Electronic Levels Induced by Irradiation in 4H-Silicon Carbide

2005 ◽  
Vol 483-485 ◽  
pp. 359-364 ◽  
Author(s):  
Antonio Castaldini ◽  
Anna Cavallini ◽  
L. Rigutti ◽  
Filippo Nava
Keyword(s):  
Silicon Carbide ◽  
Deep Level ◽  
Particle Energy ◽  
Free Carrier ◽  
Current Voltage ◽  
Capacitance Voltage ◽  
Current Voltage Characteristics ◽  
Transient Spectroscopy ◽  
Induced Defects ◽  
Irradiation Induced Defects

The effects of irradiation with protons and electrons on 4H-silicon carbide epilayers were investigated. The particle energy was 6.5 and 8.2 MeV. The electronic levels associated with the irradiation-induced defects were analyzed by current-voltage characteristics and deep level transient spectroscopy measurements up to 700 K. In the same temperature range the apparent free carrier concentration was measured by capacitance-voltage characteristics to monitor possible compensation effects due to the deep level associated to the induced defects. Introduction rate, enthalpy and capture cross-section of such deep levels were compared and some conclusions about the nature of the defects were drawn.

Correlation between Leakage Current and Ion-Irradiation Induced Defects in 4H-SiC Schottky Diodes

2006 ◽  
Vol 527-529 ◽  
pp. 1167-1170 ◽  
Author(s):  
Vito Raineri ◽  
Fabrizio Roccaforte ◽  
Sebania Libertino ◽  
Alfonso Ruggiero ◽  
V. Massimino ◽  
...  
Keyword(s):  
Leakage Current ◽  
Ion Irradiation ◽  
Deep Level ◽  
Schottky Diodes ◽  
Arrhenius Dependence ◽  
Current Voltage ◽  
Current Voltage Characteristics ◽  
Transient Spectroscopy ◽  
Induced Defects ◽  
Irradiation Induced Defects

The defects formation in ion-irradiated 4H-SiC was investigated and correlated with the electrical properties of Schottky diodes. The diodes were irradiated with 1 MeV Si+-ions, at fluences ranging between 1×109cm-2 and 1.8×1013cm-2. After irradiation, the current-voltage characteristics of the diodes showed an increase of the leakage current with increasing ion fluence. The reverse I-V characteristics of the irradiated diodes monitored as a function of the temperature showed an Arrhenius dependence of the leakage, with an activation energy of 0.64 eV. Deep level transient spectroscopy (DLTS) allowed to demonstrate that the Z1/Z2 center of 4H-SiC is the dominant defect in the increase of the leakage current in the irradiated material.

Study of Compensation Defects and Electron Irradiation-Induced Defects in Undoped SI-InP by Positron Lifetime Spectroscopy

2008 ◽  
Vol 607 ◽  
pp. 134-136
Author(s):  
Y.J. Zhang ◽  
Ai Hong Deng ◽  
You Wen Zhao ◽  
J. Yu ◽  
X.X. Yu ◽  
...  
Keyword(s):  
Electron Irradiation ◽  
Positron Lifetime ◽  
Deep Level ◽  
High Concentration ◽  
Positron Annihilation Lifetime ◽  
Donor Type ◽  
Positron Lifetime Spectroscopy ◽  
Transient Spectroscopy ◽  
Induced Defects ◽  
Irradiation Induced Defects

Positron annihilation lifetime (PAL) spectroscopy，photo-induced current transient spectroscopy (PICTS) and thermally stimulated current (TSC) have been employed to study the formation of compensation defects and their evolvement under iron phosphide (IP) ambience or pure phosphide (PP) ambience. In the formation of IP SI-InP, the diffusion of Fe atoms suppresses the formation of some open-volume defects. As to PP SI-InP, VInH4 complexes dissociate into acceptor vacancies VInHn(n-3)(n=0,1,2,3), which compensate residual donor type defects and make the sample semi-insulating. Electron irradiation-induced deep level defects have been studied by TSC in PP and IP SI-InP, respectively. In contrast to a high concentration of irradiation-induced defects in as-grown and PP annealed InP, IP SI-InP has a very low concentration of defects.

