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介绍了采用了MgB2薄膜的化学气相沉积(CVD)异位退火和双温区混合物理化学气相沉积(HPCVD)制备技术,并以B膜作为势垒层在多晶的Al2O3基底上制作了三明治结构的MgB2/B/MgB2多层膜.采用扫描电子显微镜(SEM)、X射线衍射(XRD)和标准四线法对制备的MgB2/B/MgB2多层膜的断面结构、超导薄膜晶体结构及超导特性进行了测量研究.结果表明,制备的MgB2/B/MgB2多层膜结构清晰,底层和顶层超导薄膜显示出良好的超导特性. 相似文献
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本文采用固相反应法制备了一系列纳米Pr6O11掺杂的MgB2超导块材,掺杂量分别为0,1,3,5,10wt.%.X射线衍射结果表明:随着Pr6O11掺杂量的增加,MgB2的晶格常数也逐渐增大,也就是说Pr原子部分替代了MgB2晶格中的Mg原子.磁测量结果显示,Pr6O11的掺杂对MgB2的超导转变温度(Tc)有很小的抑制.在低含量Pr6O11掺杂(1wt.%)时,MgB2的临界电流密度(Jc)和不可逆场(Hirr)均有明显的提高,但进一步提高Pr6O11的掺杂量时,会损害MgB2在高场下的性能.文中同时也讨论了Pr6O11掺杂影响MgB2的Tc和Jc性能的机理. 相似文献
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我们用混合物理化学气相沉积(Hybridphysicalchemicalvapordeposition简称为HPCVD)法在αAl2O3(00l)衬底上原位制备了一批超导性能良好的外延MgB2超导薄膜样品.用10%浓度的乙硼烷(B2H6)氢气混合气作为原料,研究了不同条件对MgB2薄膜沉积速率的影响.在一定条件下制备了一批MgB2薄膜,厚度为200nm左右,样品的零电阻转变温度(Tc0)最高达到39K.X射线衍射分析的θ~2θ扫描表明,MgB2薄膜的晶粒都具有较好的C轴取向,对样品的(101)面Φ扫描结果显示MgB2薄膜晶格与衬底有很好的外延取向,取向关系为[1010]MgB2∥[1120]Al2O3.由毕恩模型计算求得在5K和零场条件下,样品的临界电流密度Jc=9.8×106A/cm2.这些结果表明HPCVD技术在MgB2外延薄膜原位制备方面有着很大的优势,从而有利于实现MgB2薄膜在电子器件方面的应用. 相似文献
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较之高温制备,低温活化烧结技术可有效避免MgB2超导块体制备中的一些问题,如Mg易挥发、高温MgB2晶粒长大、结晶度高等问题.为进一步提高超导块体的载流能力,J Shimoyama等采用金属Ag掺杂并在550℃烧结72h后获得了高性能的MgB2超导体,使得金属Ag成为低温活化烧结的有效组元.然而,对金属Ag低温活化烧结MgB2超导块体的成相机理尚缺乏系统的分析和理解.本文系统研究了金属Ag掺杂MgB2超导块体的成相动力学过程,发展了金属Ag掺杂低温活化快速制备技术,结合液相活化烧结理论阐述了金属Ag掺杂MgB2块体的低温活化烧结机理. 相似文献
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MgB2/Fe带材Jc的各向异性及MgB2芯织构和成分不均一性的研究 总被引:1,自引:0,他引:1
本文研究了在不同磁场方向和温度下非原位Fe包套MgB2单芯带Jc的各向异性,通过对各种工艺条件下带材中MgB2芯的X-ray衍射图进行拟合分析和计算,比较了MgB2芯在Fe-MgB2界面和中心处的织构度和成份不均一性.研究发现带材Jc的各向异性受初始粉末颗粒尺寸的影响.由于受套管材料强度和形变加工工艺的影响,MgB2芯在Fe-MgB2界面处比在中心处有较强的织构.在MgB2-Fe的界面处,700℃淬火样品的X-ray衍射图中发现了由中间相Fe23B6生成的金属间化合物Fe2B.另外还研究了MgB4和MgO等主要杂质相的形成原因. 相似文献
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我们对用纳米镁粉(平均颗粒度≤40nm)在常压下制备MgB2超导样品(以下简称纳米MgB2超导样品)进行了研究.得到了一组与用普通颗粒镁粉分别在真空条件下和流动氩气下制备MgB2超导样品时得到的原位ρ-T曲线不同的曲线.实验结果表明纳米MgB2超导样品的成相温区是430℃到490℃之间,低于用普通颗粒镁粉分别在真空条件下和流动氩气下制备MgB2超导样品时的成相温度:640℃~700℃和530℃~630℃.所得到的纳米MgB2超导样品的密度是1.46g/cm3.它高于用其他各种镁粉原料在常压下制备通过一次烧结制得的MgB2超导样品. 相似文献
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测量了MgB2 和Mg0 .93Li0 .0 7B2 的电阻率 ρ(T)与霍尔系数RH(T)的温度依赖关系 .电阻率的测量结果表明 ,MgB2 和Mg0 .93Li0 .0 7B2 的正常态电阻率与温度有平方的依赖关系 .MgB2 和Mg0 .93Li0 .0 7B2 的超导转变温度几乎相同 .霍尔系数的测量结果表明 ,MgB2 和Mg0 .93Li0 .0 7B2 的载流子类型为空穴型 ,二者的霍尔系数都随温度升高而减小 ,且Mg0 .93Li0 .0 7B2 的霍尔系数比MgB2 略有减小 ,这可能与Li掺杂引入空穴有关 .二者的霍尔角都与温度平方呈线性关系 . 相似文献
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We study the complex Berry phases in non-Hermitian systems with parity- and time-reversal $\left({ \mathcal P }{ \mathcal T }\right)$ symmetry. We investigate a kind of two-level system with ${ \mathcal P }{ \mathcal T }$ symmetry. We find that the real part of the the complex Berry phases have two quantized values and they are equal to either 0 or π, which originates from the topology of the Hermitian eigenstates. We also find that if we change the relative parameters of the Hamiltonian from the unbroken-${ \mathcal P }{ \mathcal T }$-symmetry phase to the broken-${ \mathcal P }{ \mathcal T }$-symmetry phase, the imaginary part of the complex Berry phases are divergent at the exceptional points. We exhibit two concrete examples in this work, one is a two-level toys model, which has nontrivial Berry phases; the other is the generalized Su–Schrieffer–Heeger (SSH) model that has physical loss and gain in every sublattice. Our results explicitly demonstrate the relation between complex Berry phases, topology and ${ \mathcal P }{ \mathcal T }$-symmetry breaking and enrich the field of the non-Hermitian physics. 相似文献
