共查询到20条相似文献,搜索用时 93 毫秒
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利用谱表示理论和微扰展开法,从理论上给出了适合于一般微结构复合体系的有效非线性响 应的一般表示式,并结合有效媒质近似(EMA),在弱非线性条件下研究了由三阶非线性组 分(体积分数为p)和线性组分构成的非线性复合体系的有效非线性响应,讨论了复合 体系的有效介电常数ε~e=εe+χe|E0|2+ηe|E0| 4中的有效三次非线性响应χe和有效高次非线性响应ηe与体积分数p和 退极化因子L之间的关系,分析了非线性组分的介电常数为复数情形时体系的有效高阶非线 性响应,从理论上说明了组分的高次非线性响应对整个复合体系的有效介电常数的影响.
关键词:
非线性复合介质
有效非线性响应
谱表示理论 相似文献
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We propose a new two-mode thermo-and squeezing-mixed optical field, described by the new density operator ρ=1-e~f-|g|~2 e~(ga~+b~+)e~(fa~+a)|0〉 f_(bb) 〈0| e~(g*ab), where |0〉_(bb) 〈0| is the b-mode vacuum, e ~(fa~+a)represents the thermo-field, and e~(ga~+b~+) indicates squeezing. The photon statistics for ρ is studied by virtue of the method of integration within ordered product(IWOP) of operators. Such a field can be generated when a two-mode squeezed state passes through a one-mode dissipation channel. 相似文献
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考虑在渗流阈值附近弱非线性正常导体与绝缘体所构成的无规网络在任意d维空间的非线性渡越行为.系统由正常导体浓度为p,且满足弱非线性电流密度(J)电场(E)关系:J=σ1E+χ1|E|βE和浓度为1-p的绝缘体(σ2=0)构成.在略高于正常导体渗流阈值pc时,复合系统的有效响应可表示为〈J〉=σe〈E〉+χe|〈E〉|β〈E〉,当线性响应与非线性响应两者可相互比较时,此时的电流密度和电场强度被分别称为渡越电流密度|Jc|和渡越电场|Ec|,且发现略高于渗流阈值pc时具有幂指数关系:|Ec|~(p-pc)M(β
关键词: 相似文献
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SONG Tong-Qiang FAN Hong-Yi 《理论物理通讯》2001,(12)
We derive the two-mode Wigner operator in the 〈ξ| representation and 〈γ| representation, where |ξ〉 is common eigenvector of the mass-weighted relative coordinate and the mass-combinatorial momentum. As an application,we calculate the Wigner function of some two-mode state. 相似文献
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《大学物理》1983,(11)
Solve 5 of the following 6 problems.B1. Consider a neutral particle with intrinsic angular momentum where S=h/2 i. e. a spin1/2 article. Assume the particle bas a magnetic moment M =rS where r is a constant. Thequantum mechanical state of the particle can be described in a spin space spanned by the eigenvectors | + > and | - > representing alignment parallel and antiparallel to the Z axis. (i.e.Szl + ) ). At time t = 0 the state of the system is >. The particlemoves along the Y axis throug… 相似文献
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计算了三光子W态隐形传输令牌总线网的保真度.通过计算发现在整个量子网络通信过程中,对于给定的分析角θ,保真度仅与系数|a|2有关|随着分析角θ的增加,保真度出现最大值所对应的系数|a|2相应减小,取θ=π/4、π/2、3π/4时可使保真度达最大值1,此时对应的|a|2分别为0.724、0.5和0.276.对于给定的系数|a|,保真度仅与分析角θ有关|若|a|=0,则无论θ为何值,保真度始终为0|若|a|=|b|=0.707 1,则当θ=π/2、3π/2时保真度达最大值1. 相似文献
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三光子纠缠W态隐形传输令牌总线网的保真度计算 总被引:1,自引:1,他引:0
计算了三光子W态隐形传输令牌总线网的保真度.通过计算发现在整个量子网络通信过程中,对于给定的分析角θ,保真度仅与系数|a|2有关;随着分析角θ的增加,保真度出现最大值所对应的系数|a|2相应减小,取θ=π/4、π/2、3π/4时可使保真度达最大值1,此时对应的|a|2分别为0.724、0.5和0.276.对于给定的系数|a|,保真度仅与分析角θ有关;若|a|=0,则无论θ为何值,保真度始终为0;若|a|=|b|=0.7071,则当θ=π/2、3π/2时保真度达最大值1. 相似文献
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Phase diffusion of a two-component Bose-Einstein condensates:exact and short-time solutions for arbitrary coherent spin state
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We investigate phase diffusion of a two-component
