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K-Ar光学碰撞精细结构分支比 被引量:6
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作者 沈异凡 李万兴 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2001年第1期38-39,共2页
用激光激发K Ar混合气体 ,KAr分子激发态离解到K 4P1/2 和 4P3/2 态 ,测定在不同Ar密度下KD1与D2 线荧光强度比 ,得到离解率之比和精细结构转移截面。
关键词 光学碰撞 精细结构 分支比 激光激发 氩化钾分子 离解率
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Rb-He光学碰撞中精细结构分支比的测量 被引量:2
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作者 吕磊 李琳 +3 位作者 邓玉华 张岩文 戴康 沈异凡 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2009年第7期1732-1735,共4页
脉冲激光激发Rb+He混合系统,激光频率(ν)调离Rb(5S1/2)→Rb(5PJ)共振频率(rνes)Δ(Δ=ν-rνes)。研究了光学碰撞Rb(5S1/2)+He+hν→Rb(5PJ)+He转移过程。激光激发RbHe分子态。RbHe激发态解离到5P1/2或5P3/2态,其布居数密度分别为n1和... 脉冲激光激发Rb+He混合系统,激光频率(ν)调离Rb(5S1/2)→Rb(5PJ)共振频率(rνes)Δ(Δ=ν-rνes)。研究了光学碰撞Rb(5S1/2)+He+hν→Rb(5PJ)+He转移过程。激光激发RbHe分子态。RbHe激发态解离到5P1/2或5P3/2态,其布居数密度分别为n1和n2,定义分支比为n1/n2。为得到分支比,在-180cm-1<Δ<200 cm-1范围内测量了I(D1)(5P1/2→5S1/2)与I(D2)(5P3/2→5S1/2)的相对时间积分强度比R,解速率方程组,得到一个与气压成线性关系的直线方程,从该直线的截距及斜率得到5P1/2→5P3/2的碰撞转移截面及分支比,在D2线蓝翼,分支比随失谐量Δ的增加而增加到0.2。在D1线红翼分支比近似为40而与失谐量无关。从翼激发测量得的精细结构碰撞转移截面为(1.1±0.3)×10-17cm2,与从共振激发得到的截面值是一致的。测量结果表明,原子相互作用势和非绝热效应在分子解离动力学中起关键作用。 展开更多
关键词 精细结构 光学碰撞 分支比 测量 原子相互作用势 解离动力学 激光激发 直线方程
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Cs-N_2光学碰撞精细结构分支比的实验研究 被引量:2
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作者 张刚台 穆保霞 +4 位作者 袁强华 崔秀花 王淑英 戴康 沈异凡 《激光杂志》 CAS CSCD 北大核心 2006年第5期41-42,共2页
光学薄的Cs蒸气和低密度的N2混合系统被激光激发,激光频率调至Cs共振跃迁的两翼,CsN2分子激发态解离到Cs(6P1/2)或Cs(6P3/2)态,测量了分支比I(D1)/I(D2),这里I(D1)和I(D2)分别为CsD1和D2线的谱线强度,由速率方程分析,得到了解离率之比... 光学薄的Cs蒸气和低密度的N2混合系统被激光激发,激光频率调至Cs共振跃迁的两翼,CsN2分子激发态解离到Cs(6P1/2)或Cs(6P3/2)态,测量了分支比I(D1)/I(D2),这里I(D1)和I(D2)分别为CsD1和D2线的谱线强度,由速率方程分析,得到了解离率之比和精细结构转移截面。用共振激发Cs(6P3/2)态,也得到了精细结构转移截面。对结果进行了讨论。 展开更多
关键词 激光光谱 光学碰撞 光解离 截面
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Rb-Rb光学碰撞精细结构分支比的实验研究 被引量:2
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作者 赖康荣 张刚台 +3 位作者 袁强华 崔秀花 戴康 沈异凡 《新疆大学学报(自然科学版)》 CAS 2005年第4期430-433,共4页
研究了在R b52P多重态与R b原子基态的光学碰撞中的精细结构分支比,激光频率调至R b共振跃迁的红翼,定义分支比为I(D1)/I(D2),I(D1)、I(D2)分别为R b的D1和D2线的荧光强度,测量了激光频率从R b5P3/2红翼15cm-1调至50cm-1的分支比,在5P3/... 研究了在R b52P多重态与R b原子基态的光学碰撞中的精细结构分支比,激光频率调至R b共振跃迁的红翼,定义分支比为I(D1)/I(D2),I(D1)、I(D2)分别为R b的D1和D2线的荧光强度,测量了激光频率从R b5P3/2红翼15cm-1调至50cm-1的分支比,在5P3/2的近红翼,分支比与失谐量有很大的关系.同时测量了R b5PJ态的精细结构转移截面,截面值2σ1为3.2×1-0 15cm2. 展开更多
关键词 光学碰撞 分支比 RB 精细结构
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Cs-He光学碰撞中的非绝热跃迁
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作者 崔秀花 穆保霞 +4 位作者 王淑英 袁强华 张刚台 戴康 沈异凡 《新疆大学学报(自然科学版)》 CAS 2006年第2期174-176,共3页
激光激发Cs+He碰撞复合物,测量了Cs(62P)精细结构布居数分支比,由此证实了发生在光学碰撞中的非绝热跃迁.激光频率从Cs(6P3/2)红翼30cm-1调至蓝翼30cm-1,在6P3/2的近翼,分支比与矢谐量有很大的关系.同时测量了Cs(6PJ)态的精细结构转移截... 激光激发Cs+He碰撞复合物,测量了Cs(62P)精细结构布居数分支比,由此证实了发生在光学碰撞中的非绝热跃迁.激光频率从Cs(6P3/2)红翼30cm-1调至蓝翼30cm-1,在6P3/2的近翼,分支比与矢谐量有很大的关系.同时测量了Cs(6PJ)态的精细结构转移截面,截面值σ21=9.8×10-19cm2. 展开更多
关键词 光学碰撞 分支比 CS 截面
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K—He光学碰撞精细结构分支比的测定
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作者 沈异凡 《激光与光电子学进展》 CSCD 2001年第9期3-3,共1页
氩离子激光器514.5nm线激发光学薄的K蒸汽和低密度He的混合系统,得到KHe分子激发态,此激发态通过预离解,直接离解或碰撞离解,使K 4P1/2,4P3/2得到布居,同时发生精细结构碰撞转移K 4P1/2+He->K 4P3/2+He. 直径2.5 cm,长10 cm的K-He混... 氩离子激光器514.5nm线激发光学薄的K蒸汽和低密度He的混合系统,得到KHe分子激发态,此激发态通过预离解,直接离解或碰撞离解,使K 4P1/2,4P3/2得到布居,同时发生精细结构碰撞转移K 4P1/2+He->K 4P3/2+He. 直径2.5 cm,长10 cm的K-He混合池为玻璃材料,高温烘烤,真空度10-4 Pa,充入少量金属K及密度约为2~8×1017 cm-3的He,池温保持在373 K,温度由热电偶测量,激光束直径约为0.5 cm,激光功率约200 mW,在垂直激光束方向检测KD1和D2线荧光,荧光聚焦在单色仪的狭缝上,经单色仪分光后进入被冷却的光电倍增管,光子计数器记录D1和D2线荧光信号,从而得到荧光强度比R. 对D1和D2线多次扫描,得到R的平均结果,描绘出(0.62-R)-1与He原子密度的实验结果,(0.62-R)-1与N确成线性关系,由此直线的斜率和截距,得到KHe分子常数B=0.53,转移截面σ12=6.1×10-15 cm2.(OA10) 展开更多
