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1.
崔宏飞  李凯  杨晨光  贺淑莉 《物理学报》2015,64(5):57501-057501
本文采用高温有机溶剂法制备了(Fe1-xCox)3BO5纳米棒, 通过控制反应物中乙酰丙酮钴的含量合成了不同Co含量的(Fe1-xCox)3BO5. 利用高分辨透射电子显微镜(HRTEM)、超导量子干涉磁强计(SQUID)对其形貌和磁性能进行了表征. 高分辨透射电子显微镜结果表明制备出的纳米(Fe1-xCox)3BO5为多晶棒状, 且具有多折孪晶结构; 磁性测量的结果表明,(Fe1-xCox)3BO5纳米棒在室温下表现出铁磁性, 随着Co含量的增加, 纳米棒的铁磁性逐渐增加, 该纳米棒有望用来研究生物大分子的机械性能.  相似文献   

2.
The ArF-laser (193-nm)-induced discharge interruption is comparatively described in a mixture of C2H3Cl/CF 4/CH4, CF4/CH4, and C2 H3Cl/He using a hollow-cathode-type discharge tube. The unfocused ArF laser (typically 27 mJ/cm2 and 10 ns duration) illuminated both the negative glow inside the hollow cathode and the column between the two electrodes. With a 1.8-torr mixture of C2 H3Cl/CF4, the discharge current of 1 mA was decreased rapidly with a current-decay time constant of 1 μs and a current-decay rate of 1 kA/s. With a 1.5-torr mixture of CF4/CH4, 2.2 μs and 450 A/s were obtained. With a 1.5-torr mixture of CH2H3Cl/He, a time constant of over 3 μs and a rate of less than 300 A/s were obtained. An analysis of the discharge interruption induced by ArF-laser irradiation is given in terms of photon-plasma kinetics. The current peak induced by ArF irradiation is also explained for a mixture of C2H3 Cl/He in terms of photoionization and photodetachment processes  相似文献   

3.
In this paper, we report on all the electro-optic coefficients of the low-symmetry crystal YbCa4O(BO3)3 measured by the interferometric method. The new sample orientations, which have not been reported so far, have been used for measuring the skew electro-optic coefficients γ51, γ53, γ42 and γ62 independently. The results obtained are γ11=0.6, γ21=0.4, γ31=0.3, γ13=0.3, γ23=0.2, γ33=2.2, γ51=0.9, γ53=4.1, γ42=0.8 and γ62=0.4×10−12 m/V.  相似文献   

4.
In this paper, we report all of the electro-optic coefficients of the low symmetry crystal GdCa4O(BO3)3 measured by the interferometric method. The new sample orientations, which have not been reported so far, have been used for measuring the skew electro-optic coefficients γ51, γ53, γ42 and γ62 independently. The results obtained are γ11=0.4, γ21=0.5, γ31=0.6, γ13=0.1, γ23=0.4, γ33=2.0, γ51=0.7, γ53=1.5, γ42=0.5, γ62=0.8×10−12m/V.  相似文献   

5.
Two-inch sized KMgF3,BaLiF3 and LiCaAlF6 (LiCAF) single crystals were grown by the Czochralski method under a CF4 atmosphere. X-ray irradiation was used to carry out a comparative study of induced optical absorption phenomena and colour centre creation in the ultra-violet and visible spectral regions. The integral of the induced absorption spectra is significantly lower in LiCAF with respect to the other studied materials. It is found that the amplitude of the F-absorption band is suppressed more than a factor of 3 by Mg-doping. For Mg-doped crystals, the optimum doping concentration is about 0.2 mol% of Mg2+.  相似文献   

6.
本文用X射线粉末法测定了Li2K(IO3)3与Li2NH4(IO3)3的晶体结构和原子参数。发现Li3K(IO3)3,Li2NH4(IO3)3与Li2Rb(IO3)3同晶型,属单斜晶系,空间群为P21/α,每个单胞含有四个化合式量。室温的点阵常数分别为α=11.198?,b=11.046?,c=8.254?,β=111.53°,及α=11.327?,b=11.078?,c=8.341?,β=111.87°。讨论了二元化合物的形成与离子半径的关系。 关键词:  相似文献   

