Asymptotic analysis and estimates of blow‐up time for the radial symmetric semilinear heat equation in the open‐spectrum case

We estimate the blow‐up time for the reaction diffusion equation u_t=Δu+ λf(u), for the radial symmetric case, where f is a positive, increasing and convex function growing fast enough at infinity. Here λ>λ^*, where λ^* is the ‘extremal’ (critical) value for λ, such that there exists an ‘extremal’ weak but not a classical steady‐state solution at λ=λ^* with ∥w(?, λ)∥_∞→∞ as 0<λ→λ^*?. Estimates of the blow‐up time are obtained by using comparison methods. Also an asymptotic analysis is applied when f(s)=e^s, for λ?λ^*?1, regarding the form of the solution during blow‐up and an asymptotic estimate of blow‐up time is obtained. Finally, some numerical results are also presented. Copyright © 2007 John Wiley & Sons, Ltd.     

Wachstumsordnung und Index der Lösungen linearer Differentialgleichungen mit rationalen Koeffizienten

Let z=∞ be an irregular singular point of the differential equation wⁿ+p_n?1(z)w^(n?1)+...+p₀(z)w=0 with rational coefficients. The functions of the canonical set of solutions relative to z=∞ are of the form $$w(z) = z^\rho \cdot \sum { d_m (z) (\log z)^m , } \rho \varepsilon \mathbb{C}$$ with univalent functions d_m(z) in a neighbourhood of z=∞. Let λ(w)=max {λ(d_m)} denote the maximal order of growth of an irregular solution relative to z=∞, then it is shown that there exists a branch of w in the plane cut along a half ray, which attains the maximal order λ(w). An important tool for the proof is the index of the branches of w.     

Differentiable Eigenvalues of Perturbed Quadratic Matrix Functions

Let T(λ, ε ) = λ² + λC + λεD + K be a perturbed quadratic matrix polynomial, where C, D, and K are n × n hermitian matrices. Let λ₀ be an eigenvalue of the unperturbed matrix polynomial T(λ, 0). With the falling part of the Newton diagram of det T(λ, ε), we find the number of differentiable eigenvalues. Some results are extended to the general case L(λ, ε) = λ² + λD(ε) + K, where D(ε) is an analytic hermitian matrix function. We show that if K is negative definite on Ker L(λ₀, 0), then every eigenvalue λ(ε) of L(λ, ε) near λ₀ is analytic.     

Embeddings of Sλ(2, 4, v)

It is shown that the necessary condition for a given S_λ(2,4,u) to be embedded in some S_λ(2,4,v) as a subdesign, namely v ≥ 3u + 1, is also sufficient for the case of λ = 6. Combining this with the previously known results gives the same sufficiency for any positive integer λ. © 1994 John Wiley & Sons, Inc.     

Nonlinear eigenvalue problems with positively convex operators

We consider the equation u = λAu (λ > 0), where A is a forced isotone positively convex operator in a partially ordered normed space with a complete positive cone K. Let Λ be the set of positive λ for which the equation has a solution u?K, and let Λ₀ be the set of positive λ for which a positive solution—necessarily the minimum one—can be obtained by an iteration u_n = λAu_n?1, u₀ = 0. We show that if K is normal, and if Λ is nonempty, then Λ₀ is nonempty, and each set Λ₀, Λ is an interval with $\text{inf}\text{(Λ}{}_0\text{) =}\text{inf}\text{(Λ) = 0}\text{and sup}\text{(Λ}{}_0\text{) =}\text{sup}\text{(Λ) (= λ1,}\text{say}\text{)}$; but we may have λ1 ? Λ₀ and λ1 ? Λ. Furthermore, if A is bounded on the intersection of K with a neighborhood of 0, then Λ₀ is nonempty. Let u⁰(λ) = lim_n→∞(λA)ⁿ(0) be the minimum positive fixed point corresponding to λ ? Λ₀. Then u⁰(λ) is a continuous isotone convex function of λ on Λ₀.     

