Schottky Barrier Modification Of Low Energy Ar-Ion Bombarded GaAs And Si

1998 ◽  
Vol 510 ◽  
Author(s):  
P.N.K. Deenapanray ◽  
F.D. Auret ◽  
S.A. Goodman
Keyword(s):  
Schottky Barrier ◽  
Schottky Diodes ◽  
Surface States ◽  
Barrier Properties ◽  
Low Energy ◽  
Fermi Level Pinning ◽  
Barrier Heights ◽  
Current Voltage ◽  
Donor Type ◽  
High Concentrations

AbstractEpitaxially grown GaAs (p- and n-type) and n-Si were bombarded with low energy Ar-ions. Current voltage measurements on Schottky barrier diodes fabricated on the sputtered p-GaAs (Sc) and n-Si (Pd) showed that the series resistance and ideality factor were increased as the Arion dose was increased. The respective increase and decrease in barrier heights of Sc/p-GaAs and Pd/n-Si diodes were attributed to the presence of donor-type surface states in the bombarded material. The barrier heights of Au Schottky diodes made on n-GaAs changed nonmonotonically with Ar-ion sputter voltage. Variations of barrier height in the 0-1 kV range were explained by the introduction of donor-type defects. We demonstrated that the introduction of high concentrations of continuous level defects above 1 kV resulted in Fermi level pinning to become the dominant mechanism for controlling the effective barrier of current transport. Our results have shown that Schottky barrier properties could be changed by controlled amounts by varying the bombarding ion dose or sputter voltage.

Impact of Interface Traps on Current-Voltage Characteristics of 4H-SiC Schottky-Barrier Diodes

2014 ◽  
Vol 778-780 ◽  
pp. 710-713 ◽  
Author(s):  
Hamid Amini Moghadam ◽  
Sima Dimitrijev ◽  
Ji Sheng Han
Keyword(s):  
Schottky Barrier ◽  
Schottky Barrier Height ◽  
Schottky Diodes ◽  
Forward Bias ◽  
Interface Traps ◽  
Barrier Heights ◽  
Current Voltage ◽  
Donor Type ◽  
Current Voltage Characteristics ◽  
Expected Values

This paper presents a physical model based on interface traps to explain both the larger barrier heights of practical Schottky diodes in comparison to the theoretically expected values and the appearance of a knee in the log I–V characteristics. According to this model, acceptor-type interface traps near the valance band increase the Schottky barrier height, which shifts the log I–V characteristic to higher forward-bias voltages. In addition to the acceptor traps, donor-type interface traps can appear near the conduction band, and when they do, they cause the knee in the log I–V characteristics as their energy level falls below the Fermi level and the charge associated with these traps changes from positive to neutral.

Fermi Level Pinning in Au Schottky Barriers on InGaP and InGaAlP

1994 ◽  
Vol 340 ◽  
Author(s):  
V.A. Gorbyley ◽  
A.A. Chelniy ◽  
A.A. Chekalin ◽  
A.Y. Polyakov ◽  
S.J. Pearon ◽  
...  
Keyword(s):  
Quantum Well ◽  
Fermi Level ◽  
Plasma Treatment ◽  
Schottky Barrier ◽  
Hydrogen Plasma ◽  
Schottky Diodes ◽  
Schottky Barriers ◽  
Quantum Well Structures ◽  
Fermi Level Pinning ◽  
Barrier Heights

ABSTRACTIt is shown that in Au/InGaP and Au/InGaAlP Schottky diodes the Fermi level is pinned by metal-deposition-induced midgap states. Hydrogen plasma treatment of such diodes greatly improves the reverse currents. The measured Schottky barrier heights seem to correlate with the valence band offsets measured by DLTS on quantum well structures.

