Non-volatile phase-change materials (PCMs) provide a promising material platform to design reconfigurable electro-optic devices. However, for PCM-based spatial light modulators, electro-optic switching of material phases by a voltage pulse is generally affected by the filamentation effect. An alternative way to induce phase transition and reversible modulation is by on-chip micro-heaters, whereas these microheaters can only reflect light where noble metals are generally used as thermal resists. Moreover, the corresponding power consumption is very high because most heat energy dissipates into substrates, preventing the compact integration of PCM-based micro-modulators into the miniaturized and reconfigurable optical chip-array systems. Here, we propose a PCM electro-optical modulator working on the transmission mode with MEMS microheaters. The heating circuit is fabricated on a 200-nm-thick free-standing Si3N4 film, and transparent conductive oxides are used as thermal resists to allow light transmission. According to multi-physics simulations, the proposed MEMS modulators can make a thermal hotspot up to 400 °C in just 100 μs at 2 V bias voltage, indicating low power consumption. Meanwhile, by changing the phase state of PCM from amorphous to crystalline, the mid-infrared light transmission can switch from 0.71 to near zero in the mid-infrared range. The proposed MEMS modulators could inspire new applications in reconfigurable phase-change nanophotonics.
A low-loss and compact TM-pass polarizer is demonstrated based on improved hybrid plasmonic grating (HPG) on a Z-cut lithium-niobate-on-insulator (LNOI) platform. In this work, we introduced the silica partition structures surrounding an LN (LiNbO3) ridge waveguide to support two parallel metal gratings, achieving the optimal coupling coefficient for HPG. Compared with the traditional HPG structure, the transverse electric (TE) mode suffers a higher confinement and the transverse magnetic (TM) mode transmission loss exhibits a significant reduction in the improved HPG structure. The simulation shows that the polarizer achieves a broad bandwidth of 150 nm (1500 to 1650 nm) with an extinction ratio (ER) over 20 dB and an insertion loss varying from 0.18 to 0.3 dB, including a maximum ER of 36 dB at the wavelength 1550 nm. In addition, the length of the demonstrated polarizer is only 10 μm, making it compact for integration. The proposed polarizer shows a good application prospect for integrated photonics in LNOI.
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