Small quasimultiple affine and projective planes: Some improved bounds

We improve the known bounds on r(n): = min {λ| an (n², n, λ)-RBIBD exists} in the case where n + 1 is a prime power. In such a case r(n) is proved to be at most n + 1. If, in addition, n − 1 is the product of twin prime powers, then r(n) ${\ \le \ }{n \over 2}$. We also improve the known bounds on p(n): = min{λ| an (n² + n + 1, n + 1, λ)-BIBD exists} in the case where n² + n + 1 is a prime power. In such a case p(n) is bounded at worst by but better bounds could be obtained exploiting the multiplicative structure of GF(n² + n + 1). Finally, we present an unpublished construction by M. Greig giving a quasidouble affine plane of order n for every positive integer n such that n − 1 and n + 1 are prime powers. © 1998 John Wiley & Sons, Inc. J Combin Designs 6: 337–345, 1998     

Diagnosis of and remedy for imperfection sensitivity of arch bridges

Unless the hangers of arch bridges are sufficiently stiff, such bridges are imperfection sensitive [1]. Increasing the stiffness of the hangers, such structures eventually become imperfection insensitive. The mathematical definition of imperfection insensitivity follows from a series expansion of the dimensionless load parameter Δλ(κ, η), relative to the stability limit λ = λ_S, given as [2] Δλ(κ, η) = λ₁(κ)η + λ₂(κ)η² + λ₃(κ)η³ + O(η⁴), (1) where λ₁, λ₂, … are coefficients depending on the stiffness of the hangers representing the design parameter κ and η is a path parameter describing the postbuckling path. A necessary condition for imperfection insensitivity is [3] λ₁(κ) = 0 ∀κ. (2) If, for a specific value κ of κ, also λ₂(κ=κ ) > 0, (3) then the structure is imperfection insensitive for κ=κ . It will be shown numerically that the increase of the stiffness of the hangers is the remedy addressed in the title of the paper. (© 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim)     

Uniqueness and Flat Core of Positive Solutions for Quasilinear Elliptic Eigenvalue Problems in General Smooth Domains

The structure of positive solutions to the quasilinear elliptic problems –div(|Du|^p–2Du = λf(u) in Ω, u = 0 on ∂Ω, p > 1, Ω ⊂ R^Na bounded smooth domain, is precisely studied when λ is sufficiently large, for a class of logistic‐type nonlinearities f(u) satisfying that f(0) = f(a) = 0, a > 0, f(u) > 0 for u ∈ (0,a), , while u = a is a zero point of f with order ω. It is shown that if ω ≥ p – 1, the problem has a unique positive solution u_λ with sup _Ω u_λ < a, which develops a boundary layer near ∂Ω. It is shown that if 0 < ω < p – 1, the problem also has a unique positive solution u _λ, but the flat core {x ∈ Ω : u_λ(x) = a} ≠ ∅︁ exists. Moreover, the asymptotic behaviour of the flat core is studied as λ → ∞.     

Spectral parameter power series for arbitrary order linear differential equations

Let L be the n‐th order linear differential operator Ly=?₀y⁽ⁿ⁾+?₁y^(n?1)+?+?_ny with variable coefficients. A representation is given for n linearly independent solutions of Ly=λry as power series in λ, generalizing the SPPS (spectral parameter power series) solution that has been previously developed for n=2. The coefficient functions in these series are obtained by recursively iterating a simple integration process, beginning with a solution system for λ=0. It is shown how to obtain such an initializing system working upwards from equations of lower order. The values of the successive derivatives of the power series solutions at the basepoint of integration are given, which provides a technique for numerical solution of n‐th order initial value problems and spectral problems.     

Sur un probleme aux valeurs propres non line aire

In this paper, we give some sufficient conditions for which the differential operatorP(λ=P ₀+λP ₁+...+λ ^m?1 P _m?1+λ ^m , depending polynomially on the complex parameter λ, verifies the following statement: there exists λ₀ ∈ ?,u _o=0,u ₀ ∈ ?(? ⁿ ) a Schwartz space of rapidly decreasing functions, such thatP(λ₀)u ₀=0-.     

