Derivation of the linear response relations Eq. (4) and (5) in the main textIn the following we provide a detailed derivation of equations (5) and (6) of the main text used to obtain the reported numerical results. The derivation closely follows the formalisms described by Fröhlich, 1 Jackson 2 and Zhan 3 . According to the theory of macroscopic dielectrics the two fundamental equations that define the dielectric response of a system are equations (SI.1) and (SI.2). 1-3Here, E is the Maxwell field, D is the electric displacement vector, P is the polarisation, and ε is the dielectric tensor. For an isotropic system all three eigenvalues of ε are the same.However, because of the asymmetry of the confining geometry, the eigenvalues might be unequal. If one eliminates D from equations (SI.1) and (SI.2), one obtains equation (SI.3).The main problem with equation (SI.3) is that the occurrence of two unknowns in one equation, namely, the static dielectric constant and the ratio (P/E). If one assumes the applied field is weak, the application of Kubo's linear response formalism provides analytical expressions as detailed below. 4The total dipole moment (that is proportional to the polarisation) couples with the cavity field (E c ) which modifies the Hamiltonian of the system. The cavity field is