In the first phase of the study, temperature distributions, resulting from different exposure conditions of electromagnetic (EM) fields, are experimentally determined.
For the thinner nanorod films, the energy of the SP waves are mainly dissipated via radiation damping, in which the EM fields are coupling backward to the prism side and then radiate to space.
A strong pulsed electromagnetic (EM) field is used in wire crimping of aluminium connector terminal with copper wire.
An elliptical applicator with a focusing electromagnetic (EM) field is designed to successfully process Pb(Zr, Ti O3 (PZT) thick films.
The electromagnetic (EM) field is considered at high frequencies, where the time scale of the heat conduction is significantly lower than the time scale of the EM field.
Furthermore, the analysis is extended to the case of vector beams in which the components of the electromagnetic (EM) field are obtained based on different polarizations of the magnetic and electric vector potentials, which exactly satisfy Maxwell's vectorial equations and Lorenz' gauge condition.
Three dimensional (3D) simulations of an electromagnetic (EM) field were conducted using COMSOL multiphysics (ver. 4.2) based on a finite element method (FEM).
In these reports, the enhanced localized electromagnetic (EM) field was considered to be the dominant mechanism for the occurrence of random lasing, especially for small sizes of Ag NPs.
Recently, thanks to a new type recorder called electron direct detector device (DDD), cryo-EM field is experiencing revolution.
GPRs generate and detect classical EM fields that are described by Maxwell's equations.
The EM concentrators for time-varying fields were first proposed by Rahm et al.9, and developed in10.
