Cl(11)B(32)S, (35)Cl(11)B(34)S, (37)Cl(11)B(34)S, (35)Cl(10)B(32)S, (37)Cl(10)B(32)S, and (35)Cl(10)B(34)S have been analyzed to yield effective rotational and centrifugal distortion constants for the ground and a number of excited vibrational states. For the (35)Cl(11)B(32)S isotopomer the nu(1) band has also been analyzed. The rotational constants have been used to determine equilibrium bond lengths of 168.42(8) and 160.14(8) pm for the Cl-B and B-S bonds, respectively. Copyright 2000 Academic Press.  相似文献   

19.
The diode-laser absorption spectrum of the nu(19a) band of the chlorobenzene molecule cooled in a supersonic jet is presented and transitions from low J, K(a), and K(c) values (0-14) are reported. The C(6)H(5)(35)Cl band center has been found at nu(0) = 1483.894 cm(-1) and rotational constants for the upper state have been determined from a least-squares fitting to experimental data. The band center for the C(6)H(5)(37)Cl isotope has also been obtained. Copyright 2000 Academic Press.  相似文献   

20.
The nu(3), nu(5), and nu(6) fundamental bands of the (13)CH(3)D molecule have been studied with Fourier transform infrared spectroscopy. The spectra and results for the parent species (12)CH(3)D (O. N. Ulenikov, G. A. Onopenko, N. E. Tyabaeva, J. Schroderus, and S. Alanko, J. Mol. Spectrosc. 193, 249-259 (1999)) have been used to assign and analyze about 1900 lines belonging to the (13)CH(3)D isotopic species. About 850 ground state combination differences with DeltaK = 0 were calculated, which allowed us to determine the J-dependent ground state rotational constants. The K-dependent constants as well as those describing the a(1)-a(2) (K = 3) splitting were fixed to the values obtained for the (12)CH(3)D species. The (v(3) = 1), (v(5) = 1), and (v(6) = 1) states were fit simultaneously by including the intervibrational interactions in the Hamiltonian. The rotational energies, the rotational and centrifugal distortion constants, as well as the resonance parameters involving the three states have been determined and discussed. Copyright 2000 Academic Press.  相似文献   

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