共查询到20条相似文献,搜索用时 182 毫秒
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用两带Ginzburg-Landau(GL)理论分析了Lu2Fe3Si5的表面临界磁场,当超导体的表面与任一主晶面重合,且外磁场平行于超导体的表面时,比值Hc3/Hc2(HC2是Lu2Fe3Si5的上临界磁场)强烈依赖于温度. 当超导体的表面是bc平面,且
关键词:
两带超导体
GL理论
2Fe3Si5')" href="#">Lu2Fe3Si5
表面临界磁场 相似文献
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一个新颖的磷掺杂硼钒氧簇化合物[Li(H2O)2]2[Cu(en)2]3[H2en]2[V12P12B6O68(OH)4(H2O)]·3(H2O)1通过水热法合成,通过Li+连接成一维无限结构,再通过氢键连成三维立体结构。针对该化合物,通过二维红外相关光谱并作了详细分析,化合物1簇阴离子振动偶极矩对磁场和温度的变化均有响应峰,2D-IR COS提供了一种结构表征新方法。 相似文献
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本工作利用光学多道分析仪(OMA Ⅲ)测量了脉冲TEA CO2激光诱发的SiH4等离子体内H Balmer系的Hα,Hσ和Hγ线的线型。结果表明,三条谱线的FWHM(半值全宽度)随跃迁上能级的主量子数的增加而增加,即△λ1/2(Hα)<△λ1/2(Hβ)<△λ1/2(Hγ)。通过对等离子体内各类加宽机制的讨论,得出等离子体内谱线的主要加宽机制为Stark加宽。由Hα线的实验线型与Stark加宽理论线型的拟合,得到等离子体的两个重要参量,平均电子密度N≈1017cm-3,电子温度T≈40 000K。由Hβ线的时间分辨测量得到等离子体的电子密度随时间的演变曲线。
关键词: 相似文献
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采用电阻阻错结的无序二维约瑟夫森结阵列模型,数值研究超导薄膜中垂直磁场引起的涡旋运动.通过分析磁场激发产生的涡旋度Ne及低频电压噪声S0的变化特性,得到如下结论:在无序超导体中固定温度不变,随着磁场的减弱涡旋液态经过准有序的布拉格相,涡旋玻璃相重新进入到低磁场下的钉扎稀磁液相. 由于在涡旋玻璃相中,电流驱动下的噪声值表现出一个峰,表明系统处于无序与有序相互竞争的亚稳态,并且临界电流应有峰值效应. 计算得到噪声值的变化与Okuma等得到的无序超导MoxSi1-x膜实验现象一致,并能解释磁场降低引起的重新进入钉扎的稀磁液相行为.
关键词:
约瑟夫森结阵列
磁通玻璃
重新进入
峰值效应 相似文献
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本文研究单分子磁体Na9[Cu3Na3(H2O)9 (α-AsW9O33)2]·26H2O中三角自旋 环在磁场作用下的热纠缠性质, 利用数值计算求出任意两个Cu2+离子量子比特之间的配对纠缠度, 分别记为C12, C23和C13. 研究结果表明, 磁场的方向和大小以及温度对配对纠缠度具有重要影响, 而且参数的变化对C12, C23和C13的影响也是各不相同. 给出外加三个不同方向的磁场时, 配对纠缠度C12, C23和C13各自对应的临界温度Tc随磁场强度的变化图, 由此可以得到单分子磁体三角自旋环中存在纠缠态的参数范围. 通过选择适当的磁场方向和大小以及温度等实验参数, 可以有效地调节和提高单分子磁体中的配对纠缠度.