7.
A series of polyacrylonitrile–dimethylsulfoxide–CuX2 (X=CF3SO3, Cl, Br), films (foils) were prepared by means of the solution cast technique. The thickness of the foils was between 0.04 and 0.09 cm and they contained 70–80 wt.% of the solvent. Conductivities of the solid electrolytes were obtained from impedance measurements. The conductivity increases with the increase of the salt content up to 8 wt.%; at higher concentrations (>8 wt.%) the conductivity is more or less stable, and reaches, in the case of Cu(CF3SO3)2 and CuCl2, the level of ca. 10−3 Ω−1 cm−1 at room temperature. The foils based on the CuBr2 show even higher conductivity, close to 10−2 Ω−1 cm−1 at room temperature, a value comparable to that characteristic for liquid solutions. The temperature variation of the conductivity for all the systems studied is of the Arrhenius type. The activation energy, determined from linear plots lnσ=f(T−1), is of the order ca. 14 kJ mol−1 for the PAN/CuBr2/DMSO and of ca. 21 kJ mol−1 for the PAN/CuCl2/DMSO and the PAN/Cu(CF3SO3)2/DMSO systems.  相似文献   

8.
We report the discovery of a second, higher-Tc superconducting organic charge-transfer salt derived from the electron-donor molecule BEDT-TTF (or ET), the novel organometallic anion [Cu(CF3)4], and the neutral solvent molecule 1, 1, 2-trichloroethane (TCE). We have very recently reported that this charge-transfer system yields a new superconducting phase salt, L- (ET)2Cu(CF3)4·TCE, with inductive onset Tcrmc=4.0 K at ambient pressure. This phase salt ( denotes a particular packing arrangement of the ET organic donor molecules) is electrocrystallized in the habit of hexagonal plates. Crystals possessing a needle-like habit electrocrystallize simultaneously with these plates, and we find these needles to be a distinctly different superconducting phase with diamagnetic onset Tc=9.2±0.1 K at ambient pressure. On the basis of our experiments, we denote this new superconducting phase as H−(ET)2Cu(CF3)4·(TCE)x,X<1.  相似文献   

9.
测量了碱土金属正磷酸盐Ba3(PO4)2和Sr3(PO4)2常温及高温拉曼光谱, 对拉曼振动模式进行指认, 并分析了晶体拉曼振动光谱及晶体结构在高温下的变化. 在温度升高的过程中, 拉曼振动频率向低频移动且振动峰宽度展宽, 晶体中的P-O平均键长随温度升高而变长, 但O-P-O的键角并未发生变化. 晶体在900 ℃以下无结构相变发生. 关键词: 3(PO4)2和Sr3(PO4)2')" href="#">Ba3(PO4)2和Sr3(PO4)2 高温拉曼光谱 振动模式 高温结构  相似文献   

10.
运用激光拉曼光谱实验和密度泛函理论计算研究了450~1 700 cm-1光谱范围内有机-无机杂化钙钛矿材料(C6H5CH2NH3)2PbBr4的振动模式特性。对比实验所得拉曼光谱和理论计算所得拉曼光谱,发现密度泛函理论计算可以很好的模拟(C6H5CH2NH3)2PbBr4有机部分的分子振动模式。同时通过比较分析密度泛函理论计算和参考文献,对450~1 700 cm-1光谱范围内的拉曼峰的分子振动模式进行了初步的归属,并发现该光谱范围内的拉曼峰主要是由(C6H5CH2NH3)2PbBr4分子中有机部分振动所产生的。  相似文献   

11.
利用XRD、VUV及UV光谱等方法对Ce3+、Tb3+离子掺杂以及Ce3+、Tb3+离子共掺的3种BaCa2(BO3)2荧光粉的相纯度、发光性质、浓度猝灭现象进行研究。结果表明:3种荧光粉在VUV波段有较好的吸收,基质吸收带位于140~190 nm范围。Ce3+在BaCa2(BO3)2的最低4f5d跃迁带位置在360 nm附近,其5d→2FJ(J=5/2, 7/2)发射峰分别位于393,424 nm。Tb3+掺杂的样品在172 nm激发下的发射光谱由4个窄带组成,分别对应5D47FJ(J=3,4,5,6)的跃迁,其中占主导位置的是5D47F5的跃迁,大约位于543 nm处,主要为绿光发射。在Ce3+,Tb3+离子共掺杂的BaCa2(BO3)2光谱中,观察到Ce3+-Tb3+离子间有能量传递。  相似文献   

