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1.
电子辐照硅层中缺陷能级的研究   总被引:5,自引:0,他引:5       下载免费PDF全文
用12MeV电子辐照硅p+n结,在硅中除引入氧空位E1(Ec-0.19eV),双空位E2(Ec-0.24eV)和E4(Ec-0.44eV)外,还引入缺陷E3(Ec-0.37eV)。用DLTS方法和反向恢复时间测量研究了这些能级的退火行为,可以看到,E3的退火温度最高(≈520℃)。由退火特 关键词:  相似文献   

2.
Abstract

Deep level transient spectroscopy has been used to investigate the electrical properties of deep defect states in γ-ray irradiated Ge doped with the isoelectronic elements Pb or Sn. Three deep levels are observed in the irradiated Pb-doped Ge (Ev +0.28 eV, Ec ?0.33 eV, Ec ?0.39 eV) and two deep levels observed in the Sn-doped Ge (Ev + 0.19 eV, Ec ?0.15 eV). For the same γ-ray irradiation doses, Ge crystals grown from graphite crucibles and doped with Pb or Sn shows about two-thirds the total density of deep level defects observed in undoped Ge grown from synthetic quartz crucibles. All of the defect states observed were removed by a 1 hour, 250°C thermal anneal, and all but the Ec ?0.39 eV state in the Pb-doped material were neutralized by exposure to a low pressure atomic hydrogen plasma.  相似文献   

3.
6H-silicon carbide layers are grown by a liquid phase epitaxy (LPE) process. The layers are doped with boron either by ion implantation or during the LPE process from a B-doped silicon melt. Deep-level transient spectroscopy (DLTS), admittance spectroscopy and photoluminescence (PL) are used to investigate deep impurity centers. Two electrically active defect centers are detected: the isolated boron acceptor at E B=E v+0.3eV and the boron-related D-center at E D=E v+0.58eV. The yellow luminescence observed in these layers is proposed to be due to pair recombination via D-center and nitrogen donor. Formation and origin of the D-center are discussed.  相似文献   

4.
The electronic properties of defects introduced by low energy inductively coupled Ar plasma etching of n-type (Si doped) GaAs were investigated by deep level transient spectroscopy (DLTS) and Laplace DLTS. Several prominent electron traps (Ec—0.046 eV, Ec—0.186 eV, Ec—0.314 eV. Ec—0.528 eV and Ec—0.605 eV) were detected. The metastable defect Ec—0.046 eV having a trap signature similar to E1 is observed for the first time. Ec—0.314 eV and Ec—0.605 eV are metastable and appear to be similar to the M3 and M4 defects present in dc H-plasma exposed GaAs.  相似文献   

5.
Recent investigations on transition-metal impurities in silicon emphasizing the effect of the combined diffusion of two transition metals are presented and briefly discussed. The electronic properties and basic thermal kinetics are analysed by DLTS. The conversion of a Pd-related multivalent defect atE c-0.35 eV andE c-0.57 eV to the Pd-related defect atE c –0.22 eV is observed, and a Pd-Fe complex level atE c –0.32 eV is identified. The annealing characteristics of the multivalent Rh levels atE c-0.33 eV andE c-0.57 eV are observed, and used to analyse the influence of prior Rh doping on the Au diffusion. A complex formed by the codiffusion of Au and Cu is observed atE v+0.32eV andE v+0.42 eV, and shown to exhibit bistable behavior as does a similarly produced Au-Ni complex observed atE v + 0.35 eV andE v+0.48 eV.  相似文献   

6.
9 to 1013 particles/cm2 have been investigated by the deep level transient spectroscopy technique and capacitance-voltage profiling. Under low fluence irradiation at least four main electron traps have been observed. With further increase in irradiation fluence, two new levels located at Ec-0.56 eV and Ec-0.64 eV appear on the high-temperature side of the DLTS signal. The slope change observed in the amplitude variations of the singly negative charge state of the divacancy versus the dose takes place when these two new levels appear. This suggests that both are multivacancy-related defects. After annealing at 350 °C for 15 min, all electron traps have disappeared. Moreover, no shallow levels are created during the annealing. Received: 12 December 1996/Accepted: 6 May 1997  相似文献   

