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1.
In this paper we are interested in the behaviour respect tov of thekth positive zeroc′ vk of the derivative of the general Bessel functionC v(x)=J v(x)cosα?Y v(x)sinα, 0≤α<π, whereJ v(x) andY v(x) indicate the Bessel functions of first and second kind respectively. It is well known that forc′ vk>∥v∥,c′ vk increases asv increases. Here we prove several additional properties forc′ vk. Our main result is thatc′ vk is concave as a function ofv, whenc′ vk>∥v∥>0. This implies the concavity ofc′ vk for everyk=2,3, ?. In the case of the zerosJ′ vk of d dx J v(x) we extend this property tok=1 for everyv≥0.  相似文献   

2.
LetP κ,n (λ,β) be the class of functions \(g(z) = 1 + \sum\nolimits_{v = n}^\infty {c_\gamma z^v }\) , regular in ¦z¦<1 and satisfying the condition $$\int_0^{2\pi } {\left| {\operatorname{Re} \left[ {e^{i\lambda } g(z) - \beta \cos \lambda } \right]} \right|} /\left( {1 - \beta } \right)\cos \lambda \left| {d\theta \leqslant \kappa \pi ,} \right.z = re^{i\theta } ,$$ , 0 < r < 1 (κ?2,n?1, 0?Β<1, -π<λ<π/2;M κ,n (λ,β,α),n?2, is the class of functions \(f(z) = z + \sum\nolimits_{v = n}^\infty {a_v z^v }\) , regular in¦z¦<1 and such thatF α(z)∈P κ,n?1(λ,β), where \(F_\alpha (z) = (1 - \alpha )\frac{{zf'(z)}}{{f(z)}} + \alpha (1 + \frac{{zf'(z)}}{{f'(z)}})\) (0?α?1). Onr considers the problem regarding the range of the system {g (v?1)(z?)/(v?1)!}, ?=1,2,...,m,v=1,2,...,N ?, on the classP κ,1(λ,β). On the classesP κ,n (λ,β),M κ,n (λ,β,α) one finds the ranges of Cv, v?n, am, n?m?2n-2, and ofg(?),F ?(?), 0<¦ξ¦<1, ξ is fixed.  相似文献   

3.
Some estimates for simultaneous polynomial approximation of a function and its derivatives are obtained. These estimates are exact in a certain sense. In particular, the following result is derived as a corollary: Forf∈C r[?1,1],mN, and anyn≥max{m+r?1, 2r+1}, an algebraic polynomialP n of degree ≤n exists that satisfies $$\left| {f^{\left( k \right)} \left( x \right) - P_n^{\left( k \right)} \left( {f,x} \right)} \right| \leqslant C\left( {r,m} \right)\Gamma _{nrmk} \left( x \right)^{r - k} \omega ^m \left( {f^{\left( r \right)} ,\Gamma _{nrmk} \left( x \right)} \right),$$ for 0≤k≤r andx ∈ [?1,1], where ωυ(f(k),δ) denotes the usual vth modulus of smoothness off (k), and Moreover, for no 0≤k≤r can (1?x 2)( r?k+1)/(r?k+m)(1/n2)(m?1)/(r?k+m) be replaced by (1-x2)αkn2αk-2, with αk>(r-k+a)/(r-k+m).  相似文献   

4.
Let λ f(n) be the n-th normalized Fourier coefficient of a holomorphic Hecke eigenform f(z)∈Sk(Γ).In this paper,we established nontrivial estimates for ∑n≤xλf(ni)λf(nj),where 1 ≤ i j ≤ 4.  相似文献   

5.
For Ξ∈R n ,tR andfS(R n ) define $\left( {S^2 f} \right)\left( t \right)\left( \xi \right) = \exp \left( {it\left| \xi \right|^2 } \right)\hat f\left( \xi \right)$ . We determine the optimal regularitys 0 such that $\int_{R^n } {\left\| {(S^2 f)[x]} \right\|_{L^2 (R)}^2 \frac{{dx}}{{(1 + |x|)^b }} \leqslant C\left\| f \right\|_{H^s (R^n )}^2 ,s > s_0 } ,$ holds whereC is independent offS(R n ) or we show that such optimal regularity does not exist. This problem has been treated earlier, e.g. by Ben-Artzi and Klainerman [2], Kato and Yajima [4], Simon [6], Vega [9] and Wang [11]. Our theorems can be generalized to the case where the exp(it|ξ|2) is replaced by exp(it|ξ|a),a≠2. The proof uses Parseval's formula onR, orthogonality arguments arising from decomposingL 2(R n ) using spherical harmonics and a uniform estimate for Bessel functions. Homogeneity arguments are used to show that results are sharp with respect to regularity.  相似文献   

