ABSTRACT
Different size InGaN/GaN based micro-LEDs (µLEDs) are fabricated. An extremely high injection level above 16 kA/cm2 is achieved for 10 µm-diameter LED. The lateral current density and carrier distributions of the µLEDs are simulated by APSYS software. Streak camera time resolved photoluminescence (TRPL) results show clear evidence that the band-gap renormalization (BGR) effect is weakened by strain relaxation in smaller size µLEDs. BGR affects the relaxation of free carriers on the conduction band bottom in multiple quantum wells (MQWs), and then indirectly affects the recombination rate of carriers. An energy band model based on BGR effect is made to explain the high-injection-level phenomenon for µLEDs.
ABSTRACT
Mo-doped VO(2) nanowire array film with good thermochromic properties was prepared by melting-quenching followed by heat treatment in a vacuum. The formation of the new microstructure is related to the cleavage of the oxide lamella along (001) and (100) plane with large interplanar spacing. Mo doping results in the loss of V(4+)-V(4+) pairs and destabilizes the semiconductor phase and consequently lowers the semiconductor-to-metal transition temperature T(c) from 64 to 42 degrees C. Because of enhancement of the electron concentration due to the presence of Mo donors, the Fermi level shifts toward the conduction band, resulting in the decrease of activation energy E(a), hence, temperature coefficient of resistance.
ABSTRACT
Monoclinic NH(4)V(3)O(8) single-crystalline nanobelts with widths of 80-180 nm, thicknesses of 50-100 nm, and lengths up to tens of micrometers have been synthesized at large scale in an ammonium metavanadate solution by a templates/catalysts-free route. Such nanobelts grow along the direction of [010]. The individual NH(4)V(3)O(8) nanobelt exhibits nonlinear, symmetric current/voltage (I/V) characteristics, with a conductivity of 0.1-1 S/cm at room temperature and a dielectric constant of approximately 130. The dominant conduction mechanism is based on small polaron hopping due to ohmic mechanism at low electric field below 249 V/cm due to Schottky emission at medium electric field between 249 and 600 V/cm and due to the Poole-Frenkel emission mechanism at high field above 600 V/cm.
