563～660 nm波段SO2+的PHOFEX连续谱

在超声分子束条件下 ,利用 380 .85nm的电离激光使SO2 分子经由 [3+1]共振增强多光子电离(REMPI)产生纯净的SO2 + ( X 2A1)分子离子 ,用另一束解离激光在可见光波长区 (5 6 3～ 6 6 0nm)扫描获得了光解碎片SO+ 的激发 (PHOFEX)谱 .从 5 6 3～ 6 6 0nm波长区SO+ 的无结构连续谱以及SO2 + 解离的效率随波长增加而减少的实验事实 ,提供了SO2 + ( E , D , C )电子态附近存在α2 A2 对称性排斥态的证据 ,分析了产生SO+ 的 [1+1]光解机理 :(1)SO2 + ( X 2 A1)首先经由单光子激发到达 B2B2 中间态的密集能级区 ;(2 )吸收另一个光子到达SO2 + ( E , D , C )电子态附近的α2 A2 排斥态 ,经由α2 A2 排斥态产生了到SO+ (X 2Π) +O(3 Pg)的直接解离 .     

N2O+离子A2∑+电子态的光谱研究

用一束波长为360.55 nm的激光,通过N2O分子的(3+1)共振增强多光子电离过程制备纯净的母体离子N2O+X2Ⅱ3/2,1/2(000).用另一束可调谐激光将N2O+离子激发至预解离态A2Σ+,利用飞行时间质谱检测解离碎片NO+离子强度随光解光波长的变化,在278-328 nm波长范围内获得了光解碎片的激发(PHOFEX)谱.观测到了N2O+离子A2Σ+←X2Ⅱ电子跃迁较丰富的振动谱带.通过对PHOFEX光谱的标识,获得了A2∑+态较准确和全面的分子光谱常数.     

CS2+( 2Πg )的(1+1)光解离动力学研究

在气束条件下,利用483．2nm的激光（3＋1）共振增强多光子电离（REMPI）CS2分子以产生CS2＋离子源,用另一束可调谐激光在424－482nm内,通过对CS2^+(x^2∏g)(1+1)双光子共振解离产生的碎片离子发谱的探测,来获取CS2^+的光解离动力学信息,光解离碎片S^+的激光发谱（PHOFEX）可归属为CS2^+（A^2∏u,3/2(v′=0-4,v′＝v1_(1/2)v2-)←X^2′∏g,3/2(0,0,0))和（A^2∏u,1/2(v=0-4)←X^2∏g,1/2(0,0,0))跃迁,对CS2^+光解离动力学的研究表明,其产生S^+的通道为：（i)CS2吸收一个光子从基态X^2∏g共振激发至A^-2∏u态,（ii)已布居的A^-2∏u态的振动能级和X^2-∏g态的高振动能级产生耦合,（iii)吸收第二个光子从上述耦合的振动能级进一步激发至B^2∑u^+态,再通过B^-2∑u^+态与^4∑^-态间的自旋－轨道相互作用,经由4∑^-排斥态解离产生S^+_CS。     

563—660nm波段S02^＋的PHOFEX连续谱

在超声分子束条件下，利用380．85nm的电离激光使SO2分子经由[3+1]共振增强多光子电离(REM—PI)产生纯净的S02^+(X^2A1)分子离子，用另一束解离激光在可见光波长区(563—660nm)扫描获得了光解碎片S0^+的激发(PHOFEX)谱．从563—66nm波长区SO^+的无结构连续谱以及S02^+解离的效率随波长增加而减少的实验事实，提供了S02^+(E，D，C)电子态附近存在α^2A2对称性排斥态的证据，分析了产生S0^+的[1+1]光解机理：(1)S02^+(X^2A1)首先经由单光子激发到达B^2B2中间态的密集能级区；(2)吸收另一个光子到达S02^+(E，D，C)电子态附近的α^2A2排斥态，经由α^2A2排斥态产生了到S0^+(X^2∏)+O(^3P6)的直接解离．     