关键词 精细结构分支比 K-He光学碰撞 氢离子激光器
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激发态C8(6^2P)原子与N2、He的碰撞能量转移截面 被引量:1
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作者 袁强华 殷桂琴 +1 位作者 戴康 沈异凡 《激光杂志》 CAS CSCD 北大核心 2006年第3期8-9,共2页
研究了Cs(62P)多重态分别与N2、He的光学碰撞中的精细结构分支比,定义分支比为|(D1)/|(D2),|(D1)、|(D2)分别为Cs的D1和D2线的荧光强度。单模半导体激光器激发Cs原子到6P3/2态,通过与N2、He的激发转移、碰撞传能研究了62p原子的精细结... 研究了Cs(62P)多重态分别与N2、He的光学碰撞中的精细结构分支比,定义分支比为|(D1)/|(D2),|(D1)、|(D2)分别为Cs的D1和D2线的荧光强度。单模半导体激光器激发Cs原子到6P3/2态,通过与N2、He的激发转移、碰撞传能研究了62p原子的精细结构混合,得到了6P→6P的转移截面如下:Cs-He的转移截面为σ=2.25×10-19cm2,Cs-N的转移截面为σ=1.808×10-18cm2。并对结果进行了讨论。 展开更多
关键词 截面 光学碰撞 分支比 精细结构
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SUSY QCD Impact on Top-Pair Production Associated with a Z^0-Boson at a Photon-Photon Collider
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作者 DONG Chuan-Fei MA Wen-Gan ZHANG Ren-You GUO Lei WANG Shao-Ming 《Communications in Theoretical Physics》 SCIE CAS CSCD 2009年第8期302-310,共9页
The top-pair production in association with a Z^0-boson at a photon-photon collider is an important process in probing the coupling between top-quarks and vector boson and discovering the signature of possible new phy... The top-pair production in association with a Z^0-boson at a photon-photon collider is an important process in probing the coupling between top-quarks and vector boson and discovering the signature of possible new physics. We describe the impact of the complete supersymmetric QCD (SQCD) next-to-leading order (NLO) radiative corrections on this process at a polarized or unpolarized photon collider, and make a comparison between the effects of the SQCD and the standard model (SM) QCD. We investigate the dependence of the lowest-order (LO) and QCD NLO corrected cross sections in both the SM and minimal supersymmetric standard model (MSSM) on colliding energy √s in different polarized photon collision modes. The LO, SM NLO, and SQCD NLO corrected distributions of the invariant mass of tt^--pair and the transverse momenta of final Z^0-boson are presented. Our numerical results show that the pure SQCD effects in γγ →tt^- Z^0 process can be more significant in the ++ polarized photon collision mode than in other collision modes, and the relative SQCD radiative correction in unpolarized photon collision mode varies from 32.09% to -1.89% when √s goes up from 500 GeV to 1.5 TeV. 展开更多
关键词 supersymmetric QCD photon-photon collider top-gauge boson coupling
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The Top-Charm Associated Production Within the R-Parity Violating Supersymmetric Model in Photon-Proton Collisions
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作者 HOUHong-sheng MAWen-Gan 《Communications in Theoretical Physics》 SCIE CAS CSCD 2002年第3期337-346,共10页
The top-charm associated production with the effects from both B- and L-violating interactions in TeV scale photon-proton collisions is investigated in the framework of minimal supersymmetric standard model. Within t... The top-charm associated production with the effects from both B- and L-violating interactions in TeV scale photon-proton collisions is investigated in the framework of minimal supersymmetric standard model. Within the bounds on the relevant R-parity violating couplings, the total cross section will reach the order of 10 fb in some parts of the parameter space. 展开更多
关键词 R-parity violation minimal supersymmetric standard model flavor changing neutral current
