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1.
本文以aug-cc-pv5Z为基组, 采用考虑Davidson修正的多参考组态相互作用方法(MRCI+Q)得到了GeS分子基态(X1Σ+)和5个低激发态(11Σ, 11Δ, A1Π, 15Σ+, 25Σ+)的势能曲线. 计算结果表明: 25Σ+态为排斥态, 其余5个态为束缚态; 6个态有着共同的离解通道, 离解极限均为Ge(3P)+S(3P). 利用计算得到的势能曲线得了X1Σ+, 11Σ-, 11Δ, A1Π和15Σ+态的垂直跃迁能Te, 平衡键长Re, 离解能De, 谐振频率ωe, 非谐性常数ωexe及平衡位置的电偶极矩. X1Σ+态的Re 为2.034 Å, De 为5.728 eV, ωe为571.73 cm-1, ωexe为1.6816 cm-1, 平衡位置的电偶极矩为1.9593 Debye. 激发态11Σ, 11Δ, A1Π, 15Σ+的Te 依次为25904.81, 26209.22, 32601.19, 43770.26 cm-1; Re依次为2.313, 2.322, 2.188, 2.8790 Å; De依次为2.524, 2.487, 1.694, 0.3036 eV, ωe依次为358.90, 353.08, 376.32, 134.96 cm-1; ωexe依次为1.2421, 1.2151, 1.6608, 1.9095 cm-1; 平衡位置的电偶极矩依次为1.3178, 1.4719, 1.5917, -1.9785 Debye. 通过求解核运动的薛定谔方程得到了J=0时X1Σ+, 11Σ-, 11Δ, A1Π和15Σ+态前30个振动态的振动能级Gv和分子常数Bv, 得到的结果和已有的实验值及其他理论值符合较好.  相似文献   

2.
基体效应是影响LA-ICP-MS分析结果准确性的主要因素之一,但目前却没有一种量化基体效应研究的方法。提出了一种以分析元素与内标元素的强度比(Ii/Iis)为纵坐标、浓度比(ci/cis)为横坐标绘制Ii/Iis-ci/cis图,以元素对Ii/Iis-ci/cis图的线性相关系数量化基体效应的思路。以Fe为内标,考察了13个常用玻璃标准物质与2个硫化物标准及多个硫化物矿物中6个元素对的基体效应,结果显示Cu/Fe和Zn/Fe的线性相关系数r都小于0.99,而痕量元素对Mn/Fe,Co/Fe,Ga/Fe,Pb/Fe的线性相关系数r都大于0.999;以S为内标,考察了2个硫化物标准与多个硫化物矿物中三个主量元素对Fe/S,Cu/S和Zn/S的基体效应,结果显示其线性相关系数r都小于0.999。无论是以Fe为内标结合玻璃标准为外标,还是以S为内标结合硫化物标准为外标分析硫化物矿物,主量元素大多数分析结果的误差大于10%;而以Fe为内标时,绝大多数玻璃标准获得的痕量元素分析结果与MASS-1较为一致,误差小于15%。研究表明,玻璃标准及硫化物矿物标准均与硫化物矿物存在一定的基体效应差异,而采用元素对Ii/Iis-ci/cis图的线性相关系数r量化基体效应具有一定的合理性与实用性。研究也表明了以Fe为内标,采用非基体匹配的玻璃标准可用于定量分析硫化物矿物中的痕量元素,尤其是具有较高痕量元素含量的NIST610。  相似文献   

3.
研究了Yb3+/Er3+共掺60P2O5-15BaO-10Al2O3-5ZnO-10R2O(R=Na,K)以P2O5为主体的磷基有源光纤材料的光谱性质,以及不同Yb3+/Er3+掺杂浓度对光谱性质的影响规律。当Er3+浓度为9.100×1019/cm3、Yb3+的掺杂浓度为5.407×1020/cm3、Yb3+/Er3+浓度比为6:1时,玻璃样品在1 531 nm处的受激发射截面最大,为6.17×10-21 cm2。同时,其荧光寿命为9.73 ms,荧光半高宽为53.16 nm,发射截面与半高宽的乘积为3.28×10-32 m3,综合性能最佳。  相似文献   

