共查询到18条相似文献,搜索用时 418 毫秒
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从积算符理论和实验上详细地研究了弱耦合双自旋体系(CHCl3的C-H双自旋体系)的Raman磁共振谱.对不同射频场强度及频偏的Raman谱进行了细致的理论和实验研究,表明积算符理论的计算与实验不仅在弱射频场而且在强射频场时都符合得相当好,克服了微扰论的局限,这为进一步研究复杂自旋体系的Raman谱提供了强有力的理论方法.研究还表明,小的射频频偏将有利于多量子跃迁信号的观测,而适当的射频场强则会提高多量子峰的强度
关键词: 相似文献
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偶合常数是一个重要的NMR参数,其数值与分子中化学键的二面角有关,可以为分子结构研究提供很重要的信息.多维NMR谱由于具有较大的化学位移分辨率,因此常常被用来测定同核或异核自旋-自旋偶合常数.本文介绍了利用最高量子相关技术(MAXY)测定同核偶合常数的方法.MAXY是最近发展的一种多维NMR谱编辑技术,可以使不同官能团(CH,CH2,CH3)的相关峰分布于不同的图谱区域,因此比常规的二维谱具有更高的化学位移分辨率.而且被分离开来的NMR相关峰呈吸收性线型,能清楚地展示各自的偶合分裂特征,可以直接用于测定偶合常数. 相似文献
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基于大气激光后向散射光谱,研究和设计了探测大气CO2浓度的Raman激光雷达,其发射机采用Nd∶YAG激光的三倍频354.7nm作为工作波长,发射的单脉冲能量350mJ,重复频率20Hz;接收机采用了光电倍增管(量子效率25%)和光子计数器(计数速率200MHz),探测CO2的Raman散射371.66nm(频移1285cm-1)信号,(1小时累加)近地面2.5km以内信噪比不小于8.采用组合滤光片来抑制强的354.7nm Mie-Rayleigh后向散射和氧气375.4nm Raman后向散射对信号的严重干扰. 比较分别来自大气CO2和参考气体N2的Raman后向散射回波,可反演出大气中CO2的相对浓度.
关键词:
大气光学
激光雷达
Raman散射光谱
参考气体
Mie-Rayleigh散射 相似文献
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嘧螨酯为一种新型杀螨剂和STAT3激活抑制剂. 该文对嘧螨酯的紫外吸收光谱(UV)、红外吸收光谱(IR)、质谱(MS)、核磁共振氢谱(1H NMR)、核磁共振碳谱(13C NMR)、DEPT谱、1H-1H COSY谱、异核单量子相关谱(HSQC)、异核多键相关谱(HMBC)进行了解析,并对该化合物所有的核磁信号进行了全归属;同时讨论了紫外光谱吸收带位置和吸收强度与该化合物的生色团对应关系、红外光谱特征吸收峰与该化合物的各官能团的对应关系、氟原子(F)对其13C NMR的影响以及质谱离子碎片的归属和化合物的裂解规律. 该研究将为嘧螨酯的结构确证及其他相关研究提供参考. 相似文献
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利用多重散射团簇(MSC)方法计算了二己二硫醚[CH3(CH2)5S]2单分子和多分子硫原子近边x射线吸收精细结构(NEXAFS)谱,给出了二己二硫醚多层膜的局域结构模型. MSC研究显示多层膜中二己二硫醚分子作平行有序排列,彼此相距0.47nm,其横截面呈规则的正方形. 利用离散变分Xα方法计算了二己二硫醚单分子和多分子的电子结构,验证了MSC的计算结果;并阐明了NEXAFS谱中各峰的物理起源. 对多层膜中分子之间的相互作用进行了讨论,发现多层膜的局域结构有分子自组装的特性.
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3(CH2)5S]2多层膜')" href="#">二己二硫醚[CH3(CH2)5S]2多层膜
近边x射线吸收精细结构
多重散射团簇方法
离散变分Xα方法 相似文献
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Al2O3介质薄膜与纳米Ag颗粒构成的复合结构,被应用于表面增强Raman散射探测实验中,其中Al2O3介质薄膜对纳米Ag颗粒的吸收谱及增强Raman散射光谱的影响被特别关注.该复合结构的光学特性表征出纳米Ag颗粒的偶极振荡特性.从光吸收谱中可以看到,其共振吸收谱随Al2O3介质薄膜厚度增加而在整个谱域上发生红移,表明纳米Ag颗粒的周围介电常数随Al2O3介质薄膜厚度的增加而增大.采用罗丹明6G作为探针原子,6个Raman特征峰的平均增益值作为表征表面增强Raman散射衬底增益程度的量度.实验结果表明,Al2O3介质薄膜层的引入提高了纳米Ag颗粒的衬底介电常数,并引起了散射共振的增强,从而使表面增强Raman散射强度提高.
