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1.
氯化聚乙烯辐射效应的NMR研究   总被引:2,自引:1,他引:1  
1H NMR,13C NMR谱,二维谱,FT-IR等方法研究了氯化聚乙烯(CPE)在室温下限量空气中经60Co γ射线辐照后的辐照效应. 结果表明CPE在辐照过程中以发生裂解反应为主,在裂解反应过程中伴随着HCl脱出,HCl的脱出量随着辐照剂量的增加而增加. 辐照后CPE样品的大分子结构发生相应变化,序列结构为CH2CHClCHClCH2CHCl,CH2CH2CHClCH2CH2,CHClCH2CHClCH2CH2,CHClCH2CHClCH2CHCl的单元数量减少,但没有形成新的序列结构类型,T1 和T2值给出了有关辐照前后分子运动变化的信息.  相似文献   

2.
We discuss the possibility of realizing quantum computation on the basis of a cluster of single interacting nuclear spins in solids. This idea seems to be feasible because of the combination of two techniques—Single Molecule Spectroscopy and Optically Detected Electron Nuclear Double Resonance. Compared to the well-known bulk Nuclear Magnetic Resonance (NMR), the proposed method of quantum computation has the advantage that quantum computation is performed with pure spin states and the quantum processor is more easily scalable. At the same time, the advantages of NMR quantum computation are kept: long coherence time and easy construction of quantum gates. As a specific system to implement the above idea, we discuss the 13C-nuclear spins in the nearest vicinity of a single nitrogen-vacancy (NV) defect center in diamond, which can be optically detected using the technique of scanning confocal microscopy. Owing to the hyperfine coupling of the ground state electron paramagnetic spin S=1 of the center to 13C nuclear spins in a diamond lattice, the states of nuclear spins in the vicinity of the defect-center can be addressed individually. Preliminary consideration shows that it should be possible to address up to 12 individual 13C nuclear spins. The dephasing time of the nuclear spin states at low temperatures allows realization up to 105 gates.  相似文献   

3.
The diffusion of hydrogen in LaNi5+xH6 (x=?0.2, 0.0, 0.2) has been investigated by NMR from 150 to 300 K. High-temperature data of the spin-spin relaxation time T2 and the rotating frame spin lattice relaxation time T1? are independent of stoichiometry but the data of the spin lattice relaxation time T1 and low-temperature T1? data are not, and they do not fit Torrey's relaxation model.  相似文献   

4.
An NMR quantum computer based on an integrated device with CeP has been proposed by Yamaguchi and Yamamoto [Appl. Phys. A 68 1 (1999)]. We point out two problems in their scheme. We also investigate experimentally the 31P NMR spectra for our CeP. From the line width, we find that improvement of the sample quality is necessary to satisfy the experimental conditions for a quantum computer.  相似文献   

5.
Crystal lattice quantum computer   总被引:2,自引:0,他引:2  
31 P nucleus can be used to represent a quantum bit (‘qubit’) with a relatively long relaxation time. In a CeP crystal lattice, 31P nuclei are periodically situated in three dimensions at distances of about 6 Å. The application of a static magnetic field gradient in one direction causes differences in the Zeemanfrequencies of separate nuclei. This allows thousands of distinct qubits to be individually addressed. Initializations of the qubits can be done efficiently by the Pound–Overhauser double resonance effect on the nuclear spins and the antiferromagnetically ordered 4f electron spins of cerium ions. Logic operations can be performed by simple pulse sequences, and computational results after logic operations can be measured by the nuclear magnetic resonance of neighboring nuclei, or the electron resonance of neighboring 4f electrons of cerium ions. Received: 26 October 1998/Accepted: 29 October 1998  相似文献   

6.
A one-dimensional NMR method is presented for measuring the transverse relaxation time, T2,n, of intermolecular multiple quantum coherences (IMQCs) of coherence order n in highly polarized spin systems. The pulse sequence proposed in this paper effectively suppresses the effects of radiation damping, molecular diffusion, inhomogeneity of magnetic field, and variations of dipolar correlation distance, all of which may affect quantitation of T2,n. This pulse sequence can be used to measure not only IMQC transverse relaxation time T2,n(n>1) quickly and directly, but also the conventional transverse relaxation time. Experimental results demonstrate that the quantitative relationship between T2,n(n≥1) and T2 is T2,n≈T2/n. These results will be helpful for understanding the fundamental properties and mechanisms of IMQCs.  相似文献   