Explicit formulas for repeated games with absorbing states

Explicit formulas are given for the asymptotic value lim_{λ → 0} v(λ) and the asymptotic minmax lim w(λ) of finite λ-discounted absorbing games together with new simple proofs for the existence of the limits as λ goes to zero. Similar characterizations for stationary Nash equilibrium payoffs are obtained. The results may be extended to absorbing games with compact metric action sets and jointly-continuous payoff functions.     

Distribution of the spectrum of a singular positive Sturm–Liouville operator perturbed by the Dirac delta function

We consider the Sturm–Liouville operator generated in the space L ²[0,+∞) by the expression l _a,b:= ?d ²/dx ² +x+aδ(x?b) and the boundary condition y(0) = 0. We prove that the eigenvalues λ _n of this operator satisfy the inequalities λ₁ ⁰ < λ₁ < λ₂ ⁰ and λ_n ⁰ ≤ λ_n < λ_n+1 ⁰, n = 2, 3,..., where {?λ_n ⁰} is the sequence of zeros of the Airy function Ai (λ). We find the asymptotics of λ_n as n → +∞ depending on the parameters a and b.     

A bound for wilson's theorem (I)

In 1975, Richard M. Wilson proved: Given any positive integers k ? 3 and λ, there exists a constant v⁰ = v⁰(k, λ) such that v ? B(k,λ) for every integer v ? v⁰ that satisfies λ(v ? 1) ≡ 0(mod k ? 1) and λv(v ? 1) ≡ 0[mod k(k ? 1)]. The proof given by Wilson does not provide an explicit value of v⁰. We try to find such a value v⁰(k, λ). In this article we consider the case λ = 1 and v ≡ 1[mod k(k ? 1)]. We show that: if k ? 3 and v = 1[mod k(k ? 1)] where v > k^kk5, then a B(v,k, 1) exists. © 1995 John Wiley & Sons, Inc.     

Linear Differential Equations with Variable Coefficients in Regular and Some Singular Cases

In this paper the asymptotic properties as t → + ∞ for a single linear differential equation of the form x⁽ⁿ⁾ + a₁ (t)x^(n?1)+…. + a_n(t)x = 0, where the coefficients aj (z) are supposed to be of the power order of growth, are considered. The results obtained in the previous publications of the author were related to the so called regular case when a complete set of roots {λ,(t)}, j = 1, 2, …, n of the characteristic polynomial yⁿ + a₁ (t)y^n?1 + … + a_n(t) possesses the property of asymptotic separability. One of the main restrictions of the regular case consists of the demand that the roots of the set {λ,(t)} have not to be equivalent in pairs for t → + ∞. In this paper we consider the some more general case when the set of characteristic roots possesses the property of asymptotic independence which includes the case when the roots may be equivdent in pairs. But some restrictions on the asymptotic behaviour of their differences λ_i(t)→ λ_j(t) are preserved. This case demands more complicated technique of investigation. For this purpose the so called asymptotic spaces were introduced. The theory of asymptotic spaces is used for formal solution of an operator equation of the form x = A(x) and has the analogous meaning as the classical theory of solving this equation in Band spaces. For the considered differential equation, the main asymptotic terms of a fundamental system of solution is given in a simple explicit form and the asymptotic fundamental system is represented in the form of asymptotic Emits for several iterate sequences.     

Chromaticity of triangulated graphs

It is shown here that a connected graph G without subgraphs isomorphic to K₄ is triangulated if and only if its chromatic polynomial P(G,λ) equals λ(λ ? 1)^m(λ ? 2)^r for some integers m ≧ 1, r ≧ 0. This result generalizes the characterization of Two-Trees given by E.G. Whitehead [“Chromaticity of Two-Trees,” Journal of Graph Theory 9 (1985) 279–284].     

