Light-gated amorphous carbon memristors with indium-free transparent electrodes
Graphical abstract
Introduction
Bio-inspired memory and neuromorphic systems are the subject of an intensive research effort to alleviate the well-known bottleneck in von Neumann computing [[1], [2], [3]]. In 2008, the memristor was announced by HP labs as the key component in such systems and has since been touted as enabling low power, non-volatile and parallel computing [4,5]. Further ambitions to integrate memristors with high-speed photonic circuitry have also been proposed [6]. The key challenge is to be able to write electronic memory and perform computations by photonic stimulation.
On-chip optoelectronic memory devices offer extended functionality including heterogeneous-input logic operations [7], high-speed/bandwidth signal transmission [8,9], ‘non-contact’ data writing [10] and the implementation of neuromorphic learning/memory functions [[11], [12], [13]]. The advent of optogenetics is also enabling the next generation of neuroscience discoveries using photonic excitation of neurons in place of electronic stimulus [14] and optogenetic methods, in turn, have already been utilised in memristive devices to alter their emulated synaptic plasticity/memory [15].
The majority of memristor research to-date has focused on metal oxide-based devices, which operate either by the electric field-induced migration of itinerant dopants (vacancies or impurities) to form conducting pathways [16,17] or by the trapping/de-trapping of charge carriers in non-itinerant defect states [18,19]. However, several reports have emerged on carbon-based devices that can operate by similar mechanisms [[20], [21], [22], [23], [24], [25], [26]] and they have since been included in the International Technology Roadmap for Semiconductors (ITRS) [27]. Amorphous carbon, in particular, has attracted interest due to its elemental nature, reproducibility, biocompatibility and widely tunable optical/electronic properties [[28], [29], [30]]. While photonic transduction has been reported for several metal oxide-based memristors, optical-writing of amorphous carbon memory devices has yet to be achieved.
In this paper, we report on the fabrication and characterisation of light-gated amorphous carbon memristors. Several neuromorphic functions are demonstrated with the devices. An indium-free transparent electrode is used as a low-cost window layer. Amorphous zinc tin oxide (ZTO) was chosen due to its high transparency and tunable electronic properties [31,32]. Both the active carbon layers and the ZTO electrodes were energetically deposited by filtered cathodic vacuum arc (FCVA). Energetic deposition by FCVA allows dense, well adhered, high quality coatings to be formed at moderate growth temperatures and has previously been used to fabricate optical/electronic devices using the aforementioned materials [33].
Section snippets
Experimental
ZTO films were formed on a-plane sapphire at 150 °C and at floating potential by FCVA using a ZnSn metal cathode. The process pressure was 2.0 mTorr (1.3 mTorr O2, 0.6 mTorr Ar). The films were subsequently annealed in air for 1 h at 375 °C. This method has been shown previously to decrease the electrical resistivity (from >300 Ωcm to 0.2 Ωcm) [31] and the mechanism will be further discussed below. A 7 nm oxygenated amorphous carbon (a-COx) layer followed by a 25 nm layer of tetrahedral
Results and discussion
Fig. 1(a) shows the I–V characteristics of a ZTO/ta-C/Pt memristor (with the ZTO positively biased in the forward direction). No electroforming step was performed. Some hysteresis is observed in the forward bias direction. Resistive switching in the insulating regime, that is below one conductance quantum (≪ 2e2/h), in amorphous carbon-based memristors is due to the trapping/de-trapping of electrons by shallow charged defect states [34]. The empty traps screen the electric field in the high
Conclusion
In summary, a-COx/ta-C bilayer amorphous carbon memristors have been interfaced with transparent, indium-free ZTO electrodes to enable both photonic and electronic stimulation. The devices operate based on charge trapping/de-trapping from localised sp2 states and are self-rectifying due to the Schottky barrier created at the ZTO/a-COx interface. Programming is possible by either optical or electronic methods and the memory state can be actively erased electronically. PPF can also be evoked both
Acknowledgements
The authors gratefully acknowledge the Australian Research Council for financial support (Discovery Project # DP170102086). The authors also acknowledge the RMIT microscopy and microanalysis facility for granting instrument access. This work was performed in part at the Australian National Fabrication Facility, a company established under the National Collaborative Research Infrastructure Strategy, through the La Trobe University Centre for Materials and Surface Science.
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