7.
Deep-level profiles were measured radially acrossn-type FZ silicon wafers containing A-swirl defects by applying DLTS to an array of Schottky contacts. The trapparameters were obtained very accurately using a computer-fit procedure for the full DLTS peaks. Two acceptor levels atE c −0.49 eV (σ n =6.6×10−16cm2) andE c −0.07 eV (σ n =4.6×10−16cm2) were observed, which varied oppositely to the A-swirl defect density. At short ranges (1–2mm) the trap concentration-profile was smeared out and did not follow the strong fluctuations in the etch pattern. Both levels were measured together with the same concentration. The profiles indicate outdiffusion. A level atE c −0.14 eV (σ n =1.1×10−16cm2) was not related to A-swirl defects. A level atE c −0.11 eV (σ n =1.1×10−15cm2) was only detected in one ingot. The properties of the deep level atE c −0.49 eV are discussed in the light of published DLTS results reported for γ-irradiation, laser annealing after self-implantation, annealing under pressure and oxidation of silicon samples. It is concluded, that this level is related to interstitial silicon rather than to an impurity.  相似文献   

8.
陆昉  龚大卫  孙恒慧 《物理学报》1994,43(7):1129-1136
对同质硅分子束外延层的界面缺陷进行了测试与分析.对存在高浓度施主型界面缺陷的P型材料,通过解泊松方程计算了该材料的肖特基势垒的能带图,得到了该缺陷能级上电子的填充与发射随外加反向偏压变化的情况.并分析了用深能级瞬态谱(DLTS)对其进行测试所需的条件,以及与常规的DLTS测试结果的不同之处.提出了可同时对该缺陷上电子的发射和俘获过程进行DLTS测量的方法.实验测量结果表明,该高密度的界面缺陷的能级位置位于Ec-0.30eV. 关键词:  相似文献   

9.
分别采用二种不同方法测量分子束外延(MBE)生长GaAs/In0.2Ga0.8As单量子阱结构的导带不连续量ΔEc:1) 考虑样品界面电荷修正的电容-电压(C-V)分布;2) 量子阱载流子热发射产生的电容瞬态(DLTS).C-V测得的ΔEc=0.227eV,大约相当于89% ΔEg.DLTS测得的ΔEc=0.229eV,大约相当于89.9% ΔEg.结果 关键词:  相似文献   

10.
The deep level transient spectroscopy (DLTS) peaks are broader in the alloys than the peaks in binary III–V compounds. This effect is related to substitutional disorder present in the alloy which changes the sharp energy levels into a distribution. In this Communication we give relations between the broadened DLTS signal, defect energy level broadening and alloys disorder with particular reference to electron irradiation induced E3 defect in GaAs1xSbx alloys.  相似文献   

11.
Deep level transient spectroscopy (DLTS) is employed to study deep level defects in n-6H-SiC (silicon carbide) epilayers grown by the sublimation method. To study the deep level defects in n-6H-SiC, we used as-grown, nitrogen doped and nitrogen-boron co-doped samples represented as ELS-1, ELS-11 and ELS-131 having net (NDNA) ∼2.0×1012 cm−3, 2×1016 cm−3 and 9×1015 cm3, respectively. The DLTS measurements performed on ELS-1 and ELS-11 samples revealed three electron trap defects (A, B and C) having activation energies Ec – 0.39 eV, Ec – 0.67 eV and Ec – 0.91 eV, respectively. While DLTS spectra due to sample ELS-131 displayed only A level. This observation indicates that levels B and C in ELS-131 are compensated by boron and/or nitrogen–boron complex. A comparison with the published data revealed A, B and C to be E1/E2, Z1/Z2 and R levels, respectively.  相似文献   

12.
Deformation-produced deep levels, both of electron and hole traps, have been studied using deep level transient capacitance spectroscopy (DLTS) for an undopedn-type GaAs (HB grown) compressed at 440°C. Concentrations of two grown-in electron trap levels (E c −0.65eV andE c −0.74eV) and one grown-in hole trap level (E v +∼0.4eV) increase with plastic deformation, while that of a grown-in electron trap level (E c −∼0.3eV) decreases in an early stage of deformation. While no new peak appeared in the electron trap DLTS spectrum after plastic deformation, in the hole trap DLTS spectrum a broad spectrum, seemingly composed of many peaks, newly appeared in a middle temperature range, which may be attributed to electronic energy levels of dislocations with various characters.  相似文献   

13.
Tellurium-related defects inn-type silicon have been analysed by deep level transient spectroscopy (DLTS). The tellurium doping of the samples was performed by ion implantation or during epitaxy. In all the samples, a level having a thermal activation energy around 0.37 eV is observed. This activation energy is found to be dependent on the electric field. Taking into account the Poole-Frenkel (FP) effect and a temperature dependence proportional toT ?2 in the capture cross-section, a value ofE A=0.41eV is obtained. A second Te-related level having an activation energy ofE A=0.14eV without correction of the FP effect could only be measured in the implanted samples. The same concentration is observed for the two levels in the implanted samples thus indicating that both peaks in the DLTS spectra are caused by the identical Te-related defect.  相似文献   

