37,812 research outputs found

    Bell-CHSH function approach to quantum phase transitions in matrix product systems

    Full text link
    Recently, nonlocality and Bell inequalities have been used to investigate quantum phase transitions (QPTs) in low-dimensional quantum systems. Nonlocality can be detected by the Bell-CHSH function (BCF). In this work, we extend the study of BCF to the QPTs in matrix product systems (MPSs). In this kind of QPTs, the ground-state energy keeps analytical in the vicinity of the QPT points, and is usually called the MPS-QPTs. For several typical models, our results show that BCF can signal the MPS-QPTs very well. In addition, we find BCF can capture signal of QPTs in unentangled states and classical states, for which other measures of quantum correlation (quantum entanglement and quantum discord) fail. Furthermore, we find that in these MPSs, there exists some kind of quantum correlation which cannot be characterized by entanglement, or by nonlocality.Comment: 12 pages, 4 figure

    Andreev reflection through a quantum dot coupled with two ferromagnets and a superconductor

    Full text link
    We study the Andreev reflection (AR) in a three terminal mesoscopic hybrid system, in which two ferromagnets (F1_1 and F2_2) are coupled to a superconductor (S) through a quantum dot (QD). By using non-equilibrium Green function, we derive a general current formula which allows arbitrary spin polarizations, magnetization orientations and bias voltages in F1_1 and F2_2. The formula is applied to study both zero bias conductance and finite bias current. The current conducted by crossed AR involving F1_1, F2_2 and S is particularly unusual, in which an electron with spin Οƒ\sigma incident from one of the ferromagnets picks up another electron with spin ΟƒΛ‰\bar{\sigma} from the other one, both enter S and form a Cooper pair. Several special cases are investigated to reveal the properties of AR in this system.Comment: 15 pages, 7 figures, LaTe

    Probing Spin States of Coupled Quantum Dots by dc Josephson Current

    Full text link
    We propose an idea for probing spin states of two coupled quantum dots (CQD), by the dc Josephson current flowing through them. This theory requires weak coupling between CQD and electrodes, but allows arbitrary inter-dot tunnel coupling, intra- and inter- dot Coulomb interactions. We find that the Coulomb blockade peaks exhibit a non-monotonous dependence on the Zeeman splitting of CQD, which can be understood in terms of the Andreev bound states. More importantly, the supercurrent in the Coulomb blockade valleys may provide the information of the spin states of CQD: for CQD with total electron number N=1,3 (odd), the supercurrent will reverse its sign if CQD becomes a magnetic molecule; for CQD with N=2 (even), the supercurrent will decrease sharply around the transition between the spin singlet and triplet ground states of CQD.Comment: 10 pages, 3 figure

    Theory of Nonequilibrium Coherent Transport through an Interacting Mesoscopic Region Weakly Coupled to Electrodes

    Full text link
    We develop a theory for the nonequilibrium coherent transport through a mesoscopic region, based on the nonequilibrium Green function technique. The theory requires the weak coupling between the central mesoscopic region and the multiple electrodes connected to it, but allows arbitrary hopping and interaction in the central region. An equation determining the nonequilibrium distribution in the central interacting region is derived and plays an important role in the theory. The theory is applied to two special cases for demonstrations, revealing the novel effects associated with the combination of phase coherence, Coulomb interaction, and nonequilibrium distribution.Comment: 10 Pages, 5 figure

    The uniform supertrees with the extremal spectral radius

    Full text link
    For a hypergraphhypergraph G=(V,E)\mathcal{G}=(V, E) consisting of a nonempty vertex set V=V(G)V=V(\mathcal{G}) and an edge set E=E(G)E=E(\mathcal{G}), its adjacencyadjacency matrixmatrix AG=[(AG)ij]\mathcal {A}_{\mathcal{G}}=[(\mathcal {A}_{\mathcal{G}})_{ij}] is defined as (AG)ij=βˆ‘e∈Eij1∣eβˆ£βˆ’1(\mathcal {A}_{\mathcal{G}})_{ij}=\sum_{e\in E_{ij}}\frac{1}{|e| - 1}, where Eij={e∈E:i,j∈e}E_{ij} = \{e \in E : i, j \in e\}. The spectralspectral radiusradius of a hypergraph G\mathcal{G}, denoted by ρ(G)\rho(\mathcal {G}), is the maximum modulus among all eigenvalues of AG\mathcal {A}_{\mathcal{G}}. In this paper, among all kk-uniform (kβ‰₯3k\geq 3) supertrees with fixed number of vertices, the supertrees with the maximum, the second maximum and the minimum spectral radius are completely determined, respectively
    • …
    corecore