4.
钟文英  黄斌  杨硕  王妍  魏霞 《光谱实验室》2012,29(4):1964-1969
以CdTe/CdS量子点为荧光探针,荧光猝灭为理论基础,设计出一种快速、超灵敏且高选择性的检测片剂与注射剂中VB1含量的方法。结果表明,VB1在2.0×10-7—5.0×10-5mg/mL的范围内线性良好,相关系数为0.9994,检出限(S/N=3)为0.12ng/mL。将3×10-5mg/mL的VB1标准溶液平行测定7次,RSD为0.64%,加标回收实验结果满意。  相似文献   

5.
以Tb4O7和Ga2O3(化学计量比为3: 5)、Ho2O3、Yb2O3为原料,其中Yb3+的掺杂浓度为8at.%,Ho3+的掺杂浓度分别为0.5at.%、1at.%、1.5at.%、2.0at.%,以碳酸氢铵为沉淀剂,在1 200 ℃下烧结10 h得到了Ho,Yb: Tb3Ga5O12(Ho,Yb: TGG)纳米粉体。对样品进行了XRD物相分析、热重-差热分析、红外光谱分析以及扫描电镜分析、上转换发射光谱分析。实验结果表明,温度为1 200 ℃下样品平均晶粒尺寸为38.10 nm。在泵浦源为980 nm激发下,Ho3+掺杂浓度为1.5at.%,Yb3+掺杂浓度为8at.%时,在红、绿、蓝波段范围内出现了明显的上转换发光现象,并对其形成机理进行了讨论。分析认为,Ho3+由激发态5S2,5F4向基态5I8跃迁,实现了绿光输出,而Ho3+由激发态5F55F3向基态5I8跃迁,分别实现了红光和蓝光输出。  相似文献   

6.
邱玉波  龙燕秋 《计算物理》1995,12(2):227-233
利用CTMC方法计算Cq+,Nq+,Oq+与H原子的碰撞过程的截面.入射粒子的能量范围为10~250keV/amu,离子为部分电离和完全电离的离子.给出了十二个耦合的Hamilton运动方程.用六个伪随机数确定粒子的轨道. Aq+离子和作用电子的势为模型势,其他两个势为纯库仑势。在计算中,需要2000个以上的轨道.引入约化变量σtr=σtr/q,E=E/q1/2,得到了q标度的俘获截面,这些截面数据都集中在一条曲线附近.计算结果与其他理论计算结果作了比较,它们符合得很好.  相似文献   

7.
在利用可见-近红外漫透射光谱技术对苹果的可溶性固形物(SSC)检测时,由于卤素灯光照射在苹果上的位置不同,采集到的苹果光谱中所包含的可溶性固形物信息不同,导致模型得出的结果不同;找到一个最好的苹果光照位置有利于得到最佳的可溶性固形物评价模型。利用多模式可调节的光学结构在相同的实验环境和实验条件下采集了购买于同一水果批发商的尺寸相近但照射位置不同的两批苹果的近红外漫透射光谱,探索苹果可溶性固形物模型建立过程中最佳的照射位置从而得到最佳位置的可溶性固形物评价模型。通过对样品进行光谱采集、糖度真值采集并结合化学计量学方法得出最佳的建模位置,照射位置为上部且光谱没有预处理时的偏最小二乘回归(PLS)模型性能为RMSEC为0.288 2,RMSEP为0.343 6,Rc为0.960 6,Rp为0.934 9;照射位置为斜上部且光谱没有预处理的PLS模型性能为RMSEC为0.340 7,RMSEP为0.513 3,Rc为0.931 1,Rp为0.863 6;照射位置为上部且光谱没有预处理的主成分分析回归(PCR)模型性能为RMSEC为0.573 6,RMSEP为0.601 4,Rc为0.842 4,Rp为0.800 7;照射位置为斜上部且光谱没有预处理的PCR模型性能为RMSEC为0.709 2,RMSEP为0.797 4,Rc为0.701 4,Rp为0.670 7,最佳照射位置为苹果上部;进一步地采用多种预处理方法对照射位置为上部的PLS模型进行对比,得到最优模型为MSC-PLS模型,其RMSEC为0.2264 4,RMSEP为0.301 5,Rc为0.966 9,Rp为0.949 9。最后再对相同的46个苹果进行相同的实验操作得到光谱、真值后,代入到建立的MSC-PLS模型中进行外部验证,结果显示外部验证的相关系数为0.930 58,验证均方根误差为0.843 59,验证了建立的MSC-PLS模型的稳定性和可靠性,进一步表明光谱采集位置为苹果上部时的近红外漫透射模型有很好的预测能力,该研究为预测苹果可溶性固形物的检测提供了技术支持。  相似文献   

