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TFT-LCD投影显示中的彩色偏振分色系统 总被引:5,自引:3,他引:2
针对TFTLCD液晶投影显示系统中彩色偏振分色器件,从设计和制备上分析了多种S和P偏振器件并给出了设计结果,通过优化设计可以减小分色滤光片透射带内的波纹,探讨了制备过程并给出了测量结果,制备的器件及系统应用于液晶投影显示中,获得了良好的性能. 相似文献
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利用琼斯矩阵分析了双光束磁光存贮中信号读出系统偏振态的传输情况,推导了读出信号的表达式,分析了偏振分束镜与光盘盘基的相位延迟对读出信号的影响。 相似文献
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通过分析系统的杂质位与其余部分间的纠缠N1-A以及单个正常位与其余部分间的纠缠NL-A研究了匀强磁场作用下含杂质Heisenberg XX链的纠缠特性.研究表明三量子位时纠缠存在的临界温度依赖于杂质参数J1和匀强磁场B.研究发现,当量子位L为奇数时,纠缠N1-A随量子位的增加而增大,而L为偶数时则相反,并且量子位L为偶数时的纠缠大于量子位L为奇数时的纠缠;对NL-A, 量子位L为奇数时,纠缠随杂质参数J1的变化与L=3类似,而L为偶数时纠缠随杂质参数|J1|的增加而增加. 相似文献
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对多元ZnO压敏陶瓷电阻片进行了多达14000次的大电流冲击老化试验, 通过显微结构、电气性能及介电特性的测量对其缺陷结构进行了表征, 并研究了缺陷结构与大电流冲击老化之间的关系. 试验表明多次大电流冲击老化导致试样的电气性能明显下降, 发现ZnO压敏陶瓷的几何效应不仅受控于晶粒还与晶界密切相关. 另外, 通过介电谱分析观察到ZnO压敏陶瓷存在四种缺陷弛豫过程, 低温-60 ℃下的两个缺陷弛豫峰激活能约为0.24 eV和0.35 eV, 认为它们分别对应着本征的锌填隙缺陷L(Zni··)和氧空位缺陷L(VO·)并且不受冲击老化的影响. 高温80℃以上两个松弛峰的活化能约为0.71 eV和0.84 eV, 认为它们分别对应着非本征的晶间相电子陷阱L(ingr)和晶界处界面态陷阱L(gb). 发现大电流冲击后, 仅界面态陷阱激活能从0.84 eV降低到0.76 eV, 认为界面态陷阱主要控制着ZnO压敏陶瓷的电气性能和稳定性. 相似文献
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Yuika等人利用偏振CARS技术可以准确地确定分子的拉曼退偏比.其方法是,首先对不同检偏角d所对应CARS谱峰的频率分布进行数学模拟,然后由所得系数随检偏角φd的变化求得使CARS信号中共振项消失的偏振角φ0d,最后由消失条件ρ=-1/(tanθtanφ0d)求出退偏比ρ,θ为产生CARS光的Pump光与Stokes光偏振方向的夹角.本文提出的数据处理方法,即交点法.同Yuika等人处理数据的方法相比,交点法毋需关于谱峰频率分布的知识,做法也更为简便. 相似文献
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本文选取脉宽为12 fs波长为2000 nm和800 nm的两束线性偏振激光, 适当调节两束激光的偏振方向的夹角θ, 发现当θ=π/2时, 高次谐波谱的第二级平台出现了“漏斗形”凹槽.当θ为π/6时, 得到了290 eV的超宽连续谱的高次谐波发射, 利用小波变换合理的解释了高次谐波形状及截止位置. 在该段连续谱上任意截取70 eV宽度的频率, 都可以得到脉宽约为60 as的孤立阿秒脉冲. 适当减小截取范围可以得到线性偏振的脉宽94 as的孤立阿秒脉冲. 这为实验中产生能灵活调节的孤立阿秒脉冲提供了一种方案. 相似文献
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The influence of the width of a lattice-matched Al0.82In0.18N/GaN single quantum well (SQW) on the absorption coefficients and wavelength of the intersubband transition (ISBT) has been investigated by solving the Schrödinger and Poisson equations self-consistently. The wavelength of 1—2 ISBT increases with L, the thickness of the single quantum well, ranging from 2.88 μm to 3.59 μm. The absorption coefficients of 1—2 ISBT increase with L at first and then decrease with L, with a maximum when L is equal to 2.6 nm. The wavelength of 1—3 ISBT decreases with L at first and then increases with L, with a minimum when L is equal to 4 nm, ranging from approximately 2.03 μm to near 2.11 μm. The absorption coefficients of 1—3 ISBT decrease with L. The results indicate that mid-infrared can be realized by the Al0.82In0.18N/GaN SQW. In addition, the wavelength and absorption coefficients of ISBT can be adjusted by changing the width of the SQW. 相似文献
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K.M. Frahm 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,10(2):371-378
The localization length L2 of two interacting particles in a one-dimensional disordered system is studied for very large system sizes by an efficient
and accurate variant of the Green function method. The numerical results (at the band center) can be well described by the
functional form L
2
=L
1
[0.5+c(U) L
1
] where L1 is the one-particle localization length and the coefficient depends on the strength U of the on-site Hubbard interaction. The Breit-Wigner width or equivalently the (inverse) life time of non-interacting pair
states is analytically calculated for small disorder and taking into account the energy dependence of the one-particle localization
length. This provides a consistent theoretical explanation of the numerically found U-dependence of c(U).
