Electrical and Optical Properties of Erbium in MBE Silicon and Si/Ge Alloys

1991 ◽  
Vol 220 ◽  
Author(s):  
H. Efeoglu ◽  
J. H. Evans ◽  
J. M. Langer ◽  
A. R. Peaker ◽  
N. L. Rowell ◽  
...  

ABSTRACTThis paper reports the incorporation of erbium into MBE Si and Si/Ge alloys with substrate temperatures of 500°C and 700°C. Using a solid source MBE system, concentrations of erbium between 1018 and 1022 cm−3 have been studied by photoluminescence, electrical measurements, SIMS and TEM. We find no shallow donors or acceptors attributable to erbium but we observe a high concentration of deep states with an activation energy of ∼360 meV. The photoluminescence output is of greatest magnitude when [Er] =2 × 1018 cm−3. Above this concentration the onset of erbium precipitates can just be observed using TEM and at even higher concentrations structured growths of erbium suicide are apparent. The effect on the optical activity of Si:Er that has subsequently been implanted with oxygen is also reported.

2011 ◽  
Vol 8 (2) ◽  
pp. 638-645
Author(s):  
Baghdad Science Journal

In this work the structural, electrical and optical Properties of CuO semiconductor films had been studied, which prepared at three thickness (100, 200 and 500 nm) by spray pyrolysis method at 573K substrate temperatures on glass substrates from 0.2M CuCl2•2H2O dissolved in alcohol. Structural Properties shows that the films have only a polycrystalline CuO phase with preferential orientation in the (111) direction, the dc conductivity shows that all films have two activation energies, Ea1 (0.45-0.66 eV) and Ea2 (0.055-.0185 eV), CuO films have CBH (Correlated Barrier Hopping) mechanism for ac-conductivity. The energy gap between (1.5-1.85 eV).


1994 ◽  
Vol 369 ◽  
Author(s):  
C. Zhang ◽  
H. Deng ◽  
J. Varon ◽  
B. Abeles ◽  
Y. Yang ◽  
...  

AbstractThin film SrCo0.8Fe0.2O3-δ were made by pulse laser deposition. The electrical conductivity is thermally activated in the temperature 25-500 °C with an activation energy of 0.17-0.19 eV and is temperature independant from 500-800 °C. The optical absorption shows characteristic features which are interpreted qualitatively in terms of a simple band structure diagram.


2011 ◽  
Vol 287-290 ◽  
pp. 2308-2313 ◽  
Author(s):  
Yi Hua Sun ◽  
Chen Hui Li ◽  
Wei Hao Xiong ◽  
Cai Hua Huang

Transparent conducting aluminum-doped zinc oxide (AZO) films have been prepared on soda-lime glass substrates by radio frequency magnetron sputtering using a high density ceramic target at different substrate temperatures. The structural, morphology, electrical, and optical properties of the AZO thin films were investigated by X-ray diffraction, scanning electron microscope, Hall measurement, and optical transmission spectroscopy, and which were strongly influenced by substrate temperatures. Films with better texture, higher transmission, lower resistivity and larger carrier concentration were obtained for the samples fabricated at higher substrate temperature. The AZO film with the lowest resistivity of 4.63×10−4 Ω.cm and an average optical transmission of 92% in the visible range was deposited on the substrate heated at 450 °C. The optical bandgap depends on the deposition condition, and was in the range of 3.35~3.59 eV.


2012 ◽  
Vol 557-559 ◽  
pp. 1945-1949
Author(s):  
Ge Yu ◽  
Ya Liu ◽  
Dan Hong Hong ◽  
Dong Lin Li ◽  
Jian Xin Zang

Aluminum oxide-doped zinc oxide (AZO) films were deposited by radio frequency (RF) magnetron sputtering at various substrate temperatures and sputtering powers with pure argon flow. Their electrical and optical properties and microstructures were investigated by X-ray diffractometer (XRD), atomic force microscope (AFM), ultraviolet-visible spectrophotometer, four-probe tester. The investigation indicates that the electrical and optical properties and microstructures of the AZO films are remarkably influenced by substrate temperature and sputtering power. With the sputtering power increasing from 60W to 180W, the diffraction peaks rise significantly, the resistivity decreases quickly and the visible transmission is all quite high. When the substrate temperature increases from 25°C to 400°C, the diffraction peaks rise first and lower then both quickly, the resistivity decreases first sharply and then very slowly, and the visible transmission is also high. The films deposited at the substrate temperature 300°C with the sputtering power 180W have low resistivity 1.2×10–3 Ω•cm and high transmittance 92% at the same time.


2011 ◽  
Vol 324 ◽  
pp. 245-248
Author(s):  
Hassan Ghamlouche ◽  
Saleh Thaker Mahmoud ◽  
Naser Qamhieh ◽  
Ahmad I. Ayesh

The electrical and optical characteristics of indium doped Se2Sb2Te6phase-change alloy are studied. It is found that adding indium to Se2Sb2Te6 alloy (In0.3Se2Sb2Te6) increased the crystallization temperature and reduced the electrical conduction activation energy. The capacitance-temperature measurements showed a drastic change in the capacitance of the modified film when the temperature approaches the crystallization temperature, and eventually the capacitance becomes negative and nonlinear. The negativity and nonlinearity in the capacitancevoltage dependence can be attributed to the growth of conductive crystalline islands by increasing the temperature.


MRS Advances ◽  
2017 ◽  
Vol 2 (53) ◽  
pp. 3077-3082 ◽  
Author(s):  
Md Nadim Ferdous Hoque ◽  
Nazifah Islam ◽  
Kai Zhu ◽  
Zhaoyang Fan

ABSTRACTHybrid perovskite solar cells (PSCs) under normal operation will reach a temperature above ∼ 60 °C, across the tetragonal-cubic structural phase transition of methylammonium lead iodide (MAPbI3). Whether the structural phase transition could result in dramatic changes of ionic, electrical and optical properties that may further impact the PSC performances should be studied. Herein, we report a structural phase transition temperature of MAPbI3 thin film at ∼ 55 °C, but a striking contrast occurred at ∼ 45 °C in the ionic and electrical properties of MAPbI3 due to a change of the ion activation energy from 0.7 eV to 0.5 eV. The optical properties exhibited no sharp transition except for the steady increase of the bandgap with temperature. It was also observed that the activation energy for ionic migration steadily increased with increased grain sizes, and reduction of the grain boundary density reduced the ionic migration.


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