We consider boundary value problems for 1D autonomous damped and delayed semilinear wave equations of the type ∂t2u(t,x)-a(x,λ)2∂x2u(t,x)=b(x,λ,u(t,x),u(t-τ,x),∂tu(t,x),∂xu(t,x)),x∈(0,1)\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$\\begin{aligned} \\partial ^2_tu(t,x)- a(x,\\lambda )^2\\partial _x^2u(t,x)= b(x,\\lambda ,u(t,x),u(t-\\tau ,x),\\partial _tu(t,x),\\partial _xu(t,x)), \\; x \\in (0,1) \\end{aligned}$$\\end{document}with smooth coefficient functions a and b such that a(x,lambda )>0 and b(x,lambda ,0,0,0,0) = 0 for all x and lambda . We state conditions ensuring Hopf bifurcation, i.e., existence, local uniqueness (up to time shifts), regularity (with respect to t and x) and smooth dependence (on tau and lambda ) of small non-stationary time-periodic solutions, which bifurcate from the stationary solution u=0, and we derive a formula which determines the bifurcation direction with respect to the bifurcation parameter tau . To this end, we transform the wave equation into a system of partial integral equations by means of integration along characteristics and then apply a Lyapunov-Schmidt procedure and a generalized implicit function theorem. The main technical difficulties, which have to be managed, are typical for hyperbolic PDEs (with or without delay): small divisors and the “loss of derivatives” property. We do not use any properties of the corresponding initial-boundary value problem. In particular, our results are true also for negative delays tau .
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