Developing wireless nanodevices and nanosystems is of critical importance for sensing, medical science, environmental/infrastructure monitoring, defense technology and even personal electronics.It is highly desirable for wireless devices to be self-powered without using battery.Nanogenerators (NGs) have been developed based on piezoelectric, trioboelectric and pyroelectric effects, aiming at building self-sufficient power sources for mico/nano-systems.The output of the nanogenerators now is high enough to drive a wireless sensor system and charge a battery for a cell phone, and they are becoming a vital technology for sustainable, independent and maintenance free operation of micro/nano-systems and mobile/portable electronics.An energy conversion efficiency of 55% and an output power density of 500 W/m 2 have been demonstrated.This technology is now not only capable of driving portable electronics, but also has the potential for harvesting wind and ocean wave energy for large-scale power application.This talk will focus on the updated progress in NGs.For Wurtzite and zinc blend structures that have non-central symmetry, such as ZnO, GaN and InN, a piezoelectric potential (piezopotential) is created in the crystal by applying a strain.Such piezopotential can serve as a "gate" voltage that can effectively tune/control the charge transport across an interface/junction; electronics fabricated based on such a mechanism is coined as piezotronics, with applications in force/pressure triggered/controlled electronic devices, sensors, logic units and memory.By using the piezotronic effect, we show that the optoelectronc devices fabricated using wurtzite materials can have superior performance as solar cell, photon detector and light emitting diode.Piezotronics is likely to serve as a "mechanosensation" for directly interfacing biomechanical action with silicon based technology and active flexible electronics.This lecture will focus on the updated progress in the field and its expansion to 2D materials.
The theory for the absorption potential (or optical potential) in electron diffraction was established many years ago by Yoshioka. However, few studies have been devoted to examining the approximations originally introduced when the potential was derived. In this paper, the absorption potential first proposed by Yoshioka is revised for dynamic electron diffraction with consideration of the effects arising from thermal diffuse scattering and point defect scattering. A rigorous theoretical proof is given to show that the inclusion of this “potential” in the dynamical calculation automatically recovers the contributions made by the high order diffuse scatter-ing, although the calculation is done using the equation derived for single diffuse scattering. If Yoshioka’s approximation is made, i.e., the Green’s function is replaced by its form in freespace, then the inclusion of the optical potential in dynamical calculations still recovers the multiple diffuse scattering terms except the dynamic Bragg reflection after each diffuse scattering event. This conclusion establishes the basis for expanding the conventional diffraction theories developed under the first order diffuse scattering approximation to cases where the specimen thickness is large and the degree of disorder is high. It has been shown that the “optical potential” depends also on the structure of the crystal. The Fourier coefficients of this function are given in the Bloch wave representation for transmission electron diffraction.