N2O^＋离子A^2Σ^＋电子态的光谱研究

用一束波长为360．55nm的激光，通过N2O分子的(3 1)共振增强多光子电离过程制备纯净的母体离子N2O^ X^2Π3/2,1/2(000)．用另一束可调谐激光将N2O^ 离子激发至预解离态A^2Σ^ ，利用飞行时间质谱检测解离碎片NO^ 离子强度随光解光波长的变化，在278—328nm波长范围内获得了光解碎片的激发(PHOFEX)谱．观测到了N2O^ 离子A^2Σ^ ←X^2Π电子跃迁较丰富的振动谱带．通过对PHOFEX光谱的标识，获得了A^2Σ^态较准确和全面的分子光谱常数．     

N2O+离子A2Σ+电子态的光解动力学研究

用一束波长为360.55nm的激光，通过N2O分子的（3+1）共振多光子电离（REMPI）过程制备纯净且布居完全处于X2Π(000)态的母体离子N2O+，然后用另一束波长在275—328nm范围内的可调谐激光将制备的N2O+离子激发至预解离电子态A2Σ+.实验发现，由于解离碎片NO+所具有的一定的反冲速度，其TOF质谱峰明显比N2O+母体宽.通过分析NO+碎片TOF质谱峰形状，得到了解离产物的总平均平动能〈ET〉；通过考察〈ET〉随光解能量的变化，发现光解能量在32000cm-1附近约250cm-1的变化 关键词： N2O+离子A2Σ+态 TOF质谱峰 预解离机理     

N_2O~ 离子A~2Σ~ 电子态的光解动力学研究

用一束波长为 36 0 5 5nm的激光 ,通过N2 O分子的 (3 1 )共振多光子电离 (REMPI)过程制备纯净且布居完全处于X2 Π(0 0 0 )态的母体离子N2 O ,然后用另一束波长在 2 75— 32 8nm范围内的可调谐激光将制备的N2 O 离子激发至预解离电子态A2 Σ .实验发现 ,由于解离碎片NO 所具有的一定的反冲速度 ,其TOF质谱峰明显比N2 O 母体宽 .通过分析NO 碎片TOF质谱峰形状 ,得到了解离产物的总平均平动能〈ET〉 ;通过考察〈ET〉随光解能量的变化 ,发现光解能量在 32 0 0 0cm- 1 附近约 2 5 0cm- 1 的变化范围内 ,〈ET〉值由约 80 0 0cm- 1 突然减小至约 1 6 0 0cm- 1 .通过分析 ,在光解能量小于 32 0 0 0cm- 1 的区域 ,解离通道为NO (X1 Σ ) N(4 S) ;而在光解能量大于 32 0 0 0cm- 1 的区域 ,另一个具有较高解离限的解离通道 ,NO (X1 Σ ) N(2 D) ,开启并完全取代N(4 S)通道成为解离的惟一通道 .根据实验结果 ,对在所研究的光解能量范围内的N2 O 离子A2 Σ 电子态预解离机理进行了探讨     

N2O+离子A2∑+电子态的光解动力学研究

用一束波长为360.55nm的激光,通过N2O分子的(3+1)共振多光子电离(REMPI)过程制备纯净且布居完全处于X2Ⅱ(000)态的母体离子N2O+,然后用另一束波长在275-328nm范围内的可调谐激光将制备的N2O+离子激发至预解离电子态A2∑+.实验发现,由于解离碎片NO+所具有的一定的反冲速度,其TOF质谱峰明显比N2O+母体宽.通过分析NO+碎片TOF质谱峰形状,得到了解离产物的总平均平动能;通过考察随光解能量的变化,发现光解能量在32000cm-1附近约250cm-1的变化范围内,值由约8000cm-1突然减小至约1600cm-1.通过分析,在光解能量小于32000cm-1的区域,解离通道为NO+(X1∑+)+N(4S);而在光解能量大于32000cm-1的区域,另一个具有较高解离限的解离通道,NO+(X1∑+)+N(2D),开启并完全取代N(4S)通道成为解离的惟一通道.根据实验结果,对在所研究的光解能量范围内的N2O+离子A2∑+电子态预解离机理进行了探讨.     

