ABSTRACT
We consider a non homogeneous Gompertz diffusion process whose parameters are modified by generally time-dependent exogenous factors included in the infinitesimal moments. The proposed model is able to describe tumor dynamics under the effect of anti-proliferative and/or cell death-induced therapies. We assume that such therapies can modify also the infinitesimal variance of the diffusion process. An estimation procedure, based on a control group and two treated groups, is proposed to infer the model by estimating the constant parameters and the time-dependent terms. Moreover, several concatenated hypothesis tests are considered in order to confirm or reject the need to include time-dependent functions in the infinitesimal moments. Simulations are provided to evaluate the efficiency of the suggested procedures and to validate the testing hypothesis. Finally, an application to real data is considered.
Subject(s)
Cell Death/drug effects , Cell Proliferation/drug effects , Models, Biological , Neoplasms/drug therapy , Neoplasms/pathology , Animals , Antineoplastic Combined Chemotherapy Protocols/administration & dosage , Carboplatin/administration & dosage , Computer Simulation , Female , Humans , Mathematical Concepts , Mice , Neoplasms, Experimental/drug therapy , Neoplasms, Experimental/pathology , Ovarian Neoplasms/drug therapy , Ovarian Neoplasms/pathology , Paclitaxel/administration & dosage , Stochastic ProcessesABSTRACT
We present both experimentally and theoretically the transformation of radially and azimuthally polarized vector beams when they propagate through a biaxial crystal and are transformed by the conical refraction phenomenon. We show that, at the focal plane, the transverse pattern is formed by a ring-like light structure with an azimuthal node, this node being found at diametrically opposite points of the ring for radial/azimuthal polarizations. We also prove that the state of polarization of the transformed beams is conical refraction-like, i.e., that every two diametrically opposite points of the light ring are linearly orthogonally polarized.