calculation of material properties in transformation mediaby radiofeda Tags: cloaking, electromagnetic wave, material properties, tensor 

#1
Apr2310, 02:41 AM

P: 5

Hi everybody,
I'm focusing on metamaterials. I have recently read Schurig's paper "Calculation of material properties and ray tracing in transformation media" (OPTICS EXPRESS, Vol. 14 (21), 97949804, OCT 16 2006, http://www.opticsinfobase.org/oe/abs...PEX14219794). In the article, the components of the permittivity tensor are given by [tex]\varepsilon^{i'j'} = \left\rm{det}(\Lambda^{i'}_{i})\right^{1} \Lambda^{i'}_{i} \Lambda^{j'}_{j} \varepsilon^{ij}[/tex] where the Jacobian matrix [tex] \Lambda_{\alpha}^{\alpha'} = \frac{\partial x^{\alpha'}}{\partial x^{\alpha}} [/tex] and the roman indices run from1 to 3, for the three spatial coordinates, as is standard practice. Working out the algebra, the components of the permittivity (permeability) tensor can be obtained by [tex] \left(\varepsilon^{i'j'}\right) = \left\rm{det}\left(\Lambda\right)\right^{1}\Lambda^T \Lambda [/tex] where [tex] \Lambda [/tex] is a matrix, which components are the counterpart of the contravariant coefficients [tex] \Lambda_{\alpha}^{\alpha'} [/tex]. For cylindrical cloak, the components of the transformation matrix are [tex] \left(\Lambda^{i'}_{j}\right) = \left( \begin{array}{ccc} \frac{\rho'}{\rho}\frac{ax^2}{\rho^3} & \frac{axy}{\rho^3} & 0 \\ \frac{ayx}{\rho^3} & \frac{\rho'}{\rho}\frac{ay^2}{\rho^3} & 0 \\ 0 & 0 & 1 \\ \end{array} \right) [/tex] It is easy to find the material properties. For instance, the z component of the permittivity tensor is [tex]\varepsilon_z = \varepsilon^{3,3} = \frac{\rho^2}{\rho'(\rho'a)} = \frac{1}{\left\rm{det}\left(\Lambda\right)\right}[/tex] However, in the paper "Fullwave simulations of electromagnetic cloaking structure" (PHYSICAL REVIEW E, 74, 036621 (2006), http://pre.aps.org/abstract/PRE/v74/i3/e036621), the components of the relative permittivity and permeability tensor specified in cylindrical coordinates are given [tex]\varepsilon_z = \mu_z = \left(\frac{b}{ba}\right)^2 \frac{\rhoa}{\rho}[/tex] It can be seen that the two formula are not equal obviously. And the other nonzero components of the permittivity and permeability tensor are not equal too. I have deduced the formulas for many times. Depressingly, I can not figure out the problem. Could somebody please give me some comments on the calculation of material properties in transformation optics. Regards. 



#2
Apr2310, 08:11 AM

Sci Advisor
P: 5,467

I just glanced through the papers, but I wonder if you are looking in the wrong place: see, for example, eqns 2022 and 2930 in the OE paper.




#3
Apr2310, 08:50 AM

P: 5




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