Nonlocal optical response in metallic nanostructures
... of f (r, ω) (i.e. f (r, ω)dr) into our definition of ε(ω). Interestingly, equation (9) shows that scalar nonlocal response manifests itself through the Laplacian term in the wave equation, seemingly irrespective of the microscopic or semiclassical origin, and with a strength given by ξ , which relat ...
... of f (r, ω) (i.e. f (r, ω)dr) into our definition of ε(ω). Interestingly, equation (9) shows that scalar nonlocal response manifests itself through the Laplacian term in the wave equation, seemingly irrespective of the microscopic or semiclassical origin, and with a strength given by ξ , which relat ...
Theoretical treatment of miscellaneous frequency-shifts
... with classical perturbation theory The ideal Penning trap consists of a homogeneous magnetic field and an electrostatic quadrupole potential. In this configuration, the three characteristic eigenfrequencies of a trapped particle do not depend on its motional amplitudes from a classical point of view ...
... with classical perturbation theory The ideal Penning trap consists of a homogeneous magnetic field and an electrostatic quadrupole potential. In this configuration, the three characteristic eigenfrequencies of a trapped particle do not depend on its motional amplitudes from a classical point of view ...
Macroscopic Models of Superconductivity
... It is convenient in that it only involves H and not E, and is in fact nothing more than a one-phase ‘Stefan’ model [16], which is itself the simplest macroscopic model that could be written down for an evolving phase boundary in the classical theory of melting or solidification. In its simplest dime ...
... It is convenient in that it only involves H and not E, and is in fact nothing more than a one-phase ‘Stefan’ model [16], which is itself the simplest macroscopic model that could be written down for an evolving phase boundary in the classical theory of melting or solidification. In its simplest dime ...
Logical contradictions of Landau damping
... along the real axis without divergence of integrals, but with appearance their imaginary part. Besides that in the theory [2] there remains unresolved the paradox of inevitable simultaneous presence of the waves with exponentially damping and growing in x amplitudes, so one has attracted the ...
... along the real axis without divergence of integrals, but with appearance their imaginary part. Besides that in the theory [2] there remains unresolved the paradox of inevitable simultaneous presence of the waves with exponentially damping and growing in x amplitudes, so one has attracted the ...
Washabaugh, A.P. and M. Zahn, A Chemical Reaction-based Boundary Condition for Flow Electrification, IEEE Transactions on Dielectrics and Electrical Insulation, Vol. 4, No. 6, pp. 688-709, December, 1997
... A physical model is developed for the charge transfer boundary condition in semi-insulating liquids. The boundary condition is based upon interfacial chemical reactions and extends established relations for the interface by including the effects of interfacial surface charge and charge desorption at ...
... A physical model is developed for the charge transfer boundary condition in semi-insulating liquids. The boundary condition is based upon interfacial chemical reactions and extends established relations for the interface by including the effects of interfacial surface charge and charge desorption at ...