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where λR+:=0,∞), and satisfies the conditions
We prove a strong maximum principle for the linear operator defined by the left-hand side of (1), and use this to show that for every solution (λ,u) of (1)–(2), u is positive on Ta,b . In addition, we show that there exists λmax>0 (possibly λmax=∞), such that, if 0λ<λmax then (1)–(2) has a unique solution u(λ), while if λλmax then (1)–(2) has no solution. The value of λmax is characterised as the principal eigenvalue of an associated weighted eigenvalue problem (in this regard, we prove a general existence result for such eigenvalues for problems with general, nonnegative weights).

Curves of positive solutions of boundary value problems on time-scales
Authors:Fordyce A Davidson  Bryan P Rynne  
Institution:aDivision of Mathematics, Dundee University, Dundee DD1 4HN, Scotland, UK;bDepartment of Mathematics, Heriot-Watt University, Edinburgh EH14 4AS, Scotland, UK
Abstract:Let TR be a time-scale, with a=infT, b=supT. We consider the nonlinear boundary value problem
(2)
(4)
u(a)=u(b)=0,
Keywords:Time-scales  Nonlinear boundary value problem  Positive solutions  Strong maximum principle  Weighted eigenvalue problem
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