6.
Let jvk, yvk and cvk denote the kth positive zeros of the Bessel functions Jv(x), Yv(x) and of the general cylinder function Cv(x) = cos αJv(x)?sin αYv(x), 0 ? α < π, respectively. In this paper we extend to cvk, k = 2, 3,..., some linear inequalities presently known only for jvk. In the case of the zeros yvk we are able to extend these inequalities also to k = 1. Finally in the case of the first positive zero jv1 we compare the linear enequalities given in [9] with some other known inequalities.  相似文献   

7.
Summary LetC vk be thekth positive zero of the cylinder functionC v(x)=cosJ v(x)–sinY v(x), whereJ v(x),Y v(x) are the Bessel functions of first kind and second kind, resp., andv>0, 0<. Definej vk byj vk=C vk with . Using the notation 1/K=, we derive the first two terms of the asymptotic expansion ofj vk in terms of the powers of at the expense of solving a transcendental equation. Numerical examples are given to show the accuracy of this approximation.Dedicated to the memory of Professor Lothar CollatzThis work has been supported by the Hungarian Scientific Grant No. 6032/6319  相似文献   

8.
Letj vk denotes thekth positive zero of the derivativeJ v (x)=dJ v (x)/dx of Bessel functionJ v (x) fork=1, 2,…. We establish the upper bound
$$j'_{\nu k}< \nu + a_k \left( {\nu + \frac{{{\rm A}_k^3 }}{{a_k^3 }}} \right)^{\frac{1}{3}} + \frac{3}{{10}}a_k^2 \left( {\nu + \frac{{A_k^3 }}{{a_k^3 }}} \right)^{\frac{1}{3}} , \nu \geqslant 0, k = 1,2, \ldots $$  相似文献   

9.
Пусть?(x) — ограниченн ая функция на отрезке [0,1] и ее функция распределен ияΦ(t) удовлетворяет услов ию $$\Phi \left( t \right) + \Phi \left( { - t} \right) = 1.$$ Еслиf(x) — конечная поч ти всюду функция, то дл яF n (t) — функции распределе ния произведенияf(x)?(nx) — вы полнены соотношения и В частности, еслиf(x) — и нтегрируемая функци я, то из (1) следует, что $$\mathop {\lim }\limits_{n \to \infty } \mathop \smallint \limits_0^1 f\left( x \right)\varphi \left( {nx} \right)dx = 0 $$   相似文献   

10.
For a nonlinear hyperbolic equation with variable coefficients and the infinite-dimensional Lévy Laplacian Δ L , $$\beta \left( {\sqrt 2 \left\| x \right\|_H \frac{{\partial U(t,x)}} {{\partial t}}} \right)\frac{{\partial ^2 U(t,x)}} {{\partial t^2 }} + \alpha (U(t,x))\left[ {\frac{{\partial U(t,x)}} {{\partial t}}} \right]^2 = \Delta _L U(t,x),$$ we present algorithms for the solution of the boundary-value problem U(0, x) = u 0, U(t, 0) = u 1 and the exterior boundary-value problem U(0, x) = v 0, \(\left. {U(t,x)} \right|_{\Gamma = v_1 }\) , \(\lim _{\left\| x \right\|_{H \to \infty } } \left. {U(t,x) = v_2 } \right|\) for the class of Shilov functions depending on the parameter t.  相似文献   

11.
The modified Bernstein-Durrmeyer operators discussed in this paper are given byM_nf≡M_n(f,x)=(n+2)P_(n,k)∫_0~1p_n+1.k(t)f(t)dt,whereWe will show,for 0<α<1 and 1≤p≤∞  相似文献   

12.
Для функцииfC[?1, 1] с ог раниченным числом пе ремен знака строится последовательность многочленовр п , коположительных сf (т.е.f(x)p n (x)≥0, ?1≤х<1) и таких, что $$\left\| {f - p_n } \right\|_\infty \leqslant C\omega _\varphi ^3 (f,n^{ - 1} ),$$ гдеω ? 3 (f, δ) — модуль непр ерывности Дитциана-Т отика третьего порядка. Изв естно, чтоω ? 3 нельзя заменить ни наω ? 4 , ни на ω4. Таким образом, приведенная оценка точна в некотором смы сле. В качестве следст вия установлена эквивал ентность соотношений $$E_n (f) = O(n^{ - \alpha } )\user2{}E_n^{(0)} (f,r) = O(n^{ - \alpha } )\user2{}0< \alpha< 3.$$   相似文献   

