用于绝对相位还原的对称式和非对称式二元结构光编码

基于邻域分析的相移法不适合阶跃场景测量且往往会造成相位误差的积累,为此提出了用于获取绝对相位的对称式和非对称式二元阶梯相位结构光编码方法.两种方法编码图案不同,对称式编码方法编码图案黑白条纹的宽度相等,非对称式不等.通过投影多帧二元结构光编码图案,结合相移法相位提取公式获得阶梯相位.测量时,基于传统正弦条纹投影和相移法获得高准确度包裹相位,并用阶梯相位确定对应包裹相位的级次.根据级次直接进行相位展开,进而获得绝对相位.以量块作为测量对象,两种方法的测量均方根误差达到0.072mm.两种方法均能够有效还原阶跃场景,实现三维重构.     

Resonance Interactions of Symmetric Surface and Bulk Waves in Oversized Sectioned Slow-Wave Structures

Russian Physics Journal - The resonance properties of coupled electromagnetic waves at frequencies of 9 and 35 GHz in the sectioned oversized slow-wave structure of a multiwave Cherenkov generator...     

Symmetric harmonic maps between spheres

Necessary and sufficient conditions for the existence of symmetric harmonic maps between spheres are established.     

Disentangled Higher-Orbital Bands and Chiral Symmetric Topology in Confined Mie Resonance Photonic Crystals

Topological phases based on tight-binding models have been extensively studied in recent decades. By mimicking the linear combination of atomic orbitals in tight-binding models based on the evanescent couplings between resonators in classical waves, numerous experimental demonstrations of topological phases have been successfully conducted. However, in dielectric photonic crystals, the Mie resonances' states decay too slowly as $1/r$, leading to intrinsically different physics between tight-binding models and dielectric photonic crystals. Here, a confined Mie resonance photonic crystal is proposed by embedding perfect electric conductors between dielectric rods, creating the chiral symmetric band structure which ideally matches tight-binding models with nearest-neighbour couplings. As a consequence, disentangled band structure spanned by higher atomic orbitals is observed. Moreover, the result provides an effective route to achieve a 3D photonic crystal with a complete photonic bandgap and third-order topology. The implementation offers a versatile platform for studying exotic higher-orbital bands and achieving tight-binding-like 3D topological photonic crystals.     

Bose-Einstein correlations in the Lund model

By providing the Lund model fragmentation process with a quantum mechanical framework we extend the results of Andersson and Hofmann [Phys. Lett. B 169 (1986) 364] to situations where there are very many identical bosons. We investigate the features of the weight distributions in some detail and in particular exhibit three-particle BE correlations, the influence on the ϱ-spectrum and the difference between charged and neutral pion correlations.     

Stochastic Resonance in a Spatially Symmetric and Flashing Periodic Potential Subjected to Correlated Noises

A Brownian particle in a spatially symmetric and flashing periodic potential subjected to correlated noises is investigated. The exact expression of its current is analytically derived. The numerical results indicate that its current as a function of noise intensity exhibits two peaks in the case of positive correlations, and two vales in the case of negative correlations, i.e., a novel stochastic resonance （SR） phenomenon. The SR is attributed to the harmonic cooperation between the noises and the flashing periodic potential. The conditions under which the SR occurs are also presented.     

Metastates in the Hopfield Model in the Replica Symmetric Regime

We study the finite dimensional marginals of the Gibbs measure in the Hopfield model at low temperature when the number of patterns, M, is proportional to the volume with a sufficiently small proportionality constant > 0. It is shown that even when a single pattern is selected (by a magnetic field or by conditioning), the marginals do not converge almost surely, but only in law. The corresponding limiting law is constructed explicitly. We fit our result in the recently proposed language of metastates which we discuss some length. As a byproduct, in a certain regime of the parameters and (the inverse temperature), we also give a simple proof of Talagrands recent result that the replica symmetric solution found by Amit, Gutfreund, and Sompolinsky can be rigorously justified.     

Dynamical correlations in the Dual Parton Model

The effect of multiple ‘chain’ contributions to particle production, which appears in the Dual Parton Model at collider energies, is investigated in an exploratory model, in which other sources of correlations are largely neglected. Attention is given to the question of KNO scaling for the multiplicities observed in restricted or unrestricted rapidity ranges. The rapidity distribution associated with a fixed number of particles within a suitably chosen interval, is found to be sensitive to details of the mechanism of multiple chain production.     

多分量对偶超导理论和口袋模型

基于联络新参数化方案研究了多分量对偶超导模型。给出了多分量Ginzburg Landau模型中的自对偶解, 并研究了磁通量子数趋于无穷大时的墙涡旋解, 以及与口袋模型之间的联系。The multi-component dual superconductor theory has been studied based on the new parameterization of gauge potential. The self dual vortices of the multi component Ginzburg Landau model was investigated. Then we considered the wall vortex whose flux goes to infinity. At last, the relationship between the bag model and wall vortices is considered.     