关键词:
配对纠缠
单分子磁体
三角自旋环 相似文献
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用粒子模拟方法求解描述环形等离子体中电子温度梯度静电模的回旋动力学方程.方程采用圆磁通面的轴对称环形几何系统,考虑了有限拉摩半径、电子渡越频率k∥v ∥以及环形漂移(曲率和磁场梯度)运动wD(v2⊥,v 2∥,θ)的效应.简述了粒子模拟的基本方法.采用了四阶变步长积分格式,使计算省时、简便.讨论了模的基本特征 , 并且给出了临界梯度对电子温度与离子温度之
关键词:
电子温度梯度不稳定性
粒子模拟
变步长积分格式
临界梯度 相似文献
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以8-羟基喹啉为配体的金属配合物是一种性能优良的有机电致发光材料,其中有关8-羟基喹啉铝(Alq3)研究已有大量报道,8-羟基喹啉锌(Znq2)研究还有待发展。介绍了两种以Znq2为基体的新型有机电致发光材料Znq2(H2O)2和(Znq2)4的合成方法。用IR、XRD、TG、DTA和荧光测试方法进行表征与分析表明:Znq2(H2O)2和(Znq2)4的玻璃化温度(Tg)分别为104.2℃和204.9℃;在161℃下Znq2(H2O)2脱去水分子成为Znq2,在361℃高温下四聚体(Znq2)4裂解为单体Znq2;Znq2(H2O)2和(Znq2)4具有很好的发光性能,在光致发光谱中λmax分别是505,550nm。 相似文献
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本文利用耦合的技巧,建立了Ising模型与接触过程的联系。由此给出了Ising模型临界温度的上界,即n维Ising模型的临界点βc(n)应满足 exp{2βc(n)(2n-1)}·(exp{2βc(n)}-1)≥2/2n-1。特别是三维Ising模型的临界点βc(3)>1/2ln1.17。
关键词: 相似文献
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M. Gitterman I. ShapiroB.Ya. Shapiro 《Physica C: Superconductivity and its Applications》2012,472(1):83-86
In a nonuniform superconductor with randomly distributed local critical temperature both the macroscopic critical temperature and the upper critical magnetic field strongly depend on the characteristic correlation length ρ0 of correlated disorder. The shift of the macroscopic critical parameters from those for non-correlated disorder, which does not exist for white noise, is obtained for small ρ0 in the framework of the Ginzburg-Landau theory. 相似文献
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根据两带Ginzburg-Landau 理论计算了层状超导材料NbS2的上临界磁场, 以及上临界磁场各向异性参数随温度的变化情况, 并将NbS2与MgB2, NbSe2上临界磁场的各向异性进行比较. 所得计算结果与已有实验数据符合得很好, 充分说明了NbS2的超导电性具有两能隙特征. NbS2上临界磁场各向异性参数在5.0 K附近逐渐变小, 这与MgB2和NbSe2有相似之处. 但NbS2的上临界磁场各向异性参数大约为7.3, 明显大于MgB2和NbSe2. 计算结果还表明, NbS2较大能隙所对应能带的有效质量比约为54, 另一能带的有效质量基本为各向同性. 相似文献
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实验研究了温度对液相外延石榴石磁泡薄膜中条状普通硬磁畴壁内的垂直布洛赫线(VBL)链解体临界面内磁场区间的影响。发现存在一对特征温度T(1)0 和 T(2)0(前者比后者略低但均高于室温),在从室温到T(2)0的每个温度T下,使VBL逐渐消失的面内磁场Hip都分布于一个与T有关的区间[Hip(1)(T), Hip(2)(T)]内,称为临界面内磁场区间:Hip<Hip(1)(T)时,VBL链保持不变;Hip(1)(T)< Hip < Hip(2)(T)时,随着Hip的增加,越来越多的VBL消失;Hip > Hip(2)(T)时,所有VBL都消失。Hip(1)(T),Hip(2)(T)及Hip(2)(T)-Hip(1)(T)均随T的升高而下降,前二者分别于T(1)0 和 T(2)0降为零。比值Hip(2)(T)/Hip(1)(T)随T的升高而升高,在低温段(包括室温)升高缓慢且约为21/2,在T(1)0附近急剧升高且至T(1)0时趋于∞。对以上结果做了理论分析。
关键词: 相似文献
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《Physica C: Superconductivity and its Applications》2002,360(3):247-255
In this paper, we employ a continuous Ginzburg–Landau model to study the behaviors of the parallel upper critical field of an intrinsically layered superconductor. Near Tc where the order parameter is nearly homogeneous, the parallel upper critical field is found to vary as (1−T/Tc)1/2. With a well-localized order parameter, the same field temperature dependence holds over the whole temperature range. The profile of the order parameter at the parallel upper critical field is of a Gaussian type, which is consistent with the usual Ginzburg–Landau theory. In addition, the influences of the unit cell dimension and the average effective masses on the parallel upper critical field and the associated order parameter are also addressed. 相似文献
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C. Ferdeghini V. Ferrando V. Braccini M.R. Cimberle D. Marré P. Manfrinetti A. Palenzona M. Putti 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,30(2):147-151