Transport Properties and Conduction Band Offset of n-ZnO/n-6H-SiC Heterostructures

2006 ◽  
Vol 957 ◽  
Author(s):  
Yahya Alivov ◽  
Xiao Bo ◽  
Fan Qian ◽  
Daniel Johnstone ◽  
Cole Litton ◽  
...  
Keyword(s):  
Conduction Band ◽  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
Band Offset ◽  
Measured Temperature ◽  
Temperature Dependent ◽  
Conduction Band Offset ◽  
Current Voltage ◽  
Current Voltage Characteristics ◽  
Transient Spectroscopy

ABSTRACTThe conduction band offset of n-ZnO/n-6H-SiC heterostructures fabricated by rf-sputtered ZnO on commercial n-type 6H-SiC substrates has been measured. Temperature dependent current-voltage characteristics, photocapacitance, and deep level transient spectroscopy measurements showed the conduction band offsets to be 1.25 eV, 1.1 eV, and 1.22 eV, respectively.

Electronic Properties of ZnO/Si Heterojunction Prepared by ALD.

2011 ◽  
Vol 178-179 ◽  
pp. 130-135 ◽  
Author(s):  
Vincent Quemener ◽  
Mari Alnes ◽  
Lasse Vines ◽  
Ola Nilsen ◽  
Helmer Fjellvåg ◽  
...  
Keyword(s):  
Electronic Properties ◽  
Deep Level ◽  
Atomic Layer ◽  
Substantial Improvement ◽  
Conduction Band Edge ◽  
Energy Position ◽  
Layer Deposition ◽  
Current Voltage ◽  
Capacitance Voltage ◽  
Transient Spectroscopy

ZnO/n-Si and ZnO/p-Si heterostructures were prepared by Atomic layer deposition (ALD) and the electronic properties have been investigated by Current-Voltage (I-V), Capacitance-Voltage (C-V) and Deep level transient spectroscopy (DLTS) measurements. DLTS measurements show two dominants electron traps at the interface of the ZnO/n-Si junction with energy position at 0.07 eV and 0.15 eV below the conduction band edge, labelled E(0.07) and E(0.15), respectively, and no electrically active defects at the interface of the ZnO/p-Si junction. E(0.07) is reduced by annealing up to 400°C while E(0.15) is created at 500°C. The best heterostructure is found after heat treatment at 400°C with a substantial improvement of the current rectification for ZnO/n-Si and the formation of Ohmic contact on ZnO/p-Si. A reduction of the interface defects correlates with an improvement of the crystal structure of the ZnO film with a preferred orientation along the c-axis.

Electrical Characterization of N+-implanted n-type ZnO Single Crystals: p-n Homojunction and Deep Level Defects

2007 ◽  
Vol 1035 ◽  
Author(s):  
Qilin Gu ◽  
Xuemin Dai ◽  
Chi-Chung Ling ◽  
Shijie Xu ◽  
Liwu Lu ◽  
...  
Keyword(s):  
Single Crystals ◽  
Thermal Evolution ◽  
Deep Level ◽  
Schottky Diodes ◽  
Control Sample ◽  
Electrical Characterization ◽  
Type Layer ◽  
Current Voltage ◽  
Transient Spectroscopy ◽  
Induced Defects

AbstractUnintentionally doped n-type ZnO single crystals were implanted by nitrogen ions with different fluences of 1013, 1014 and 1015 cm−2 respectively. ZnO p-n homojunction was successfully fabricated due to the formation of p-type layer after 650°C post-implantation annealing in air for 30 minutes. Further thermal evolution of deep level defects was studied through thermal annealing up to 1200°C. Electrical characterization techniques including current-voltage (I-V), capacitance-voltage (C-V), Deep Level Transient Spectroscopy (DLTS) and double-correlation DLTS (DDLTS) were used for investigating the control sample, all the as-implanted and annealed samples through Au/n-ZnO Schottky diodes as well as ZnO p-n junctions. Detailed electrical properties of fabricated devices and characteristics of implantation induced defects were analyzed based on plentiful DLTS spectra. Moreover, low-temperature photoluminescence experiments of all the as-implanted and annealed samples were performed and the correlation between results from electrical and optical characterizations was discussed.