14.
DLTS and thermally stimulated capacitance (TSCap) studies of α-particle irradiated p-Si were undertaken to obtain additional information about the self-interstitial related defect E1=Ec−0.39 eV. The E1 defect can be retained frozen up to room temperature without any minority carrier injection, but under injection conditions at 77–300 K the E1 becomes mobile. As a result of annealing of the E1 defect, the carbon interstitial concentration grows. The E1 defect production rate under reverse bias as well as thermal annealing behavior depends strongly on the temperature and impurity concentration. Numerical estimates of the E1 migration via a Bourgoin–Corbett mechanism are in good agreement with the experimental data obtained.  相似文献   

15.
We discuss DLTS andC-V measurements on Al/Si3N4/Si(2nm)/n-GaAs (≈ 5×1017 cm?3) structures. Three discrete deep traps superimposed on a U-shaped interface-state continuum have been identified, with respective thermal energies:E c?0.53 eV,E c?0.64 eV, andE v+0.69 eV. The second one (0.64 eV) is presented as an electric field sensitive level, its enhanced phonon-assisted emission resulting in a rapid shift of the corresponding DLTS peak to lower temperatures, as the applied (negative) reverse bias voltage increases. An interpretation through emission from the quantum well, introduced by means of the intermediate ultrathin Si layer, has failed.  相似文献   

16.
Deep level transient spectroscopy (DLTS) and Laplace-DLTS have been used to investigate the defects created in Sb doped Ge after irradiation with 2 MeV protons having a fluence of 1×1013 protons/cm2. The results show that proton irradiation resulted in primary hole traps at EV +0.15 and EV +0.30 eV and electron traps at EC ?0.38, EC ?0.32, EC ?0.31, EC ?0.22, EC ?0.20, EC ?0.17, EC ?0.15 and EC ?0.04 eV. Defects observed in this study are compared with those introduced in similar samples after MeV electron irradiation reported earlier. EC ?0.31, EC ?0.17 and EC ?0.04, and EV +0.15 eV were not observed previously in similar samples after high energy irradiation. Results from this study suggest that although similar defects are introduced by electron and proton irradiation, traps introduced by the latter are dose dependent.  相似文献   

17.
The electric field enhanced thermal emission rate was measured for the Ec -0.35 eV level of GaAs using a new reverse-bias pulsed DLTS technique. It is shown that the observed field and its temperature dependencies are probably the result of the Poole-Frenkel emission from a polarization potential well. From this study and with other annealing and the capture cross-section data, it is concluded that the defect is probably of a neutral-impurity type.  相似文献   

18.
This paper describes the effect of 24 MeV proton irradiation on the electrical characteristics of a pnp bipolar junction transistor 2N 2905A. I-V, C-V and DLTS measurements are carried out to characterize the transistor before and after irradiation. The properties of deep level defects observed in the bulk of the transistor are investigated by analysing the DLTS data. Two minority carrier levels, E C − 0.27 eV and E C − 0.58 eV and one majority carrier level, E V +0.18 eV are observed in the base collector junction of the transistor. The irradiated transistor is subjected to isochronal annealing. The influence of isochronal annealing on I-V, C-V and DLTS characteristics are monitored. Most of the deep level defects seem to anneal out above 400°C. It appears that the deep level defects generated in the bulk of the transistor lead to transistor gain degradation. A comparison of proton- and electron-induced gain degradation is made to assess the vulnerability of pnp transistor as against npn transistors.  相似文献   

19.
2 structures implanted with 50-keV boron ions is studied by deep-level transient spectroscopy (DLTS) measurements. The DLTS spectra of ion-implanted samples exhibit one peak which corresponds to a deep level located in the forbidden gap of the silicon matrix at Ec-0.40 eV below the conducting band edge. New additional shallower levels are found in the spectra following bombardment by high-energy electrons, the peak intensity being dependent on the irradiation dose. The corresponding activation energy of the created defects, the density of the traps, and the electron-capture cross sections are evaluated. Received: 27 October 1997/Accepted: 8 December 1997  相似文献   

20.
Deep levels in iron-dopedp-type silicon are investigated by means of Deep Level Transient Spectroscopy (DLTS) and the Hall effect. Pairs of Fe with the acceptors B, Al, and Ga are observed at 0.1, 0.19, and 0.24 eV above the valence band edgeE v. For interstitial iron, (Fe i ), a level energy ofE v+0.39+-0.02 eV is obtained with DLTS after correction with a measured temperature dependence of the capture cross section. The Hall effect yieldsE v+0.37 eV for Fei. The annealing behavior of levels related to Fe is investigated up to 160 °C. Iron participates in at least four different types of impurity states: Fe i , Fe-acceptor pairs, precipitations (formed above 120 °C) and an additional electrically inactive state, which is formed at room temperature.  相似文献   

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