共查询到19条相似文献,搜索用时 125 毫秒
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本文对激光等离子体细丝的线性转换理论作了研究.通过对激光等离子体二次谐波的能量通量的计算发现,二次谐波的平面波理论关于在垂直密度梯度方向没有二次谐波辐射的结论与实验结果不符.在此基础上,我们提出了等离子体细丝的二次谱波线性转换理论,在垂直密度梯度方向有较强的二次谐波发射,这与实验结果较为一致. 相似文献
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利用钛宝石飞秒激光器输出的基频脉冲ω及其倍频脉冲2ω所构成双色场作用空气, 实验中检测到了中心波长处于真空紫外波段的四阶谐波. 在气体未发生电离的情况下, 四次谐波强度对双色场的能力依赖关系显示其产生是参量过程2ω+ω+ω→4ω的贡献. 当气体发生电离, 四次谐波强度与双色场相对相位有关, 可通过双色场相干控制. 实验研究了四次谐波对双色场相位的依赖性以及与太赫兹波的关联性, 其结果与数值模拟结果相符, 分析发现当气体发生电离时四次谐波的产生过程存在太赫兹辐射ΩTHz的参与, 是参量过程2ω+2ω±ΩTHz→4ω和2ω+ω+ω→4ω的共同贡献. 相似文献
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为了研究阻变存储器导电细丝的形成位置和分布规律, 使用X射线光电子能谱研究了Ti/HfO2/Pt阻变存储器件单元中Hf 4f的空间分布, 得到了阻变层的微结构信息. 通过I-V测试, 得到该器件单元具有典型的阻变特性; 通过针对Hf 4f的不同深度测试, 发现处于低阻态时, 随着深度的增加, Hf4+化学组分单调地减小; 而处于高阻态和未施加电压前, 该组分呈现波动分布; 通过Hf4+在高阻态和低阻态下组分含量以及电子能损失谱分析, 得到高阻态下Hf4+组分的平均含量要高于低阻态; 另外, 高阻态和低阻态下的O 1s谱随深度的演变也验证了Hf4+的变化规律. 根据实验结果, 提出了局域分布的氧空位聚簇可能是造成这一现象的原因. 空位簇间的链接和断裂决定了导电细丝的形成和消失. 由于导电细丝容易在氧空位缺陷聚簇的地方首先形成, 这一研究为导电细丝的发生位置提供了参考. 相似文献
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将Guo-Åberg-Crasemann形式散射理论推广到高次谐波产生过程, 获得了高次谐波产生概率公式. 利用这一公式, 计算了不同惰性气体原子的高次谐波谱. 理论分析和数值计算显示高次谐波有新的截断定律qcħω = (9 -4√2) Up + (2√2-1) Ip ≈ 3.34 Up + 1.83 Ip, 其中, Up 为电子的有质动能, Ip 为原子电离能, ħω 为激光光子能量, qc 为高次谐波的截断阶数. 这一截断定律与近期Popmintchev等 (Popmintchev et al. 2012 Science 336 1287) 的实验观测符合得很好. 相似文献
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利用不同加热机制产生的超热电子所导致的相干渡越辐射(CTR)在谐波分量强度比上的不同,给出了区分飞秒激光等离子体相互作用产生超热电子过程中的主要与次要加热机制的一种可能方法.得到了加热周期不同的加热机制所产生超热电子的比例与CTR谐波分量的二倍频和一倍频的强度比之间的具体关系式.如果在实验上测到此谐波分量强度比,就可以推出不同加热机制在加热过程中所起作用的大致比例关系.另外,CTR谐波分量的强度比还与超热电子的温度、实验上所使用靶的厚度有一定依赖关系,对此作了较为详细的讨论.
