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本文研究了在接近转变温度Tc的区域内,超导薄膜在磁场中的性质。磁场是沿着超导膜的表面。在文章中,首先对Γорьков理论进行了分析,指出这个理论实际上是采用了局域近似,这个近似主要是隐含在他所采用的磁场中电子Green函数Gω0(rr′)的表示式中。作者指出,Γорьков所采用的Gω0(rr′)表示式对于本文研究的问题是不适用的,本文采用Gω0(rr′)按矢势的微扰展开式。本文把Γорьков的补偿方程和电流方程推广到超导膜。对于d<δ0(T)的膜,求出了这二个方程的解,得到超导薄膜的矢势、磁矩、能隙和临界电流的表达式,并研究了超导薄膜在磁场中的相变问题,求得超导薄膜的临界磁场。本文所得到的结果,对比较厚的膜(d?ξ0)和ГЛ理论一致,而对比较薄的膜(d<ξ0)和ГЛ理论有着显著不同(除了临界电流和超导膜在磁场中相变级数的判据外),二者的差异特别是表现在对厚度依赖关系上。由于本文所采用的近似,所得到的结果适用于δ0(T)>d?d*情形,其中2d*=(1/(0.36)×ξ0/p0)1/2,对于Sn,2d*~10-6cm。 相似文献
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本文研究了90nm CMOS工艺下栅氧化层厚度为1.4 nm沟道长度为100 nm的轻掺杂漏(LDD)nMOSFET栅电压VG对栅致漏极泄漏 (GIDL)电流Id的影响,发现不同VG下ln (Id/(VDG-1.2))-1/(VDG-1.2)曲线相比大尺寸厚栅器件时发生了分裂现象. 通过比较VG变化下ln(Id/(VDG-1.2))的差值,得出VG与这种分裂现象之间的作用机理,分裂现象的产生归因于VG的改变影响了GIDL电流横向空穴隧穿部分所致. 随着|VG|的变小,ln(Id/(VDG-1.2))曲线的斜率的绝对值变小.进一步发现不同VG对应的ln (Id/(VDG-1.2))曲线的斜率c及截距d与VG呈线性关系,c,d曲线的斜率分别为3.09和-0.77. c与d定量的体现了超薄栅超短沟器件中VG对GIDL电流的影响,基于此,提出了一个引入VG 影响的新GIDL电流关系式. 相似文献
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研究了两光束的合成方式(相干和非相干合成)对俘获金属瑞利粒子的辐射力和稳定性的影响,着重研究了辐射力与合成方式、离轴距离、相干参数和粒子半径的关系.结果表明,不同合成方式下,离轴距离和相干参数都分别存在临界值dc和αc,在0dc或α>αc时,焦面处光强呈中心凹陷分布,此时横向梯度力不能作为回复力俘获金属瑞利粒子.在0<d≤dc时,与非相干合成光束比较,相干合成光束在焦面处光强、辐射力、俘获刚性和纵向俘获范围更大.因此,适当选择合成方式,较小离轴距离和较低相干参数可有利于合成光束对金属瑞利粒子的俘获. 相似文献
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利用夸克模型计算了核子的自旋相关结构函数随Q2的依赖关系.在小动量转移区研究高扭曲效应a2(Q2),d2(Q2)对结构函数的影响.计算结果和其它的一些模型理论计算做了比较. 相似文献
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Electronic structures and magnetoelectric properties of tetragonal BaFeO3: an ab initio density functional theory study 下载免费PDF全文
First-principles calculations have been performed to investigate the ground state electronic properties of BaFeO3 (BFO). Local spin density approximation (LSDA) plus U (LSDA+U) treatment modified the metallic behaviour to insulated one with a band gap of 4.12eV. The spontaneous polarization was found to be 89.3\muC/cm2 with Berry phase scheme in terms of the modern theory of polarization. Fe-3d eg were split into two singlet states (dz2 and d x2-y2}), and Fe-3d t2g were split into one doublet states(dxz and dyz) and one singlet states(dxy) after Fe and O displaced along the c axis. Meanwhile the occupation numbers of dz2, dyz, dxz and OT pz (on the top of Fe) were increased at the expense of those in xy plane. Our results showed that it was the sensitivity of hybridization to ferroelectric distortions, not just the total change of hybridization, that produced the possibility of ferroelectricity. Moreover, the increasing occupation numbers of OT pz and Fe dz2 favoured the 180o coupling between Fe-3d eg and Fe-3d t2g, leading to ferromagnetic ordering, which has been confirmed by the increase of magnetic moment by 0.13μB per formula unit in the polarized direction. Hence, the magnetization can be altered by the reversal of external electric field. 相似文献
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设计出一种新型的渐变空气孔径THz波超平坦色散光子晶体光纤.应用时域有限差分方法(finite-difference time-domain,FDTD)计算光纤色散,所得结果表明渐变空气孔径光子晶体光纤比孔直径不变光子晶体光纤控制色散的能力更强;且当第三层与第四层空气孔直径相同时,孔直径渐变的光子晶体光纤的色散更趋于平坦,而当空气孔直径取d1=0.85d4, d2=0.95d4,d3=d4(d1,d2,d3,d4分别为包层从内到外空气孔的直径)时,此种光子晶体光纤可以在波长60—65 μm(4.61—5 THz)范围内将波导色散值控制在-0.1±0.3 ps/(km·nm)范围内,得到趋于超平坦色散的、具有很好的束缚THz波的能力和良好的损耗特性的新型THz波光子晶体光纤.
关键词:
THz波光子晶体光纤
时域有限差分方法
超平坦色散 相似文献
