Toader平均的二次与调和平均界

该文证明了双向不等式αQ(a,b)+(1-α)H(a,b)T(a,b)βQ(a,b)+(1-β)H(a,b)和λ/H(a,b)+(1-λ)/Q(a,b)1/T(a,b)μ/H(a,b)+(1-μ)/Q(a,b)对所有a,b0且a≠b成立的充分和必要条件是α≤5/6,β≥22~(1/2)π,λ0和μ1/6.其中Q(a,b)=((a~2+b~2)/2)~(1/2),H(a,b)=2ab/(a+b)和T(a,b)=2/π∫_0~(π/2)(a~2cos~2θ+b~2sin~2θ)~(1/2)dθ分别表示正数a和b的二次平均,调和平均和Toader平均.     

Toader型平均与几种经典平均的确界

给出了最佳参数α_1,α_2,α_3,β_1,β_2,β_3∈R,使得双向不等式α_1Q(a,b)+(1-α_1)G(a,b)0且a≠b成立.其中A(a,b)=(a+b)/2,H(a,b)=2ab/(a+b),G(a,b)=(ab)~(1/2),Q(a,b)=((a~2+b~2)/2)~(1/2),C(a,b)=(a~2+b~2)/(a+b),T(a,b)=2/π∫_0~(π/2)(a~2cos~2t+b~2sin~2)~(1/2)tdt分别是两个正数a和b的算术平均,调和平均,几何平均,二次平均,反调和平均和Toader平均.     

关于第二类Seiffert平均的最佳双边不等式

得到了使得不等式αD(a,b)+(1-α)H(a,b)T(a,b)βD(a,b)+(1-β)H(a,b)对所有的a,b0且a≠b成立的α和β的最佳值.其中D(a,b)、H(a,b)和T(a,b)分别表示2个不同正数a与b的第二类反调和平均、调和平均、第二类Seiffert平均.     

小区间上的素变数三角和估计Ⅰ

设α是实数,x≥A≥2,e(θ)=e^2πiθ,以及A(n)是Mangoldt 函数。本文主要证明以下结论(见定理1):设δ是任给的正数,x^91/96+ε≤A≤x。那么,对任给的正数c,一定存在正数c₁,使当A^-1log^cx≤|α|≤(log x)^-c1)时,A(n)e(nα)<<A(log x)^-c     

对数平均和双参数广义Muirhead平均之间的比较

本文讨论了两个不同正实数x和y的对数平均L(x,y)=(x-y)/(logx-logy)与双参数广义Muirhead平均M(a,b;x,y)=[(x~ay~b+x~by~a)/2]~(1/(a+b))之间的比较,得到了如下三个结论:(11)若(a,b)∈D_1∪E_1∪L_0,则M(a,b;x,y)L(x,y);(2)若(a,b)∈D_2∪E_2,则M(a,b;x,y)L(x,y);(3)若(a,b)∈D_3∪E_3,则存在x_1,y_1,x_2,y_2,使得M(a,b;x_1;y_1)L(x_1,y_1)和M(a,b;x_2,y_2)L(x_2,y_2).其中D_1={(a,b)∈R~2:a+b≠0,ba,ω_1(a,b)≤0,ω_2(a,b)≤0},E_1={(a,b)∈R~2:a+b≠0,ba,ω_1(a,b)≤0,ω_2(a,b)≤0},D_2={(a,b)∈R~2:ab≤0,ba,ω_1(a,b)≥0},E_2={(a,b)∈R~2:ab≤0,ba,ω_1(a,b)≥0},D_3={(a,b)∈R~2:ba0,ω_1(a,b)0)∪{(a,b)∈R~2:ba0,ω_1(a,b)=0,ω_2(a,b)0}∪{(a,b)∈R~2:ba,ab≤0,ω_1(a,b)0,ω_2(a,b)0},E_3={(a,b)∈R~2:ab0,ω_1(a,b)0}∪{(a,b)∈R~2:ab0,ω_1(a,b)=0,ω_2(a,b)0}∪{(a,b)∈R~2:ab,ab≤0,ω_1(a,b)0,ω_2(a,b)0},L_0={(a,b)∈R~2:a=b≠0},ω_1(a,b)=(a+b)[3(a-b)~2-(a+b)],ω_2(a,b)=(a+b)[2(a-b)~2+1]-3(a~2+b~2).     