13.
It is proved that if an entire function f: ? → ? satisfies an equation of the form α 1(x)β 1(y) + α 2(x)β 2(y) + α 3(x)β 3(y), x,y ∈ C, for some α j , β j : ? → ? and there exist no \({\widetilde \alpha _j}\) and ?\({\widetilde \beta _j}\) for which \(f\left( {x + y} \right)f\left( {x - y} \right) = {\overline \alpha _1}\left( x \right){\widetilde \beta _1}\left( y \right) + {\overline \alpha _2}\left( x \right){\widetilde \beta _2}\left( y \right)\), then f(z) = exp(Az 2 + Bz + C) ? σ Γ(z - z 1) ? σ Γ(z - z 2), where Γ is a lattice in ?; σ Γ is the Weierstrass sigma-function associated with Γ; A,B,C, z 1, z 2 ∈ ?; and \({z_1} - {z_2} \notin \left( {\frac{1}{2}\Gamma } \right)\backslash \Gamma \).  相似文献   

14.
In this paper,a uniqueness theorem for meromorphic mappings partially sharing 2N+3 hyperplanes is proved.For a meromorphic mapping f and a hyperplane H,set E(H,f) = {z|ν(f,H)(z) 0}.Let f and g be two linearly non-degenerate meromorphic mappings and {Hj}j2=N1+ 3be 2N + 3 hyperplanes in general position such that dim f-1(Hi) ∩ f-1(Hj) n-2 for i = j.Assume that E(Hj,f) E(Hj,g) for each j with 1 j 2N +3 and f = g on j2=N1+ 3f-1(Hj).If liminfr→+∞ 2j=N1+ 3N(1f,Hj)(r) j2=N1+ 3N(1g,Hj)(r) NN+1,then f ≡ g.  相似文献   

15.
Let n ≥ 2 and let Ω ? ? n be an open set. We prove the boundedness of weak solutions to the problem
$$u \in W_0^1 L^\Phi \left( \Omega \right) and - div\left( {\Phi '\left( {\left| {\nabla u} \right|} \right)\frac{{\nabla u}}{{\left| {\nabla u} \right|}}} \right) + V\left( x \right)\Phi '\left( {\left| u \right|} \right)\frac{u}{{\left| u \right|}} = f\left( {x,u} \right) + \mu h\left( x \right) in \Omega ,$$
where ? is a Young function such that the space W 0 1 L Φ(Ω) is embedded into an exponential or multiple exponential Orlicz space, the nonlinearity f(x, t) has the corresponding critical growth, V(x) is a continuous potential, hL Φ(Ω) is a non-trivial continuous function and µ ≥ 0 is a small parameter. We consider two classical cases: the case of Ω being an open bounded set and the case of Ω = ? n .
  相似文献   

16.
For ν≥0 let cνk be the k-th positive zero of the cylinder functionC v(t)=J v(t)cosα-Y v(t)sinα, 0≤α>π whereJ ν(t) andY ν(t) denote the Bessel functions of the first and the second kind, respectively. We prove thatC v,k 1+H(x) is convex as a function of ν, ifc νk≥x>0 and ν≥0, whereH(x) is specified in Theorem 1.1.  相似文献   

17.
Let fC[?1, 1]. Let the approximation rate of Lagrange interpolation polynomial of f based on the nodes $ \left\{ {\cos \frac{{2k - 1}} {{2n}}\pi } \right\} \cup \{ - 1,1\} $ be Δ n + 2(f, x). In this paper we study the estimate of Δ n + 2(f,x), that keeps the interpolation property. As a result we prove that $$ \Delta _{n + 2} (f,x) = \mathcal{O}(1)\left\{ {\omega \left( {f,\frac{{\sqrt {1 - x^2 } }} {n}} \right)\left| {T_n (x)} \right|\ln (n + 1) + \omega \left( {f,\frac{{\sqrt {1 - x^2 } }} {n}\left| {T_n (x)} \right|} \right)} \right\}, $$ where T n (x) = cos (n arccos x) is the Chebeyshev polynomial of first kind. Also, if fC r [?1, 1] with r ≧ 1, then $$ \Delta _{n + 2} (f,x) = \mathcal{O}(1)\left\{ {\frac{{\sqrt {1 - x^2 } }} {{n^r }}\left| {T_n (x)} \right|\omega \left( {f^{(r)} ,\frac{{\sqrt {1 - x^2 } }} {n}} \right)\left( {\left( {\sqrt {1 - x^2 } + \frac{1} {n}} \right)^{r - 1} \ln (n + 1) + 1} \right)} \right\}. $$   相似文献   

