苯二酚异构体的电动毛细管色谱-玻碳微电极柱上安培检测分析方法研究

在玻碳纤维微电极上研究了电解液中β－环糊精（ＣＤ）的浓度对邻、间、对苯二酚的循环伏安特性的影响,从实验结果和分子结构水平方面考察了β－ＣＤ与邻、间、对苯二酚的包结作用。研究结果表明,β－ＣＤ与邻、间、对苯二酚的包结作用强弱顺序为间苯二酚、邻苯二酚、对苯二酚。讨论了电泳缓冲液中ΝΗ４Ｃｌ,ＳＤＳ,β－ＣＤ的浓度及ｐＨ值对邻、间、对苯二酚迁移时间的影响。建立了苯二酚异构体胶束电动毛细管色谱－玻碳微电极柱上安培检测分析方法,方法的回收率在９８％～１０３％之间。     

SOI高温器件及其在汽车电子等领域中的应用

石油钻井,航空航天,汽车等工业领域急需在高温下工作的器件和电路。ＳＯＩ技术在高温器件和电路方面有着广泛的应用前景。文章简要介绍了ＳＯＩ技术应用于制造高温器件和电路方面的进展情况。     

Non-Markovian stochastic Schrödinger equations in different temperature regimes: a study of the spin-boson model

Stochastic Schrodinger equations are used to describe the dynamics of a quantum open system in contact with a large environment, as an alternative to the commonly used master equations. We present a study of the two main types of non-Markovian stochastic Schrodinger equations, linear and nonlinear ones. We compare them both analytically and numerically, the latter for the case of a spin-boson model. We show in this paper that two linear stochastic Schrodinger equations, derived from different perspectives by Diosi, Gisin, and Strunz [Phys. Rev. A 58, 1699 (1998)], and Gaspard and Nagaoka [J. Chem. Phys. 13, 5676 (1999)], respectively, are equivalent in the relevant order of perturbation theory. Nonlinear stochastic Schrodinger equations are in principle more efficient than linear ones, as they determine solutions with a higher weight in the ensemble average which recovers the reduced density matrix of the quantum open system. However, it will be shown in this paper that for the case of a spin-boson system and weak coupling, this improvement does only occur in the case of a bath at high temperature. For low temperatures, the sampling of realizations of the nonlinear equation is practically equivalent to the sampling of the linear ones. We study further this result by analyzing, for both temperature regimes, the driving noise of the linear equations in comparison to that of the nonlinear equations.     

Vibronic energies and spectra of molecular dimers

We consider three distinct methods of calculating the vibronic levels and absorption spectra of molecular dimers coupled by dipole-dipole interactions. The first method is direct diagonalization of the vibronic Hamiltonian in a basis of monomer eigenstates. The second method is to use creation and annihilation operators leading in harmonic approximation to the Jaynes-Cummings Hamiltonian. The adiabatic approximation to this problem provides insight into spectral behavior in the weak and strong coupling limits. The third method, which serves as a check on the accuracy of the previous methods, is a numerically exact solution of the time-dependent Schrodinger equation. Using these methods, dimer spectra are calculated for three separate dye molecules and show good agreement with measured spectra.     

Fermi surface studies in the low- and high-T c phase of the organic superconductor β-(BEDT-TTF)2I3

We report de Haas-van Alphen (dHvA) measurements of the high-T _c modification (T _c = 7 - 8 K) and Shubnikov-de Haas results of the low-T _c modification (Tc ≈ 1:4 K) of the organic superconductor β-(BEDT-TTF)₂I₃. In the high-T _c phase we find a single closed two-dimensional orbit with a dHvA frequency F ₀ = (3815±10) T and a 1/cosθ dependence as expected for a quasi two-dimensional system (where θ is the angle between the magnetic field and the direction normal to the conducting planes). The effective cyclotron mass is m _c = (4:2±0:2)m _e. The dHvA signal shows a beating pattern caused by the three-dimensional warping of the Fermi cylinder. The inter-plane transfer integral estimated from the maximum beating frequency ΔF is t _⊥/εF ≈ 1/175. At the angles where the beating disappears, i.e., ΔF ≈ 0, the oscillations have a harmonic content which is much larger than expected from the Lifshitz-Kosevich formula. In the low-T _c phase weak SdH oscillations with a frequency of F _SdH ≈ 110 T and an effective cyclotron mass m _c ≈ 1:0m _e is found. These results suggest a possible reconstruction of the Fermi surface in the low-T _c phase.     

Universality of decoherence

We consider environment induced decoherence of quantum superpositions to mixtures in the limit in which that process is much faster than any competing one generated by the Hamiltonian H(sys) of the isolated system. While the golden rule then does not apply we can discard H(sys). By allowing for couplings to different reservoirs, we reveal decoherence as a universal short-time phenomenon independent of the character of the system as well as the bath and of the basis the superimposed states are taken from. We discuss consequences for the classical behavior of the macroworld and quantum measurement: For decoherence of superpositions of macroscopically distinct states H(sys) is always negligible.     

Magnetic nanowires fabricated by anodic aluminum oxide template—a brief review

Anodic aluminum oxide(AAO) with highly ordered nanoscale pores which are monodisperse and mutually parallel can be produced through a self-organized electrochemical process.Subsequent deposition of materials into the nanopores produces AAO embedded nanowire arrays.Whilst the templates can be further removed to obtain free individual nanowires,the embedded nanowires form an interesting nanocomposite structure.Recent research activities on the fabrication and characteriza-tion of AAO template based magnetic n...