12.
The observation of an anomalous temperature dependence of Mn2+ EPR spectra linewidth and nonaxial crystal-field parameter in K3H(SO4)2 and Rb3H(SO4)2 allows one to suggest the presence of “local mode” predicted by Yamada (Ferroelectrics 170 (1995) 23). The activation energy for this kind of excitation was found and equals 11.3 (0.5) and 7.4 (0.3) meV for Mn2+ doped K3H(SO4)2 and Rb3H(SO4)2, respectively.  相似文献   

13.
气溶胶颗粒的吸湿性决定了其尺寸、浓度、化学组成以及相态,从而显著影响着全球气候、大气异相化学以及人类健康。运用在线、原位、连续扫描衰减全反射傅里叶变换红外光谱(ATR-FTIR)技术, 结合线性湿度(RH)控制系统,实现了RH连续变化条件下气溶胶FTIR-ATR光谱的快速测量。根据水弯曲振动谱带(~1 640 cm-1)峰面积随RH的变化,得到了(NH4)2SO4,NH4NO3和(NH4)2SO4/NH4NO3混合气溶胶的质量增长因子(MGFs)、潮解点(DRH)和风化点(ERH)。与气溶胶的E-AIM模型预测值相比较,实验结果表现出良好的一致性,证实该方法是一种测量大气气溶胶MGFs,ERH和DRH的快速测量方法。  相似文献   

14.
A new procedure for the preparation of Tl2Ba2CaCu2O8-δ is presented. In the first step stoichiometric amounts of Cu(NO3)2·3H2O, Ba(OH)2·H2O, CaO and Tl2O3 are reacted in a closed alumina crucible at 760°C to form a mixture of Tl- 2212, CuO, CaO and other oxide phases. In the second step this material is milled, pelletized and fired in a gold-sealed alumina crucible at 860–900°C for three to eight hours. Three batches of Tl-2212 prepared by this method were investigated showing less than 1% loss of thallium while Tc was close to 110 K. Rietveld refinements using time-of-flight neutron-diffraction data demonstrate that the method produces pure material in a reproducible way and that the materials are substoichiometric with respect to oxygen (δ=0.3). Investigations using electron diffraction and high-resolution electron microscopy indicate the absence of stacking faults.  相似文献   

15.
稀土掺杂发光材料一直是科研领域研究的热点,被广泛应用于白光LED、温度传感、显示显像、新能源和激光等领域。基质的结构对于稀土离子光致发光特性有非常重要的影响,在众多发光基质材料中,硼酸盐具有透光范围宽、光学损伤阈值高、较好的热稳定性和化学稳定性等优点。碱土-稀土金属硼酸盐Sr3Y2(BO3)4具有出色的光学性能,对其发光性能的研究具有重要意义。稀土离子Eu3+具4f6电子层,是一种典型的下转换发光中心离子,常被选作红色发光材料的激活剂。Dy3+具4f9电子层,也是一种典型的下转换发光中心离子,在紫外光激发下,在蓝色光区和橙色光区有较强的荧光发射。采用高温固相法合成了Sr3Y2(BO3)4∶Eu3+/Dy3+荧光粉,通过XRD和SEM对样品的结构和形貌进行了表征,XRD结果表明,1 000 ℃烧结5 h,H3BO3过量20%为最佳制备条件,且少量的Eu3+和Dy3+掺杂并未改变Sr3Y2(BO3)4的晶格结构。SEM图像表明Sr3Y2(BO3)4基质的平均晶粒尺寸为2~4 μm,10%Eu3+单掺和5%Eu3+/5%Dy3+双掺样品与基质Sr3Y2(BO3)4的SEM图像相比,形貌和尺寸并没有发生明显的改变。Sr3Y2(BO3)4∶Eu3+荧光粉的发光结果表明,分别在395和466 nm激发下,浓度为5%,10%和15%的Eu3+单掺Sr3Y2(BO3)4荧光粉的主要发光位于593和613 nm的红光发射,峰强度随着Eu3+浓度的增加呈现先增加后降低的变化形式,掺杂浓度为10%时发光强度最大,说明存在浓度猝灭现象。色坐标结果显示,激发波长由395 nm变化到466 nm,Sr3Y2(BO3)4∶Eu3+荧光粉的发光颜色从橙红色向红色转变。引入Dy3+后,Sr3Y2(BO3)4∶Eu3+/Dy3+样品的发射光谱出现Dy3+的486 nm的蓝光发射(4F9/2→6H15/2)和576 nm的橙光发射(4F9/2→6H13/2),并且随着Dy3+浓度的增加,对Eu3+的5D0→7F1, 2, 3, 4跃迁有抑制作用。色坐标结果显示通过调整掺杂离子Eu3+和Dy3+的比例可实现Sr3Y2(BO3)4∶Eu3+/Dy3+荧光粉的颜色从红色区域向橙色区域转变,说明其在显示方面具有良好的应用前景。  相似文献   

