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Opaque perfect lenses

Graeme W. Milton·Nicolae-Alexandru P. Nicorovici·Ross C. McPhedran
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Abstract

The response of the ``perfect lens'', consisting of a slab of lossless material of thickness $d$ with $ε=μ=-1$ at one frequency $ω_0$ is investigated. It is shown that as time progresses the lens becomes increasingly opaque to any physical TM line dipole source located a distance $d_0<d/2$ from the lens and which has been turned on at time $t=0$. Here a physical source is defined as one which supplies a bounded amount of energy per unit time. In fact the lens cloaks the source so that it is not visible from behind the lens either. For sources which are turned on exponentially slowly there is an exact correspondence between the response of the perfect lens in the long time constant limit and the response of lossy lenses in the low loss limit. Contrary to the usual picture where the field intensity has a minimum at the front interface we find that the field diverges to infinity there in the long time constant limit.

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Graeme W. Milton, Nicolae-Alexandru P. Nicorovici, Ross C. McPhedran. 2006-11-25. Opaque perfect lenses. https://doi.org/10.1016/j.physb.2006.12.010

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