关键词:
纳米Ag薄膜
共振吸收
表面增强Raman散射
介电常数 相似文献
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《Journal of Magnetic Resonance (1969)》1986,66(1):14-31
It is shown that, under what may be called an “intermediate” decoupling condition, off-resonance heteronuclear spin decoupling of an abundant spin causes not only a line broadening, but also a line splitting, and a frequency shift of the NMR spectra of the dilute spin in solids. Typical examples of the fineshape behavior as a function of off-resonance decoupling frequency are presented and analyzed for the CH, CH2, and CH3 carbon nuclei in a single crystal of dimedone. The quadratic dependence of the linewidth on the off-resonance decoupling frequency, under the “strong near resonance” decoupling condition, is examined for both the single-crystal case, and for the CP-MAS spectrum of dimedone. 相似文献
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Coherent control of the precession motion of magnetizations in a single crystal YFeO3 with double half-cycle pulse terahertz waves was demonstrated. Quasiferromagnetic (0.299 THz) and quasiantiferromagnetic (0.527 THz) precession modes were selectively excited by choosing an appropriate interval of two pulses and were observed as free induction decay (FID) signals from the spin system. By observing the circularly polarized FID signals due to ferromagnetic resonance, we also succeeded in confirming directly the energy storage in the spin system and recovery from that to the electromagnetic radiation. 相似文献
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Free induction decay (FID) signals in solid state NMR measurements performed with magic angle spinning can often be extended in time by factors on the order of 10 by a simple pulsed spin locking technique. The sensitivity of a structural measurement in which the structural information is contained in the dependence of the integrated FID amplitude on a preceding evolution period can therefore be enhanced substantially by pulsed spin locking in the signal detection period. We demonstrate sensitivity enhancements in a variety of solid state NMR techniques that are applicable to selectively isotopically labeled samples, including 13C-15N rotational echo double resonance (REDOR), 13C-13C dipolar recoupling measurements using the constant-time finite-pulse radio-frequency-driven recoupling (fpRFDR-CT) and constant-time double-quantum-filtered dipolar recoupling (CTDQFD) techniques, and torsion angle measurements using the double quantum chemical shift anisotropy (DQCSA) technique. Further, we demonstrate that the structural information in the solid state NMR data is not distorted by pulsed spin locking in the detection period. 相似文献
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Adiabatic passage schemes in coupled semiconductor quantum dots are discussed. For optical control, a doped double-dot molecule is proposed as a qubit realization. The quantum information is encoded in the carrier spin, and the flexibility of the molecular structure allows to map the spin degrees of freedom onto the orbital ones and vice versa, which opens the possibility for high-finesse quantum gates by means of stimulated Raman adiabatic passage. For tunnel-coupled dots, adiabatic passage of two correlated electrons in three coupled quantum dots is shown to provide a robust and controlled way of distilling, transporting and detecting spin entanglement, as well as of measuring the rate of spin disentanglement. Employing tunable interdot coupling the scheme creates, from an unentangled two-electron state, a superposition of spatially separated singlet and triplet states, which can be discriminated through a single measurement. Finally, we discuss phonon-assisted dephasing in quantum dots, and present control strategies to suppress such genuine solid-state decoherence losses. 相似文献
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M. Sassetti F. Napoli B. Kramer 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,11(4):643-654
Using the bosonization technique, a theory for the collective excitations of the interacting electrons in quantum wires with
two subbands occupied is developed. The dispersion relations for the inter-subband charge and spin density excitations are
determined. The results are used to interpret the features observed in recent measurements of the Raman spectra of AlGaAs/GaAs
quantum wires, particularly for photon energies near band gap resonance. It is shown that peaks previously identified as “single
particle excitations” are signatures of higher order collective spin density excitations. Predictions about the observability
of the interband modes are made.
Received 8 February 1999 相似文献
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Shekar SC Lee DK Ramamoorthy A 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2002,157(2):223-234
The effect of an offset term in the cross-polarization (CP) Hamiltonian of a heteronuclear spin-12 pair due to off-resonant radio frequency (rf) irradiation and/or chemical shift anisotropy on one of the rf channels is investigated. Analytical solutions, simulations, and experimental results are presented. Formulating the CP spin dynamics in terms of an explicit unitary evolution operator enables the CP period to be inserted as a module in a given pulse scheme regardless of the initial density matrix present. The outcome of post-CP manipulation via pulses can be calculated on the resulting density matrix as the phases and amplitudes of all coherence modes are available. Using these tools it is shown that the offset can be used to reduce the rf power on that channel and the performance is further improved by a post-CP pulse whose flip angle matches and compensates the tilt of the effective field on the offset channel. Experimental investigations on single crystalline and polycrystalline samples of peptides confirm the oscillatory nature of CP dynamics and prove the slowing down of the dynamics under offset and/or mismatch conditions. 相似文献
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The free induction decay (FID) of the transverse magnetization in a dipolar-coupled rigid lattice is a fundamental problem in magnetic resonance and in the theory of many-body systems. As it was shown earlier the FID shapes for the systems of classical magnetic moments and for quantum nuclear spin ones coincide if there are many nearly equivalent nearest neighbors n in a solid lattice. In this paper, we reduce a multispin density matrix of above system to a two-spin matrix. Then we obtain analytic expressions for the mutual information and the quantum and classical parts of correlations at the arbitrary spin quantum number S, in the high-temperature approximation. The time dependence of these functions is expressed via the derivative of the FID shape. To extract classical correlations for S > 1/2 we provide generalized POVM measurement (positive-operator-valued measure) using the basis of spin coherent states. We show that in every pair of spins the portion of quantum correlations changes from 1/2 to 1/(S + 1) when S is growing up, and quantum properties disappear completely only if S → ∞. 相似文献