8.
利用一种来源于PPV的发蓝光的齐聚物材料2,5,2',5'-tetra(4'-biphenylenevinyl)-biphenyl(TBVB)制作非掺杂的有机电致蓝光和白光器件。蓝光器件的结构为ITO/NPB/TBVB/Alq3/LiF/Al,其中TBVB用作发光层;白光器件的结构为ITO/NPB/TBVB/rubrene/Alq3/LiF/Al,其中TBVB与超薄层(平均“厚度”0.05~0.20nm)的Rubrene相结合用作发光层,二者分别发蓝光和黄光。在蓝光器件中,当TBVB的厚度为30nm时,器件发出色坐标为(0.20,0.26)的蓝光,其最大亮度和效率分别达到2154cd/m2和1.62cd/A。在白光器件中,可通过调节TBVB和Rubrene的厚度实现对器件发光色度的调节。当TBVB和Rubrene的厚度分别为10,0.15nm时,器件在亮度为4000cd/m2时发光色坐标为(0.33,0.34),非常接近白光等能点,且随着电压的变化始终处于白光区。当电压为16V时该器件达到最高亮度4025cd/m2;当电压为6V时器件有最高的效率3.2cd/A。  相似文献   

9.
在室温下采用直流磁控溅射以SiO2/Si为衬底制备了不同沟道层厚度的底栅式In2O3薄膜晶体管,讨论了沟道层厚度对底栅In2O3薄膜晶体管的电学性能的影响。实验结果表明:器件的特性与沟道层厚度有关,最优沟道层厚度的In2O3薄膜晶体管为增强型,其阈值电压为2.5 V,开关电流比约为106,场效应迁移率为6.2 cm2·V-1·s-1。  相似文献   

10.
介绍了一种具有高阈值电压和大栅压摆幅的常关型槽栅AlGaN/GaN金属氧化物半导体高电子迁移率晶体管。采用原子层淀积(ALD)方法实现Al2O3栅介质的沉积。槽栅常关型AlGaN/GaN MOS-HEMT的栅长(Lg)为2 μm,栅宽(Wg)为0.9 mm(0.45 mm×2),栅极和源极(Lgs)之间的距离为5 μm,栅极和漏极(Lgd)之间的距离为10 μm。在栅压为-20 V时,槽栅常关型AlGaN/GaN MOS-HEMT的栅漏电仅为0.65 nA。在栅压为+12 V时,槽栅常关型AlGaN/GaN MOS-HEMT的栅漏电为225 nA。器件的栅压摆幅为-20~+12 V。在栅压Vgs=+10 V时,槽栅常关型AlGaN/GaN MOS-HEMT电流和饱和电流密度分别达到了98 mA和108 mA/mm (Wg=0.9 mm), 特征导通电阻为4 mΩ·cm2。槽栅常关型AlGaN/GaN MOS-HEMT的阈值电压为+4.6 V,开启与关断电流比达到了5×108。当Vds=7 V时,器件的峰值跨导为42 mS/mm (Wg=0.9 mm,Vgs=+10 V)。在Vgs=0 V时,栅漏间距为10 μm的槽栅常关型AlGaN/GaN MOS-HEMT的关断击穿电压为450 V,关断泄露电流为0.025 mA/mm。  相似文献   

11.
Two-dimensional scanning of a 0.6328 mum guided-light beam has been realized using noncolinear acousto-optic (AO) coplanar Bragg diffraction together with colinear AO guided-mode to substrate radiation-mode conversion in a Z-cut Xpropagation LiNbO3 proton-exchanged (PE) waveguide. The two surface acoustic (SAW) waves utilized are at the center frequencies of 500 and 200 MHz, propagating in the Y and X axes, respectively. Two-dimensional scanning of approximately 720 resolvable light beam spots, namely, 18 40 (horizontal vertical) scanning, has been demonstrated using a light beam of 1.0 mm aperture. The total number of resolvable beam spots can be greatly increased from 720 by simply utilizing SAW transducers of larger bandwidth and a light beam of greater aperture. It should also be possible to significantly increase the diffraction efficiency from 3 % by optimizing the parameters of the PE waveguide and the SAWs.  相似文献   

