Room-Temperature Ferromagnetic Wide Bandgap Semiconducting Fluorinated Graphene-hBN Vertical Heterostructures

2021 ◽  
pp. 100547
Author(s):  
Krishna Rani Sahoo ◽  
Rahul Sharma ◽  
Sumit Bawari ◽  
S. Vivek ◽  
Pankaj Kumar Rastogi ◽  
...  
2021 ◽  
Vol 2021 (HiTEC) ◽  
pp. 000013-000017
Author(s):  
Emad Andarawis ◽  
Cheng-Po (Paul) Chen ◽  
Baokai Cheng

Abstract A high temperature optical link capable of multi-megabits per second data rates at 300°C is presented. The system utilizes wide bandgap optical sources and detectors to achieve extreme temperature operation. Testing was conducted at multiple temperatures between room temperature and 325°C and at multiple light source currents. Light coupling into and out of a UV capable optical fiber was evaluated, and a model was created utilizing the test data of the photodiode dark current and the fiber optic cable insertion loss and attenuation and assess optical communications capability to 325°C and beyond.


2003 ◽  
Vol 1 (2) ◽  
pp. 213-218
Author(s):  
M. Godlewski ◽  
J. Szmidt ◽  
A. Olszyna ◽  
A. Werbowy ◽  
E. Łusakowska ◽  
...  

Science ◽  
2020 ◽  
Vol 367 (6477) ◽  
pp. 555-559 ◽  
Author(s):  
Ke Chen ◽  
Bai Song ◽  
Navaneetha K. Ravichandran ◽  
Qiye Zheng ◽  
Xi Chen ◽  
...  

Materials with high thermal conductivity (κ) are of technological importance and fundamental interest. We grew cubic boron nitride (cBN) crystals with controlled abundance of boron isotopes and measured κ greater than 1600 watts per meter-kelvin at room temperature in samples with enriched 10B or 11B. In comparison, we found that the isotope enhancement of κ is considerably lower for boron phosphide and boron arsenide as the identical isotopic mass disorder becomes increasingly invisible to phonons. The ultrahigh κ in conjunction with its wide bandgap (6.2 electron volts) makes cBN a promising material for microelectronics thermal management, high-power electronics, and optoelectronics applications.


1994 ◽  
Vol 358 ◽  
Author(s):  
Fereydoon Namavar ◽  
F. Lu ◽  
C.H. Perry ◽  
A. Cremins ◽  
N.M. Kalkhoran ◽  
...  

ABSTRACTWe have demonstrated a strong, room-temperature, 1.54 μm emission from erbium-implanted at 190 keV into red-emitting porous silicon. Luminescence data showed that the intensity of infrared (IR) emission from Er implanted porous Si annealed at ≤ 650°C, was a few orders of magnitude stronger than Er implanted quartz produced under identical conditions, and was almost comparable to IR emission from In0.53Ga0.47As material which is used for commercial IR light-emitting diodes (LEDs).The strong IR emission (much higher than Er in quartz) and the weak temperature dependency of Er in porous Si, which is similar to Er3+ in wide-bandgap semiconductors, suggests that Er is not in SiO2 or Si with bulk properties but, may be confined in Si light-emitting nanostructures. Porous Si is a good substrate for rare earth elements because: 1) a high concentration of optically active Er3+ can be obtained by implanting at about 200 keV, 2) porous Si and bulk Si are transparent to 1.54 μm emission therefore, device fabrication is simplified, and 3) although the external quantum efficiency of visible light from porous Si is compromised because of self-absorption, it can be used to pump Er3+.


2018 ◽  
Vol 140 (5) ◽  
pp. 1894-1899 ◽  
Author(s):  
Wenwen Lin ◽  
Constantinos C. Stoumpos ◽  
Oleg Y. Kontsevoi ◽  
Zhifu Liu ◽  
Yihui He ◽  
...  

2018 ◽  
Vol 9 ◽  
pp. 1085-1094 ◽  
Author(s):  
Kelvin Chung ◽  
Yu H Leung ◽  
Chap H To ◽  
Aleksandra B Djurišić ◽  
Snjezana Tomljenovic-Hanic

Fluorescence properties of crystallographic point defects within different morphologies of titanium dioxide were investigated. For the first time, room-temperature single-photon emission in titanium dioxide optical defects was discovered in thin films and commercial nanoparticles. Three-level defects were identified because the g (2) correlation data featured prominent shoulders around the antibunching dip. Stable and blinking photodynamics were observed for the single-photon emitters. These results reveal a new room-temperature single-photon source within a wide bandgap semiconductor.


2018 ◽  
Vol 86 (5) ◽  
pp. 3-21
Author(s):  
Fengwen Mu ◽  
Yinghui Wang ◽  
Tadatomo Suga

2017 ◽  
Vol 5 (36) ◽  
pp. 19116-19125 ◽  
Author(s):  
Yeon Hoo Kim ◽  
Ji Soo Park ◽  
You-Rim Choi ◽  
Seo Yun Park ◽  
Seon Yong Lee ◽  
...  

Detection of ppb level ammonia at room temperature is demonstrated using chemically fluorinated graphene oxide (CFGO). Fluorine adatom extremely enhances ammonia sensing capabilities through the changes of the charge distributions on adjacent functional groups, resulting in the variation in gas adsorption energies.


2017 ◽  
Vol 8 (1) ◽  
Author(s):  
Abhinav Prakash ◽  
Peng Xu ◽  
Alireza Faghaninia ◽  
Sudhanshu Shukla ◽  
Joel W. Ager ◽  
...  

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Amirhossein Bayani ◽  
Karin Larsson

AbstractThis is a theoretical investigation where Density Functional Theory (DFT) has been used in studying the phenomenon of Au intercalation within the 4H-SiC/graphene interface. The electronic structure of some carefully chosen morphologies of the Au layer has then been of special interest to study. One of these specific Au morphologies is of a more hypothetical nature, whilst the others are, from an experimental point of view, realistic ones. The latter ones were also found to be energetically stable. Band structure calculations showed that intercalated Au layers with morphologies different from a planar Au layer will induce a band gap at the Dirac point of graphene (with up to 174 meV for the morphologies studied in the present work). It should here be mentioned that this bandgap size is four times larger than the energy of thermal motion at room temperature (26 meV). These findings reveal that a wide bandgap at the Dirac point of graphene comes from an inhomogeneous staggered potential on the Au layer, which non-uniformly breaks the sublattice symmetry. The presence of spin-orbit (SO) interactions have also been included in the present study, with the purpose to find out if SO will create a bandgap and/or band splitting of graphene.


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