基于固定校正板和透镜阵列的机载共形窗口像差校正

为了校正大扫描视场机载共形窗口引入的像差,提出一种基于固定校正板和透镜阵列的静态校正方法。首先使用固定校正板校正静态像差;然后在像面前安置固定的透镜阵列,利用透镜阵列中的各个透镜单元分别校正不同扫描角度的动态像差;最后基于所提方法设计应用在机载共形光学系统中的像差校正器。设计结果表明,所提方法在±42°的扫描视场范围内能够良好地校正共形窗口引入的像差。与其他动态或静态校正方法相比,所提方法可以实现大扫描视场机载共形光学系统像差的校正,同时降低机载共形光学系统的质量,提高系统的稳定性。     

Search for exotic state 1－+ π1(1400) at BESⅢ

The J/ψ hadronic decays provide good laboratory to search for the hybrid states with exotic quantum numbers. A full Partial Wave Analysis (PWA) is performed to the generated Monte Carlo J/ψ→ρηπ data, based on the design of BESⅢ detector, to study the sensitivity of searching for a possible exotic state at BESⅢ.     

人眼自动对焦及瞳孔中心自动对准系统

针对现今非接触眼科测量仪器对焦对准速度慢、通用性差和操作复杂的问题,搭建了应用于眼科测量仪器的人眼自动对焦及瞳孔中心自动对准系统,并提出了基于四邻域-多方向两级梯度函数的自动对焦算法以及融合卷积神经网络智能感兴趣区域（ROI）窗口的瞳孔中心定位算法。通过实验实拍人眼离焦图像序列及人眼图像测试集,分别对提出的两个算法进行验证。结果显示：所提出的自动对焦算法的平均计算时间约为13 ms,清晰度比率为93.531,优于6种传统的评价算法;所提出的瞳孔中心定位算法的平均计算时间为10.2 ms,准确度为97.14%,相比Hough法、改进Hough法有较大的性能提升。实验结果证明所搭建的系统能够满足眼生物参数测量的准确性、实时性和鲁棒性要求,提升了仪器的自动化水平,有助于眼科测量仪器的智能化发展。     

Pole Analysis of Unitarized One Loop χ PT Amplitudes——A Triple Channel Study

In a previous paper [Commun.Theor.Phys.,[arxiv:hep-ph11081451]],we proposed a method to distinguish poles of different dynamical origin,in unitarized amplitudes ofππ,KˉK system.That is based on the observation that "A Breit-Wigner resonance should exhibit two poles on different Riemann sheets which meet each other on the real axis when N c = ∞".In this paper,we extend our previous work [Commun.Theor.Phys.,[arXiv:hep-ph11081451]] to the ππ-KˉK-ηη three channel system.We reconfirm most of the predictions in our previous work [Commun.Theor.Phys.,[arxiv:hep-ph11081451]].Especially the f 0(980) is of KˉK molecule nature.Other poles,including the σ,are of Breit-Wigner type.     

New insights on low energy πN scattering amplitudes:comprehensive analyses at ■(p~3) level

A production representation of partial-wave S matrix is utilized to construct low-energy elastic pion-nucleon scattering amplitudes from cuts and poles on complex Riemann sheets. Among them, the contribution of left-hand cuts is estimated using the ■(p~3) results obtained in covariant baryon chiral perturbation theory within the extendedon-nass-shell scheme. By fitting to data on partial-wave phase shifts, it is indicated that the existences of hidden poles in S11 and P11 channels, as conjectured in our previous paper [Eur. Phys. J. C, 78(7): 543(2018)], are firmly established. Specifically, the pole mass of the S11 hidden resonance is determined to be(895±81)-(164±23)i MeV,whereas,the virtual pole in the P11 channel locates at(966±18) MeV. It is found that analyses at the■ (p~3) level improves significantly the fit quality, comparing with the previous■ (p~2) one. Quantitative studies with cautious physical discussions are also conducted for the other S-and P-wave channels.     

Dispersive analysis of low energyγN→πN process and studies on the N^*(890)resonance

We present a dispersive representation of the γN→πN partial-wave amplitude based on unitarity and analyticity.In this representation,the right-hand-cut contribution responsible for πN final-state-interaction effects is taken into account via an Omnes formalism with elastic πN phase shifts as inputs,while the left-hand-cut contribution is estimated by invoking chiral perturbation theory.Numerical fits are performed to pin down the involved subtraction constants.Good fit quality can be achieved with only one free parameter,and the experimental data regarding the multipole amplitude E0+ in the energy region below the △(1232) are well described.Furthermore,we extend the γN →μN partial-wave amplitude to the second Riemann sheet to extract the couplings of the N*(890).The modulus of the residue of the multipole amplitude E0+(S11pE) is 2.41 mfm·GeV2,and the partial width of N*(890)→ yN at the pole is approximately 0.369 MeV,which is almost the same as that of the N*(1535) resonance,indicating that N*(890) strongly couples to the πN system.