12.
A simple technique of pulse compression, based on the linear chirp compensation of self-phase modulation (SPM) spectra in dispersion shifted fibers, is demonstrated. The optimization procedure is carried out, for a short span of a single-mode fiber, using a parabolic law, which describes the behavior of the squared output pulse width versus the pump peak power in the case of Gaussian pulses. The experimental results give a minimum pulse duration of 233 fs, which is in good agreement with the model. Shorter and coherent pulses, down to 90 fs, have been obtained by inserting an interference filter at the optical output.  相似文献   

13.
Results of a study of the effect of γ-radiation on the spectral luminescence properties of cadmium tungstate crystals doped with silver, bismuth, and molybdenum cations are presented. Spectral characteristics of the nondnnnoped crystals are briefly described. Absorption and photo and X-ray luminescence spectra of the crystals taken before and after exposure to γ-radiation (5.5·104 Gy) are compared. It is found that the spectral characteristics of the crystals doped with silver, bismuth, and molybdenum cations do not change markedly after the exposure. The relation between the type of impurity-induced defects, individual characteristics of the impurity cations, and the character of the effect of γ-radiation on the spectral luminescence properties of impure crystals is analyzed (preliminarily). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 64, No. 1, pp. 55–60, January–February, 1997.  相似文献   

14.
A multi-conjugate adaptive optics (MCAO) can offer a possibility of widening field of view (FOV) characterized by the isoplanatic angle, and the choose of conjugate height becomes a basic problem for MCAO, which influences the size of iosplanatic angle. Considering the application of lidar, the isoplanatic angle's expressions of two deformable mirrors (DMs) MCAO for uplink and downlink are deduced. The effects of conjugate heights for dual-conjugate AO are thoughtfully discussed, and the isoplanatic angles are further analyzed. The results show that the isopanatic angle varies with the conjugate height and reaches the maximum as the conjugate height is at the optimal altitude. Moreover, the optimal conjugate height changes with the propagation distance.  相似文献   

15.
Due to the limit of response speed of the present single-photon detector, the code rate is still too low to come into practical use for the present quantum key distribution (QKD) system.A new idea is put up to design a quick single-photon detector.This quick single-photon detector is composed of a multi-port optic-fiber splitter and many avalanche photo diodes (APDs).Au of the ports with APDs work on the time division and cooperate with a logic discriminating and deciding unit driven by the clock signal.The operation frequency lies on the number N of ports, and can reach N times of the conventional single-photon detector.The single-photon prompt detection can come true for high repetition-rate pulses.The applying of this detector will largely raise the code rate of the QKD, and boost the commercial use.  相似文献   

16.
17.
The Shanghai Synchrotron Radiation Facility(SSRF)booster ring,a full energy injector for the storage ring,is deigned to accelerate the electron beam energy from 150MeV to 3.5GeV that demands high extraction efficiency at the extraction energy with low beam loss rate when electrons are ramping.Closed orbit distortion(COD)caused by bending magnet field uniformity errors which affects the machine performance harmfully could be effectively reduced by bending magnet location sorting.Considering the affections of random errors in measurement,both ideal sorting and realistic sorting are studied based on measured bending magnet field uniformity errors and one reasonable combination of bending magnets which can reduce the horizontal COD by a factor of 5is given as the final installation sequence of the booster bending magnets in this paper.  相似文献   

18.
19.
40-GHz clock modulated signal as a pump to improve the efficiency of four-wave mixing (FWM)-based wavelength conversion in a 26.5-km dispersion shifted fiber (DSF) is investigated. The experimental results demonstrate that the conjugated FWM component has higher intensity with the clock pumping than that with the continuous-wave (CW) light pumping. The improvement of FWM-based wavelength conversion efficiency is negligible when the pump power is less than Brillouin threshold. But when the pump power is greater than Brillouin threshold, the improvement becomes significant and increases with the increment of pump power. The improvement can increase up to 9 dB if pump power reaches 17 dBm.  相似文献   

20.
Characterization of PolyA and PolyC mismatches by Raman spectroscopy   总被引:1,自引:0,他引:1  
A.C mismatches are studied by Raman spectral characterization of PolyA, PolyC, and their equimolar complex in solution of 0.14 mol/L Na ,pH7.0.Experimental results show that A·C mismatches occur to be A/B (mainly A) conformers, and unlike Watson-Crick base pairing, this kind of mismatches is stabilized by only one hydrogen bond involving cytosine N4H2 and adenine N7.The formation of A·C complex makes the base stacking interactions much stronger, and conformation of the backbone more ordered, which leads to obvious Raman hypochromic effect with some shifts in corresponding bands.  相似文献   

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