Magnetic photocatalysts with a p–n junction: Fe3O4 nanoparticle and FeWO4 nanowire heterostructures

Nanoscale ◽  
2014 ◽  
Vol 6 (21) ◽  
pp. 12366-12370 ◽  
Author(s):  
Xuan Cao ◽  
Yan Chen ◽  
Shihui Jiao ◽  
Zhenxing Fang ◽  
Man Xu ◽  
...  
Keyword(s):  
Hydrothermal Process ◽  
Fe3o4 Nanoparticle ◽  
Nanowire Heterostructures ◽  
Type Semiconductor ◽  
One Step ◽  
P Type

Magnetic n-type semiconductor Fe3O4 nanoparticle and p-type semiconductor FeWO4 nanowire heterostructures were successfully synthesized without any surfactants or templates via a facile one-step hydrothermal process at 160 °C.

Electrodeposition and Properties of CuInS2 Thin Films

2013 ◽  
Vol 690-693 ◽  
pp. 1659-1663
Author(s):  
Hai Fang Zhou ◽  
Xiao Hu Chen
Keyword(s):  
Thin Films ◽  
Photocurrent Density ◽  
Enhancement Effect ◽  
X Ray Diffraction ◽  
X Ray ◽  
Glass Substrates ◽  
Ito Glass ◽  
Type Semiconductor ◽  
One Step ◽  
P Type

The preparation and characterization of CuInS2 thin films on ITO glass substrates prepared by one-step electrodeposition have been reported. Samples were characterized using X-ray diffraction (XRD), energy dispersive X-ray spectroscopy (EDX) and scanning electron microscopy (SEM). The results indicate that CuInS2 is the major phase for the film deposited at -1.0 V, after annealing at 550°C in sulfur atmosphere, and the sample is Cu-rich and p-type semiconductor. Additionally, the energy band gap and carrier concentration for the sample were found to be 1.43 eV and 4.20×1017 cm−3, respectively. Furthermore, the maximum photocurrent density of the sample was found to be -1.15 mA/cm2 under 255 lx illumination, the sample shows the photo-enhancement effect.

One-step electrodeposition of CuInxGa1−xSe2 thin films from a mixture system of ionic liquid and ethanol

2015 ◽  
Vol 39 (10) ◽  
pp. 7742-7745 ◽  
Author(s):  
Ye Lian ◽  
Shanshan Ji ◽  
Lei Zhao ◽  
Jie Zhang ◽  
Peixia Yang ◽  
...  
Keyword(s):  
Thin Film ◽  
Thin Films ◽  
Ionic Liquid ◽  
Band Gap ◽  
High Crystalline Quality ◽  
Cigs Thin Film ◽  
Type Semiconductor ◽  
One Step ◽  
P Type ◽  
Mixture System

Synthesizing high crystalline quality p-type semiconductor CIGS thin film with a band gap of 1.41 eV by galvanostatic electrodeposition.

scholarly journals Effects of Preparation Conditions on the CuInS2Films Prepared by One-Step Electrodeposition Method

2015 ◽  
Vol 2015 ◽  
pp. 1-8 ◽  
Author(s):  
Rongfeng Guan ◽  
Liu Cao ◽  
Qian Sun ◽  
Yuebin Cao
Keyword(s):  
Thin Films ◽  
Sulfur Content ◽  
Indium Tin Oxide ◽  
Deposition Potential ◽  
X Ray Diffraction ◽  
Preparation Conditions ◽  
Sulfurization Temperature ◽  
Type Semiconductor ◽  
One Step ◽  
P Type

CuInS2thin films were prepared onto indium tin oxide (ITO) substrates by sulfurization of electrodeposited CuxInySzprecursor films under S atmosphere. The influences of deposition potential, Cu2+/In3+ratio, sulfurization temperature, and sulfur content on the CuInS2thin films were investigated. Phases and structures were characterized by powder X-ray diffraction and Raman spectroscopy; surface morphology was characterized by Scanning Electron Microscopy; optical and electrical properties were characterized by UV-Vis absorption and Mott-Schottky curves, respectively. As a result, the optimal well-crystallized CuInS2films preparation parameters were determined to be deposition potential of −0.8 V, Cu2+/In3+ratio of 1.4, sulfur content of 1 g, and the sulfurization temperature of 550°C for 1 h; CuInS2thin films prepared by one-step electrodeposition present the p-type semiconductor, with thickness about 4-5 μm and their optical band gaps in the range of 1.53~1.55 eV.

Synthesis and properties of dimeric porphyrin based on the hydroxyphenylporphyrin scaffold

2006 ◽  
Vol 10 (12) ◽  
pp. 1392-1397 ◽  
Author(s):  
Di Li ◽  
Yingyan Shi ◽  
Huanbao Fa ◽  
Wenqi Zheng ◽  
Ning Shan ◽  
...  
Keyword(s):  
Mass Spectrum ◽  
Surface Photovoltage ◽  
Surface Photovoltage Spectroscopy ◽  
Maldi Tof ◽  
Type Semiconductor ◽  
One Step ◽  
Photochemical Properties ◽  
P Type ◽  
Porphyrin Dimer

A porphyrin dimer was prepared by coupling H2MHTPP and 1,4-dichloro-2,5-dinitrobenzene in a one-step synthesis. Its structure was established by a MALDI-TOF mass spectrum and its electrochemical and photochemical properties were investigated. Surface photovoltage spectroscopy (SPS) revealed that the porphyrin dimer is a p-type semiconductor.

