关键词:
Fractional Laplacian
Schrodinger equation
gauge
摘要:
Let Omega subset of R-n be an open set, where n >= 2. Suppose omega is a locally finite Borelmeasure on Omega. For alpha is an element of (0, 2), define the fractional Laplacian (-Delta)(alpha/2) via the Fourier transform on R-n, and let G be the corresponding Green's operator of order alpha on Omega. Define T (u) = G(u omega). If parallel to T parallel to(L2(omega)-> L2(omega)) < 1, we obtain a representation for the unique weak solution u in the homogeneous Sobolev space L-0(alpha/2,2) (Omega) of (-Delta)(alpha/2) u = u omega + nu on Omega, u = 0 on Omega(c), for nu in the dual Sobolev space L-(alpha/2,2)(Omega). If Omega is a bounded C-1,C-1 domain, this representation yields matching exponential upper and lower pointwise estimates for the solution when nu = chi(Omega). These estimates are used to study the existence of a solution u(1) (called the "gauge") of the integral equation u(1) = 1 + G(u(1)omega) corresponding to the problem (-Delta)(alpha/2)u = u omega on Omega, u >= 0 on Omega, u = 1 on Omega(c). We show that if parallel to T parallel to < 1, then u(1) always exists if 0 < alpha < 1. For 1 <= alpha < 2, a solution exists if the norm of T is sufficiently small. We also show that the condition parallel to T parallel to < 1 does not imply the existence of a solution if 1 < alpha < 2. The condition parallel to T parallel to <= 1 is necessary for the existence of u(1) for all 0 < alpha = 2.