The anisotropy of MgB2 is still under debate: its value, strongly dependent on the kind of sample and on the measuring method, ranges between 1.2
and 13. In this work we present our results on MgB2 c-oriented superconducting thin film. To evaluate the anisotropy, we followed two different approaches. Firstly, magnetoresistivity
was measured as a function of temperature at selected magnetic fields applied both parallel and perpendicular to the c-axis; secondly, we measured magnetoresistivity at selected temperatures and magnetic fields, varying the angle θ between the magnetic field and the c-axis. The anisotropy estimated from the ratio between the upper critical fields parallel and perpendicular to the c-axis and the one obtained in the framework of the scaling approach within the anisotropic Ginzburg-Landau theory are different
but show a similar trend in the temperature dependence. Some differences in the upper critical field and in its anisotropy
of our film with respect to single crystals are emphasized: some of these aspects can be accounted for by an analysis of upper
critical fields within a two-band model in presence of disorder and/or crystallographic strain.
Received 12 July 2002 / Received in final form 17 September 2002 Published online 29 November 2002 相似文献
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E. Z. Kuchinskii N. A. Kuleeva M. V. Sadovskii 《Journal of Experimental and Theoretical Physics》2017,125(6):1127-1136
We study disorder effects upon the temperature behavior of the upper critical magnetic field in an attractive Hubbard model within the generalized DMFT+Σ approach. We consider the wide range of attraction potentials U—from the weak coupling limit, where superconductivity is described by BCS model, up to the strong coupling limit, where superconducting transition is related to Bose–Einstein condensation (BEC) of compact Cooper pairs, formed at temperatures significantly higher than superconducting transition temperature, as well as the wide range of disorder—from weak to strong, when the system is in the vicinity of Anderson transition. The growth of coupling strength leads to the rapid growth of Hc2(T), especially at low temperatures. In BEC limit and in the region of BCS–BEC crossover Hc2(T), dependence becomes practically linear. Disordering also leads to the general growth of Hc2(T). In BCS limit of weak coupling increasing disorder lead both to the growth of the slope of the upper critical field in the vicinity of the transition point and to the increase of Hc2(T) in the low temperature region. In the limit of strong disorder in the vicinity of the Anderson transition localization corrections lead to the additional growth of Hc2(T) at low temperatures, so that the Hc2(T) dependence becomes concave. In BCS–BEC crossover region and in BEC limit disorder only slightly influences the slope of the upper critical field close to T c . However, in the low temperature region Hc2 (T may significantly grow with disorder in the vicinity of the Anderson transition, where localization corrections notably increase Hc2 (T = 0) also making Hc2(T) dependence concave. 相似文献
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本文指出,对于实际的归一化有效声子谱函数g(ω),一般来说,zph≡F(-ωph-2是函数z=F(y)≡∫0(ωph)(ω2y)/(ω2y+1)g(ω)dω的反函数的分支点。因此,在估算超导Tc级数的收敛半径时,应当予以考虑。
关键词: 相似文献