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Cross-linked polypropylene (XPP) foams are modified by a hot-stretching process and charged to be piezoelectric. The results show that a piezoelectric d33 -coefficient of 308pC/N is obtained for sample with an elongation ratio of 200%. The dynamic d33 value is smaller than the quasi-static value, which is probably due to the rise of Young’s modulus with increasing frequency. All the samples show pressure-independent d33 in the range up to 30 kPa. Improved d33 was obtained in the sample rough surface exposed to the corona during charging. Compared to linear PP, the stretched XPP shows pressure independence of d33 in larger range. 相似文献
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Michael E. Gersh Lawrence S. Bernstein Lauren M. Peterson 《Journal of Quantitative Spectroscopy & Radiative Transfer》1981,26(5):411-429
Two experimental techniques were used to determine the high temperature infrared absorption coefficients of the v3 band of BF3. A high temperature flow tube fitted with a multipass infrared absorption cell was used to determine the BF3 absorption coefficients at 295, 585, 870, 1150, and 1440K. BF3 was also used in a flame emission-absorption apparatus to determine the BF3 absorption coefficients at 2400 K.A generalized formulation for predicting the S/d and 1/d band model parameters of symmetric top perpendicular bands of MX3 molecules is presented. The effect of including nuclear spin statistics in computing the S/d and 1/d band model parameters is considered. It is shown that nuclear spin statistic?s effect only the 1/d parameter and are significant only for the case of zero nuclear spin. A number of practical considerations, which arise in designing a computer algorithm to calculate the S/d and 1/d parameters, are discussed.Comparisons of the theoretical and experimental BF3 absorption coefficients are made. Good agreement between theory and experiment at all temperatures was obtained by adjusting only two vibrational energy coupling constants, χ23 and χ34. Predicted S/d and 1/d band model parameters at 300, 600, 900, 1200, 1500, 2000, 2500, and 3000 K are presented. 相似文献
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Implementation of an adiabatic quantum algorithm for factorization on two qudits with the number of levels d 1 and d 2 is considered. A method is proposed for obtaining a time-dependent effective Hamiltonian by means of a sequence of rotation operators that are selective with respect to the transitions between neighboring levels of a qudit. A sequence of RF magnetic field pulses is obtained, and a factorization of the numbers 35, 21, and 15 is numerically simulated on two quadrupole nuclei with spins 3/2 (d 1 = 4) and 1 (d 2 = 3). 相似文献
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M.J. Zuckermann 《Solid State Communications》1973,12(7):745-747
The Curie temperature Tc of a proximity sample composed of a thin film of a weak itinerant ferromagnet of thickness df in contact with a thick film of an enhanced parmagnetic metal is calculated using the Hubbard model in the Hartree-Fock approximation. The sample is paramagnetic for values of df less than a critical thickness df0 of the order of the coherence length. The shape of the curve of Tc vs. df for df > df0 depends on whether the bulk ferromagnet exhibits a Curie-Weiss or a Pauli susceptibility above the bulk Curie temperature. The letter is concluded by comments on the experimental situation. 相似文献
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Aloysius Soon Joel Wallman Bernard Delley Catherine Stampfl 《Current Applied Physics》2013,13(8):1707-1712