Maskless Formation of Tungsten Films by Ion Beam Assisted Deposition Technique

1989 ◽  
Vol 158 ◽  
Author(s):  
Zheng Xu ◽  
Toshihiko Kosugi ◽  
Kenji Gamo ◽  
Susumu Namba
Keyword(s):  
Deep Level ◽  
Ion Beam ◽  
Low Energy ◽  
Deposition Technique ◽  
Film Properties ◽  
Ion Beam Assisted Deposition ◽  
Current Voltage ◽  
Residual Damage ◽  
Current Voltage Characteristics ◽  
Transient Spectroscopy

ABSTRACTW films were deposited on n-GaAs by ion beam assisted deposition technique using low energy H2+ and Ar+, and film properties and residual damage in the substrate were investigated by measuring X-ray photoemission, current-voltage characteristics and deep level transient spectroscopy. Films with a resistivity of 1O−5 ohm·cm were formed. It was observed that damage can be reduced using the low energy beams and that Schottky contacts with n-factor of almost 1 and barrier height of 0.88 eV were formed.

Ion Implantation-Induced Defects and the Influence of Titanium Silicidation

1998 ◽  
Vol 510 ◽  
Author(s):  
D.Z. Chi ◽  
S. Ashok ◽  
D. Theodore
Keyword(s):  
Ion Implantation ◽  
Thermal Processing ◽  
Thermal Evolution ◽  
Deep Level ◽  
Rapid Thermal Processing ◽  
Current Voltage ◽  
Transient Spectroscopy ◽  
Thermal Signature ◽  
P Type ◽  
Induced Defects

AbstractThermal evolution of ion implantation-induced defects and the influence of concurrent titanium silicidation in pre-amorphized p-type Si (implanted with 25 KeV, 1016 cm2Si+) under rapid thermal processing (RTP) have been investigated. Presence of implantation-induced electrically active defects has been confirmed by current-voltage (IV) and deep level transient spectroscopy (DLTS) measurements. DLTS characterization results show that the evolution of electrically active defects in the Si implanted samples under RTP depend critically on the RTP temperature: Hole traps HI (0.33 eV) and H4 (0.47 eV) appear after the highest temperature (950 °C) anneal, while a single trap H3 (0.26 eV) shows up at lower anneal temperatures (≤ 900 °C). The thermal signature of H4 defect is very similar to that of the iron interstitial while those of HI and H3 levels appear to originate from some interstitial-related defects, possibly complexes. A most interesting finding is that the above interstitial related defects can be eliminated completely with Ti silicidation, apparently a result of vacancy injection. However the silicidation process itself introduces a new H2 (0.30 eV) level, albeit at much lower concentration. This same H2 level is also seen in unimplanted samples under RTP. The paper will present details of defect evolution under various conditions of RTP for samples with and without the self-implantation and silicidation.

