压缩角对介观耦合电压缩效应的影响

从无耗散的电感耦合是电路的经典运动方程出发,研究了压缩真空态下介观电感耦合电路中电荷和电流的量子涨落;着重分析了压缩幅角参数对电荷和电流量子压缩效应的影响,结果表明：在任意幅角θ下,电荷或电流的量子涨落不是随压缩参数r增加而单调地减小,而是存在着一个极小值。     

平移压缩Fock态下无耗散介观电感耦合电路的量子效应

研究了在平移压缩Fock态下介观电感耦合电路中电荷和电流的量子涨落.结果表明:每个回路中电荷、电流的量子涨落只依赖于两回路的器件参量和压缩参量,而与平移参量无关.     

含芴酮的低聚物的激发态特征研究

采用量子化学计算方法和跃迁密度及电荷差分密度分析方法对含芴酮的低聚物激发态性质进行理论研究。计算得到的跃迁能和振子强度与实验数据一致。跃迁密度分析显示跃迁偶极矩的大小和方向,电荷差分密度分析揭示了分子间电荷转移的方向和结果。研究表明含芴酮的低聚物在光诱导下产生的第一激发态为分子内电荷转移激发态,而第五激发态为局域激发态。跃迁密度矩阵分析和电荷差分密度的理论分析结果易于理解含芴酮低聚物的激发态特性。     

含芴酮的低聚物的激发态特征研究

采用量子化学计算方法和跃迁密度及电荷差分密度分析方法对含芴酮的低聚物激发态性质进行理论研究。计算得到的跃迁能和振子强度与实验数据一致。跃迁密度分析显示跃迁偶极矩的大小和方向，电荷差分密度分析揭示了分子间电荷转移的方向和结果。研究表明含芴酮的低聚物在光诱导下产生的第一激发态为分子内电荷转移激发态，而第五激发态为局域激发态。跃迁密度矩阵分析和电荷差分密度的理论分析结果易于理解含芴酮低聚物的激发态特性。     

非耗散介观LC电路中电荷和电流的压缩与反压缩效应

利用全量子理论,对非耗散介观LC电路中电荷和电流的压缩与反压缩效应进行了详细的讨论.结果表明:1)通过保持非耗散介观LC电路的固有频率不变,而使电感参量作阶跃函数变化,就可将介观LC电路由初始的真空态经相干态而演化到压缩相干态;并由此进一步分别制备出电荷与电流的压缩最小测不准态;2)通过控制电感参量的改变,可使电荷与电流的量子涨落呈现出压缩与反压缩效应.     

压缩真空态下介观RLC电路中电荷和电流的量子涨落

发展了一种有源RLC电路的量子力学处理方案,在此基础上研究了压缩真空态下介观RLC电路中电荷和电流的量子涨落,着重研究了电阻和压缩参数对量子涨落的影响. 关键词：     

平移压缩Fock态下介观电容耦合电路的量子涨落

从经典电容耦合电路的运动方程出发,研究了在平移压缩Fock态下介观电容耦合电路中每个回路的电荷和电流的量子涨落.结果表明,每个回路中电荷、电流的量子涨落只依赖于两个回路的器件参数和压缩参量,而与平移参量无关. 关键词： 介观电路 电容耦合 平移压缩Fock态 量子涨落     

RLC介观电路中的量子涨落

从线性谐振子哈氏量出发,通过正则变换,得到了受迫阻尼谐振子哈氏量,还讨论了在压缩态下的电荷和电流的量子涨落。     

非耗散介观含源电路的量子力学效应

本文对非耗散介观含源电路的量子力学效应进行了详细研究.导出了非耗散介观含源电路在压缩真空态下其电荷和电流的量子零点涨落,并得到了该电路在绝对零度时的量子噪音.     

N，N-二甲基苯胺和苯醌间光诱导电荷转移

研究了N ,N 二甲基苯胺和苯醌间光诱导电荷转移的溶剂效应 .首先在B3LYP/ 6 31G 水平上对给体和受体进行构型优化 ,然后采用优化的给受体构型在Cs 对称性下计算得到两种相对稳定的复合物构象P和T .在CIS/ 6 31+G 水平上计算复合物气相激发态 ,结果发现 ,构象P的第三单重激发态发生分子间的完全电荷分离 ,构象T的第三激发单重态发生分子间的部分电荷分离 .在上述同样水平上计算复合物溶剂条件下的激发态性质 ,与气相结果相比表明 ,溶剂中两种构象的第三单重激发态均发生完全电荷分离 ,吸收光谱均发生较大红移 .     

压缩真空态下介观电路的量子涨落

从有源LC回路的运动方程出发，研究了在压缩真空态下介观LC电路中电荷、电流的量子涨落． 关键词：     

Quantum fluctuations of mesoscopic damped double resonance RLC circuit with mutual capacitance-inductance coupling

Based on the scheme of damped harmonic oscillator quantization and thermo-field dynamics （TFD）, the quantization of mesoscopic damped double resonance RLC circuit with mutual capacitance-inductance coupling is proposed. The quantum fluctuations of charge and current of each loop in a squeezed vacuum state are studied in the thermal excitation case. It is shown that the fluctuations not only depend on circuit inherent parameters, but also rely on excitation quantum number and squeezing parameter. Moreover, due to the finite environmental temperature and damped resistance, the fluctuations increase with the temperature rising, and decay with time.     

The Quantum Fluctuations of Mesoscopic Damped Mutual Capacitance Coupled Double Resonance RLC Circuit in Excitation State of the Squeezed Vacuum State

Mesoscopic damped double resonance mutual capacitance coupled RLC circuit is quantized by the method of damped harmonic oscillator quantization. The Hamiltonian is diagonalized by unitary transformation. The eigenenergy spectra of this circuit are given. The quantum fluctuations of the charges and current of each loop are researched in excitation state of the squeezed vacuum state, the squeezed vacuum state and in vacuum state. It is show that, the quantum fluctuations of the charges and current are related to not only circuit inherent parameter and coupled magnitude, but also quantum number of excitation, squeezed coefficients, squeezed angle and damped resistance. And, because of damped resistance, the quantum fluctuation decay along with time. PACS numbers: 03.65.-w,42.50.Lc.     

Coherent and Squeezed States for Light in Homogeneous Conducting Linear Media by an Invariant Operator Method

With the choice of Coulomb gauge, we investigated coherent state and squeezed state of the light propagating through homogeneious conducting linear media with no charge density using quantum results of the LR invariant operator method. We described coherent and squeezed properties of electric and magnetic fields. The fields in coherent and squeezed states are decayed exponentially with time due to the conductivity of the media. We studied probability density of the coherent wave packet and the highly squeezed wave packets. The uncertainty relation between the two orthogonal phase amplitudes, â₁ and â₂, in coherent state is same as the uncertainty relation in vacuum number state. The envelope of the relative noise in coherent state alternately become large and small with time and position. The uncertainty relation between canonical variables are varied depending on the value of conductivity in squeezed state, but not lowered below /2 which is quantum-mechanically acceptable minimum uncertainty.