7.
 本文在高Tc超导体BiSrCaCu2Oy常压制备的基础上,研究了热压烧结和冷压处理对其形成、结构及超导电性的影响,并与常压结果进行了比较。结果表明,高压可以使样品的合成时间缩短,合成温度降低。但同时它也抑制了晶格参数较大的相(高Tc相)的形成,使小晶格参数的杂相含量增多。对于提高样品的超导电性而言,1.5 GPa时一个较好的压力点。  相似文献   

8.
核磁共振二维谱反演   总被引:4,自引:0,他引:4  
顾兆斌  刘卫 《波谱学杂志》2007,24(3):311-319
核磁共振二维谱包含扩散系数 D 和横向弛豫时间 T2 的信息,利用核磁共振仪来测量多孔介质中物质的信息,根据其弛豫时间和扩散系数的差别来区分不同物质;利用全局反演方法,提出了核磁共振二维谱反演的物理模型和数学模型;介绍了传统的奇异值分解(SVD)和改进的奇异值分解反演算法;采用改进的奇异值分解法对核磁共振二维谱进行反演,其反演算法具有计算速度快和二维谱分布连续等优点. 它适合于信噪比较高的数据反演,当原始数据信噪比SNR≥100时,可以对二维谱图进行定量分析;当60≤SNR<100时,可以对二维谱图进行定性分析. 核磁共振二维谱可以一次性直接区分油和水,为核磁共振测井提供了新的科学技术.  相似文献   

9.
The quadrupole 209Bi spin–spin and spin–lattice relaxation were studied within 4.2–300 K for pure and doped Bi4Ge3O12 single crystals which exhibit, as was previously found, anomalous magnetic properties. The results revealed an unexpectedly strong influence of minor amounts of paramagnetic dopants (0.015–0.5 mol.%) on the relaxation processes. Various mechanisms (quadrupole, crystal electric field, electron spin fluctuations) govern the spin–lattice relaxation time T 1 in pure and doped samples. Unlike T 1, the spin–spin relaxation time T 2 for pure and Nd-doped samples was weakly dependent on temperature within 4.2–300 K. Doping Bi4Ge3O12 with paramagnetic atoms strongly elongated T 2. The elongation, although not so strong, was also observed for pure and doped crystals under the influence of weak (~30 Oe) external magnetic fields. To confirm the conclusion about strong influence of crystal field effects on the temperature dependence of T 1 in the temperature range 4.2–77 K, the magnetization vs. temperature and magnetic field was measured for Nd- and Gd-doped Bi4Ge3O12 crystals using a SQUID magnetometer. The temperature behavior of magnetic susceptibility for the Nd-doped crystal was consistent with the presence of the crystal electric field effects. For the Gd-doped crystal, the Brillouin formula perfectly fitted the curve of magnetization vs. magnetic field, which pointed to the absence of the crystal electric field contribution into the spin–lattice relaxation process in this sample.  相似文献   

10.
The temporal characteristics of stimulated Raman scattering (SRS) under 22-ps laser excitation were studied in eight oxide crystals with a T 2 optical-phonon dephasing time variable by up to two orders of magnitude. The measured SRS pulse width was shortened from 13.8 ps for Ba(NO3)2 (T 2 = 26.5 ps) to 4 ps for the LiNbO3 (T 2 = 0.38 ps) crystal. The dependence of SRS pulse width on the dephasing time was analyzed in the framework of the known SRS theory.  相似文献   

11.
CeP and CeAs are characterized by low temperature measurements of the specific heat, the thermal expansion, the electrical resistivity and the magnetization of single crystal specimens. These physical properties are found to be very sensitive to crystal perfection and chemical composition in both the paramagnetic and the magnetically ordered state. In the intrinsically antiferromagnetic CeP, imperfections can give rise to a remanent magnetization belowT N .  相似文献   

12.
Dipolar relaxation of multiple quantum (MQ) nuclear magnetic resonance (NMR) coherence is investigated on the evolution period of the MQ NMR experiment in chains of 19F nuclei in a single crystal of calcium fluorapatite. The dependence of the relaxation time of the MQ coherence of the second order on the size of the coherent spin cluster formed on the preparation period is obtained. The dipolar relaxation of MQ NMR coherences is considered as a model for the investigation of decoherence of quantum states of many-qubit spin clusters.  相似文献   

