Abstract:Boundary value problems of Sturm-Liouville and periodic type for the second order nonlinear ODE u + λ f (t, u) = 0 are considered. Multiplicity results are obtained for λ positive and large under suitable growth restrictions on f (t, u) of superlinear type at u = 0 and of sublinear type at u = ∞. Only one-sided growth conditions are required. Applications are given to the equation u + λq(t)f(u) = 0, allowing also a weight function q(t) of nonconstant sign.Mathematics Subject Classification. 34C25, 34C28.
“…We see that, for all (θ 0 , ρ 0 ) with θ 0 ∈ R and ρ 0 > 0, uniqueness and global continuability of solutions hold for any Cauchy problem associated with (21) and with (22). Let r − (· ; θ 0 , ρ 0 ), r + (· ; θ 0 , ρ 0 ) (in the sequel, sometimes denoted by r ∓ for simplicity) be the solutions of (21) and (22), respectively, satisfying r ∓ (θ 0 ) = ρ 0 .…”
Section: Small Classical Subharmonic Solutionsmentioning
confidence: 86%
“…As uniqueness of solutions holds for any Cauchy problem associated with (22), by a classical result on differential inequalities (see, e.g., [27, Section I.6, Theorem 6.1]), we conclude that (θ) ≤ γ(θ), for all θ ∈ [θ(t 0 ), θ(σ)], and hence ρ(t) ≤ γ(θ(t)), for all t ∈ [t 0 , σ]. In particular, we have…”
Section: As Limmentioning
confidence: 99%
“…, m − 1, then it is referred to as a subharmonic solution of order m. As a general rule in this context, one tries to get as much information as possible about the minimality of the period. In particular, in [22] the existence of subharmonic solutions of (3) has been proved assuming that either f is superlinear at 0, i.e.,…”
Section: Introductionmentioning
confidence: 99%
“…uniformly in t. More precisely, it is shown in [22] that condition (4), even assumed only at 0 + , or at 0 − , implies the existence of two sequences of arbitrarily small subharmonic solutions having a prescribed number of zeroes and condition (5), even assumed only at +∞, or at −∞, implies the existence of two sequences of arbitrarily large subharmonic solutions having a prescribed number of zeroes. The proof is performed by a phase-plane analysis and relies on the Poincaré-Birkhoff fixed point theorem; the nodal properties of the solutions are obtained by using the rotation number which counts the number of turns of the solutions around the origin in the phase-plane.…”
Section: Introductionmentioning
confidence: 99%
“…Assuming that f is superlinear at 0, we prove in Theorem 3.4 the existence of small classical subharmonic solutions having suitable nodal properties; in this case the proof, which borrows some arguments from [22], is based on the use of the rotation number and on a version of the Poincaré-Birkhoff theorem given in [23,Theorem 8.2] and not requiring uniqueness of solutions for the Cauchy problems associated with (1). In particular, the following result holds.…”
We study the existence of subharmonic solutions of the prescribed curvature equationAccording to the behaviour at zero, or at infinity, of the prescribed curvature f , we prove the existence of arbitrarily small classical subharmonic solutions, or bounded variation subharmonic solutions with arbitrarily large oscillations.
“…We see that, for all (θ 0 , ρ 0 ) with θ 0 ∈ R and ρ 0 > 0, uniqueness and global continuability of solutions hold for any Cauchy problem associated with (21) and with (22). Let r − (· ; θ 0 , ρ 0 ), r + (· ; θ 0 , ρ 0 ) (in the sequel, sometimes denoted by r ∓ for simplicity) be the solutions of (21) and (22), respectively, satisfying r ∓ (θ 0 ) = ρ 0 .…”
Section: Small Classical Subharmonic Solutionsmentioning
confidence: 86%
“…As uniqueness of solutions holds for any Cauchy problem associated with (22), by a classical result on differential inequalities (see, e.g., [27, Section I.6, Theorem 6.1]), we conclude that (θ) ≤ γ(θ), for all θ ∈ [θ(t 0 ), θ(σ)], and hence ρ(t) ≤ γ(θ(t)), for all t ∈ [t 0 , σ]. In particular, we have…”
Section: As Limmentioning
confidence: 99%
“…, m − 1, then it is referred to as a subharmonic solution of order m. As a general rule in this context, one tries to get as much information as possible about the minimality of the period. In particular, in [22] the existence of subharmonic solutions of (3) has been proved assuming that either f is superlinear at 0, i.e.,…”
Section: Introductionmentioning
confidence: 99%
“…uniformly in t. More precisely, it is shown in [22] that condition (4), even assumed only at 0 + , or at 0 − , implies the existence of two sequences of arbitrarily small subharmonic solutions having a prescribed number of zeroes and condition (5), even assumed only at +∞, or at −∞, implies the existence of two sequences of arbitrarily large subharmonic solutions having a prescribed number of zeroes. The proof is performed by a phase-plane analysis and relies on the Poincaré-Birkhoff fixed point theorem; the nodal properties of the solutions are obtained by using the rotation number which counts the number of turns of the solutions around the origin in the phase-plane.…”
Section: Introductionmentioning
confidence: 99%
“…Assuming that f is superlinear at 0, we prove in Theorem 3.4 the existence of small classical subharmonic solutions having suitable nodal properties; in this case the proof, which borrows some arguments from [22], is based on the use of the rotation number and on a version of the Poincaré-Birkhoff theorem given in [23,Theorem 8.2] and not requiring uniqueness of solutions for the Cauchy problems associated with (1). In particular, the following result holds.…”
We study the existence of subharmonic solutions of the prescribed curvature equationAccording to the behaviour at zero, or at infinity, of the prescribed curvature f , we prove the existence of arbitrarily small classical subharmonic solutions, or bounded variation subharmonic solutions with arbitrarily large oscillations.
We study the second order nonlinear differential equation u ′′ +a(t)g(u) = 0, where g is a continuously differentiable function of constant sign defined on an open interval I ⊆ R and a(t) is a sign-changing weight function. We look for solutions u(t) of the differential equation such that u(t) ∈ I, satisfying the Neumann boundary conditions. Special examples, considered in our model, are the equations with singularity, for I = R Mathematics Subject Classification. 34B15, 34B09.
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