N2O+离子A2Σ+电子态高振动能级的转动结构分析

利用一束波长为36055nm的激光,通过(3+1)共振多光子电离方法制备纯净的且处于X²Π_1/2,3/2(000)态的N₂O⁺离子,用另一束激光激发所制备的离子到第一电子激发态A²Σ⁺的不同振动能级,然后解离,通过检测解离碎片NO⁺强度随光解光波长的变化,得到了转动分辨的N₂ 关键词： 2O⁺离子A²Σ⁺电子态')" href="#">N₂O⁺离子A²Σ⁺电子态 共振增强多光子电离 光解碎片激发光谱 光谱常数     

N2O+离子A2Σ+电子态高振动能级的转动结构分析

利用一束波长为360.55nm的激光,通过(3 1)共振多光子电离方法制备纯净的且处于X2Π1/2,3/2(000)态的N2O 离子,用另一束激光激发所制备的离子到第一电子激发态A2Σ 的不同振动能级,然后解离,通过检测解离碎片NO 强度随光解光波长的变化,得到了转动分辨的N2O 碎片激发谱.通过对光谱转动结构的拟合,获得了N2O 离子A2Σ 电子态一系列高振动能级的转动常数和自旋分裂常数.     

Critical point phenomena in the electrical resistivity of binary liquid systems: CS2 + CH3CN and CS2 + CH3NO2

Electrical resistance measurements are reported on the binary liquid mixtures CS₂ + CH₃CN and CS₂ + CH₃NO₂ with special reference to the critical region. Impurity conduction seems to be the dominant mechanism for charge transport. For the liquid mixture filled at the critical composition, the resistance of the system aboveT _c follows the relationR=R _c−A(T−T _c) ^b withb=0·6±0·1. BelowT _c the conductivities of the two phases obey a relation σ₂−σ₁=B(T _c−T)^β with β=0·34±0·02, the exponent of the transport coefficient being the same as the exponent of the order parameter, an equilibrium property.     

Nonadiabatic couplings and charge transfer study in H + CS+ collision using time-dependent quantum dynamics

Experiments have reported the high stability of HCS⁺ ion and inhibit to decompose over the range of collision energies. In this study, the various energy transfer channels of atomic H collision with CS⁺ molecular ion has been performed by ab initio computations at the multireference configuration interaction/aug-cc-pVQZ level of theory. The ground and several low-lying excited electronic state potential energy surfaces in three different molecular orientations, namely, two collinear configurations with, (1) H approaching the S atom (γ = 0°), (2) H approaching the C atom (γ = 180°) and one perpendicular configuration, (3) H approaching the centre of mass of CS (γ = 90°) with the diatom fixed at the equilibrium bond length, have been obtained. Nonadiabatic effects with Landau–Zener coupling leading to avoided crossings are observed between the ground- and the first-excited states in γ = 90° orientation, and also between the first- and second-excited states in γ = 180° orientation. Quantum dynamics have been performed to study the charge transfer using time-dependent wave packet method on the diabatic potential energy surfaces. The probability of charge transfer is found to be highest with 42% in γ = 180°. The high charge transfer probability result in the formation of H⁺ + CS channel which ascertains the high stability of HCS⁺ ion.     

CS21B2(1Σ+u)态预离解产物CS的振转布居研究

用一束波长为 2 10 .2 7nm的激光将CS2 分子激发至预离解态1B2 (1Σ+ u) ,用另一束激光通过激光诱导荧光 (LIF)方法检测碎片CS ,在 2 5 0 .5～ 2 86 .5nm获得了CS碎片A1Π←X1Σ+ 振转分辨的激发谱 .通过对光谱强度的分析 ,获得了CS碎片v″ =0～ 8的振动布居和v″=1,4～ 8振动态的转动布居 .结果发现 ,碎片CS的振动布居呈双模结构 ,分别对应于CS2 分子1B2 (1Σ+ u)态的两个解离通道 ,即CS(X1Σ+ ,v″=0～ 9) +S(3 PJ)和CS(X1Σ+ ,v″ =0～ 1)+S(1B2 ) .由此得到两个解离通道的分支比S(3 PJ) :S(1B2 )为 5 .6± 1.2 .与前人 193nm处的研究结果相比 ,2 10 .2 7nm激发更有利于S(3 PJ)通道的生成 .此外 ,实验还发现CS的转动布居不满足热平衡分布 ,为两个Boltzmann分布的合成     

