Oxide Degradation Resulting from Photoresist Ashing

1993 ◽  
Vol 309 ◽  
Author(s):  
P. I. Mikulan ◽  
T. T. Koo ◽  
O. O. Awadelkarim ◽  
S. J. Fonash ◽  
T. Ta ◽  
...  

AbstractIn this study, possible SiO2 damage that could result from several different photoresist ashing techniques has been assessed using patterned photoresist over blanket oxides. The types of ashing systems used were RF power (RF), upstream ozone generator (Upstream) and two microwave power reactors (Microwave 1 and Microwave 2). Aluminum capacitors were evaporated on the samples after the ashing for oxide evaluation. Electrical characterization of these MOS structures included capacitance verses voltage and time dependent dielectric breakdown measurements. We also looked for Si substrate damage in these samples using deep level transient spectroscopy and Schottky barrier current-voltage measurements. This characterization showed oxide damage varied widely with ashing tool. In all cases, however, there was no significant Si substrate damage.

Materials ◽  
2021 ◽  
Vol 14 (8) ◽  
pp. 1966
Author(s):  
Domenico Pellegrino ◽  
Lucia Calcagno ◽  
Massimo Zimbone ◽  
Salvatore Di Franco ◽  
Antonella Sciuto

In this study, 4H-SiC p–n junctions were irradiated with 700 keV He+ ions in the fluence range 1.0 × 1012 to 1.0 × 1015 ions/cm2. The effects of irradiation were investigated by current–voltage (I–V) and capacitance–voltage (C–V) measurements, while deep-level transient spectroscopy (DLTS) was used to study the traps introduced by irradiation defects. Modifications of the device’s electrical performances were observed after irradiation, and two fluence regimes were identified. In the low fluence range (≤1013 ions/cm2), I–V characteristics evidenced an increase in series resistance, which can be associated with the decrease in the dopant concentration, as also denoted by C–V measurements. In addition, the pre-exponential parameter of junction generation current increased with fluence due to the increase in point defect concentration. The main produced defect states were the Z1/2, RD1/2, and EH6/7 centers, whose concentrations increased with fluence. At high fluence (>1013 ions/cm2), I–V curves showed a strong decrease in the generation current, while DLTS evidenced a rearrangement of defects. The detailed electrical characterization of the p–n junction performed at different temperatures highlights the existence of conduction paths with peculiar electrical properties introduced by high fluence irradiation. The results suggest the formation of localized highly resistive regions (realized by agglomeration of point defects) in parallel with the main junction.


2007 ◽  
Vol 1035 ◽  
Author(s):  
Qilin Gu ◽  
Xuemin Dai ◽  
Chi-Chung Ling ◽  
Shijie Xu ◽  
Liwu Lu ◽  
...  

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.


1998 ◽  
Vol 510 ◽  
Author(s):  
P.N.K. Deenapanray ◽  
F.D. Auret ◽  
M.C. Ridgway ◽  
S.A. Goodman ◽  
G. Myburg

AbstractWe report on the electrical properties of defects introduced in epitaxially grown n-Si by 1 keV He-, Ne-, and Ar-ion bombardment. Epitaxial layers with different O contents were used in this study. We demonstrate using deep level transient spectroscopy that the low energy ions introduced a family of similarly structured defects (DI) with electronic levels at ∼0.20 eV below the conduction band. The introduction of this set of identical defects was not influenced by the presence of O. Ion bombardment of O-rich Si introduced another family of prominent traps (D2) with levels close to the middle of the band gap. Both sets of defects were thermally stable up to ∼400 °C, and their annealing was accompanied by the introduction of a family of secondary defects (D3). The “D3” defects had levels at ∼0.21 eV below the conduction band and were thermally stable at 650 °C. We have proposed that the “DI”, “D2”, and “D3” defects are higherorder vacancy clusters (larger than the divacancy) or complexes thereof.


2004 ◽  
Vol 241 (12) ◽  
pp. 2811-2815 ◽  
Author(s):  
J. S. Kim ◽  
E. K. Kim ◽  
H. J. Kim ◽  
E. Yoon ◽  
I.-W. Park ◽  
...  

