We introduce a nonreciprocal nongyrotropic magnetless metasurface. In
contrast to previous nonreciprocal structures, this metasurface does not
require a biasing magnet, and is therefore lightweight and amenable to
integrated circuit fabrication. Moreover, it does not induce Faraday rotation,
and hence does not alter the polarization of waves, which is a desirable
feature in many nonreciprocal devices. The metasurface is designed according to
a Surface-Circuit-Surface (SCS) architecture and leverages the inherent
unidirectionality of transistors for breaking time reversal symmetry.
Interesting features include transmission gain as well as broad operating
bandwidth and angular sector operation. It is finally shown that the
metasurface is bianisotropic in nature, with nonreciprocity due to the
electric-magnetic coupling parameters, and structurally equivalent to a moving
uniaxial metasurface
Light trapping and photon management of silicon thin film solar cells can be improved by a separate optimization of the front and back contact textures. A separate optimization of the front and back contact textures is investigated by optical simulations taking realistic device geometries into consideration. The optical simulations are confirmed by experimentally realized 1 μm thick microcrystalline silicon solar cells. The different front and back contact textures lead to an enhancement of the short circuit current by 1.2 mA/cm2 resulting in a total short circuit current of 23.65 mA/cm2 and an energy conversion efficiency of 8.35%.
A coupling matrix technique is presented for the synthesis of nonreciprocal lossless two-port networks. This technique introduces complex inverters to build the nonreciprocal transversal network corresponding to the nonreciprocal coupling matrix. It subsequently transforms this matrix into canonical topologies through complex similarity transformations. The complex inverters in the final topology are transformed into real inverters and gyrators for implementation simplicity. A secondorder example is then given to illustrate the proposed technique. Possible implementations of the gyrators involved in the final design are also discussed.
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