Schottky Barrier Heights of PT Silicides on SiGe

1993 ◽  
Vol 320 ◽  
Author(s):  
J.R. Jimenez ◽  
X. Xiao ◽  
J.C. Sturm ◽  
P.W. Pellegrini ◽  
M. Chi
Keyword(s):  
Schottky Barrier ◽  
Barrier Height ◽  
Schottky Diodes ◽  
Infrared Detector ◽  
Schottky Barriers ◽  
Band Offset ◽  
Barrier Heights ◽  
Semiconductor Interfaces ◽  
Metal Thickness ◽  
Deposited Metal

ABSTRACTSilicide/SiGe Schottky barriers are of importance for applications in infrared detectors and SiGe contacts, as well as for fundamental studies of metal-semiconductor interfaces. We have fabricated silicide/SiGe Schottky diodes by the reaction of evaporated Pt and Ir films on p-SiGe alloys with a thin Si capping layer. The onset of metal-SiGe reactions was controlled by the deposited metal thickness. The Schottky barrier heights were determined from internal photoemission. Pt-SiGe and Ir-SiGe reacted diodes have barrier heights that are higher than the corresponding silicide/p-Si diodes. PtSi/Si/SiGe diodes, on the other hand, have lower “barrier heights” that decrease with increasing Ge concentration. The smaller barrier heights in such silicide/Si/SiGe diodes are due to tunneling through the unconsumed Si layer. Equations are derived accounting for this tunneling contribution, and lead to an extracted “barrier height” that is the Si barrier height reduced by the Si/SiGe band offset. Highly bias-tunable barrier heights are obtained (e.g. 0.30 eV to 0.12 eV) by allowing the SiGe/Si band offset to extend higher in energy than the Schottky barrier, leading to a cut-off-wavelength-tunable silicide/SiGe/Si Schottky diode infrared detector.

Electrical Properties and Schottky Barriers of Metal-Semiconductor Interfaces

1990 ◽  
Vol 181 ◽  
Author(s):  
M.O. Aboelfotoh
Keyword(s):  
Electrical Properties ◽  
Temperature Dependence ◽  
Schottky Barrier ◽  
Barrier Height ◽  
Fermi Level Pinning ◽  
Barrier Heights ◽  
Semiconductor Interfaces ◽  
Barrier Formation ◽  
Indirect Band Gap ◽  
P Type

ABSTRACTThe electrical properties of metal/Si(100) and metal/Ge(100) interfaces formed by the deposition of metal on both n-type and p-type Si(100) and Ge(100) have been studied in the temperature range 77-295 K with the use of current- and capacitance-voltage techniques. Compound formation is found to have very little or no effect on the Schottky-barrier height and its temperature dependence. For silicon, the barrier height and its temperature dependence are found to be affected by the metal. For germanium, on the other hand, the barrier height and its temperature dependence are unaffected by the metal. The temperature dependence of the Si and Ge barrier heights is found to deviate from the predictions of recent models of Schottky-barrier formation based on the suggestion of Fermi-level pinning in the center of the semiconductor indirect band gap.

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.

Quasi-Schottky Diodes on (n)In.53Ga.47as with Barrier Heights of 0.6 eV

1991 ◽  
Vol 240 ◽  
Author(s):  
M. Marso ◽  
P. Kordoš ◽  
R. Meyer ◽  
H. Lüth
Keyword(s):  
Schottky Barrier ◽  
Barrier Height ◽  
Schottky Diodes ◽  
Reverse Current ◽  
Surface Layers ◽  
Fully Depleted ◽  
Barrier Heights ◽  
Effective Barrier ◽  
Basic Parameters ◽  
And Control

ABSTRACTThe modification and control of the Schottky barrier height on (n)InGaAs is an important tool at the device preparation as the barrier height is very low, øB° = 0.2 eV. We report about the Schottky barrier enhancement on (n)InGaAs by thin fully depleted surface layers of high doped (p+)InGaAs. Structures with different thicknesses of (p+)InGaAs in the range from 8 to 80 nm were grown by LP MOVPE technique and quasi-Schottky diodes with different contact areas were prepared using titanium as a barrier metal. I-V and I-T characteristics were measured and analysed to obtain basic parameters of prepared diodes, i. e. ideality factor n, effective barrier height øB, series resistance Rgand reverse current density JR (1V). The barrier height enhancement increases with the thickness of the (p+)-layer. Effective barrier heights of øB>0.6 eV, i.e. higher than reported until now, can be obtained with the surface layers of (p+)InGaAs with thicknesses exceeding 25 nm.

W/Si Schottky Diodes: Effect of Metal Deposition Conditions on the Barrier Height

1994 ◽  
Vol 356 ◽  
Author(s):  
M. Mamor ◽  
E. Finkman ◽  
F. Meyer ◽  
K. Bouziane
Keyword(s):  
Schottky Barrier ◽  
Barrier Height ◽  
Schottky Barrier Height ◽  
Schottky Diodes ◽  
X Ray Diffraction ◽  
Experimental Conditions ◽  
X Ray ◽  
Barrier Heights ◽  
P Type ◽  
Deposition Conditions

AbstractThe Schottky barrier heights (ΦB) for W/Si Schottky diodes have been determined from I–V measurements. The effects of the sputter deposition conditions of the W-films were studied. X-ray diffraction was used to examine the structure and the lattice parameters of the W-films while the stress was determined by using a profilometer from the measurement of the curvature of the substrate after metallization. The resistivity is determined by using a four-point probe. A compressive-to-tensile stress transition is associated with the transformation of the ±—W-phase into the (β—W-phase as the working gas pressure is increased. These effects, which are frequently observed, coïncide with a significant increase of the W-film resistivity and a change (△ΦB≈50 meV) in the Schottky barrier height on n-type. On the other hand, the barrier height on the p-type remains constant under all the experimental conditions investigated. These results are discussed in terms of effects of strain and structure of W-films on the work function of the W, as well as in terms of modification of the pinning position of the Fermi level or else change in the value of the Richardson constant.

