函数方程f_1~n+af_1~mf_2~m+f_2~n=1的整函数解

对函数方程fn1+af1mf2m+fn2=1,其中a∈C/{0},n,m∈N,给出所有可能的非常数整函数解的形式.     

关于函数方程f1n1+af1m1f2m2+f2n2=1

对于函数方程f1n1+af1m1f2m2+f2n2=1,其中a∈C/{0},n1,n2,m1,m2∈N,给出存在非常数亚纯函数解和整函数解的必要条件.     

线性分式函数n次迭代的简便计算

分式线性函数f(x)=(ax b)/(cx d)的n次迭代的计算方法已有很多文章作了讨论,本文介绍一种简便的计算方法,可以很方便地求出fn(x).定理1已知f(x)=(ax b)/(cx d)设f0(x)=x,f1(x)=f(x),fn(x)=f[fn-1(x)](n≥1),a,b,c,d∈R且ad≠bc,c≠0,则fn(x)=(α(qqnn--βppnn))xx ααpβn(-p     

函数y=(ax~2+bx+c)e~(x+m)(a≠0)探究

函数Y=(ax~2+bx+c)e~(x+m)(a≠0,x∈R)与二次函数Y=ax~2+bx+c(a≠0,x∈R)有着千丝万缕的关系,下面讨论函数Y=(ax~2+bx+c)e~(x+m)(a≠0,x∈R)的性质和图象以及运用.1性质和图象的讨论     

在W2^1（R）空间中函数逼近的一种新方法

在再生核空间W2^1(R)中，利用再生核的性质实现了既不用计算导数也不需要计算积分，而只用函数值就可以将函数展开成级数的一种方法，并且这种级数的部分和{fn(x)}作为逼近f(x)的序列，它的误差rn(x)=f(x)-fn(x)在空间范数意义下单调下降．     

关于Dini定理

关于函数序列或函数级数的一致收敛性判别准则 ,我们熟知的有 M判别法 ,Abel定理及Dirichlet定理 .在作者的《数学分析》(下册 P95 ,高等教育出版社 ,1 995年 )中还介绍了 Dini定理 ,以下称之为第一 Dini定理 .第一 Dini定理　设 [a,b] R是一有界闭区间 , n∈N,fn∶ [a,b]→R是一连续函数且满足下述条件 :1 )函数序列 { fn}是单调的 ,即 n∈ N ,fn≤ fn+ 1或 n∈ N ,fn≥ fn+ 1.2 )函数序列 { fn}在 [a,b]上逐点收敛于一连续函数 f :[a,b]→ R ,那末函数序列 { fn}在 [a,b]上一致收敛于函数 f.注意 ,上述条件 1 )中的单调性是指函数…     

鞅的极大函数的Lp-范数的上界

设 2 ≤ p<∞ ,(fn)是一个鞅 ,利用P(｜fn｜>λ‖T(fn)‖∞)型的概率指数界 ,其中 ,T是作用在鞅上的拟线性算子 ,本文估计了鞅的极大函数的Lp_范数的上界。本文结果改进与推广了先前由HITCZENKO [7,8,9]与作者 [1 0 ]得到的结果     

对线性分式函数n次迭代的一个补充

线性分式函数的迭代有着较为广泛的应用.现有的求函数的n次迭代式的方法有:定义法、数学归纳法、不动点法和桥函数相似法等.文[1]利用矩阵的特征多项式理论,得到了线性分式函数的n次迭代式的一般计算公式,此公式只能解决特征根互异的情形.本文就特征根相等的情形作了一些讨论,得到了特征根相等时的线性分式函数的n次迭代式的一般计算公式,并举例说明了它的应用.定义设函数y=f(x),记f0(x)=x,fn(x)=f(f…f(x)…)(n∈N ),则称fn(x)为函数f(x)的n次迭代,显然,fn(x)=f(fn-1(x))(n≥1).定理设f(x)=caxx db,a,b,c,d∈R,ad-bc≠0,若方程λ2-(a b)…     

关于复合函数的一个错误命题

文[1]称:若已知f[g(x)]的定义域为A,则f(x)的定义域就是函数g(x)(x∈A)的值域.错误!例1设函数f(x)=2x,函数g(x)=x2,则复合函数f[g(x)]=2x2.显然,复合函数f[g(x)]的定义域是R,函数g(x)(x∈R)的值域[0,+∞),但函数f(x)的定义域是R,而不是函数g(x)(x∈R)的值     

关于一类函数的代数逼近度的注记

设A（z)是函数列{fn(z)}的极限函数，已知^[4],当|fn(z)-A(z)|在z=0的阶满足一定的条件时，A（z)是超越函数。本文给出了极限函数的代数逼近度函数。     

Bounded Fatou components of transcendental entire functions with order less than 1/2

Let f be a transcendental entire function with order ρ 12and let σ be a sufficiently large constant. We prove that if there exists r0 1 such that, for all r r0 and any small ε 0,M(rσ, f) ≥ M(r, f)σ+ε,then every component of the Fatou set F(f) is bounded.     

On the growth of solutions to the complex differential equation f'+Af'+Bf=0

In this paper, we consider the differential equation f'+ Af'+ Bf = 0, where A(z) and B(z) ≡ 0are entire functions. Assume that A(z) has a finite deficient value, then we will give some conditions on B(z)which can guarantee that every solution f ≡ 0 of the equation has infinite order.     

Il sistema diofanteo N+1=x2, 3N+1=y2, 8N+1=z2

Sunto Nel 1969 A. Baker e H. Davenport hanno dimostrato che il sistema3x ² −2=y ² ,8x ² −7=z ² ha soltanto le soluzioni |x|=|y|=|z|=1; |x|=11, |y|=19, |z|=31. Una seconda dimostrazione di P. Kanagasabapathy — Tharmambikai Ponmudurai è apparsa nell'ottobre 1975. L'A. dà una terza dimostrazione che consente, con l'uso dei metodi classici dell'aritmetica, di controllare i ragionamenti in ogni punto. A Dario Graffi nel suo 70° compleanno Entrata in Redazione il 26 novembre 1975.     

Fermions in strong external fields in 2+1 and 1+1 dimensions

The creation of electron-positron pairs from a vacuum by an external Coulomb field is examined within (2+1)-dimensional quantum electrodynamics. If the electromagnetic coupling constant exceeds 0.62 (Z= 85), then in a simple model with a finite-size nucleus, the lower electron level crosses the boundary of the negative-energy continuum (i.e., Dirac sea), and a hole (i.e., positively charged fermion) appears in the negative-energy continuum. An equation is obtained that describes the levels of the ground and excited electron states in a strong Coulomb field of the nucleus. The critical nucleus charge is found for a few lowest electron states. The critical charge in 2+1 dimensions is significantly smaller than in 3+1 dimensions. The problem is reduced to the case of a bounded Coulomb field in 1+1 dimensions without a magnetic field. The interaction of a fermion and an external scalar field in 2+1 and 1+1 dimensions is investigated. Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol 122, No. 3, pp. 372–384, March, 2000