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Microwave One-way Transparency by Large Synthetic Motion of Magnetochiral Polaritons in Metamolecules

Kentaro Mita, Toshiyuki Kodama, Toshihiro Nakanishi, Tetsuya Ueda, Kei Sawada, Takahiro Chiba, Satoshi Tomita

Abstract

We observe microwave nonreciprocal one-way transparency via ultrastrongly-coupled magnetochiral polaritons (MChPs) in a metamolecule at room temperature. The experimental results using MCh metamolecules with simultaneous breaking of time-reversal and space-inversion symmetries are reproduced by numerical simulations. Based on effective polarizability tensor analyses, we verify massive synthetic motion of MChPs as an origin of the one-way transparency. This study paves a way to hybrid quantum systems and synthetic gauge fields using metamaterials.

Microwave One-way Transparency by Large Synthetic Motion of Magnetochiral Polaritons in Metamolecules

Abstract

We observe microwave nonreciprocal one-way transparency via ultrastrongly-coupled magnetochiral polaritons (MChPs) in a metamolecule at room temperature. The experimental results using MCh metamolecules with simultaneous breaking of time-reversal and space-inversion symmetries are reproduced by numerical simulations. Based on effective polarizability tensor analyses, we verify massive synthetic motion of MChPs as an origin of the one-way transparency. This study paves a way to hybrid quantum systems and synthetic gauge fields using metamaterials.

Paper Structure

This paper contains 4 figures.

Figures (4)

  • Figure 1: (a) A photo of the MCh metamolecule consisting of YIG magnetic meta-atom and Cu chiral meta-atom. A white bar corresponds to 5 mm. (b) Microwave measurement setup. The metamolecule is oriented along the $y$-axis in the WR-90 waveguide. A DC magnetic field $\mu_{0} H_{\rm ext}$ up to 500 mT is applied in the +$z$ direction using an electromagnet. (c) $x$-$y$ plane views of the metamolecule. The coil's endpoints are arranged to have 180-degree rotational symmetry with respect to the $x$-axis. (d) A cross-sectional view in the $x$-$y$ plane of the WR-90 waveguide. Red arrows correspond to the AC electric fields of the TE$_{10}$ mode.
  • Figure 2: (a) Measured $T^{+}$ (red) and $T^{-}$ (blue) spectra at various external DC magnetic fields, $\mu_{0} H_{\rm ext}$ of 0 - 500 mT. Black and white triangles indicate dips caused by Mie-coupled MChPs. (b) Numerically calculated $T^{+}$ (red) and $T^{-}$ (blue) spectra at various external DC magnetic fields of 0 - 500 mT. The phenomenological Gilbert damping parameter $\alpha$ is set to 0.004 in the calculation.
  • Figure 3: 2D plots of experimentally observed (a) $T^{-}$ and (b) $T^{+} - T^{-}$ of the $y$-axis-oriented metamolecule, and (c) $T^{-}$ and (d) $T^{+} - T^{-}$ of the $x$-axis-oriented metamolecule as a function of $\mu_{0} H_{\rm ext}$ (horizontal) and frequency (vertical).
  • Figure 4: Effective polarizabilities evaluated from numerical simulation of the $y$-axis-oriented metamolecule using $y$-polarized waves. Frequency versus extracted (a) $\alpha_{yy}^{\rm ee} \omega Z_0$ (red) and $\alpha_{xx}^{\rm mm} \omega Z_0^{-1}$ (blue), (b) $\alpha_{yy}^{\rm me} \omega$ (gold) and $\alpha_{xx}^{\rm em} \omega$ (cyan), (c) $\alpha_{xy}^{\rm ee} \omega Z_0$ (black) and $\alpha_{yx}^{\rm mm} \omega Z_0^{-1}$ (pink), (d) $\alpha_{yx}^{\rm em} \omega$ (green) and $\alpha_{xy}^{\rm me} \omega$ (purple). (e) MO and (f) moving effects of the $y$-axis-oriented metamolecules (blue) are compared with those of the $x$-axis-oriented metamolecules (red). Solid and dashed lines present real and imaginary parts, respectively. External magnetic field $\mu_{0} H_{\rm ext}$ is 400 mT.