18.
We prove that if a functionfC (1) (I),I: = [?1, 1], changes its signs times (s ∈ ?) within the intervalI, then, for everyn > C, whereC is a constant which depends only on the set of points at which the function changes its sign, andk ∈ ?, there exists an algebraic polynomialP n =P n (x) of degree ≤n which locally inherits the sign off(x) and satisfies the inequality $$\left| {f\left( x \right) - P_n \left( x \right)} \right| \leqslant c\left( {s,k} \right)\left( {\frac{1}{{n^2 }} + \frac{{\sqrt {1 - x^2 } }}{n}} \right)\omega _k \left( {f'; \frac{1}{{n^2 }} + \frac{{\sqrt {1 - x^2 } }}{n}} \right), x \in I$$ , where ω k (f′;t) is thekth modulus of continuity of the functionf’. It is also shown that iffC (I) andf(x) ≥ 0,xI then, for anynk ? 1, there exists a polynomialP n =P n (x) of degree ≤n such thatP n (x) ≥ 0,xI, and |f(x) ?P n (x)| ≤c(k k (f;n ?2 +n ?1 √1 ?x 2),xI.  相似文献   

19.
For two-dimensional Navier-Stokes equations defined in a bounded domain Ω and for an arbitrary initial vector field, we construct the boundary Dirichlet condition that is tangent to the boundary ?Ω of Ω and satisfies the property: the solutionυ(t, x) of the mentioned boundary-value problem equals zero at a certain finite time momentT. Moreover, $$\parallel x(t, \cdot )\parallel _{L_2 (\Omega )} \leqslant c\exp \left( {\tfrac{{ - k}}{{(T - t)^2 }}} \right)ast \to T,$$ wherec > 0,k > 0 constants.  相似文献   

20.
It is the aim of this paper to introduce two new notions of discrepancy. They are defined by the formulas $$\begin{gathered} \Delta _N^r \left( {\omega ;f} \right) = \mathop {\sup }\limits_{\left| z \right| = r} \left| {\left( {{1 \mathord{\left/ {\vphantom {1 N}} \right. \kern-\nulldelimiterspace} N}} \right)\sum\limits_{n = 1}^N {f\left( {z e^2 \pi i\omega \left( n \right)} \right)} - f\left( 0 \right)} \right|, and \hfill \\ \delta _N^r \left( {\omega ;f} \right) = \mathop {\sup }\limits_{\left| z \right| = r} \left| {\left( {{1 \mathord{\left/ {\vphantom {1 N}} \right. \kern-\nulldelimiterspace} N}} \right)\sum\limits_{n = 1}^N {f\left( {z \omega \left( n \right)} \right)} \cdot z - \int\limits_0^z {f\left( \zeta \right)d\zeta } } \right|, \hfill \\ \end{gathered} $$ wheref is a holomorphic function defined in the unit disc withf (k) (0)≠0 for allk∈?,r<1 is a positive number, and ω is a sequence in [0, 1]. The first of these discrepancies can be generalized for multidimensional sequences. ω is uniform distributed if and only if lim N→∞ Δ N r (ω;f)=0 resp. lim N→∞δ N r (ω;f)=0. These results are proved in a quantitative way by estimating the classical discrepancyD N (ω) by means ofΔ N r (ω;f) and δ N r (ω;f): $$\begin{gathered} \Delta _N^r \left( {\omega ;f} \right) \ll D_N \left( \omega \right) \ll \Phi \left( {\Delta _N^r \left( {\omega ;f} \right)} \right), \hfill \\ \delta _N^r \left( {\omega ;f} \right) \ll D_N \left( \omega \right) \ll \Psi \left( {\delta _N^r \left( {\omega ;f} \right)} \right). \hfill \\ \end{gathered} $$ The functions Φ and Ψ only depend onf andr. These estimations are based on the inequalities ofKoksma-Hlawka andErdös-Turán.  相似文献   

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