1996 ◽  
Vol 442 ◽  
Author(s):  
D. Seghier ◽  
H.P. Gislason

AbstractUsing current-voltage measurements, deep-level transient spectroscopy and admittance spectroscopy we investigated nitrogen doped ZnSe grown on p-GaAs substrates by molecular beam epitaxy. Three major hole traps were observed with energy levels at 0. 11, 0.46, and 0.56 eV from the valence band. We attribute the level at 0.11 eV to a nitrogen acceptor. No other direct observations of this important acceptor level in p-ZnSe have been reported in the literature so far. The two remaining levels may originate from the nitrogen doping process. In addition, reverse current-voltage characteristics of the ZnSe/GaAs heterojunction show a hysteresis at low temperature and a soft saturation. At a constant reverse bias the current increases slowly until it reaches a steady state value. This behavior is attributed to a slow voltage-induced barrier lowering due to the presence of mismatch interface states. Therefore, these analyses are of a major interest for applications of ZnSe/GaAs based devices and illustrates the necessity of improving the growth conditions of such structures.


1995 ◽  
Vol 78 (9) ◽  
pp. 5325-5330 ◽  
Author(s):  
Jaime M. Martin ◽  
S. García ◽  
I. Mártil ◽  
G. González‐Díaz ◽  
E. Castán ◽  
...  

2018 ◽  
Vol 924 ◽  
pp. 253-256 ◽  
Author(s):  
Giovanni Alfieri ◽  
Lukas Kranz ◽  
Lars Knoll ◽  
Vinoth Kumar Sundaramoorthy

The electrical characterization of high-purity semi-insulating 4H-SiC is carried out by means of current deep level transient spectroscopy (I-DLTS). Measurements are performed by employing either an electrical or optical pulse (below/above bandgap). The study performed on as-grown material, either annealed or oxidized, reveals the presence of six levels with ionization energies in the 0.4-1.3 eV range.


2011 ◽  
Vol 679-680 ◽  
pp. 804-807 ◽  
Author(s):  
F. Danie Auret ◽  
Walter E. Meyer ◽  
M. Diale ◽  
P.J. Janse Van Rensburg ◽  
S.F. Song ◽  
...  

Gallium nitride (GaN), grown by HVPE, was implanted with 300 keV Eu ions and then annealed at 1000 oC . Deep level transient spectroscopy (DLTS) and Laplace DLTS (L-DLTS) were used to characterise the ion implantation induced defects in GaN. Two of the implantation induced defects, E1 and E2, with DLTS peaks in the 100 – 200 K temperature range, had DLTS signals that could be studied with L-DLTS. We show that these two defects, with energy levels of 0.18 eV and 0.27 eV below the conduction band, respectively, are two configurations of a metastable defect. These two defect states can be reproducibly removed and re-introduced by changing the pulse, bias and temperature conditions, and the transformation processes follow first order kinetics.


2003 ◽  
Vol 764 ◽  
Author(s):  
M. Ahoujja ◽  
H. C. Crocket ◽  
M. B. Scott ◽  
Y.K. Yeo ◽  
R. L. Hengehold

AbstractWe report on the electrical properties of defects introduced in epitaxial 4H-SiC by 2 MeV protons using deep level transient spectroscopy (DLTS). After proton irradiation with a dose of about 1.5×1014 cm-2, the DLTS measurements were made, and the rate window shows a single broad peak between 280 and 310 K. The intensity of this peak remains unchanged after a thermal anneal at 900°C for 20 min. However, after annealing at or above 1100°C, the peak intensity gradually decreases with anneal temperature up to 1500°C, indicating a decrease in the defect concentration. Because a complete damage recovery of the SiC is not observed even after annealing at 1500°C, we believe a higher temperature annealing is necessary for a complete recovery. Using a curve fit analysis, a set of deep levels of defect centers were found with energy ranging between 567 and 732 meV. These traps do not exhibit a significant change in the trap energy or capture cross-section parameters as a function of anneal temperature, but the decrease in the trap density with increasing anneal temperature demonstrates a damage recovery.


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