共查询到20条相似文献,搜索用时 20 毫秒
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H. Kuratsuji R. Botet 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,49(1):111-116
We investigate a novel aspect of rotational tunneling of the macroscopic spin for multicomponent spinor Bose-Einstein condensate (BEC). The Lagrangian is deduced from
the multi-component BEC system formalism, and is written in terms of spin coherent states. From the effective Hamiltonian
for the collective spin, the tunneling rate is obtained through a functional integral of the spin variable. It is pointed
out that the cooperative effect between the Zeeman energy and the anisotropic nature of the spin-dependent inter-atomic interaction
plays a key role for occurrence of collective spin tunneling. 相似文献
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We use a tunneling Hamiltonian model to study the behavior of a thin film superconducting-normal metal sandwich in a parallel magnetic field including the effects of Pauli spin paramagnetism. The field acts to spin-split the density of states of the superconductor and the normal metal. With increasing magnetic field the sandwich displays zero temperature electron spin paramagnetism and a first-order transition to the normal state. We present a calculation of the field dependence of the density of states and order parameter. 相似文献
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Elie A. Moujaes Michel Abou Ghantous 《The European Physical Journal B - Condensed Matter and Complex Systems》2014,87(8):178
Elastic exchange between two nearest Jahn-Teller (JT) centers in two or three dimensional dense crystals, can give an ordered macroscopic distortion known as cooperative JT effect (CJTE). A very diluted JT crystal does not show this effect. In the dynamic JT effect (DJTE), tunneling between different equivalent distorted wells has a pronounced influence on the CJTE. We investigate this phenomenon using a progressive increase in the concentration of these centers in the JT crystals, based on a bond percolation vector spin analogy technique within the framework of effective field theory (EFT). Mean field theory (MFT) was extensively used in previous studies of CJTE; however it neither includes correlation between JT centers in the lattice due to the complexity of the distortion field in the crystal nor the effect of tunneling between wells. We resort to an alternative procedure, by describing a JT center as a pseudo-spin vector \(\vec S\), induced to represent the degenerate JT-distorted states, where two nearest JT centers interact via an elastic exchange described by an Ising type spin interaction. The DJTE is considered to be similar to an elastic transverse field term in the Hamiltonian portraying the effect of tunneling between equivalent wells in the adiabatic potential energy surface (APES). We will be particularly discussing S = 1, S = 3/2 and S = 5/2 spin cases, where 2S + 1 wells in the APES are present and what JT systems they actually represent, with a percolative mechanism applied to the interactions between different JT centers. The different lattices are distinguished by their coordination numbers. Strong tunneling effects can suppress the CJTE and lead to a new state of criticality. Generalizations to higher spin systems will be obtained using a scaling technique. For the relevant distortions, we determine single site correlations, the macroscopic average distortion describing a structural phase transition and the elastic isothermal susceptibility as a function of temperature. The critical bond percolation threshold and the critical tunneling parameter are also obtained. 相似文献
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Within the band gap of a semiconductor no electronic propagating states are allowed, but there exist evanescent states which govern charge transport such as tunneling. In this Letter, we address the issue of their spin dependence in III-V semiconductors. Taking into account the spin-orbit interaction, we treat the problem using a k . p 14 x 14 Hamiltonian that we numerically compute for GaAs. Our results show that the removed spin degeneracy in the band gap can lead to giant energy splittings and induces forbidden zones in space where evanescent states are suppressed. 相似文献
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研究了电子的自旋相关的隧穿和极化。在外加磁场的作用下,自旋向上的电子与自旋向下的电子具有不同的隧穿系数。当电子的自旋方向与磁场方向相反时,其隧穿概率受到磁场的抑制而变小;反之,当两平行时,电子的了隧穿系数增大。这种差异可以用本中定义的自旋极化率来表示。本对不同磁场下的自旋极化率进行了计算,结果也表明当电子的动能较小,这种自旋极化的效应越显。 相似文献
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Modified by the strong correlation existing in the high-TC cuprates, the photon-electron interaction Hamiltonian and tunneling Hamiltonian can cause the photoelectrons and the tunneling electrons to scatter the spin and charge fluctuations inelastically, in addition to the usual elastic scattering. The inelastic term is not only responsible for the three anomalies observed recently in ARPES or BIS, i.e, the large background, the non-sum rule and the dip, but also accounts for the V-shape behavior and the dip present in the SIN tunneling. The theoretical predictions are qualitatively in agreement with the experiments. 相似文献