Contact-Related Deep States in AI-GaInP/GaAs Interface

1993 ◽  
Vol 325 ◽  
Author(s):  
Z.C. Huang ◽  
C.R. Wie
Keyword(s):  
Deep Level ◽  
Schottky Diodes ◽  
Schottky Contact ◽  
Temperature Dependent ◽  
Current Voltage ◽  
Oxygen Contamination ◽  
Related Defect ◽  
Current Voltage Characteristics ◽  
Transient Spectroscopy ◽  
Recombination Current

AbstractDeep levels have been measured in molecular beam epitaxy grown Ga0.51In0.49P/GaAs heterostructure by double correlation deep level transient spectroscopy. Gold(Au) and Aluminum (Al) metals were used for Schottky contact. A contact-related hole trap with an activation energy of 0.50-0.75eV was observed at the A1/GaInP interface, but not at the Au/GaInP interface. To our knowledge, this contact-related trap has not been reported before. We attribute this trap to the oxygen contamination, or a vacancy-related defect, VIn or VGa. A new electron trap at 0.28eV was also observed in both Au- and Al-Schottky diodes. Its depth profile showed that it is a bulk trap in GaInP epilayer. The temperature dependent current-voltage characteristics (I-V-T) show a large interface recombination current at the GaInP surface due to the Al-contact. Concentration of the interface trap and the magnitude of recombination current are both reduced by a rapid thermal annealing at/or above 450°C after the aluminum deposition.

Electronic Properties Of Defects Formed In n-Si During Sputter-Etching In An Ar Plasma

1996 ◽  
Vol 442 ◽  
Author(s):  
P. N. K. Deenapanray ◽  
F. D. Auret ◽  
C. Schutte ◽  
G. Myburg ◽  
W. E. Meyer ◽  
...  
Keyword(s):  
Plasma Etching ◽  
Deep Level ◽  
High Energy ◽  
Barrier Heights ◽  
Opposite Trend ◽  
Current Voltage ◽  
Capacitance Voltage ◽  
Ar Plasma ◽  
Transient Spectroscopy ◽  
Sputter Etching

AbstractWe have employed current-voltage (IV), capacitance-voltage (CV) and deep level transient spectroscopy (DLTS) techniques to characterise the defects induced in n-Si during RF sputter-etching in an Ar plasma. The reverse leakage current, at a bias of 1 V, of the Schottky barrier diodes fabricated on the etched samples was found to decrease with etch time reaching a minimum at 6 minutes and thereafter increased. The barrier heights followed the opposite trend. The plasma processing introduced six prominent deep levels below the conduction band of the substrate. A comparison with the defects induced during high energy (MeV) alpha-particle, proton and electron irradiation of the same material revealed that plasma-etching created the VO- and VP-centres, and V2-10. Some of the remaining sputter-etching-induced (SEI) defects have tentatively been related to those formed during either 1 keV He- or Ar-ion bombardment.

Characterization of CdS–CuInSe2 solar cells by current–voltage, capacitance–voltage, and capacitance-transient measurements

1987 ◽  
Vol 65 (8) ◽  
pp. 966-971 ◽  
Author(s):  
N. Christoforou ◽  
J. D. Leslie ◽  
S. Damaskinos
Keyword(s):  
Solar Cells ◽  
Deep Level ◽  
Current Voltage ◽  
Capacitance Voltage ◽  
Carrier Trap ◽  
Transient Spectroscopy ◽  
Increasing Temperature ◽  
P Type ◽  
Capacitance Transient ◽  
Transient Measurements

CdS–CuInSe2 solar cells, which have an efficiency of 9%, have been studied by current–voltage, capacitance–voltage, and capacitance-transient measurements over the temperature range 90–380 K. Deep-level transient spectroscopy analysis of the capacitance transient measurements reveals one majority carrier trap with an activation energy of 0.70 ± 0.02 eV. Although the present experiment cannot establish definitely if the trap is in the CdS or CuInSe2 layer, arguments are presented that it is a hole trap in the p-type CuInSe2 layer. Current–voltage measurements indicate a reversible increase in the reverse-bias leakage current with increasing temperature above 300 K. Evidence is presented that suggests that the rectifying barrier height in the CdS–CuInSe2 solar cell decreases rapidly with temperature above 300 K. Capacitance versus voltage measurements suggest that the depiction layer being studied is primarily in the CuInSe2, but the temperature dependence of the ionized charge concentration N(x) cannot be totally explained although one possible cause is suggested.

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