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The chirality-asymmetry macroscopic force mediated by light
pseudoscalar particles between α -quartz and some achiral
matter is studied. If this force between achiral source mass and
α -quartz with some chirality is attractive, it will become
repulsive when the chirality of the α -quartz crystal is
changed. According to the tested limits of the coupling constant
gs gp /\hbar c< 1.5× 10-24 at the
Compton wavelength λ = 10-3 m, the force (F) between
a 0.08× 0.08× 0.002 m3 block of α -quartz
and a 0.08× 0.08× 0.01 m3 copper block with a
separation being 0.5× 10-3 \mbox{m} in between, is
estimated from the published data at less than 4.64× 10-24 N, i.e. F < 4.64× 10-24 N. 相似文献
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X-ray diffraction study of effect of deposition conditions on α--β phase transition and stress evolution in sputter-deposited W coatings 下载免费PDF全文
Pure W and W-Cu-W trilayer coatings were deposited on an Fe substrate by d.c. magnetron sputtering. The α-β phase evolution, intragranular stress evolution in sputter-deposited W layer were investigated by x-ray diffraction. They are directly related to the film microstructure, density and adhesion. Therefore, control of the film stress and phase component transition is essential for its applications. The phase component transition from β-W to α-W and intragranular stress evolution from tensile to compressive strongly depend on the deposition parameters and can be induced by lowering Ar pressure and rising target power. The compressively stressed films with α-W phase have a dense microstructure and high adhesion to Fe substrate. 相似文献
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报道了CuGeO3单晶在96GHz频率,1 4K温度下的电子顺磁共振(EPR)实验,测量了主轴g因子.导出了Cu2+离子在CuGeO3自旋佩尔斯系统中的混合d轨道基态波函数.采用近似自洽场方法计算了CuGeO3的主轴g因子.使实验结果得到了解释. 相似文献
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白花刺参中的咖啡酰基奎宁酸成分 总被引:16,自引:0,他引:16
著名藏药白花刺参Morina nepalensis var. albaHand. Mazz.的全株的水溶性部分通过硅胶、RP-8、Sephadex LH-20柱层析分离,得到4个咖啡酰基奎宁酸1~4 ,运用光谱和波谱方法, 分别鉴定为3-O-咖啡酰基奎宁酸(1)、3,5-O-双咖啡酰基奎宁酸(2)、3,4-O-双咖啡酰基-奎宁酸(3)和4,5-O-双咖啡酰基-奎宁酸(4). 应用2D NMR图谱, 对其氢和碳的化学位移进行全归属, 并报道1, 2在氘代甲醇和氘代二-甲亚砜两种溶剂下测定1H和13C化学位移. 4个化合物都是首次分离自刺参属植物. 相似文献
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Nanosecond-time-resolved infrared spectroscopic study of fast relaxation kinetics of protein folding by means of laser-induced temperature-jump 下载免费PDF全文
Elucidating the initial kinetics of folding pathways is critical to the understanding of the protein folding mechanism. Transient infrared spectroscopy has proved a powerful tool to probe the folding kinetics. Herein we report the construction of a nanosecond laser-induced temperature-jump (T-jump) technique coupled to a nanosecond timeresolved transient mid-infrared (mid-IR) spectrometer system capable of investigating the protein folding kinetics with a temporal resolution of 50 ns after deconvolution of the instrumental response function. The mid-IR source is a liquid N2 cooled CO laser covering a spectral range of 5.0μm (2000 cm^-1)-6.5μm (1540 cm^-1). The heating pulse was generated by a high pressure H2 Raman shifter at wavelength of 1.9μm. The maximum temperature-jump could reach as high as 26±1℃. The fast folding/unfolding dynamics of cytochrome C was investigated by the constructed system, providing an example. 相似文献