We present a trend study of a large variety of dopants at the cation site in Cu2O (i.e. substituting Cu), focussing largely on the early 3d-, 4d-, and 5d-transition metals (TMs) in which many of them are known to be non-magnetic. We also include s-, sp- and d10-metals for comparison. We find that doping with sp-elements results in zero spin moment while dopants with a partially filled d-band show a stronger tendency to magnetize and 3d-TM dopants exhibit a larger magnetic moment than most of the 4d- and 5d-TM dopants. From this trend study, we also find a correlation between their substitution enthalpy and associated interatomic relaxations. In particular, Ti-doped Cu2O appears to be an interesting system, given its “peculiar” ability to exhibit a spin moment when doped with a non-magnetic substituent like Ti. We also find that the interaction between two doped Ti atoms in Ti2:Cu2O is predominantly antiferromagnetic, and interestingly (and unexpectedly), this interaction rapidly declines as a function of inter-dopant distance, as in the case for the magnetic late-TM dopants like Co2:Cu2O. 相似文献
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M. Potthoff W. Nolting 《The European Physical Journal B - Condensed Matter and Complex Systems》1999,8(4):555-568
The correlation-driven transition from a paramagnetic metal to a paramagnetic Mott-Hubbard insulator is studied within the
half-filled Hubbard model for a thin-film geometry. We consider simple-cubic films with different low-index surfaces and film
thickness d ranging from d=1 (two-dimensional) up to d=8. Using the dynamical mean-field theory, the lattice (film) problem is self-consistently mapped onto a set of d single-impurity Anderson models which are indirectly coupled via the respective baths of conduction electrons. The impurity models are solved at zero temperature using the exact-diagonalization
algorithm. We investigate the layer and thickness dependence of the electronic structure in the low-energy regime. Effects
due to the finite film thickness are found to be the more pronounced the lower is the film-surface coordination number. For
the comparatively open sc(111) geometry we find a strong layer dependence of the quasi-particle weight while it is much less
pronounced for the sc(110) and the sc(100) film geometries. For a given geometry and thickness d there is a unique critical interaction strength U
c2
(d) at which all effective masses diverge and there is a unique strength U
c1
(d) where the insulating solution disappears. U
c2
(d) and U
c1
(d) gradually increase with increasing thickness eventually approaching their bulk values. A simple analytical argument explains
the complete geometry and thickness dependence of Uc2. Uc1 is found to scale linearly with Uc2.
Received 19 August 1998 相似文献
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The double differential dilepton spectrum d/(d
2
d
⊥
2) at fixed transverse mass M
⊥ allows a direct access to the vector meson spectral functions. Within a fireball model the sensitivity of d/(d
2
d
⊥
2) against variations of both the in-medium properties of mesons and the dynamics of the fireball is investigated. In contrast
to the integrated invariant-mass spectrum d/d
2, in the spectrum d/(d
2
d
⊥
2) with fixed M
⊥ the ω signal is clearly seen as bump riding on the ρ background even in case of strong in-medium modifications.[3mm]
Received: 16 November 2000 / Accepted: 16 January 2001 相似文献