Ultrasensitive optical sensing based on non-Hermitian metasurfaces

We present here an ultrasensitive optical sensing technique based on the parity-time (PT)-symmetric non-Hermitian metasurfaces. The system is composed of a pair of active and passive metasurfaces with the subtle gain-loss balance. Specifically, these two metasurfaces are made of the photoexcited, nanopatterned 2D material (gain) and the lossy metallic structure (i.e., loss). By suitably tailoring the impedance profiles of the PT-symmetric metasurfaces, the system can exhibit an exotic point where the coherent perfect absorption (CPA) and lasing could occur at the same wavelength, switchable via tuning the complex amplitude of incoming light. At this point, tiny perturbation in the effective optical impedance could drastically vary eigenvalues of the scattering matrix, leading to greatly modulated scattering coefficients and output factor, well beyond conventional optical sensors. Our results show that the proposed PTsymmetric metasurfaces may enable ultrasensitive optical sensors for detecting low-density chemical, gas and molecular agents, as well as refractive-index sensing of a nanofilm.

[1]  Stefano Longhi,et al.  PT-symmetric laser absorber , 2010, 1008.5298.

[2]  M. Ryzhii,et al.  Emission and Detection of Terahertz Radiation Using Two-Dimensional Electrons in III–V Semiconductors and Graphene , 2013, IEEE Transactions on Terahertz Science and Technology.

[3]  Z. Musslimani,et al.  Theory of coupled optical PT-symmetric structures. , 2007, Optics letters.

[4]  Pai-Yen Chen,et al.  Superluminal plasmons with resonant gain in population inverted bilayer graphene , 2017, Physical Review B.

[5]  Tianjing Guo,et al.  Tunable terahertz amplification based on photoexcited active graphene hyperbolic metamaterials [Invited] , 2018, Optical Materials Express.

[6]  R. Morandotti,et al.  Observation of PT-symmetry breaking in complex optical potentials. , 2009, Physical review letters.

[7]  Taiichi Otsuji,et al.  Carrier-carrier scattering and negative dynamic conductivity in pumped graphene. , 2014, Optics express.

[8]  M. Segev,et al.  Observation of parity–time symmetry in optics , 2010 .

[9]  Yuang Wang,et al.  Lasing and anti-lasing in a single cavity , 2016, Nature Photonics.

[10]  Pai-Yen Chen,et al.  P T Symmetry and Singularity-Enhanced Sensing Based on Photoexcited Graphene Metasurfaces , 2016 .

[11]  Z. Musslimani,et al.  Beam dynamics in PT symmetric optical lattices. , 2008, Physical review letters.

[12]  S. Longhi,et al.  Bloch oscillations in complex crystals with PT symmetry. , 2009, Physical review letters.

[13]  University of Central Florida,et al.  Unidirectional nonlinear PT-symmetric optical structures , 2010, 1005.5189.

[14]  Min-Hsiu Hsieh,et al.  Local PT symmetry violates the no-signaling principle. , 2013, Physical review letters.