ISSN 0001-4346, Mathematical Notes, 2015, Vol. 97, No. 5, pp. 745–758. © Pleiades Publishing, Ltd., 2015. Original Russian Text © L. E. Rossovskii, A. L. Tasevich, 2015, published in Matematicheskie Zametki, 2015, Vol. 97, No. 5, pp. 733–748. The First Boundary-Value Problem for Strongly Elliptic Functional-Dierential Equations with Orthotropic Contractions L. E. Rossovskii * and A. L. Tasevich ** Peoples’ Friendship University of Russia, Moscow, Russia Received October 9, 2014 AbstractWe obtain a number of necessary and sucient strong ellipticity conditions for a functional-dierential equation containing, in its leading part, orthotropic contractions of the argument of the unknown function. We establish the unique solvability of the rst boundary-value problem and the discreteness, semiboundedness, and sectorial structure of its spectrum. DOI: 10.1134/S0001434615050090 Keywords: strong elliptic functional-dierential equation, rst boundary-value problem, or- thotropic contraction, G ˚ arding-type inequality, strong ellipticity condition, Plancherel’s theorem, Fourier transform, Riesz theorem, dierence operator. 1. INTRODUCTION The paper deals with the boundary-value problem A R u ≡− 2 i,j =1 (R ij u x i ) x j = f (x), x Ω, u| Ω =0 (1.1) in a bounded domain Ω R 2 , where R ij v(x)= a ij 0 v(x)+ a ij 1 v(q 1 x 1 , px 2 )+ a ij,1 v(qx 1 ,p 1 x 2 ), p, q > 1, a ij 0 ,a ij,±1 C, i, j =1, 2, and the complex-valued function f (x) belongs to the space L 2 (Ω). The subject matter of the paper is mostly related to the study of the well-known inequality Re(A R u, u) L 2 (Ω) c 1 u 2 H 1 (Ω) c 2 u 2 L 2 (Ω) for all u C 0 (Ω), (1.2) called a G ˚ arding-type inequality, as well as to the coercitivity condition for the operator A R . If we set a ij,±1 =0, then the operator A R becomes a second-order linear dierential operator with constant coecients and, in this case, estimate (1.2) is equivalent to the well-known strong ellipticity condition Re 2 i,j =1 a ij 0 ξ i ξ j c 1 |ξ | 2 . The question of the validity of inequality (1.2) for dierential operators, including higher-order equations, systems of equations, and variable coecients, was solved in [1], [2] and, for dierence-dierential operators in bounded domains, in [3]. Functional dierential equations containing contractions and dilations of the arguments of the unknown function in the leading part were considered in [4][7], where it was assumed that the contraction (dilation) coecient is the same for all variables: v(x 1 ,x 2 ) v(qx 1 ,qx 2 ). (1.3) * E-mail: lrossovskii@gmail.com ** E-mail: atasevich@gmail.com 745