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.

scholarly journals A Study about Schottky Barrier Height and Ideality Factor in Thin Film Transistors with Metal/Zinc Oxide Nanoparticles Structures Aiming Flexible Electronics Application

Nanomaterials ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 1188
Author(s):  
Ivan Rodrigo Kaufmann ◽  
Onur Zerey ◽  
Thorsten Meyers ◽  
Julia Reker ◽  
Fábio Vidor ◽  
...  
Keyword(s):  
Thin Film ◽  
Zinc Oxide ◽  
Schottky Barrier ◽  
Barrier Height ◽  
Flexible Electronics ◽  
Thin Film Transistors ◽  
Zinc Oxide Nanoparticles ◽  
Schottky Barrier Height ◽  
Oxide Nanoparticles ◽  
Semiconductor Interfaces

Zinc oxide nanoparticles (ZnO NP) used for the channel region in inverted coplanar setup in Thin Film Transistors (TFT) were the focus of this study. The regions between the source electrode and the ZnO NP and the drain electrode were under investigation as they produce a Schottky barrier in metal-semiconductor interfaces. A more general Thermionic emission theory must be evaluated: one that considers both metal/semiconductor interfaces (MSM structures). Aluminum, gold, and nickel were used as metallization layers for source and drain electrodes. An organic-inorganic nanocomposite was used as a gate dielectric. The TFTs transfer and output characteristics curves were extracted, and a numerical computational program was used for fitting the data; hence information about Schottky Barrier Height (SBH) and ideality factors for each TFT could be estimated. The nickel metallization appears with the lowest SBH among the metals investigated. For this metal and for higher drain-to-source voltages, the SBH tended to converge to some value around 0.3 eV. The developed fitting method showed good fitting accuracy even when the metallization produced different SBH in each metal-semiconductor interface, as was the case for gold metallization. The Schottky effect is also present and was studied when the drain-to-source voltages and/or the gate voltage were increased.

Electron Transport Through Epitaxial Metal/Semiconductor Heterostructures

1986 ◽  
Vol 77 ◽  
Author(s):  
A. F. J. Levi ◽  
R. T. Tung ◽  
J. L. Batstone ◽  
J. M. Gibson ◽  
M. Anzlowar ◽  
...  
Keyword(s):  
Electron Transport ◽  
Schottky Barrier ◽  
Semiconductor Heterostructures ◽  
Perfect Single Crystal ◽  
Barrier Heights ◽  
Semiconductor Interfaces ◽  
Semiconductor Contacts ◽  
First Time ◽  
Silicon Heterostructures

ABSTRACTAbrupt, epitaxial silicide/silicon heterostructures may be grown so that, for the first time, the physics of electron transport across near perfect, single crystal, metal/semiconductor interfaces may be probed experimentally. Transport measurements through type-A and -B oriented NiSi2 layers on Si(111) substrates have revealed Schottky barrier heights differing by 140 meV. In this paper we present results of experiments designed to explore the possible role of bulk and interface defects in determining the potential barrier at these near ideal epitaxial metal-semiconductor contacts. We have found little evidence for the presence of defects and the Schottky barrier is insensitive to details of the microscopic interfacial perfection. By contrast we find that both the electrical quality and magnitude of the barrier occurring at the NiSi2 /Si(100) heterojunction are dependent upon details of the microscopic interfacial perfection.

scholarly journals Electric dipole effect in PdCoO2/β-Ga2O3 Schottky diodes for high-temperature operation

2019 ◽  
Vol 5 (10) ◽  
pp. eaax5733 ◽  
Author(s):  
T. Harada ◽  
S. Ito ◽  
A. Tsukazaki
Keyword(s):  
High Temperature ◽  
Schottky Barrier ◽  
Barrier Height ◽  
Schottky Barrier Height ◽  
Schottky Diodes ◽  
Extreme Environments ◽  
Oxide Interface ◽  
Electric Dipoles ◽  
Bandgap Semiconductors ◽  
High Temperature Operation

High-temperature operation of semiconductor devices is widely demanded for switching/sensing purposes in automobiles, plants, and aerospace applications. As alternatives to conventional Si-based Schottky diodes usable only at 200°C or less, Schottky interfaces based on wide-bandgap semiconductors have been extensively studied to realize a large Schottky barrier height that makes high-temperature operation possible. Here, we report a unique crystalline Schottky interface composed of a wide-gap semiconductor β-Ga2O3 and a layered metal PdCoO2. At the thermally stable all-oxide interface, the polar layered structure of PdCoO2 generates electric dipoles, realizing a large Schottky barrier height of ~1.8 eV, well beyond the 0.7 eV expected from the basal Schottky-Mott relation. Because of the naturally formed homogeneous electric dipoles, this junction achieved current rectification with a large on/off ratio approaching 108 even at a high temperature of 350°C. The exceptional performance of the PdCoO2/β-Ga2O3 Schottky diodes makes power/sensing devices possible for extreme environments.

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