13.
The proton spin-lattice relaxation time T1, in the nematic liquid crystal 4-pentyl-4′-cyanobiphenyl confined in a glassy porous matrix has been measured in a wide Larmor frequency range of 1 · 102?2 · 107 Hz employing the fast field-cycling NMR technique. A strong influence of the restricted geometry on the character of the T1 dispersion was found. Our investigation clearly demonstrates the importance of the translationally induced molecular reorientations in inhomogeneous director field for the relaxation in the samples with 200 and 80 nm mean pore size. The experimental results are in a good agreement with the theoretical predictions. In the sample with 7 nm pore size the main contribution to the relaxation is ascribed to the slowing down of the molecular motion in the near-surface layer. Zero-field 1H NMR spectra of a microconfined liquid crystal are reported for the first time.  相似文献   

14.
The solvent and temperature dependence of the rate constant for spin echo dephasing, 1/Tm, for 0.2 to 1.2 mM glassy solutions of chromyl bis(1-hydroxy-cyclohexanecarboxylic acid), CrO(HCA)2; aquo vanadyl ion, VO2+(aq), and vanadyl bis(trifluoroacetylacetonate), VO(tfac)2were examined. At low temperatures where 1/T1⪡ 1/Tm, 1/Tmin 1:1 H2O:glycerol is dominated by solvent protons. At low temperature 1/Tmincreases in the order 1:1 H2O:glycerol or 9:1 CF3CH2OH:ethyleneglycol (no methyl groups) < 9:1i-PrOH:MeOH (hindered methyl groups) < 9:1n-PrOH:MeOH (less hindered methyl groups). This solvent dependence of 1/Tmis similar to that observed for nitroxyl radicals, which indicates that the effect of solvent methyl groups on spin-echo dephasing at low temperature is quite general. At higher temperatures the echo dephasing is dominated by spin–lattice relaxation and is concentration dependent. As the glass softens, echo dephasing is dominated by the onset of molecular tumbling.  相似文献   

15.
核磁共振T2谱换算孔隙半径分布方法研究   总被引:4,自引:0,他引:4  
岩芯核磁共振T2谱和压汞分析数据均在一定程度上反映了岩石的孔隙结构特征,理论分析和二者频率分布图对比表明,这两组数据有较好的相关性,核磁共振T2谱能够换算为反映岩石孔隙结构特征的孔隙半径分布图. 本文应用最大相关性原理、最小二乘法及插值算法等数学方法,给出了一个改进的将T2谱换算为孔隙半径分布图的实用有效新方法,求得了T2弛豫时间与岩芯孔隙半径r之间的换算系数C,计算过程中着重对比了T2谱与压汞数据的主要分布区间,并考虑了压汞进汞饱和度小于100%对换算结果的影响. 天然砂岩岩芯核磁共振T2谱换算为孔隙半径分布图的实际应用效果表明,着重对比T2谱与压汞数据的主要分布区间,同时考虑压汞进汞饱和度小于100%对换算结果的影响是必要的,换算结果更加真实可信.  相似文献   

16.
We have studied the motion of lithium ions in LixTiS2 (x = 0.33, 0.94) using pulsed NMR techniques. The temperature dependences of the spin lattice relaxation in the rotating frame (T1?) suggest comparable activation energies for lithium ion diffusion for both samples, 3370 K, but an appreciably longer hopping time for the x = 0.94 sample. Low temperature values of T2 agree with calculated and measured second moments for both materials.  相似文献   

