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Surface plasmon polaritons (SPPs) are coherent electron-plasma oscillations at the interface of materials with opposite dielectric functions. The excitation and propagation of these polariton modes are strongly affected by material dispersion, geometric behaviour and the excitation frequency. In this paper, we studied the excitation of SPPs at metal/lithium niobate (ferroelectric) interfaces and their dispersion characteristics. The plasmonic waveguides with Ag/LiNbO.sub.3 interfaces provide the coupling of ferroelectric properties in to plasmon modes. We observed a marked propagation length, and both geometrical and material dispersion properties which ensure a sensitive plasmonic system operating at plasmon frequencies.

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Topological refractions created by valley sonic crystals (VSCs) have attracted great attentions in the communities of physics and engineering owing to the advantage of zero reflection of sound and the potential for designing advanced acoustic devices. In previous works, topological refractions of valley edge states are demonstrated to be determined by the projections of the valleys K and K7, and two types of topological refractions generally exist at opposite terminals or different frequency bands. However, the realization of tunable topological refractions at the fixed frequency band and terminal still poses great challenge. To overcome this, we report the realization of tunable topological refractions by VSCs with triple valley Hall phase transitions. By simply rotating rods, we realize 3 types of topological waveguides (T1, T2, and T3) composed of two VSCs, in which the projections of the observed valley edge states can be modulated between K and K. Additionally, based on the measured transmittance spectra, we experimentally demonstrate that these valley edge states are almost immune to backscattering against sharp bends. More importantly, we realize tunable topological refractions at the fixed frequency band and terminal, and experimentally observe the coexistence of positive and negative refractions for T1 and T3, and negative refractions for T2. The proposed tunable topological refractions have potential applications in designing multi-functional sound antennas and advanced communication devices.

The nonlocal emitter-waveguide coupling, which gives birth to the so called giant atom, represents a new paradigm in the field of quantum optics and waveguide QED. We investigate the single-photon scattering in a one-dimensional waveguide on a two-level or three-level giant atom. Thanks to the natural interference induced by the back and forth photon transmitted/reflected between the atom-waveguide coupling points, the photon transmission can be dynamically controlled by the periodic phase modulation via adjusting the size of the giant atom. For the two-level giant-atom setup, we demonstrate the energy shift which is dependent on the atomic size. For the driven three-level giant-atom setup, it is of great interest that, the Autler-Townes splitting is dramatically modulated by the giant atom, in which the width of the transmission valleys (reflection range) is tunable in terms of the atomic size. Our investigation will be beneficial to the photon or phonon control in quantum network based on mesoscopical or even macroscopical quantum nodes involving the giant atom. Keywords giant atom, single-photon scattering, quantum interference, Autler-Townes splitting

This paper presents the design of an optical transport architecture for the fronthaul segment in a 5G New Radio (NR) network based on both polarization and wavelength multiplexing using Polarization Splitters (PS) and an Arrayed Waveguide Grating (AWG), respectively. The proposed architecture is assessed by the transport of Orthogonal Frequency Division Multiplexing (OFDM) services, which allows the definition of different numerologies and service profiles; those are key aspects in the framework of 5G RN. The proposed design shows a flexible and scalable management of numerologies per polarized light component, featuring a suitable response in terms of Bit Error Rate (BER) and Error Vector Magnitude (EVM) measurements for 15 kHz, 30 kHz, and 60kHz subcarrier spacing of an OFDM based on 4QAM modulation format.

Pattern recognition of optical label is utilized not only in packet switches but also in the field of data security due to its wide range of applications. In particular, pattern recognition using waveguide devices is highly valued because it eliminates the need for encoder processing. However, existing methods suffer from the problem of degraded contrast ratio because half of the input power are emitted from non‐target waveguides. In this article, a method is proposed to improve the contrast ratio employing a 4× $\\times$ 4 multi‐mode interference (MMI) coupler with multiple input signals. The theoretical results reveal that the proposed method improves the contrast ratio from 3.0 dB to 9.5 dB and ∞ $\\infty$dB for the three‐input and four‐input cases, respectively, for quadrature phase‐shift keying (QPSK)‐modulated signal. Furthermore, numerical simulation was performed through the three dimension finite‐difference time‐domain (3D‐FDTD) method, and the proposed scheme successfully discriminated each QPSK pattern. The power value |E|2 $|E|^2$at all ports closely matches the theoretical value, and the ratios of 9.5 dB and > $>$ 30.0 dB are numerically obtained. This article introduces a novel method to enhance contrast ratio in optical label pattern recognition, crucial for packet switches and data security. By employing a 4× $\\times$ 4 multi‐mode interference coupler with multiple input signals, the proposed approach significantly improves contrast ratio, theoretically from 3.0 dB to 9.5 dB and infinitely for certain cases. Numerical simulations confirm its efficacy, demonstrating successful discrimination of QPSK patterns with results closely matching theoretical predictions.