共查询到20条相似文献,搜索用时 62 毫秒
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研究了高位振动态RbH(X1∑+,v″=15~21)与CO2碰撞转移过程.脉冲激光激发RbH至高位态,利用激光感应荧光光谱(LIF)得到RbH(X1∑+,v″)与CO2的猝灭速率系数kv″(CO2),kv″=21(CO2)=2.7kvn=15(CO2).利用激光泛频光谱技术,测量了CO2(000,J)高转动态分布,得到了转动温度,从而获得了平均转动能rot>和转动能的变化<△Erot>,发现<△Erot>v″=21≈2.9<△Erot>v″=15.对于v″=16,证实了振动—振动能量转移的4-1近共振过程.在一次碰撞条件下,通过速率方程分析,得到RH(v″)-CO2振转速率系数.对于v″=15,J=32-48,速率系数在1.25-0.33×10-13cm3s-1.之间;对于v″=21,速率系数在2.47-1.53×10-13cm3s-1之间,其能量相关性是明显的. 相似文献
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制备了用过渡金属氧化物V2O5修饰Al源、漏电极的C60/Pentacene双层异质结有机场效应管.该构型器件与未修饰器件相比,呈现出典型的双极型晶体管传输特性.电子迁移率和空穴迁移率分别达到8.6×10-2cm2/V·s-1和6.4×10-2cm2/V·s-1,阈值电压分别为25 V和-25 V.器件性能改善的原因主要是由于插入V2O5修饰层后,可以明显降低Al电极与Pentacene之间的接触势垒,提高空穴的有效注入,从而使电子和空穴的注入接近平衡.研究表明,采用V2O5修饰电极方法,是制备低成本、高性能的双极型有机场效应管并实现其商业应用的有效途径. 相似文献
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本文用固相反应烧结制备出Li2Mo2O6多晶材料。经X射线分析、红外光谱和电子顺磁共振谱(EPR)的研究,确定了它的结构是Li2Mo2O4和MoO2两个晶相组成的烧结体。钼离子以四价状态存在于MoO2晶相结构中。采用交流阻抗谱分析了晶界与温度变化的相关性。测得了样品的ln(σ总T)-1/T 曲线是由两段直线和一段曲线所组成;总电导率化能σ27℃=1.36×10-3(Ω·cm)-1,σ115℃=1.49×10-3(Ω·cm)-1,σ300℃=9.71×10-3(Ω·cm)-1,σ370℃=2.42×10-3(Ω·cm)-1;电导活化能E1=0.043eV,E2=0.235eV,E平均=0.76eV。采用维格纳极化电池法测得电子电导率σe,σe27℃=2.240×10-5(Ω·cm)-1,σe300℃=4.476×10-3(Ω·cm)-1。实验证明,室温下材料为固体电解质,300℃附近为良好的离子与电子混合导体。
关键词: 相似文献
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对一种低温易烧结的Yb:Y2-2xLa2xO3激光透明陶瓷的光谱性能进行了初步研究,Yb:Y2-2xLa2xO3激光透明陶瓷具有宽的吸收带和大的吸收截面,在最强的吸收峰977nm处吸收截面达4.0×10-20cm2;其荧光发射寿命为1.1ms,发射截面在1033nm处为1.0×10-20cm2,在1077nm处为0.7×10-20cm2.Yb:Y2-2xLa2xO3陶瓷的各项光学性能指标接近或达到单晶的指标.
关键词:
氧化镧钇
激光陶瓷
低温烧结
光谱性能 相似文献
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近红外波段的气体吸收强度低,不利于痕量气体的测量。利用分子在中红外波段的基频吸收特性,使用单个新型室温连续输出量子级联激光器(CW-QCL)结合波长调制光谱技术(WMS)和长程光学吸收池,建立了一套高灵敏度和高精度的大气多组分温室气体同时检测的激光光谱系统。该系统的输出波数范围为2202.8~2205.6 cm-1,覆盖了CO、N2O和H2O的中心吸收谱线。实验测试结果表明:在1 s的时间分辨率下,CO、N2O和H2O的测量精度分别为1.83×10-8,1.86×10-9,1.19×10-4;当满足最佳积分时间(100 s)时,系统的最低检测限可以达到1.8×10-9(CO),0.16×10-9(N2O),1.5×10-5(H2O)。通过长时间测量和分析可知,所提系统部件简单,使用方便,满足大气多组分气体... 相似文献
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利用X射线粉末衍射确定了Tm3+掺杂硅酸镓镧(La3Ga5SiO14,LGS)晶体的晶体结构;运用DICVOL91程序计算了该晶体不同部位的晶胞参数;测定了Tm:LGS晶体的室温吸收谱和470nm光激发下的发射光谱;根据Judd-Ofelt理论拟合了Tm3+的三个晶场调节参数Ωt(t=2,4,6),分别为2.694×10-20cm2,1.842×10-20cm2,0.030×10-20cm2;计算了各个能级跃迁的谱线强度、振子强度、吸收截面等,进而计算了3H4和3F4态的自发跃迁概率、辐射寿命、荧光分支比和积分发射截面,并对结果进行了分析.
