Photonics Research, 2019, 7 (8): 08000862, Published Online: Jul. 17, 2019  

Exceptional points of any order in a single, lossy waveguide beam splitter by photon-number-resolved detection Download: 587次

Author Affiliations
1 Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Apartado Postal 70-543, 04510 Cd. Mx., Mexico
2 Max-Born-Institut, Max-Born-Straße 2A, 12489 Berlin, Germany
3 Humboldt-Universität zu Berlin, Institut für Physik, AG Theoretische Optik & Photonik, D-12489 Berlin, Germany
4 Tecnológico de Monterrey, Escuela de Ingeniería y Ciencias, Ave. Eugenio Garza Sada 2501, 64849 Monterrey, N.L., Mexico
5 Instituto Nacional de Astrofísica, Óptica y Electrónica, Calle Luis Enrique Erro No. 1, Sta. Ma. Tonantzintla, Pue. CP 72840, Mexico
6 Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA
7 Department of Physics, Indiana University Purdue University Indianapolis (IUPUI), Indianapolis, Indiana 46202, USA
8 e-mail: yojoglek@iupui.edu
9 e-mail: roberto.leon@nucleares.unam.mx
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Fig. 1. (a) Schematic of a single, lossy waveguide beam splitter excited with N indistinguishable photons prepared in the state |m)|Nm,m=|Nma|mb, where a represents the neutral (gray) waveguide and b is the lossy (red) waveguide. (b) Mapping onto the N-photon subspace spanned by (N+1) multiphoton states |m), represented as a tight-binding lattice model. The coupling between adjacent “modes” is given by matrix elements of J^x; the linearly increasing loss is also shown. (c) Flow of eigenvalues of H^N for N=4. R(λr) shows level attraction with an EP of order five at Γ=2κ; I(λr) shows the emergence of slow modes past the transition. (d) Intensity I(z) shows the fraction of trials where the system remains in the N-photon subspace, i.e., the post-selection probability. It reflects the order of the exceptional point. The beam splitter parameters are ω0=κ=1  cm1, and the initial state is |ψ(0)=|0).

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Fig. 2. Evolution of spin-projections Jr for the N+1 eigenmodes in the post-selected manifold with N=4 (left column) and N=5 (right column) photons, considering different values of the dissipation coefficient: (a), (b) Γ=Γc/2, (c), (d) Γ=0.99Γc, and (e), (f) Γ=1.5Γc. The vector coordinates in the (Jx,Jy,Jz) space are defined by the expectation values of the J^α operators in each eigenstate. When Γ<Γc, the spin projections are in the xy plane; at the EP, they coalesce along the positive y axis; and when Γ>Γc, they are in the xz plane.

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Fig. 3. Mode occupation dynamics in the post-selected manifold with NOON state input. (a) For N=5 and small loss, the dynamics show asymmetric oscillations. (b) At the EP, P(|m),z) reaches a steady state with most of the weight localized in the low-loss region. (c) After the transition, the steady-state is reached more slowly. (d)–(f) show qualitatively similar results for an N=8 NOON state input. The waveguide beam splitter parameters are set to ω0=κ=1  cm1.

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Mario A. Quiroz-Juárez, Armando Perez-Leija, Konrad Tschernig, Blas M. Rodríguez-Lara, Omar S. Magaña-Loaiza, Kurt Busch, Yogesh N. Joglekar, Roberto de J. León-Montiel. Exceptional points of any order in a single, lossy waveguide beam splitter by photon-number-resolved detection[J]. Photonics Research, 2019, 7(8): 08000862.

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