Reduction of interface state density in coaxial TiO2/Ge nanowire assembly-based heterostructure and superior photodetection

2021 ◽  
Vol 853 ◽  
pp. 157344 ◽  
Author(s):  
Singh H. Manas ◽  
Bijit Choudhuri ◽  
P. Chinnamuthu
Keyword(s):  
Interface State ◽  
State Density ◽  
Interface State Density

Interface-State-Density Evaluation of p-type and n-type Ge/GeNx Structures by Conductance Technique

2013 ◽  
Vol 133 (7) ◽  
pp. 1279-1284
Author(s):  
Takuro Iwasaki ◽  
Toshiro Ono ◽  
Yohei Otani ◽  
Yukio Fukuda ◽  
Hiroshi Okamoto
Keyword(s):  
Interface State ◽  
State Density ◽  
Interface State Density ◽  
Conductance Technique ◽  
Density Evaluation ◽  
P Type

Identification of Charging Effects in Plasma-Enhanced TEOS Deposition with Non-Contact Test Techniques

1998 ◽  
Author(s):  
Tomasz Brozek ◽  
James Heddleson
Keyword(s):  
Vapor Deposition ◽  
Chemical Vapor ◽  
Interface State ◽  
State Density ◽  
Interface State Density ◽  
Wafer Surface ◽  
Oxide Charge ◽  
Contact Test ◽  
Deposition Power ◽  
Oxide Deposition

Abstract Use of non-contact test techniques to characterize degradation of the Si-SiO2 system on the wafer surface exposed to a plasma environment have proven themselves to be sensitive and useful in investigation of plasma charging level and uniformity. The current paper describes application of the surface charge analyzer and surface photo-voltage tool to explore process-induced charging occurring during plasma enhanced chemical vapor deposition (PECVD) of TEOS oxide. The oxide charge, the interface state density, and dopant deactivation are studied on blanket oxidized wafers with respect to the effect of oxide deposition, power lift step, and subsequent annealing.

scholarly journals Preparation and Characterization of Nitridation Layer on 4H SiC (0001) Surface by Direct Plasma Nitridation

2014 ◽  
Vol 778-780 ◽  
pp. 631-634 ◽  
Author(s):  
Yoshiyuki Akahane ◽  
Takuo Kano ◽  
Kyosuke Kimura ◽  
Hiroki Komatsu ◽  
Yukimune Watanabe ◽  
...  
Keyword(s):  
Interface State ◽  
Nitride Layer ◽  
State Density ◽  
Interface State Density ◽  
Process Temperature ◽  
Pure Nitrogen ◽  
Interface Property ◽  
Plasma Nitridation

A nitride layer was formed on a SiC surface by plasma nitridation using pure nitrogen as the reaction gas at the temperature from 800°C to 1400°C. The surface was characterized by XPS. The XPS measurement showed that an oxinitride layer was formed on the SiC surface by the plasma nitridation. The high process temperature seemed to be effective to activate the niridation reaction. A SiO2film was deposited on the nitridation layer to form SiO2/nitride/SiC structure. The interface state density of the SiO2/nitride/SiC structure was lower than that of the SiO2/SiC structure. This suggested that the nitridation was effective to improve the interface property.

Low Interface State Density Oxide-GaAs Structures Fabricated by In-Situ Molecular Beam Epitaxy

1996 ◽  
Vol 421 ◽  
Author(s):  
M. Passlack ◽  
M. Hong
Keyword(s):  
Molecular Beam Epitaxy ◽  
Molecular Beam ◽  
Molecular Beams ◽  
Interface State ◽  
State Density ◽  
Interface State Density ◽  
In Situ Deposition ◽  
Interface Recombination Velocity ◽  
Recombination Velocity

AbstractWe have extended the spectrum of molecular-beam epitaxy (MBE) related techniques by introducing in-situ deposition of oxides. The oxide films have been deposited on clean, atomically ordered (100) GaAs wafer surfaces using molecular beams of gallium-, magnesium-, silicon-, or aluminum oxide. Among the fabricated oxide-GaAs heterostructures, Ga2O3-GaAs interfaces exhibit unique electronic properties including an interface state density Dit in the low 1010 cm−2eV−1 range and an interface recombination velocity S of 4000 cm/s. The formation of inversion layers in both n- and p-type GaAs has been clearly established. Further, thermodynamic and photochemical stability of excellent electronic interface properties of Ga2O3-GaAs structures has been demonstrated.

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