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Longitudinal or transverse magnetic fields applied on a crystal of Mn12 acetate allows one to observe independent tunnel transitions between m = -S+p and m = S-n-p ( n = 6-10, p = 0-2 in longitudinal field and n = p = 0 in transverse field). We observe a smooth transition (in longitudinal) from coherent ground-state to thermally activated tunneling. Furthermore, two ground-state relaxation regimes show a crossover between quantum spin relaxation far from equilibrium and near equilibrium, when the environment destroys multimolecule correlations. Finally, we stress that the complete Hamiltonian of Mn12 should contain odd spin operators of low order. 相似文献
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用平均场的方法,研究了线性扫描磁场中自旋-1玻色-爱因斯坦凝聚体系的自旋隧穿.集中考虑87Rb这种典型的碱金属原子凝聚体,根据外磁场扫描率的不同,研究了它的隧穿动力学.在慢扫描(即绝热条件)和快扫描条件下,体系无隧穿现象.对中等大小的扫描率,发现隧穿现象,且这个隧穿动力学对磁场扫描率非常的敏感,表现为看似混沌的隧穿区的存在.然而,把这个看似混沌的区域放大,发现在扫描率精度为10-8T/s的量级上,隧穿率对磁场扫描率的关系实际是有规律的类周期结构.此外,还发现,实
关键词:
玻色-爱因斯坦凝聚
自旋
隧穿 相似文献
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用平均场的方法,研究了线性扫描磁场中自旋-1玻色-爱因斯坦凝聚体系的自旋隧穿.集中考虑87Rb这种典型的碱金属原子凝聚体,根据外磁场扫描率的不同,研究了它的隧穿动力学.在慢扫描(即绝热条件)和快扫描条件下,体系无隧穿现象.对中等大小的扫描率,发现隧穿现象,且这个隧穿动力学对磁场扫描率非常的敏感,表现为看似混沌的隧穿区的存在.然而,把这个看似混沌的区域放大,发现在扫描率精度为10-8T/s的量级上,隧穿率对磁场扫描率的关系实际是有规律的类周期结构.此外,还发现,实 相似文献
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Numerical study on tunneling splitting in biaxial spin systems is done by performing diagonalization of the Hamilton operator. It is found that the calculated energy splitting agrees quantitatively with theoretical prediction of instanton method. Our result shows that both the instanton method and the large spin limit work well for the total spin around 10. By including the fourth-order term in Hamiltonian, experimental observation can be re-covered quantitatively. 相似文献
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By means of a diagram technique for Hubbard operators, we show the existence of a spin-dependent renormalization of the localized levels in an interacting region, e.g., quantum dot, modeled by the Anderson Hamiltonian with two conduction bands. It is shown that the renormalization of the levels with a given spin direction is due to kinematic interactions with the conduction subbands of the opposite spin. The consequence of this dressing of the localized levels is a drastically decreased tunneling current for ferromagnetically ordered leads compared to that of paramagnetically ordered leads. Furthermore, the studied system shows a spin-dependent resonant tunneling behavior for ferromagnetically ordered leads. 相似文献
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Y. Guo B. Wang B.-L. Gu Y. Kawazoe 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,23(4):509-513
We investigate characteristics of spin tunneling time in ZnSe/Ze1-xMnxSe multilayers under the influence of both an electric field and a magnetic field. The results indicate that the tunneling
time shows complicated oscillations and significant spin separation for electrons with different spin orientations traversing
semimagnetic semiconductor heterostructures. It is also shown that the tunneling time exhibits obvious asymmetry in opposite
tunneling directions for electrons tunneling through asymmetric heterostructures, which mainly occurs in resonant regions.
The degree of the asymmetry of the tunneling time is not only spin-polarization dependent but also external-field induced.
Received 10 July 2001 相似文献
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Magnetization measurements of a truly axial symmetry molecular nanomagnet with a spin ground state of S = 10 show resonant tunneling. This compound has the same magnetic anisotropy as but the molecules are better isolated and the crystals have less disorder and a higher symmetry. Hysteresis loop measurements at several temperatures reveal a well-resolved step fine structure which is due to level crossings of excited states. All step positions can be modeled by a simple spin Hamiltonian. The results establish a sharp crossover between thermally assisted and pure quantum tunneling, as had been previously predicted. 相似文献
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考虑自旋场效应晶体管中Rashba自旋轨道相互作用和自旋输运量子相干性,研究了势垒强度对自旋场效应晶体管的自旋相关量子输运的影响. 研究发现,势垒强度较低时,隧道结电导随Rashba自旋轨道相互作用强度的变化呈现明显的振荡现象,势垒强度较高时,电导表现出明显的势垒相关“电导开关”现象. 当势垒强度逐渐增强时,平行结构电导呈现出单调下降趋势,而反平行结构电导产生波动,这种波动导致该隧道磁阻也随势垒强度的变化表现出振荡现象,且在合适的准一维电子气厚度情况下隧道磁阻值可以产生正负反转,这个效应将会在基于自旋的电子器件信息的存储上获得应用.
关键词:
自旋场效应管
开关效应
量子相干
隧道磁阻 相似文献
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J.-L. Zhu R. Lü X.-B. Wang X. Chen L. Chang F.-C. Pu 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,4(2):223-231
The tunneling behaviors of the magnetization vector are studied in ferromagnetic systems with trigonal and hexagonal crystal
symmetries, respectively. The Euclidean transition amplitudes between the energetically degenerate easy directions are evaluated
with the help of the dilute instanton-gas approximation. By using the effective Hamiltonian method, the ground-state tunneling
level splittings are clearly shown for each kind of symmetry and are found to depend on the parity of the total spin of the
ferromagnetic particle. The effective Hamiltonian method is demonstrated to be equivalent to the dilute instanton-gas approximation.
Possible relevance to experiments is discussed.
Received: 18 November 1997 / Revised: 18 March 1998 / Accepted: 6 April 1998 相似文献