外延单晶La2/3Ca1/3MnO3-δ薄膜中磁电阻的磁场依赖关系

采用直流磁控溅射法在NdGaO₃ ( 110 )衬底上制备了La_2/3Ca_1/3MnO_3-δ外延单晶薄膜 .在 0～8T的磁场范围内测量了不同温区下的磁电阻随磁场的变化关系 .结果表明 ,ρ(H )遵循以下规律 :当温度高于居里温度T_C 时 ,ρ(H ) =1α(T) + β(T)H² ;当T <Tc时,ρ(H ) =ρ0(T ) +1A(T)+B(T)exp(H/C(T));而当温度远低于居里温度时,ρ(H ) =1σ(T) + ν(T)H。表明负巨磁电阻的产生主要起因于磁场引起的电导率的增加。     

SHARP BOUNDS FOR NEUMAN-SNDOR MEAN IN TERMS OF THE CONVEX COMBINATION OF QUADRATIC AND FIRST SEIFFERT MEANS

In this article, we prove that the double inequalityαP(a, b) +(1- α)Q(a, b) M(a, b) βP(a, b) +(1- β)Q(a, b)holds for any a, b 0 with a = b if and only if α≥ 1/2 and β≤ [π(√2 log(1 +√2)-1)]/[(√2π- 2) log(1 +√2)] = 0.3595, where M(a, b), Q(a, b), and P(a, b) are the NeumanS′andor, quadratic, and first Seiffert means of a and b, respectively.     

La2/3Ca1/3MnO3-δ薄膜中磁致电阻温度关系的一种经验描述

在不同磁场H下 ,在 300～ 77K范围内测量了外延L_{a2 /3} Ca_1/3 MnO_3-y薄膜的电阻率ρ(T) ,发现电阻率的温度依赖关系可以按如下的经验公式来描述:ρ(T) =1σ(T) =1/α(M/M_s)² + βexp(-E0/k_BT) ,其中拟合参数α ,β随磁场的变化略有变化,E₀为磁极化子热激活能 ,约等于1 160k_B,M_s 为饱和磁化强度 ,M/Ms采用平均场近似求得,据此对提高CMR效应的可能性作了讨论.     

一道世界数学团体锦标赛试题的解法与推广

<正>1试题呈现(第1届世界数学团体锦标赛(WMTC)青年组团体赛)设a,b,c皆为正实数,a+b+c=1,则M=(3a+1)(1/2)+(3b+1)(1/2)+(3c+1)(1/2)的整数部分是___.     

一个与Wiener过程增量连续模有关的下极限收敛速度问题

设W(t),t≥0为标准Wiener过程,α_T为T的函数且0<α_T≤T,lim_T→∞ log(T/α_T)/loglogT=r,本文证明了 c₁(r/(1+r))^1/2≤liminf_T→∞(loglogT)^1/2max_αT≤t≤T|W(T)-W(T-t)|/{2t[log(T/t)+loglogt]}^1/2≤c₂(r/(1+r))^1/2,a.s,这儿c₁和c₂为正常数。     

关于F2n中的和集

设F₂为两个元素组成的有限域, F₂ⁿ 为F₂上的n维向量空间. 对于集合A, B ⊆ F₂ⁿ , 它们的和集定义为所有两两互异的和a+b所组成的集合, 其中a∈A, b∈B. Green 和Tao 证明了: 设K > 1,如果A, B ? F₂ⁿ 且|A + B|≤K|A|^1/2|B|^1/2, 则存在一个子空间H?F₂ⁿ 满足
|H|>>exp(-O(√KlogK))|A|
以及x,y∈F₂ⁿ, 使得
|A∩(x+H)|^1/2|B∩(y+H)|^1/2≥1/2K|H|.
本文我们将使用Green 和Tao 的方法并作一些修改, 证明如果|H|>>exp(-O(√K))|A|,
则以上的结论仍然成立.     

Asymptotic properties for the loglog laws under positive association

Let {X _n : n ?? 1} be a strictly stationary sequence of positively associated random variables with mean zero and finite variance. Set $S_n = \sum\limits_{k = 1}^n {X_k }$ , $Mn = \mathop {\max }\limits_{k \leqslant n} \left| {S_k } \right|$ , n ?? 1. Suppose that $0 < \sigma ^2 = EX_1^2 + 2\sum\limits_{k = 2}^\infty {EX_1 X_k < \infty }$ . In this paper, we prove that if E|X ₁|^2+?? < for some ?? ?? (0, 1], and $\sum\limits_{j = n + 1}^\infty {Cov\left( {X_1 ,X_j } \right) = O\left( {n^{ - \alpha } } \right)}$ for some ?? > 1, then for any b > ?1/2 $$\mathop {\lim }\limits_{\varepsilon \searrow 0} \varepsilon ^{2b + 1} \sum\limits_{n = 1}^\infty {\frac{{(\log \log n)^{b - 1/2} }} {{n^{3/2} \log n}}} E\left\{ {M_n - \sigma \varepsilon \sqrt {2n\log \log n} } \right\}_ + = \frac{{2^{ - 1/2 - b} E\left| N \right|^{2(b + 1)} }} {{(b + 1)(2b + 1)}}\sum\limits_{k = 0}^\infty {\frac{{( - 1)^k }} {{(2k + 1)^{2(b + 1)} }}}$$ and $$\mathop {\lim }\limits_{\varepsilon \nearrow \infty } \varepsilon ^{ - 2(b + 1)} \sum\limits_{n = 1}^\infty {\frac{{(\log \log n)^b }} {{n^{3/2} \log n}}E\left\{ {\sigma \varepsilon \sqrt {\frac{{\pi ^2 n}} {{8\log \log n}}} - M_n } \right\}} _ + = \frac{{\Gamma (b + 1/2)}} {{\sqrt 2 (b + 1)}}\sum\limits_{k = 0}^\infty {\frac{{( - 1)^k }} {{(2k + 1)^{2b + 2} }}} ,$$ where x ₊ = max{x, 0}, N is a standard normal random variable, and ??(·) is a Gamma function.     