scholarly journals Schottky diodes based on 4H-SiC epitaxial layers

2021 ◽  
Vol 2103 (1) ◽  
pp. 012235
Author(s):  
A M Strel’chuk ◽  
E V Kalinina
Keyword(s):  
Schottky Barrier ◽  
Barrier Height ◽  
Schottky Barrier Height ◽  
Alternative Explanation ◽  
Schottky Diodes ◽  
Reverse Current ◽  
Epitaxial Layers ◽  
Barrier Heights ◽  
Current Voltage ◽  
Significant Spread

Abstract Forward and reverse current-voltage (IV) characteristics of Cr-SiC (4H) Schottky diodes based on epitaxial layers with doping (1-3)· 1015 cm-3 were studied in the temperature range of 300-550 K. It is shown that in many cases the IV characteristics are close to ideal, but a significant spread of the forward IV characteristics of diodes manufactured in the same way on the same epitaxial layer was found, probably due to the spread of the Schottky barrier heights reaching 0.3 eV. Heating of the diode, as well as packaging, can also change the Schottky barrier height. An alternative explanation suggests the presence of a powerful shunt.

Fermi-level pinning and Schottky barrier heights on epitaxially grown fully strained and partially relaxed n-type Si1−xGex layers

1999 ◽  
Vol 86 (12) ◽  
pp. 6890-6894 ◽  
Author(s):  
M. Mamor ◽  
O. Nur ◽  
M. Karlsteen ◽  
M. Willander ◽  
F. D. Auret
Keyword(s):  
Fermi Level ◽  
Schottky Barrier ◽  
Fermi Level Pinning ◽  
Barrier Heights

Current-voltage characteristics of low energy proton and alpha particle irradiated Au and Schottky barrier diodes

1997 ◽  
Vol 41 (5) ◽  
pp. 802-805 ◽  
Author(s):  
S Arulkumaran ◽  
J Arokiaraj ◽  
N Dharmarasu ◽  
J Kumar ◽  
P Magudapathy ◽  
...  
Keyword(s):  
Schottky Barrier ◽  
Alpha Particle ◽  
Low Energy ◽  
Schottky Barrier Diodes ◽  
Energy Proton ◽  
Current Voltage ◽  
Current Voltage Characteristics

scholarly journals Surface Modification on the Sputtering-Deposited ZnO Layer for ZnO-Based Schottky Diode

2013 ◽  
Vol 2013 ◽  
pp. 1-9 ◽  
Author(s):  
Ren-Hao Chang ◽  
Kai-Chao Yang ◽  
Tai-Hong Chen ◽  
Li-Wen Lai ◽  
Tsung-Hsin Lee ◽  
...  
Keyword(s):  
Schottky Barrier ◽  
Schottky Diode ◽  
Ohmic Contact ◽  
Indium Tin Oxide ◽  
Photoelectron Spectroscopy ◽  
Layer Surface ◽  
Barrier Heights ◽  
Ammonium Sulfide ◽  
Current Voltage ◽  
Contact Electrode

We prepare a zinc oxide- (ZnO-) based Schottky diode constructed from the transparent cosputtered indium tin oxide- (ITO-) ZnO ohmic contact electrode and Ni/Au Schottky metal. After optimizing the ohmic contact property and removing the ion-bombardment damages using dilute HCl etching solution, the dilute hydrogen peroxide (H2O2) and ammonium sulfide (NH4)2Sxsolutions, respectively, are employed to modify the undoped ZnO layer surface. Both of the Schottky barrier heights with the ZnO layer surface treated by these two solutions, evaluated from the current-voltage (I-V) and capacitance-voltage (C-V) measurements, are remarkably enhanced as compared to the untreated ZnO-based Schottky diode. Through the X-ray photoelectron spectroscopy (XPS) and room-temperature photoluminescence (RTPL) investigations, the compensation effect as evidence of the increases in the O–H and OZnacceptor defects appearing on the ZnO layer surface after treating by the dilute H2O2solution is responsible for the improvement of the ZnO-based Schottky diode. By contrast, the enhancement on the Schottky barrier height for the ZnO layer surface treated by using dilute (NH4)2Sxsolution is attributed to both the passivation and compensation effects originating from the formation of the Zn–S chemical bond andVZnacceptors.