From regular boundary graphs to antipodal distance-regular graphs

Let Γ be a regular graph with n vertices, diameter D, and d + 1 different eigenvalues λ > λ₁ > ··· > λ_d. In a previous paper, the authors showed that if P(λ) > n − 1, then D ≤ d − 1, where P is the polynomial of degree d − 1 which takes alternating values ± 1 at λ₁, …, λ_d. The graphs satisfying P(λ) = n − 1, called boundary graphs, have shown to deserve some attention because of their rich structure. This paper is devoted to the study of this case and, as a main result, it is shown that those extremal (D = d) boundary graphs where each vertex have maximum eccentricity are, in fact, 2-antipodal distance-regular graphs. The study is carried out by using a new sequence of orthogonal polynomials, whose special properties are shown to be induced by their intrinsic symmetry. © 1998 John Wiley & Sons, Inc. J Graph Theory 27: 123–140, 1998     

On computing minimal realizable spectral radii of non‐negative matrices

For decades considerable efforts have been exerted to resolve the inverse eigenvalue problem for non‐negative matrices. Yet fundamental issues such as the theory of existence and the practice of computation remain open. Recently, it has been proved that, given an arbitrary (n–1)‐tuple ?? = (λ₂,…,λ_n) ∈ ?^n–1 whose components are closed under complex conjugation, there exists a unique positive real number ?(??), called the minimal realizable spectral radius of ??, such that the set {λ₁,…,λ_n} is precisely the spectrum of a certain n × n non‐negative matrix with λ₁ as its spectral radius if and only if λ₁ ? ?(??). Employing any existing necessary conditions as a mode of checking criteria, this paper proposes a simple bisection procedure to approximate the location of ?(??). As an immediate application, it offers a quick numerical way to check whether a given n‐tuple could be the spectrum of a certain non‐negative matrix. Copyright © 2004 John Wiley & Sons, Ltd.     

Zur lokalen Werteverteilung der Lösungen linearer Differentialgleichungen

Every solution w of the linear differential equation (*) $$L_n (w) = w^{(n)} + a_{n - 1^{w^{(n - 1)} } } + \ldots + a_0 w = 0$$ with polynomial coefficients a_j is a polynomial or an entire function of finite order λ>0. In this paper we prove the following theorem: Let w be a solution of (*) and no polynomial. Let further λ be the order of w and n_a (R, 1/(w?c)) the number of the zeros in the disc |z?a|4^1/λ $$n_a \left( {L|a|^{1 - \lambda } ,1/(w - c)} \right) \leqq N.$$ It is also shown, that for certain solutions of (*) there exists a constant r₀>0 such that we can replace N by n+α for |a|> r₀. α₀ is the degree of the polynomial a₀. An important tool for the proofs is the index of an entire function.     

Spin depolarization decay rates in α-symmetric stable fields on cubic lattices

We study the asymptotic, long-time behavior of the energy function where {X_s : 0 ≤ s < ∞} is the standard random walk on the d-dimensional lattice Z^d, 1 < α ≤ 2, and f:R⁺ → R⁺ is any nondecreasing concave function. In the special case f(x) = x, our setting represents a lattice model for the study of transverse magnetization of spins diffusing in a homogeneous, α-stable, i.i.d., random, longitudinal field {λV(x) : x ∈ Z^d} with common marginal distribution, the standard α-symmetric stable distribution; the parameter λ describes the intensity of the field. Using large-deviation techniques, we show that S_c(λ α f) = lim_t→∞ E(t; λ f) exists. Moreover, we obtain a variational formula for this decay rate S_c. Finally, we analyze the behavior S_c(λ α f) as λ → 0 when f(x) = x^β for all 1 ≥ β > 0. Consequently, several physical conjectures with respect to lattice models of transverse magnetization are resolved by setting β = 1 in our results. We show that S_c(λ, α, 1) ≈ λ^α for d ≥ 3, λ^agr;(ln 1/λ)^α−1 in d = 2, and in d = 1. © 1996 John Wiley & Sons, Inc.