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Anisotropic 2D materials for post-Moore photoelectric devices

Since the discovery of two-dimensional (2D) graphene[1], 2D materials have been widely investigated due to their intriguing physical/chemical property and outstanding optoelectronic performance[1−3]. Generally, 2D materials can be divided into… Click to show full abstract

Since the discovery of two-dimensional (2D) graphene[1], 2D materials have been widely investigated due to their intriguing physical/chemical property and outstanding optoelectronic performance[1−3]. Generally, 2D materials can be divided into isotropy and anisotropy according to crystal structures. For isotropic 2D materials like graphene and hexagonal boron nitride, they have obvious lattice symmetry. Whereas, anisotropic 2D materials possess strong anisotropic crystal structure (Fig. 1(a)), providing new degree of freedom for exploring 2D materials. Currently, 2D materials with high anisotropy, due to their anisotropic electrical, optical, thermal, and phonon properties, are finding applications in polarizationsensitive photodetection, neural network construction, spinpolarized transport and other emerging fields[3−6]. In layered 2D materials, the in-plane atoms are held together by strong covalent bonds, while different layers are stacked by weak van der Waals (vdW) forces[7]. 2D materials can be easily exfoliated from layered crystals, and present a large surface-to-volume ratio. Interestingly, anisotropic 2D materials possess excellent polarized photodetection abilities because of their intrinsic sensitivity to polarized light[8]. A novel polarization-sensitive photodetector based on anisotropic 2D materials has recently been proposed (Fig. 1(b)). In such devices, the laser is set to pass through a polarizer, and then the direction of incident light can be controlled by a halfwave plate. 2D anisotropy phototransistor can convert polarization characteristics into electrical signals. Such polarizationsensitive photodetectors will find applications in optical communication, near-field imaging, navigation, and military fields[7−9]. In 2020, Pi et al.[4] reported a highly sensitive polarized photodetector based on 2D palladium diselenide (PdSe2). PdSe2 not only possesses high room-temperature mobility and high air stability, but also has a puckered pentagonal structure with highly anisotropic properties, which gifts it advantages in polarization detection. The strong anisotropic photoelectric properties of 2D PdSe2 were revealed by azimuthdependent reflectance difference microscopy. The polarized photodetector presented excellent performance with dichroic ratios as high as ~2.2 at 369 nm and ~1.8 at 532 nm, respectively (Fig. 1(c)). Moreover, their primary polarization orientations differed by 90°, which is due to the characteristic difference between a-axis and b-axis. This phenomenon was ascribed to the inherent linear dichroism of PdSe2. Very recently, Li et al.[5] also demonstrated that PdSe2 photodetector possesses excellent polarization sensitivity and high stability. The phonon anisotropy of PdSe2 was confirmed by polarization-dependent Raman. Such polarization-sensitive photoresponse based on photothermoelectric effect was also demonstrated. These results indicate that anisotropic 2D materials can promote the development of next-generation high-performance polarized photodetection systems. Compared with traditional 2D materials, anisotropic 2D materials like black phosphorus, ReS2, and PdSe2 show strong anisotropy in their crystal structure and photoelectric property[4−8]. The related devices can offer a high intrinsic heterogeneity for information transmission. In biological synapses, the heterogeneity of synaptic connections is the basis for the diversity of neural activity[6]. The realization of heterogeneity in synaptic plasticity is very crucial for constructing high-complexity neural networks. Therefore, the setup based on anisotropic 2D materials can bring intrinsic heterogeneity into new-generation neuromorphic electronics. Tian et al.[6] realized the first anisotropic neuronal transistor based on black phosphorus. They used structure anisotropy of 2D materials to imitate the heterogeneity of synaptic behavior. The key characteristics of biological synapses were successfully emulated, such as long-term plasticity and spike-timing-dependent plasticity. More importantly, a simple axon-multi-synapse heterogeneity network was demonstrated. These devices can be regarded as the building blocks for future neuromorphic systems. Recently, Qin et al.[9] used 2D trigonal selenium (t-Se) nanosheet to make an anisotropic electrolyte-gated synaptic transistor (EGT) (Fig. 1(d)). t-Se is a one-dimensional vdW material, where Se atoms are covalently bonded along c-axis direction while stacked together along the perpendicular plane via vdW interactions. 2D t-Se nanosheets tend to crystallize in an irregular quadrilateral. In the EGT devices based on t-Se nanosheets, the synaptic weight variation and temporal filtering capability showed a strong anisotropic response because of the inherent heterogeneity of channel conductance. Moreover, the complex axon-multi-synapse system with heterogeneous signal-transmission ability was also realized in multiterminal EGT devices (Fig. 1(e)). For the same stimulus input, the system exhibited an anisotropic filtering behavior (Fig. 1(f)). The devices based on 2D anisotropic materials can be used to build heterogeneous artificial neural networks. Some isotropic 2D materials with special structures may

Keywords: pdse2; heterogeneity; anisotropy; polarization; structure; anisotropic materials

Journal Title: Journal of Semiconductors
Year Published: 2022

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