Stochastic Resonance in the Tumour Cell Growth Model

The phenomenon of stochastic resonance （SR） in the tumour cell growth model subjected cross-correlated noises is investigated. When a weakly periodic signal is added to the system, the signal-to-noise ratio RSNR is derived by the quasi-steady-state probability distribution function and the adiabatic elimination method. Based on the derived RSNR, the effects of these parameters （the cross-correlated strength λ and the cross-correlated time τ） are analysed by numerical calculation. It is found that the existence of a maximum in RSNR is the identifying characteristic of the SR phenomenon. The maximum of RsNR decreases with the increase of λ and increases with the increase of τ.     

Boundary Scattering,Symmetric Spaces and the Principal Chiral Model on the Half-Line

We investigate integrable boundary conditions (BCs) for the principal chiral model on the half-line, and rational solutions of the boundary Yang-Baxter equation (BYBE). In each case we find a connection with (type I, Riemannian, globally) symmetric spaces G/H: there is a class of integrable BCs in which the boundary field is restricted to lie in a coset of H; these BCs are parametrized by G/H×G/H; there are rational solutions of the BYBE in the defining representations of all classical G parametrized by G/H; and using these we propose boundary S-matrices for the principal chiral model, parametrized by G/H×G/H, which correspond to our boundary conditions.An erratum to this article can be found at     

Particle Model for the Reservoirs in the Simple Symmetric Exclusion Process

Journal of Statistical Physics - In this paper, we will study the long time behavior of the simple symmetric exclusion process in the “channel” $$varLambda _N=[1,N]cap mathbb {N}$$...     

圆柱形Bragg微腔的共振模特性

利用圆柱形介质设计了一个Bragg微腔结构,含有圆柱形和环形两个微腔.基于传输矩阵理论,通过研究会聚柱面波的反射相移,根据反射相移在Bragg禁带中的尖锐突变来确定微腔结构的共振模.较之其他计算方法,相移方法操作简单,图像直观,且行之有效.研究表明,随着中心圆柱形微腔的半径增大,方位指数相同的两微腔共振模之间会发生相互作用,在腔模光子能量相近时耦合效应最强,导致双微腔的耦合共振模曲线出现反交叉现象.最后给出了耦合共振模的空间电磁场分布.     

光子晶体光纤中级联长周期光栅双谐振波长干涉的研究

通过分析单模光纤SMF中的LPG对的传输特性及几个因素对干涉透射谱的影响,并结合前期工作,主要研究光子晶体光纤(PCF)中的LPG对在1665 nm附近U波段传输特性.结合光栅耦合强度与波长的关系以及拍长与波长的关系,对PCF中LPG对的参数进行选择设计,得到双谐振波长的干涉谱,级联LPG对构成的MZI干涉光谱在两个谐振波长处由于耦合强度不同而不同.     

Phenomenology of Friedberg-Lee Texture in Left-Right Symmetric Model

We consider that the Higgs triplet Yukawa coupling takes the Friedberg-Lee texture, and the Higgs doublet Yukawa coupling simply identifies with the diagonal Yutawa coupling of charged lepton in the context of left-right symmetric model. In this scenario, the phenomenology, including effective neutrino masses, mixings, and thermal flavor-dependent leptogenesis and lepton flavor violation decays are studied. We investigate the combined constrain of the parameters in this scenario and test its consistency with present data.     

The diagonalisation of the Lund fragmentation model I

We will in this note show that it is possible to diagonalise the Lund fragmentation model. We show that the basic original result, the Lund area law, can be factorised into a product of transition operators, each describing the production of a single particle and the two adjacent break up points (vertex positions) of the string field. The transition operator has a discrete spectrum of (orthonormal) eigenfunctions, describing the vertex positions (which in a dual way correspond to the momentum transfers between the particles produced) and discrete eigenvalues, which only depend upon the particle produced. The eigenfunctions turn out to be the well-known two-dimensional harmonic oscillator functions and the eigenvalues are the analytic continuations of these functions to timelike values (corresponding to the particle mass). In this way all observables in the model can be expressed in terms of analytical formulas. In this note only the 1+1-dimensional version of the model is treated, but we end with remarks on the extensions to gluonic radiation, transverse momentum generation etc., to be performed in future papers. Received: 7 April 2000 / Published online: 18 May 2000     

Proton-Proton Interaction in a Dual Model

The “background-pomeron” component of the amplitude is studied in the framework of a dual model with square-root trajectories. Double pomeron poles are used as vacuum exchanges in various channels, with exotic Regge poles dual to them. The expressions obtained are applied to describe total and differential cross sections of proton-proton interaction in wid eenergy regions.     

Density and Symmetric Potential Dependences of Isoscaling Behaviour in the Lattice Gas Model

Isoscaling behaviour of the statistical emission fragments from the equilibrated sources with Z=30 and N=30, 33, 36 and 39 is investigated in the framework of the isospin-dependent lattice gas model. The dependences of isoscaling parameters α on source isospin asymmetry, temperature andfreeze-out density are studied, and the `symmetry energy' is deduced from isoscaling parameters. The results show that symmetry energy C_sym is insensitive to the change of temperature but follows the power-law dependence on the freeze-out density ρ. The effect of strength of asymmetry of nucleon--nucleon interaction potential on the density dependence of the symmetry energy is discussed.