Nonlinear refraction in CS2

The nonlinear refractive index () of CS₂ was measured using the Z-scan technique and laser radiation of various (femto-, pico-, and nano-second) pulse durations. We observed the growth of with the increase of the pulse duration (from (3±0.6)×10^-15 cm²W^-1 at 110 fs to (4±2)×10^-14 cm²W^-1 at 75 ns) due to the additional influence of the molecular reorientational Kerr effect in the case of longer (picosecond and nanosecond) pulses. Acoustic wave induced negative nonlinear refraction was observed using wavefront analysis. We analyzed the simultaneous influence of both electronic and molecular processes leading to the positive nonlinear refraction and acoustic processes leading to the negative nonlinear refraction in carbon disulfide. Variations of the refractive index due to the thermal effect at high pulse repetition rates were also investigated. PACS 42.65.An; 42.65.Jx; 78.66.Nk     

Multistep ionization of CS2 vapour

We report on the multistep ionization process observed in CS₂ vapour irradiated by 337 nm nitrogen laser light. We propose and discuss a model in which optical as well as collisional excitation are involved in the ionization process.     

二极管阵列紫外分光光度法测定西埃斯

利用紫外分光光度法对西埃斯进行检测,在0.2072-10.36μg/mL浓度范围内线性关系良好(R2=0.9990),检出限为0.0518μg/mL,相对标准偏差(RSD)为0.82％,回收率在99.3％-100.1％之间.本法操作简便,准确,能较好的应用于气溶胶中痕量西埃斯的测定.     

Laser induced lasing in CS2 vapor

When CS₂, contained in a tube at pressures ranging from 350 to 450 mTorr, was optically excited by a pulsed laser at a wavelength of 343.6 nm to the J=29, v=(0, 10, 0), R ³ B ₂ state (i.e., the =0 component of the a ³ A ₂ state), six coherent emissions were observed along the same axis from both ends of the tube. These emissions possess the characteristics of the pump laser, such as linewidth, pulse duration and polarization, but do not need a cavity to gain amplification. The emissions terminate on the high vibrational states of the ground electronic state. A time delay between the pump laser and the emissions was observed. The emission intensity depends non-linearly on the CS₂ pressure and exhibits a third order power dependence. A cooperative stimulated emission model is proposed to explain this phenomenon.     

CFETR CSģ����Ȧ�ĵ�ŷ���

在中国聚变工程试验堆(CFETR)的概念设计阶段,为了将来正确设计和顺利加工其中心螺线管(CS)线圈,设计了一个由Nb3Sn内线圈和NbTi外线圈组成的模型线圈。采用线电流模型和后期数据处理的方法对其磁场做了精确计算,解决了线电流模型不能计算导线内部磁场的问题。在此基础上计算了线圈的电感和电磁应力等参数。     

CFETR CS模型线圈的电磁分析

在中国聚变工程试验堆(CFETR)的概念设计阶段,为了将来正确设计和顺利加工其中心螺线管(CS)线圈,设计了一个由Nb₃Sn内线圈和NbTi外线圈组成的模型线圈。采用线电流模型和后期数据处理的方法对其磁场做了精确计算,解决了线电流模型不能计算导线内部磁场的问题。在此基础上计算了线圈的电感和电磁应力等参数。     

Molecule opacity study on low-lying states of CS

CS molecule, which plays a key role in atmospheric and astrophysical circumstances, has drawn great attention for long time. Owing to its large state density, the detailed information of the electronic structure of CS is still lacking. In this work, the high-level MRCI+Q method is used to compute the potential energy curves, dipole moments and transition dipole moments of singlet and triplet states correlated with the lowest dissociation limit of CS, based on which high accurate vibration—rotation levels and spectroscopic constants of bound states are evaluated. The opacity of CS relevant to atmospheric circumstance is computed at a pressure of 100 atms for different temperatures. With the increase of temperature, band systems from different transitions mingle with each other, and band boundaries become blurred, which are originated from the increased population on vibrational excited states and electronic excited states at high temperature.