High Voltage Schottky Barrier Diodes on P-Type SiC using Metal-Overlap on a Thick Oxide Layer as Edge Termination

1999 ◽  
Vol 572 ◽  
Author(s):  
Q. Zhang ◽  
V. Madangarli ◽  
S. Soloviev ◽  
T. S. Sudarshan
Keyword(s):  
Schottky Barrier ◽  
Oxide Layer ◽  
Breakdown Voltage ◽  
Schottky Diodes ◽  
Schottky Barrier Diodes ◽  
Edge Termination ◽  
Forward Current ◽  
Current Voltage ◽  
Thick Oxide Layer ◽  
P Type

ABSTRACTP-type 6H SiC Schottky barrier diodes with good rectifying characteristics upto breakdown voltage as high as 1000V have been successfully fabricated using metal-overlap over a thick oxide layer (∼ 6000 Å) as edge termination and Al as the barrier metal. The influence of the oxide layer edge termination in improving the reverse breakdown voltage as well as the forward current – voltage characteristics is presented. The terminated Schottky diodes indicate a factor of two higher breakdown voltage and 2–3 times larger forward current densities than those without edge termination. The specific series resistance of the unterminated diodes was ∼228 mΩ-cm2, while that of the terminated diodes was ∼84 mΩ-cm2.

Evolution of Ti Schottky Barrier Heights on n-Type GaN with Annealing

1996 ◽  
Vol 449 ◽  
Author(s):  
Michèle T. Hirsch ◽  
Kristin J. Duxstad ◽  
E. E. Haller
Keyword(s):  
Barrier Height ◽  
Schottky Diodes ◽  
Electron Beam Evaporation ◽  
Organic Vapor ◽  
Barrier Heights ◽  
Effective Barrier ◽  
Mott Model ◽  
Current Voltage ◽  
Metal Organic ◽  
Ti Films

ABSTRACTWe report the effect of mild annealing on Ti Schottky diodes on n-type GaN. The Ti films were deposited by electron beam evaporation on n-type GaN grown by metal organic vapor deposition. We determine the effective barrier height Ф60 by current-voltage measurements as a function of temperature. The as-deposited Ti contacts show rectifying behavior with low barrier heights Ф60 ≤ 200meV. At annealing temperatures as low as 60°C we observe an increase of the barrier height to values of 250meV. After annealing at 230°C and above a stable barrier height of 450meV is measured. The increase in barrier height is not due to any macroscopic interfacial reaction. The origin of the observed changes are discussed in terms of the Schottky-Mott model and possible microscopic interfacial reactions.

Schottky Barrier Height Dependence on the Metal Work Function for p-type Si Schottky Diodes

2004 ◽  
Vol 59 (11) ◽  
pp. 795-798 ◽  
Author(s):  
Güven Çankaya ◽  
Nazım Uçar
Keyword(s):  
Fermi Level ◽  
Schottky Barrier ◽  
Schottky Diodes ◽  
Metal Work Function ◽  
Current Voltage ◽  
Current Voltage Characteristics ◽  
Work Functions ◽  
P Type ◽  
Relationship Of ◽  
Metal Work

We investigated Schottky barrier diodes of 9 metals (Mn, Cd, Al, Bi, Pb, Sn, Sb, Fe, and Ni) having different metal work functions to p-type Si using current-voltage characteristics. Most Schottky contacts show good characteristics with an ideality factor range from 1.057 to 1.831. Based on our measurements for p-type Si, the barrier heights and metal work functions show a linear relationship of current-voltage characteristics at room temperature with a slope (S=ϕb/ϕm) of 0.162, even though the Fermi level is partially pinned. From this linear dependency, the density of interface states was determined to be about 4.5 · 1013 1/eV per cm2, and the average pinning position of the Fermi level as 0.661 eV below the conduction band

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