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Electric and magnetic losses and gains in determining the sign of refractive index
Authors:Jingsong Wei  Mufei Xiao  
Affiliation:

aShanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China

bCentro de Ciencias de la Materia Condensada, Universidad Nacional Autónoma de México, Apartado Postal 2681, CP 22800 Ensenada, Baja California, Mexico

Abstract:
Within the framework of classic electromagnetic theories, we have studied the sign of refractive index of optical medias with the emphases on the roles of the electric and magnetic losses and gains. Starting from the Maxwell equations for an isotropic and homogeneous media, we have derived the general form of the complex refractive index and its relation with the complex electric permittivity and magnetic permeability, i.e. View the MathML source, in which the intrinsic electric and magnetic losses and gains are included as the imaginary parts of the complex permittivity and permeability, respectively, as epsilon (Porson) = epsilon (Porson)r + iepsilon (Porson)i and μ = μr + iμi. The electric and magnetic losses are present in all passive materials, which correspond, respectively, to the positive imaginary permittivity and permeability epsilon (Porson)i > 0 and μi > 0. The electric and magnetic gains are present in materials where external pumping sources enable the light to be amplified instead of attenuated, which correspond, respectively, to the negative imaginary permittivity and permeability epsilon (Porson)i < 0 and μi < 0. We have analyzed and determined uniquely the sign of the refractive index, for all possible combinations of the four parameters epsilon (Porson)r, μr, epsilon (Porson)i, and μi, in light of the relativistic causality. A causal solution requires that the wave impedance be positive Re{Z} > 0. We illustrate the results for all cases in tables of the sign of refractive index. One of the most important messages from the sign tables is that, apart from the well-known case where simultaneously epsilon (Porson) < 0 and μ < 0, there are other possibilities for the refractive index to be negative n < 0, for example, for epsilon (Porson)r < 0, μr > 0, epsilon (Porson)i > 0, and μi > 0, the refractive index is negative n < 0 provided μi/epsilon (Porson)i > μr/midepsilon (Porson)rmid.
Keywords:78.20.Ci   41.20.Jb   42.25.Bs
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