关键词:
相干渡越辐射
超热电子
加热机制 相似文献
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提出了能够很好地描述非过渡金属无序和非晶态超导体的2Δ0/(kBTc)与声子谱参量之间关系的一个公式:2Δ0(kBTc=4.95[1-(T0<ω>1/2)/A(1/(λω0)+1/(20λ<ω>)+1/(20<ω>))]。计算了大量已知声子谱的非晶和无序超导体的能隙2Δ0对Tc的比,结果表明在百分之几的范围内与实验值符合。指出了非过渡金属和合金的非晶态超导体,既可以是一个2Δ0/(kBTc)值远大于BCS理论值(3.53)的强耦合超导体,也可以是一个2Δ0/(kBTc)值比BCS理论值还要小得多的弱耦合超导体。
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基于对复变函数Fα(y)=∫0(ωph-α)(ω2y)/(ω2y+1)g(ω)dω解析性质的分析,本文认为:在决定的收敛半径以外,吴杭生等提出的Tc级数解的部分和作为近似Tc公式仍可用于1/λ的适当范围。但它可能达到的精度依赖于谱形,一般来说是有限的。
关键词: 相似文献
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Y. Avishai 《Zeitschrift für Physik A Hadrons and Nuclei》1978,286(3):285-290
The effective barrier at low energies is approximated by a Coulomb and parabolic barriers. A simple closed formula is obtained for the total reaction cross section which is the natural extension of Wong's results into the low energy domain. Theoretical predictions of averaged energy behaviour agree fairly well with various experimental results. The relation?ω 0≧π(2kh 2Z1Z2 e 2/μ)1/2 R 0 ?3/2 between the curvature and the extremum point of the nucleus-nucleus potential is suggested, based on low energy fusion experiments. By assuming equality sign, it is possible to extract the parameters of the barrier directly from experiment. Incidentally it is found that?ω 0 remains persistently arround 4.5 MeV for all the reactions which have been investigated. 相似文献
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The paper presents the first report on χ(2) polarization induced in molecular glass of conjugated compound by all-optical poling. Transparent thin film of molecular glass of 1,4-bis[2-[4-[N,N-di(p-tolyl)amino]phenyl]vinyl]benzene (BTAPVB) was prepared using a spin-cast technique. Dipolar as well as octupolar components in BTAPVB contributed to the formation of photoinduced χ(2) polarization. Growth rate of χ(2) polarization has good linear relation with Eω4E2ω, which suggested that the simultaneous processes of two-photon (ω + 2ω) and three-photon (ω + ω + ω) excitation on the same electronic level contributed to the formation of photoinduced χ(2) polarization. 相似文献
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The first observation of interference effects between two sharp resonant contributions to the third-order nonlinear susceptibility χ(3) (ω3=ω0+ω1?ω2) is reported. Using two tunable near ir frequencies, ω0=ω1 and ω2, the was seen in crystalline CuCl when 2ω1 and ω1?ω2 were close to the sharp Z3 exciton at 3.21 eV and the 210 cm-1 Raman line, respectively. Three different tunable visible frequencies were used to observe similar interference effects in a benzene-cyclohexane mixture when ω0?ω2 and ω1?ω2 were close to the 992 cm-1 Raman line of benzene and the 801 cm-1 Raman line of cyclohexane, respectively. 相似文献
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In the frame work of TREDER 's gravitational theory we consider two classes of field equations which are derivable from two classes of LAGRANGE ian densities Ω(1)(ω1, ω2), Ω(2)(s?1, s?2). ω1, ω2; s?1, s?2 are parameters. Ω(2)(ω1, ω2) gives us field equations which are up to the post-NEWTON ian approximation in the sense of NORDTVEDT , THORNE and WILL equivalent to the field equations given by BRANS and DICKE . For ω2 = ?1 ?2ω1 field equations follow from Ω(1)(ω1, ?1 ?2ω1) which are in the above mentioned sense of post-NEWTON ian approximation equivalent to EINSTEIN 's equations. The field equations following from Ω(1)(ω1, ω2) have a cosmological model with the well known cosmological singularities for T → ± ∞ in case that ω1/(1 +3ω1 +ω2) ? γ > 0. For ω1/(1 +3ω1 +ω2) ≤ 0 cosmological models with no cosmological singularities exist. From Ω(2)(s?1, s?2) we obtain field equations which at the best give us perihelion rotation 7% above EINSTEIN 's value and light deflection 7% below the corresponding EINSTEIN 's value. But in that case we are able to show the existence of a cosmological model without any cosmological singularity. 相似文献