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Measurement of Collision Conditions in Magnetic Pulse Welding Processes
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作者 Joerg Bellmann Eckhard Beyer +3 位作者 Joem Lueg-Althoff Soeren Gies A. Erman Tekkaya Sebastian Schulze 《Journal of Physical Science and Application》 2017年第4期1-10,共10页
MPW (magnetic pulse welding) is a solid state joining technology that allows for the generation of strong metallic bonds, even between dissimilar metals. Due to the absence of external heat, critical intermetallic p... MPW (magnetic pulse welding) is a solid state joining technology that allows for the generation of strong metallic bonds, even between dissimilar metals. Due to the absence of external heat, critical intermetallic phases can largely be avoided. In this process, Lorentz forces are utilized for the rapid acceleration of at least one of the two metallic joining partners leading to the controlled high velocity impact between them. The measurement of the collision conditions and their targeted manipulation are the key factors of a successful process development. Optical measuring techniques are preferred, since they are not influenced by the prevalent strong magnetic field in the vicinity of the working coil. In this paper, the characteristic high velocity impact flash during MPW was monitored and evaluated using phototransistors in order to measure the time of the impact. The results are in good accordance with the established PDV (photon Doppler velocimetry) and show a good repeatability. Furthermore, the collision front velocity was investigated using adapted part geometries within a series of tests. This velocity component is one of the key parameters in MPW; its value decreases along the weld zone. With the help of this newly introduced measurement tool, the magnetic pressure distribution or the joining geometry can be adjusted more effectively. 展开更多
关键词 Magnetic pulse welding impact welding process monitoring collision conditions dissimilar metal joining.
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A Derivation of the Entropy-Based Relativistic Smoothed Particle Hydrodynamics by Variational Principle
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作者 Philipe Mota Wei-Xian Chen Wei-Liang Qian 《Communications in Theoretical Physics》 SCIE CAS CSCD 2017年第9期382-386,共5页
In this work, a second order smoothed particle hydrodynamics is derived for the study of relativistic heavy ion collisions. The hydrodynamical equation of motion is formulated in terms of the variational principle. In... In this work, a second order smoothed particle hydrodynamics is derived for the study of relativistic heavy ion collisions. The hydrodynamical equation of motion is formulated in terms of the variational principle. In order to describe the fluid of high energy density but of low baryon density, the entropy is taken as the base quantity for the interpolation. The smoothed particle hydrodynamics algorithm employed in this study is of the second order, which guarantees better particle consistency. Furthermore, it is shown that the variational principle preserves the translational invariance of the system, and therefore improves the accuracy of the method. A brief discussion on the potential implications of the model in heavy ion physics as well as in general relativity are also presented. 展开更多
关键词 HYDRODYNAMICS SPH method variational principle
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