连通图的最小Laplace谱半径的排序

首先找出了具有最小Laplace谱半径的第2个至第5个n阶单圈图和具有最小Laplace谱半径的n阶双圈图.然后结合有关n阶树的最小Laplace谱半径的排序,给出了所有n阶连通图中Laplace谱半径最小的14个图,当n为偶数时,它们达到了所有佗阶连通图中Laplace谱半径最小的9个值(其中有并列的),而当n为奇数时,它们则达到了Laplace谱半径最小的8个值(其中有并列的).     

第V类两态叠加多模叠加态光场的广义非线性等阶N次方Y压缩

本文构造了由多模真空态|{0_j}>_q和多模虚相干态的相反态|{-iZ_j}>_q这两者的线性叠加所组成的第V类两态叠加多模叠加态光场|ψ₅⁽²⁾>_q.利用多模压缩态理论,研究了态|ψ₅⁽²⁾>_q的广义非线性等阶N次方Y压缩特性.结果发现:1)态|ψ₅⁽²⁾>_q是一种典型的多模非经典光场;无论压缩阶数N取奇还是取偶,只要各模的初始相位φ_j(j=1,2,3,…,…,q)和态间的初始相位差(θ_nq^(I)-θ_oq^(o))等满足一定的取值条件,态|ψ₅⁽²⁾>_q总可呈现出周期性变化的、任意奇数阶和任意偶数阶的广义非线性等阶N次方Y压缩效应.2)态|ψ₅⁽²⁾>_q所分别呈现的任意奇数阶和任意偶数阶的等阶N次方Y压缩效应,其压缩条件、压缩特征以及压缩程度和压缩深度等各不相同.3)无论压缩阶数N取奇还是取偶,态|ψ₅⁽²⁾>_q的第一和第二这两个正交分量的等阶N次方Y压缩效应总是呈现出周期性的互补关系.     

巧记逐差法

处理纸带问题时往往要用到逐差法求加速度, 从Δ x=a T2 开始逐步展示逐差法的推导过程, 最终得 到逐差法求加速度的公式, 分为偶数段和奇数段. 并给出对应公式的巧记方法, 对学生解决纸带问题有很大的帮 助     

第Ⅰ种非对称两态叠加多模叠加态光场等阶N次方H压缩——1.腔模总数与压缩阶数两者之积取偶的情形

本文利用多模压缩态理论研究了第Ⅰ种非对称两态叠加多模叠加态光场|Ψ_Ⅰ^(ab)>_q的广义非线性等阶N次方H压缩特性.结果发现:在腔模总数q与压缩阶数N这两者之积qN为偶数亦即qN=2p的条件下,无论p=2m(m=1,2,3,…,…)还是p=2m+1(m=0,1,2,…,…),当两非对称态中各模的初始相位和 =φ_j^(a)、 =φ_j^(b)、态间的初始相位差(θ_pq^bI-θ_nq^aR),以及各单模相干态光场的光子干涉项之和 =[R_j^(a)R_j^(b)]cos(φ_j^(a)-φ_j^(b))]等满足一定条件时,态|Ψ_Ⅰ^(ab)>_q可分别呈现出周期性变化的奇数模-偶数阶、偶数模-奇数阶和偶数模-偶数阶的等阶N次方H压缩效应.     

第Ⅰ种偶数模四态叠加多模叠加态光场的等幂次N次方X压缩特性

构造了同一偶数模的多模偶相干态与多模奇相干态这两者的线性叠加组成的第Ⅰ种偶数模四态叠加多模叠加态光场|Ψ(4),I>2q利用多模压缩态理论,详细研究了态|Ψ(4),I>2q的等幂次N次方X压缩特性。结果表明态|Ψ(4),I>2q是一种典型的非经典多模叠加态光场。(1)当场模数q与压缩幂次N的乘积q·N为偶数且各模光子数nj小于N时,态|Ψ(4),I>2q的两个正交分量可同时呈现程度相同的等幂次N次方X压缩效应;(2)当q·N为奇数且nj小于N,而且偶相干态几率幅r(e)2q大于奇相干态几率幅r(0)2q时,则在N与各模初始相位φj的乘积N(∑qjc=1φjc-∑2qjL=q+1φjL)取不同的特定值的条件下,态|Ψ(4),I>2q的两个正交分量可分别呈现等幂次N次方X压缩效应。     

关于蕴含3Gl可图序列的极值问题

设σ（3C1，n）是具有下述性质的最小正偶数，每个项和至少为σ（3C1，n）的n项可图序列π都有一个实现含有长为3，4，…，l的圈，本文确定了当7≤t≤8且n≥l≥以及当l=9且n≥12时σ（2C1，n）的值。     

关于偶数Goldbach数的均值性质

设D(n)表示方程n=p1+p2的解数,其中p1,p2为奇素数,若D(n)>0,则我们称n为偶数G o ldbach数.主要目的是利用初等和解析方法从两个不同的角度来研究偶数G o ldbach数的均值性质,并给出了两个相同的渐近公式,从而为进一步证明偶数G o ldbach猜想的正确性提供了有力的证据.     

The exceptional set for sums of unlike powers of primes

It is established that all even positive integers up to N but at most O(N15/16+ε) exceptions can be expressed in the form p21+ p32+ p43+ p54,where p1,p2,p3 and p4 are prime numbers.     

Fano Resonance by Symmetry Breaking Stub in a Metal-Dielectric-Metal Waveguide

The coupling of a stub obliquely intersected with a metal-dielectric-metal plasmonic waveguide is investigated by using the finite difference in time domain method. Results show that an odd mode, except for the usual even mode, is excited in the stub due to the symmetry breaking of the oblique intersection. Moreover, the results show that tile quality factor of the odd mode is very high in comparison with that of the usual even mode, which is then explained by the symmetry breaking of the oblique stub intersection. The superposition of the even and the odd mode generates a Fano shaped spectrum with a very narrow linewidth. The effect of metallic loss and compensation are also discussed. Both the stub and the waveguide are compact in size, and simple in structure, which are beneficial for the achievements of narrow band filtering, sensing, lasing, and nonlinearity enhancement.     

Chen’s Theorem with Small Primes

Let N be a sufficiently large even integer. Let p denote a prime and P2 denote an almost prime with at most two prime factors. In this paper, it is proved that the equation N - p+ P2 (p ≤ AT0.945) is solvable.