17.
聚3-羟基丁酸酯(PHB)是微生物细胞在其生长的特定时期在胞内合成的具有相应生物功能的聚羟基烷酸酯类物质, 是一种具有潜在的广泛应用前景的生物可降解的高分子材料. 由于天然的PHB其较高的结晶度和较窄的温度处理范围,它在应用过程中受到较大的局限性. 人们将结构相似的单体3-羟基戊酸(HV)与3-羟基丁酸(HB)共聚形成共聚物(PHBV)以后, 显著改善了PHB的物理机械性能,譬如:冲击强度和韧性有所增加,而硬度脆性有一定程度的下降. 人们虽然在这些降解高分子材料的开发、制备和物理机械性能以及这些材料的应用等方面有很多研究,但是有关分子水平的问题并未得到系统的探索. 因此,针对这些分子基础问题(结构域特征和分子动力学等)做了一些初步的研究.  全氟磺酸树脂(Nafion)是杜邦公司生产的一种燃料电池电极薄膜材料,其较低的使用温度(<100℃)严重地限制了它的应用范围. 人们发现,当把层状硅酸盐(蒙脱土)和Nafion合成为有机无机纳米复合材料之后,在一定程度上提高了它的使用温度. 虽然这种复合材料很容易合成出来并且已经运用到了实际工业应用之中,但是这种热稳定性提高的原因却不甚清楚. 通过固体NMR等分析方法从微观相互作用方面来认识这种宏观性能改善的原因.  使用固体13C CP MAS、13C SPE MAS NMR以及XRD方法测定了PHB和两种PHBV的结晶度(Xc),发现随着HV的引入它们的Xc 逐渐减小. 研究同时发现在测量Xc 的这几种方法中13C SPE MAS NMR误差较小. 实验中我们利用质子弛豫诱导谱编辑(PRISE)、质子自旋扩散(Spin-diffusion)等固体NMR技术研究了PHB以及不同含量HV的PHBV的结构域特征和相应结构域的运动性. 实验结果表明随着HV含量的增加,它们的非晶相结构域尺寸增大,晶相结构域尺寸减小,可以看出HV的引入导致PHB的结构域特征的变化是其宏观性能改善的原因.  进一步通过低分辨固体NMR测量了PHB和PHBV的变温质子弛豫时间(T1, T, T2), 然后通过理论拟合获得了它们不同运动状态的分子运动相关频率(τc)和分子活化能(Ea)等动力学信息,研究发现随着HV含量的增加,分子运动加快,活化能减小,在分子水平上认识了HV的引入使得PHB宏观性能改善的微观原因.  通过溶胶凝胶法合成了燃料电池电极薄膜(Nafion)和层状硅酸盐(蒙脱土)纳米复合材料来提高Nafion的使用温度,FT-IR和29Si MAS NMR实验结果表明在杂化材料中虽然质子化的十二烷基胺修饰的蒙脱土(MMT)的引入没有导致MMT的骨架结构发生明显变化,而且Nafion也没有插入到MMT的层间,但是TGA分析表明杂化材料中的Nafion的热稳定性比纯的Nafion高. 通过一系列固体NMR技术包括19F MAS、1H-13C CP MAS NMR和1H-13C HETCOR 2D NMR实验初步证实了这种材料的热稳定性的提高可能是由于MMT表面吸附的NH+3与Nafion侧链上的SO-3之间存在较强的静电相互作用,初步可以认为这种相互作用是导致电极材料性能改善的原因.  相似文献   

18.
The 133Cs spin-lattice relaxation time in a CsHSO4 single crystal was measured in the temperature range from 300 to 450 K. The changes in the 133Cs spin-lattice relaxation rate near Tc1 (=333 K) and Tc2 (=415 K) correspond to phase transitions in the crystal. The small change in the spin-lattice relaxation time across the phase transition from II to III is due to the fact that during the phase transition, the crystal lattice does not change very much; thus, this transition is a second-order phase transition. The abrupt change of T1 around Tc2 (II-I phase transition) is due to a structural phase transition from the monoclinic to the tetragonal phase; this transition is a first-order transition. The temperature dependences of the relaxation rates in phases I, II, and III are indicative of a single-phonon process and can be represented by T1−1=A+BT. In addition, from the stress-strain hysteresis loop and the 133Cs nuclear magnetic resonance, we know that the CsHSO4 crystal has ferroelastic characteristics in phases II and III.  相似文献   

19.
The impurity and lattice contributions to the spin-lattice relaxation of Al27 nuclei in nominally pure and lightly chromium-doped corundum (Al2O3) crystals are separated experimentally under the conditions of additional stationary resonance magnetic saturation of a pulsed NMR signal. The relaxation time T i lat due to the lattice mechanism of the spin-phonon interaction is determined. Fiz. Tverd. Tela (St. Petersburg) 39, 1041–1043 (June 1997)  相似文献   

20.
We solve the quantum mechanical problem of the inelastic scattering of phonons by a quadrupole defect in a crystal lattice for the case of solid parahydrogen whose matrix contains pair complexes of H2 orthomolecules. By employing the pseudospin approximation for the operator of the energy of quadrupole-quadrupole interaction of the molecules in an orthopair we derive an effective Hamiltonian that describes the interaction of phonons with a pair quadrupole orthodefect in the lattice. We set up the scattering matrix and calculate the effective phonon relaxation time τ(ω, T) as a function of the frequency ω and the crystal temperature T. We also find that a pair quadrupole defect, which has a complicated system of levels, can be replaced by an effective two-level system with temperature-dependent parameters. The fact that a pair quadrupole orthocluster has internal degrees of freedom results in a resonant scattering peak near a certain critical temperature T 0. Our estimates for H2 yield T 0≃ 6–7 K. Finally, we discuss the contribution of this mechanism to the low-temperature thermal conductivity of solid hydrogen. Zh. éksp. Teor. Fiz. 114, 555–569 (August 1998)  相似文献   

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