16.
Intensities have been measured for individual transitions in the Q and R branches of the ν1 band of NH3 using a difference-frequency laser spectrometer. The data yield an integrated band strength of S0v=219.36±1.03 cm-2/MPa at 297 K, corresponding to a transition moment of μv = 8.535(20) × 10-32 C·m, and a Herman-Wallis correction factor, (1 + jm)2, where j = 0.0209(20). The intensities of a few lines for K 7 were noticeably perturbed by a perpendicular Coriolis interaction with 2ν4 (E, L = 2), so were excluded from the fit. A small sample of ν3 band lines occurring in the ν1 band scans also yields a rough estimate of the ν3 band intensity with evident irregular perturbations.  相似文献   

17.
利用高温固相法制备了BaGd_2(MoO_4)_4∶Tb~(3+)与BaGd_2(MoO_4)_4∶Tb~(3+),Eu~(3+)荧光粉,并借助于X射线衍射(XRD)、激发光谱、发射光谱及荧光衰减曲线对样品的结构及发光性能进行了表征。在290 nm激发下,BaGd_2(MoO_4)_4∶Tb~(3+)样品在550 nm处具有较强的绿光发射,表明该样品可用作绿色荧光粉。Tb~(3+)离子的最佳掺杂浓度为50%,电偶极间相互作用是引起浓度猝灭效应的主要原因。当在BaGd_2(MoO_4)_4∶Tb~(3+)荧光粉中共掺入Eu~(3+)离子后,可同时观测到Tb~(3+)与Eu~(3+)离子的特征发射峰。随Eu~(3+)掺杂浓度的升高,Tb~(3+)离子的发光强度逐渐下降,而Eu~(3+)离子的发光强度逐渐增加。根据BaGd_2(MoO_4)_4∶Tb~(3+),Eu~(3+)中Tb~(3+)离子的荧光寿命计算了Tb~(3+)与Eu~(3+)离子间的能量传递效率,并根据荧光寿命与激活离子掺杂浓度的关系证实了能量传递机制为电偶极间相互作用。  相似文献   

18.
Deuteration of the readily-exchangeable protons in [(CH3)3NH]-CoCl3·2H2O causes little or no change in the long-range magnetic ordering temperature. This is consistent with the strong two-dimensional anisotropy of exchange interactions in this chained compound.  相似文献   

19.
Efficient intracavity second-harmonic generation (SHG) has been realized in a new Li-doped GdCa4O(BO3)3 (GdCOB) crystal. 2.55 W CW SHG output power was obtained with an optical conversion efficiency of 19.6%, while the effective intracavity SHG efficiency was determined to be 44%. Compared to that of undoped GdCOB crystal, the effective SHG efficiency of the Li-doped GdCOB crystal was found to increase by 12.5%.  相似文献   

20.
Spin-lattice relaxation times T1 and T are determined for protons in three polycrystals (CH3NH3)5Bi2Cl11, (CD3NH3)5Bi2Cl11 and (CH3ND3)5Bi2Cl11. The temperature dependencies of the relaxation times obtained for (CH3NH3)5Bi2Cl11 and (CD3NH3)5Bi2Cl11 are interpreted as a result of correlated motions of the three-proton groups of the monomethylammonium cation. The minimum of the T relaxation time is explained as a result of the oscillations of the symmetry axis of the whole cation.  相似文献   

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