arXiv subjects

X. H. Yan

Publications and source records attributed to X. H. Yan.

4 recordsLinked to original sources

arXiv2013

Magnetic response of mesoscopic rings: a quantum size effect

We analytically study the magnetic response of persistent current (PC) in normally non-interacting mesoscopic rings of bimodal potential with nearest neighboring interactions (t) and alternating site energies. It is shown that a ring of perimeter (N) and width (M) generally shows weak diamagnetic, breaking the even-odd rule of electron filling. Especially, a maximal paramagnetic current in primary F0/2 period is predicted at N=(2p+1)(M+1) with odd M and integer p, while a maximal diamagnetic F0/2- current obtained at N=(2p+1)(M+1)+/-1 with even M. The current amplitudes depend strongly on both N and M, varied by at least 1~2 orders of magnitude, exhibiting a remarkable quantum size effect. A current limit of paramagnetic harmonics is expected at N=2p(M+1), independent of the sizes of N and M, in favor of experiment observation. A new mechanism of magnetic response is proposed that an electron circling the ring shall pass successively each channel within one flux quantum, accumulating an additional phase on each inter-channel transition, which leads to the paramagnetic-diamagnetic transition and period halving. The results unify and unveil the contradictions in PC between theory and experiments, validating quantum mechanics at mesoscopic scale.

cond-mat.mes-hall↗

arXiv2008

Localized gap soliton trains of Bose-Einstein condensates in an optical lattice

We develop a systematic analytical approach to study the linear and nonlinear solitary excitations of quasi-one-dimensional Bose-Einstein condensates trapped in an optical lattice. For the linear case, the Bloch wave in the $nth$ energy band is a linear superposition of Mathieu's functions $ce_{n-1}$ and $se_n$; and the Bloch wave in the $nth$ band gap is a linear superposition of $ce_n$ and $se_n$. For the nonlinear case, only solitons inside the band gaps are likely to be generated and there are two types of solitons -- fundamental solitons (which is a localized and stable state) and sub-fundamental solitons (which is a lacalized but unstable state). In addition, we find that the pinning position and the amplitude of the fundamental soliton in the lattice can be controlled by adjusting both the lattice depth and spacing. Our numerical results on fundamental solitons are in quantitative agreement with those of the experimental observation [Phys. Rev. Lett. {\bf92}, 230401 (2004)]. Furthermore, we predict that a localized gap soliton train consisting of several fundamental solitons can be realized by increasing the length of the condensate in currently experimental conditions.

cond-mat.other↗

arXiv2007

Density functional calculations for stability of Titanium-doped Gold clusters AunTi (n=2-16)

The stability and structures of Titanium-doped Gold clusters AunTi (n=2-16) are studied under the relativistic all-electron density-functional calculations. It is found that the most stable structures of AunTi clusters with n=2-7 are planar. A structural transition of AunTi clusters from two-dimensional to three-dimensional geometry occurs at n=8, while the AunTi (n=12-16) prefer gold cage structure with Ti atom locating at the center. The size-dependence of cluster properties such as binding energy, energy gaps, ionization potentials, and electron affinities have been calculated and analyzed. The Au14Ti cluster is found to have special stability, which may be due to the electron shell effects. Further calculations are performed to study cluster-cluster interaction between two Au14Ti clusters.

physics.atm-clus↗

arXiv2001

Resonant peak splitting for ballistic conductance in magnetic superlattices

We investigate theoretically the resonant splitting of ballistic conductance peaks in magnetic superlattices. It is found that, for magnetic superlattices with periodically arranged $n$ identical magnetic-barriers, there exists a general $(n-1)$-fold resonant peak splitting rule for ballistic conductance, which is the analogy of the $(n-1)$-fold resonant splitting for transmission in $n$-barrier electric superlattices (R. Tsu and L. Esaki, Appl. Phys. Lett. {\bf 22}, 562 (1973)).

cond-mat.mes-hall↗