Received 16 September 1998 相似文献
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S. De Toro Arias X. Waintal J.-L. Pichard 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,10(1):149-158
The interplay between the quantum interferences responsible for one particle localization over a length L1, and the partial dephasing induced by a local interaction of strength U with another particle leading to partial delocalization over a length L
2
> L
1
, is illustrated by a study of the motion of two particles put close to each other at the initial time. Localization is reached
in two steps. First, before the time t1 necessary to propagate over L1, the interaction slows down the ballistic motion. On the contrary, after t1 the interaction favors a very slow delocalization, characterized by a spreading of the center of mass, until L2 is reached. This slow motion is related to the absence of quantum chaos in this one dimensional model, the interaction being
only able to induce weaker chaos with critical spectral statistics. Under appropriate initial conditions, the motion remains
invariant under the duality transformation mapping the behavior at small U onto the behavior at large U.
Received 24 August 1998 相似文献
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《Journal of Macromolecular Science: Physics》2013,52(5):1075-1093
Abstract Polystyrene/poly(cis‐butadiene) rubber blends were prepared by melt blending. The morphology development of the blend system was examined by intermittent extraction of material and scanning electron microscopy. The mixing process of the immiscible system was described through the characteristic length L and the average characteristic length L m. The distribution of L was shown to be consonant with a log‐normal distribution. The mixing system was demonstrated to possess self‐similarity in a certain range of time and space, as shown through a scale function. Furthermore, the fractal dimension D at different times was calculated and shown to be a parameter that can be used to describe the dynamic process of the melt blending. 相似文献
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Mechanisms of ‘environmental decoherence’ such as surface scattering, Elliot–Yafet process and precession mechanisms, as well as their influence on the spin phase relaxation are considered and compared. It is shown that the ‘spin ballistic’ regime is possible, when the phase relaxation length for the spin part of the wave function (L(s)) is much greater than the phase relaxation length for the ‘orbital part’ (L(e)). In the presence of an additional magnetic field, the spin part of the electron's wave function (WF) acquires a phase shift due to additional spin precession about that field. If the structure length L is chosen to be L(s)>L>L(e), it is possible to ‘wash out’ the quantum interference related to the phase coherence of the ‘orbital part’ of the WF, retaining at the same time that related to the phase coherence of the spin part and, hence, to reveal corresponding conductance oscillations. 相似文献
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Quantum transport in a single‐molecule contact made of a prismane cluster C8 attached to quasi‐one‐dimensional gold (100) electrodes is calculated using the ab initio methodology based on the density‐functional theory and the nonequilibrium Green's functions formalism. Varying the junction length L we calculate the length dependence of the zero‐bias conductance G (L) and, for a set of the interelectrode distances, the current–voltage (I –V) characteristics. It is shown that the G (L) dependence is strongly nonmonotonic with a sharp dip at some value of L. With increase in L, the I –V curves change their shape from monotonic curves to curves with a negative differential resistance area and, for a larger L, the junction exhibits the super‐insulating state, i.e., within some applied bias voltage range the current through the junctions is about two orders of magnitude less than the current outside this bias range. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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M.A. Rego-Monteiro 《The European Physical Journal C - Particles and Fields》2001,21(4):749-756
We show that the Heisenberg-type algebra describing the first levels of the quantum harmonic oscillator on a circle of large
length L is a deformed Heisenberg algebra. The successive energy levels of this quantum harmonic oscillator on a circle of large length
L are interpreted, similarly to the standard quantum one-dimensional harmonic oscillator on an infinite line, as being obtained
by the creation of a quantum particle of frequency w at very high energies.
Received: 29 March 2001 / Revised version: 17 July 2001 / Published online: 31 August 2001 相似文献