Strain engineering is a promising method to manipulate the electronic and optical properties of two-dimensional (2D) materials. However, with weak van der Waals interaction, severe slippage between 2D material and substrate could dominate the bending or stretching processes, leading to inefficiency strain transfer. To overcome this limitation, we report a simple strain engineering method by encapsulating the monolayer 2D material in the flexible PVA substrate through spin-coating approach. The strong interaction force between spin-coated PVA and 2D material ensures the mechanical strain can be effectively transferred with negligible slippage or decoupling. By applying uniaxial strain to monolayer MoS 2 , we observe a higher bandgap modulation up to~300 meV and a highest modulation rate of~136 meV/%, which is approximate two times improvement compared to previous results achieved. Moreover, this simple strategy could be well extended to other 2D materials such as WS 2 or WSe 2 , leading to enhanced bandgap modulation.

Two-dimensional (2D) Ruddlesden-Popper perovskites are currently drawing significant attention as highly-stable photoactive materials for optoelectronic applications. However, the insulating nature of organic ammonium layers in 2D perovskites results in poor charge transport and limited performance. Here, we demonstrate that Al 2 O 3 /2D perovskite heterostructure can be utilized as photoactive dielectric for high-performance MoS 2 phototransistors. The type-II band alignment in 2D perovskites facilitates effective spatial separation of photo-generated carriers, thus achieving ultrahigh photoresponsivity of >10 8 A/ W at 457 nm and >10 6 A/W at 1064 nm. Meanwhile, the hysteresis loops induced by ionic migration in perovskite and charge trapping in Al 2 O 3 can neutralize with each other, leading to low-voltage phototransistors with negligible hysteresis and improved bias stress stability. More importantly, the recombination of photo-generated carriers in 2D perovskites depends on the external biasing field. With an appropriate gate bias, the devices exhibit wavelengthdependent constant photoresponsivity of 10 3-10 8 A/W regardless of incident light intensity.

The emerging Ruddlesden−Popper two-dimensional perovskite (2D PVK) has recently joined the family of 2D semiconductors as a potential competitor for building van der Waals (vdW) heterostructures in future optoelectronics. However, to date, most of the reported heterostructures based on 2D PVKs suffer from poor spectral response that is caused by intrinsic wide bandgap of constituting materials. Herein, a direct heterointerface bandgap (∼0.4 eV) between 2D PVK and ReS 2 is demonstrated. The strong interlayer coupling reduces the energy interval at the heterojunction region so that the heterostructure shows high sensitivity with the spectral response expanding to 2000 nm. The large type-II band offsets exceeding 1.1 eV ensure fast photogenerated carriers separation at the heterointerface. When this heterostructure is used as a self-driven photodetector, it exhibits a record high detectivity up to 1.8 × 10 14 Jones, surpassing any reported 2D selfdriven devices, and an impressive external quantum efficiency of 68%.

No abstract

Since the continuous scaling down of the transistor channel length, extraordinary improvement is achieved in the switching speed. However, the rising leakage current degrades the power consumption seriously. In this regard, reducing supply voltage might be the most effective method. This requirement can be fulfilled well by tunnel field‐effect transistors (TFETs), because carriers transport via a band‐to‐band tunneling manner in the TFETs. Relying on the special transport mechanism, the TFETs often require band structure modulations and steep interfaces without trap state, which are challenging for bulk materials. Therefore, these challenges have boosted TFET designs based on low‐dimensional materials ranging from Si/Ge nanowires to state‐of‐art van der Waals heterostructures. Here, the key concepts of the currently developed TFETs are studied from the aspects of structure, material, transportation characteristic, and mechanism. According to the heterojunction bonding types, they can be divided into lateral and vertical TFETs in general. Furthermore, other related transistors based on tunneling are also included. Emerging problems and promotion methods toward these TFETs are introduced with the assistance of simulations. The main goal is to introduce the frontiers of TFET explorations and provide readers with a perspective on how to realize TFET applications in the future.