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. 2025 Jul 9;16(1):6340.
doi: 10.1038/s41467-025-61536-0.

PZT optical memristors

Affiliations

PZT optical memristors

Chenlei Li et al. Nat Commun. .

Abstract

Optical memristors represent a monumental leap in the fusion of photonics and electronics for neuromorphic computing and artificial intelligence. Here, we reveal the first lead zirconate titanate (PZT) optical memristor, working with a paradigm of functional duality: non-volatile setting and ultrafast volatile modulation via the Pockels effect. Fine-tuning and large modulation depth are achieved with an index change of 4.6 × 10-3 when setting above a threshold voltage Vth and the switching energy is 12.3 pJ only. The non-volatility is highly stable even with >100,000 cycles. Sub-nanosecond volatile modulation (48 Gbps, 432 fJ/bit) is realized with high efficiency (VπL ~ 0.5 V·cm) via the strong Pockels effect below Vth. Our wafer-scale manufacturing process shows great potential for mass production. The present PZT optical memristors bridge the gap between high-speed photonics and non-volatile memory, offering transformative potential for high-speed and energy-efficient optical interconnects, quantum computing, neural networks, in-memory computing, and brain-like architecture.

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Conflict of interest statement

Competing interests: The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. PZT optical memristor.
a Wafer-scale sol-gel fabrication processes of PZT Optical Memristors. b Photograph of the spin-coating wafer. c Scanning electron microscopy (SEM) picture of the top view of the thin-film PZT (thickness~ 300 nm). d AFM image of the thin-film PZT. e Photograph of a 4-inch wafer patterned by using an ultraviolet stepper lithography system. f Colorized SEM of PZT MRR (blue). g SEM picture of the cross-section of a PZT ridge waveguide. h Simulated field distribution for the TE0 mode. i PZT unit cell representation before and after poling. j Schematic diagram of the ridge waveguide cross-section and the poling process. k The dependence of the refractive index changes ∆neff (Pν) against the net ferroelectric domain polarization, and the corresponding simplified top-view schematic of ferroelectric domains in PZT.
Fig. 2
Fig. 2. MRR-based PZT optical memristor.
a Optical microscopy image of an MRR with a bending radius of 60 μm. b Single-cycle demonstration of one distinct non-volatile state. c Measured transmissions at the through port of the MRR-based PZT optical memristor with different setting voltages Vset. d Measured resonance-wavelength detuning of the MRR-based PZT optical memristor set with different setting voltages Vset as the driving voltage Vdr varies. e Eye diagrams for NRZ modulation at the data rate of 48 Gbps with a driving voltage Vdr of 3 V.
Fig. 3
Fig. 3. The present MZI-based PZT optical memristors.
a Schematic of the MZI -based 2 × 2 PZT optical memristors, consisting of two imbalanced arms with 1-mm-long phase shifters and two 2 × 2 multimode interferometers with a splitting ratio of 50%: 50%; the purple arrow represents the direction of the poling electric field; the blue arrow represents the direction of the applied drive voltage Vdr. b Optical microscopy image of the fabricated 2 × 2 MZI optical memristors. c Non-volatile tuning of the wavelength notch with the setting voltage Vset varying from 8 V to 32 V. Before the setting voltage is applied to set any state, this optical memristor was re-initialized by applying a high poling voltage Vpol of 80 V. d Real-time optical modulation measurements. Normalized output intensity from the through port when the device operates with a drive voltage Vdr of 4 Vpp at the frequency of 10 MHz. The upper one represents the input electrical signals, and the bottom one represents the switched optical signals. e Measured transmissions at the cross port when operating with Vdr = 0 and 5.0 V, respectively.
Fig. 4
Fig. 4. The present FP-cavity-based PZT optical memristor.
a Schematic configuration. MWGs, multimode waveguide gratings, Modemux, mode multiplexers. b Optical microscopy image of the fabricated device. c Measured transmission spectral responses at the through port with different setting voltages Vset. d Extracted resonance wavelength shifts (detuning with 1559.2 nm) versus different setting voltages Vset. e Five distinct non-volatile states correspond to the setting voltages Vset of 30, 21, 23, 25, and 36 V. For each non-volatile state, there are 20 cycles measured for the resonance-wavelength detuning. f Time domain measurements after 10 and 10000 cycles, showing that the optical memristor operates well without any degradation. s. Real-time optical modulation measurements: gj Normalized output optical intensity at the through port when operating with rectangular driving-voltage signals (Vdr=4Vpp) at the frequency of 1 Hz (g), 100 kHz (h), and 5 MHz (i). j The rising/falling edge of the switched optical signals. k Measured spectral responses at the through port of the FP cavity when operating with different driving voltages Vdr of −1, 0, and +1 V, respectively.
Fig. 5
Fig. 5. Examples of multifunctional photonic circuits enabled by scalable PZT optical memristors.
a Optical microscopy image of the 4 × 4 optical switch. b Chart of the measured transmissions from the input ports (I1, I2, I3, and I4) to the output ports (O1, O2, O3, and O4) at the initial state with random phase errors. ce Chart of the measured transmissions from the input ports (I1, I2, I3, and I4) to the output ports (O1, O2, O3, and O4) when all the 2 × 2 MZI switches are reconfigured with the desired optical routines (as defined by configurations #1, #2 and #3) by applying the appropriate setting voltages. f Measured eye diagrams for the optical signals propagating along the routines (I1-O2, I2-O1, I3-O3, I4-O4) as defined by configuration #3. FP-cavity-based PZT optical memristors in cascade for adaptive memristive spectral manipulation: (g) Schematic configuration; (h) Optical microscopy image of the fabricated device; (i) Measured transmission spectra at the through ports for the initial state without any correction; (j) Measured transmission spectra at the through/cross ports when the resonance wavelength of each FP cavity was aligned carefully to have uniform channel spacing by applying the corresponding setting voltage Vset; (k) Measured transmission spectra at the through/cross ports when channels #1 and #3 are erased and retrospectively set so that their resonance wavelengths are respectively aligned with channels #2 and #4.
Fig. 6
Fig. 6. Part of the potential applications in the Future.
PZT optical memristors enable compact wavelength-division-multiplexed optical interconnects, microwave photonics, neural networks, and LiDAR by combining volatile high-speed modulation (below Vth) and non-volatile trimming (Vset).

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