关键词:
Tm:LGS晶体
吸收谱
Judd-Ofelt理论
光谱参数 相似文献
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激发态Na2与H2碰撞,使H2(v=3,J=3)得到布居,在H2和He总气压为800Pa及温度为700K的条件下,利用相干反斯托克斯拉曼散射(CARS)光谱技术研究了H2(3,3)与H2(He)间转动能量转移过程。改变CARS激光束与激发Na2的激光之间的延迟时间,测量He不同摩尔配比时H2(3,J)态CARS谱强度的时间演化,得到H2(3,3)的总弛豫速率系数分别为=(21±5)×10-13cm3s-1和=(5.6±1.6)×10-13cm3s-1。测量H2(3,J)各转动态的相对CARS谱强度,由速率方程分析,得到H2(3,3)+H2→H2(3,J)+H2中,对于J=2,4,转移速率系数分别为11±4和8.2±3.1cm3s-1。在H2(3,3)+He→H2(3,J)+He中,对于J=2,4,转移速率系数分别为3.1±1.2和2.1±0.7cm3s-1。对于H2(3,3),单量子弛豫׀∆J׀=1约占该态总弛豫率的90%。 相似文献
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Collision-induced absorption in the translation-rotation band of H2 and H2-He mixtures has been measured from 20 to 900 cm-1 at 77.4, 195 and 292 K. To establish the accuracy of the results, various sources of error are investigated. The zeroth and first spectral moments are evaluated from experiment and theory for H2 at the various temperatures. To obtain theoretical moments consistent with the experimental values, the quantum pair-distribution function must be used. The major portion of the experimental moments can be accounted for by quadrupole-induced dipoles in H2 pairs. The remaining portion is attributable to an anistropic overlap interaction, although its magnitude depends on the value of the molecular parameters required to calculate the quadrupole contribution. 相似文献
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M. Kimura L. Pichl Y. Li H.-P. Liebermann R. J. Buenker I. F. Schneider 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2006,38(1):85-91
The positive water and hydronium ions are of interest in a
variety of chemical and biological applications. Here we study the
steric effect in charge transfer collisions, i.e. the spatial
dependence of single electron capture, in collisions mediated by
these ions. In particular, the steric effect is demonstrated in the
O+(2D)/H2 and H+/H2O charge transfer collisions in
the energy range of 100 eV/amu to 10 keV/amu. 相似文献
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Using a photon-particle delayed coincidence method the energy distributions of H +H(2p) and H++H(2p) fragment pairs have been measured arising from collisional dissociation of 10 keV H 2 + ions incident on various target gases. H fragments in their 2p state are identified by the Lymanα radiation emitted. The distribution of H+H(2p) fragment pairs arising from dissociative charge exchange reveals a sharp increase below 0.2 eV in the center-of-mass frame of the H 2 + ion. This is ascribed to predissociation of vibrational levels of higher H2 Rydberg states close above then=2 dissociation limit by those H2 Rydberg states which separate into H+H(2p) fragments. Only direct transitions into the continuum of theGK 1 ∑ g + state may compete. Some structure at 0.3–0.5 eV is attributed to the three statesI 1 П g,i 3 П g, andh 3 bE g + having potential barriers of this height. The distributions for H++H(2p) have maxima at 3.4, 3.8, and 4.2 eV for a H2, Ar, and He target, respectively, indicating that the 2pπ u state as well as the 3dσ g state ofH 2 + is excited. The H+H(2p) process has a greater probability than the H++H(2p) process for Ar and H2 targets, though all electronic H2 states under consideration are bound. 相似文献
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The collision-induced fundamental infrared absorption band of hydrogen in binary mixtures H2He and H2Ne at 77, 195, 273, and 298 K has been studied with absorption path lengths of 27 and 105 cm for gas densities up to 530 amagat for several base densities of hydrogen. In each of these mixtures the enhancement absorption profiles show, in addition to the usual splitting of the Q branch into the main QP and QR components, a splitting of the S(1) line into the SP(1) and SR(1) components at all the experimental temperatures and a secondary splitting of the main QP component into the QP(3) and QR(3) components at 273 and 298 K. The profiles of H2He at 77 K also show a splitting of the S(0) line into SP(0) and SR(0). Integrated absorption coefficients were measured and binary and ternary absorption coefficients were derived. Van Kranendonk's theory of the ‘exponential-4’ model for the induced dipole moment was applied to the experimental binary absorption coefficients. The quadrupolar parts of these coefficients were calculated from the known molecular parameters and were then subtracted from the experimental values to obtain the overlap parts. The overlap parameters λ and ρ, giving respectively the magnitude and range of the overlap moment, were determined for each of the mixtures by obtaining the best fit of the calculated overlap part of the binary absorption coefficient as a function of temperature to the experimental values of the overlap parts. The values of λ, ρ, and μ(σ) (the overlap induced dipole moment at the Lennard-Jones intermolecular diameter σ) are as follows:
Mixture | λ | ρ | μ(σ) |
H2He | 5.6 × 10?3 | 0.24 Å | 2.92 × 10?2ea0 |
H2Ne | 9.0 × 10?3 | 0.29 Å | 4.85 × 10?2ea0 |