On energy functionals for second-order elliptic systems with constant coefficients

preprint2022arXivOpen access

Abstract

We consider the Dirichlet problem for second-order elliptic systems with constant coefficients. We prove that non-reducible strongly elliptic systems of this type do not admits non-negatively defined energy functionals of the form f↦∫DΦ(ux,vx,uy,vy) dxdyf\mapsto\int_{D}\varPhi(u_x,v_x,u_y,v_y)\,dxdy, where DD is the domain where the problem we are interested in is considered, Φ\varPhi is some quadratic form in R4\mathbb R^4, and f=u+ivf=u+iv is a function in the complex variable. The proof is based on reducing the system under consideration to a special (canonical) form, when the differential operator defining this system is represented as a perturbation of the Laplace operator with respect to two small real parameters (the canonical parameters of the system under consideration).

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