Bose--Einstein condensates prepared initially in arbitrary coherent
spin state |θ0,φ0|. Analytical expression of the
phase-diffusion time is presented for θ0~π/2 case. In
comparison with the symmetrical case (i.e., θ0=π/2), we
find that the diffusion process becomes slow due to the reduced
atom number variance. 相似文献
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根据量子力学的线性叠加原理 ,构造了由多模偶相干态与多模虚偶相干态组成的第 种四态叠加多模叠加态光场态 |Ψ(4)e , 〉q的等阶 N次方 Y压缩特性 .结果发现 :1 )当压缩阶数 N=4m,( m=1 ,2 ,3 ,… )时 ,态 |Ψ(4)e , 〉q 恒处于等阶数 N-Y最小测不准态 ;2 )当压缩阶数 N =4m′+2 ,( m′=0 ,1 ,2 ,… )时 ,在 (θ1-θ2 ) ,q,Rj,r1,r2 等取不同的组合定值下 ,态|Ψ(4)e , 〉q可分别呈现出等阶 N次方 Y压缩效应与“半相干态”效应 ;3 )当压缩阶数 N为奇数时 ,在 (θ1-θ2 ) ,q,Rj,r1,r2 等取不同的组合定值下 ,态 |Ψ(4)e , 〉q 可呈现出等阶 N次方 Y压缩效应 相似文献
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通过使用含时量子波包方法,对HF分子该类型的布居转移动力学进行了研究. 提出双Σ型激光控制方案,用于控制布居从|v=16>能级向|v=0>能级进行转移. 该方案的第一步是将布居从|v=16>经过中间能级|v=11>向|v=7>转移,第二步是将布居从|v=7>经过中间能级|v=3>向|v=0>转移. 在每一个步骤中,三个振动能级在两束重叠的激光脉冲作用下形成一个Σ型的布居转移路径. 通过优化激光的强度、频率和延迟时间,得到了最大的布居转移效率. 计算并比较了正序脉冲和反序脉冲两种情况,在这两种情况下,布居都可以超过90%从|v=16>能级向|v=0>能级进行转移. 相似文献
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HU MingLiang & TIAN DongPing School of Science Xi''''an Jiaotong University Xi''''an China Xi''''an Institute of Posts Telecommunications Xi''''an China 《中国科学G辑(英文版)》2007,50(2):208-214
We investigate the entanglement of the three-qubit Heisenberg XXX chain in the presence of impurity and obtain the analytical expressions of the concurrence C. It is found that for impurity entanglement, C appears only when J1 > J for J > 0, and J1 > 0 for J < 0, and in these two regions C increases with the increase of J1, so is the critical temperature Tc. When J1 >>|J| , C reaches its maximum value 0.5 and Tc reaches the asymptotic value Tc = 3.41448J1. For entanglement between the normal lattices, C appears only when J > 0 and 2J < J1 < J, and initially increases with the increase of J1 and arrives at the maximum value Cmax = (e4JIT-3)/(e4JIT+3) before it decays to zero gradually, so is the critical temperature Tc with, however, the maximum value Tcmax = 4J/ln3. 相似文献
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《中国科学:物理学 力学 天文学(英文版)》2010,(10)
The most general duality gates were introduced by Long,Liu and Wang and named allowable generalized quantum gates (AGQGs,for short).By definition,an allowable generalized quantum gate has the form of U=YfkjsckUK,where Uk's are unitary operators on a Hilbert space H and the coefficients ck's are complex numbers with |Yfijo ck\ ∧ 1 an d 1ck| 1 for all k=0,1,...,d-1.In this paper,we prove that an AGQG U=YfkZo ck∧k is realizable,i.e.there are two d by d unitary matrices W and V such that ck=W0kVk0 (0kd-1) if and only if YfkJt 1c*|m that case,the matrices W and V are constructed. 相似文献
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根据量子力学的线性叠加原理,构造了由多模偶相干态与多模虚偶相干态组成的第Ⅲ种四态叠加多模叠加态光场态|Ψ(4)e,Ⅲ〉q的等阶N次方Y压缩特性.结果发现:1) 当压缩阶数N=4m,(m=1,2,3,…)时,态|Ψ(4)e,Ⅲ〉q恒处于等阶数N-Y最小测不准态;2) 当压缩阶数N=4m′+2,(m′=0,1,2,…)时,在(θ1-θ2),q,Rj,r1,r2等取不同的组合定值下,态|Ψ(4)e,Ⅲ〉q可分别呈现出等阶N次方Y压缩效应与"半相干态"效应;3) 当压缩阶数N为奇数时,在(θ1-θ2),q,Rj,r1,r2等取不同的组合定值下,态|Ψ(4)e,Ⅲ〉q可呈现出等阶N次方Y压缩效应. 相似文献