Transparent P-type Conducting LaCuOS Layered Oxysulfide

2001 ◽  
Vol 666 ◽  
Author(s):  
Kazushige Ueda ◽  
Shin-ichiro Inoue ◽  
Sakyo Hirose ◽  
Hiroshi Kawazoe ◽  
Hideo Hosono
Keyword(s):  
Electrical Conductivity ◽  
Visible Region ◽  
Optoelectronic Devices ◽  
Promising Material ◽  
High Transparency ◽  
Conducting Oxides ◽  
Excitonic Absorption ◽  
Type Semiconductor ◽  
Optical Applications ◽  
P Type

ABSTRACTMaterials design for transparent p-type conducting oxides was extended to oxysulfide system. LaCuOS was selected as a candidate for a transparent p-type semiconductor. It was found that the electrical conductivity of LaCuOS was p-type and controllable from semiconducting to semi-metallic states by substituting Sr2+ for La3+. LaCuOS films showed high transparency in the visible region, and the bandgap estimated was approximately 3.1 eV. Moreover, it was revealed that LaCuOS showed sharp excitonic absorption and emission at the bandgap edge, which is advantageous for optical applications. A layered oxysulfide, LaCuOS, was proposed to be a promising material for optoelectronic devices.

A self-assembled 3D urchin-like Ti0.8Sn0.2O2–rGO hybrid nanostructure as an anode material for high-rate and long cycle life Li-ion batteries

2017 ◽  
Vol 5 (17) ◽  
pp. 8087-8094 ◽  
Author(s):  
Yutao Dong ◽  
Dan Li ◽  
Chengwei Gao ◽  
Yushan Liu ◽  
Jianmin Zhang
Keyword(s):  
Anode Material ◽  
Hydrothermal Process ◽  
Cycle Life ◽  
High Rate ◽  
Li Ion Batteries ◽  
Long Cycle ◽  
Long Cycle Life ◽  
One Step ◽  
Li Ion ◽  
Self Assembled

Self-assembled 3D urchin-like Ti0.8Sn0.2O2–rGO was fabricated by a one-step hydrothermal process as an anode material for high-rate and long cycle life LIBs.

The Study of p-n and Schottky Junction for Magnetodiode

2011 ◽  
Vol 378-379 ◽  
pp. 663-667 ◽  
Author(s):  
Toempong Phetchakul ◽  
Wittaya Luanatikomkul ◽  
Chana Leepattarapongpan ◽  
E. Chaowicharat ◽  
Putapon Pengpad ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Electrical Properties ◽  
Simulation Model ◽  
Hall Effect ◽  
Schottky Junction ◽  
Field Sensitivity ◽  
Field Response ◽  
Type Semiconductor ◽  
Simulation Results ◽  
P Type

This paper presents the simulation model of Dual Magnetodiode and Dual Schottky Magnetodiode using Sentaurus TCAD to simulate the virtual structure of magneto device and apply Hall Effect to measure magnetic field response of the device. Firstly, we use the program to simulate the magnetodiode with p-type semiconductor and aluminum anode and measure electrical properties and magnetic field sensitivity. Simulation results show that sensitivity of Dual Schottky magnetodiode is higher than that of Dual magnetodiode.

Study on Phases and Thermoelectric Properties of Bulk Fe4Sb12 and Fe3CoSb12 Prepared by Milling and Sintering

2011 ◽  
Vol 121-126 ◽  
pp. 1526-1529
Author(s):  
Ke Gao Liu ◽  
Jing Li
Keyword(s):  
Thermoelectric Properties ◽  
Impurity Phase ◽  
Semiconductor Materials ◽  
Thermal Constant ◽  
X Ray Diffraction ◽  
X Ray ◽  
Seebeck Coefficients ◽  
Maximum Value ◽  
Type Semiconductor ◽  
P Type

Bulk Fe4Sb12 and Fe3CoSb12 were prepared by sintering at 600 °C. The phases of samples were analyzed by X-ray diffraction and their thermoelectric properties were tested by electric constant instrument and laser thermal constant instrument. Experimental results show that, the major phases of bulk samples are skutterudite with impurity phase FeSb2. The electric resistivities of the samples increase with temperature rising at 100~500 °C. The bulk samples are P-type semiconductor materials. The Seebeck coefficients of the bulk Fe4Sb12 are higher than those of bulk Fe3CoSb12 samples at 100~200 °C but lower at 300~500 °C. The power factor of the bulk Fe4Sb12 samples decreases with temperature rising while that of bulk Fe3CoSb12 samples increases with temperature rising at 100~500 °C. The thermal conductivities of the bulk Fe4Sb12 samples are relatively higher than those of and Fe3CoSb12, which maximum value is up to 0.0974 Wm-1K-1. The ZT value of bulk Fe3CoSb12 increases with temperature rising at 100~500 °C, the maximum value is up to 0.031.The ZT values of the bulk Fe4Sb12 samples are higher than those of bulk Fe3CoSb12 at 100~300 °C while lower at 400~500 °C.

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