Maximal inequalities for a continuous semimartingale

Let X =( X t ) t S 0 be a continuous semimartingale given by d X t = f ( t ) w ( X t )d d M ¢ t + f ( t ) σ ( X t )d M t , X 0 =0, where M =( M t , F t ) t S 0 is a continuous local martingale starting at zero with quadratic variation d M ¢ and f ( t ) is a positive, bounded continuous function on [0, X ), and w , σ both are continuous on R and σ ( x )>0 if x p 0. Denote X 𝜏 * =sup 0 h t h 𝜏 | X t | and J t = Z 0 t f ( s ) } ( X s )d d M ¢ s ( t S 0) for a nonnegative continuous function } . If w ( x ) h 0 ( x S 0) and K 1 | x | n σ 2 ( x ) h | w ( x )| h K 2 | x | n σ 2 ( x ) ( x ] R , n >0) with two fixed constants K 2 S K 1 >0, then under suitable conditions for } we show that the maximal inequalities c p , n log 1 n +1 (1+ J 𝜏 ) p h Á X 𝜏 * Á p h C p , n log 1 n +1 (1+ J 𝜏 ) p (0< p < n +1) hold for all stopping times 𝜏 .     

对一个非线性分数阶微分方程组爆破解的研究

The paper focuses on the blow-up solution of system of time-fractional differential equations
where ^cD₀₊^α, ^cD₀₊^β are Caputo fractional derivatives, n-1 < α < n, n-1 < β < n,A(t),B(t) are continuous functions. We obtain a system of the integral equations which is equivalent to the system of nonlinear partial differential equations with time-fractional derivative via the approach of Laplace transformation, and prove the local existence of solutions to the system of the integral equations. Secondly, this paper investigates the blow-up solutions to the a nonlinear system of fractional differential equations by making use of Hölder’s inequality and obtains a solution of system to blow up in a finite time, and gives an upper bound on the blow-up time.     

The lattice point discrepancy of a torus in ℝ3

This article provides an asymptotic formula for the number of integer points in the three-dimensional body $$ \left( \begin{gathered} x \hfill \\ y \hfill \\ z \hfill \\ \end{gathered} \right) = t\left( \begin{gathered} (a + r\cos \alpha )\cos \beta \hfill \\ (a + r\cos \alpha )\sin \beta \hfill \\ r\sin \alpha \hfill \\ \end{gathered} \right),0 \leqq \alpha ,\beta < 2\pi ,0 \leqq r \leqq b, $$ for fixed a > b > 0 and large t.     

一类两点边值问题的多重非负解

该文考虑两点边值问题[1/q(t)][q(t)y′(t)]′+p(t)f(y(t))= 0,λ_1 y(α)-λ_2y′(α)=0 and y(β)=B非负解的存在性, 其中p(t)可能在t=α或t=β附近具有奇异性, f(0)≥0, lim_(y→+∞)f(y)/y=+∞, 并且存在y>0, 使得f(y)<0.      

Scale invariant elliptic operators with singular coefficients

We show that a realization of the operator \({L=|x|^\alpha\Delta +c|x|^{\alpha-1}\frac{x}{|x|}\cdot\nabla -b|x|^{\alpha-2}}\) generates a semigroup in \({L^p(\mathbb{R}^N)}\) if and only if \({D_c=b+(N-2+c)^2/4 > 0}\) and \({s_1+\min\{0,2-\alpha\} < N/p < s_2+\max\{0,2-\alpha\}}\), where \({s_i}\) are the roots of the equation \({b+s(N-2+c-s)=0}\), or \({D_c=0}\) and \({s_0+\min\{0,2-\alpha\} < N/p < s_0+\max\{0,2-\alpha\}}\), where \({s_0}\) is the unique root of the above equation. The domain of the generator is also characterized.     

Some extremal problems for algebraic polynomials in loaded spaces

In a loaded Jacobi space with the inner product

Precise Asymptotics in the Law of the Iterated Logarithm of Moving-Average Processes

In this paper, we discuss the moving-average process Xk = ∑i=-∞ ^∞ ai＋kεi, where {εi;-∞ 〈 i 〈 ∞} is a doubly infinite sequence of identically distributed ψ-mixing or negatively associated random variables with mean zeros and finite variances, {ai;-∞ 〈 i 〈 -∞） is an absolutely solutely summable sequence of real numbers.