共查询到19条相似文献,搜索用时 156 毫秒
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本文从广义协变的运动方程和麦克斯韦方程出发,导出了电子等离子体波各量的解析表达式。指出△ω=2ωp的等离子体波是完全简谐的。完全共振的条件由△ω=2ω(p0)[1+(e2(A2((1)2)+(A2((2)2))/(2m2c4)+(3e2A2(1)A2(2))/(m2c4)]-1/2 给出。
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采用两维PIC/MCC模型模拟了氮气微空心阴极放电以及轰击离子 (N2+,N+) 的钛阴极溅射. 主要计算了氮气微空心阴极放电离子 (N2+,N+) 及溅射原子Ti的行为分布, 并研究了溅射Ti 原子的热化过程. 结果表明: 在模拟条件下, 空心阴极效应是负辉区叠加的电子震荡; 在对应条件下, 微空心较传统空心放电两种离子 (N2+,N+) 密度均大两个量级, 两种离子的平均能量的分布及大小几乎相同; 在放电空间N+的密度约为N2+的1/6, 最大能量约大2倍; 在不同参数 (P, T, V)下, 轰击阴极内表面的氮离子(N2+,N+)的密度近似均匀, 其平均能量几乎相等; 从阴极溅射出的Ti原子的初始平均能量约6.8 eV, 离开阴极约0.15 mm处几乎完全被热化. 模拟结果为N2微空心阴极放电等离子体特性的认识提供了参考依据.
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微空心阴极放电
PIC/MC模拟
2等离子体')" href="#">N2等离子体 相似文献
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本文指出,对于实际的归一化有效声子谱函数g(ω),一般来说,zph≡F(-ωph-2是函数z=F(y)≡∫0(ωph)(ω2y)/(ω2y+1)g(ω)dω的反函数的分支点。因此,在估算超导Tc级数的收敛半径时,应当予以考虑。
关键词: 相似文献
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The optical properties of deep hole traps H4 and H5 in p type and of the deep electron trap E11 in n type InP, introduced by electron irradiation, have been studied using deep level optical spectroscopy. Comparison of the optical threshold with the thermal activation energy of H5 level shows that it is highly relaxed with a Frank-Condon shift dFc = 0.45 eV. The electron level E11 is weakly relaxed and its optical cross section σ 0 is well accounted for by transitions to the Γ6c minimum. The optical absorption σp0 associated to level H4 shows two successive onsets at hν = 0.5 and hν = 1.2 eV which can be attributed to hole transitions to the Γ7–8 and to the L4–5 valence band extrema, respectively. The deduced Frank-Condon shift, dFc = 0.23 eV, agrees with the measured difference of 40 meV between its apparent activation energy Ea and its thermal activation energy ET. 相似文献
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F.D. Auret P.J. Janse van Rensburg W.E. Meyer S.M.M. Coelho Vl. Kolkovsky J.R. Botha C. Nyamhere A. Venter 《Physica B: Condensed Matter》2012,407(10):1497-1500
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
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Two new DLTS bands I and II have been observed in n-type germanium containing 1016 cm-3 interstitial oxygen. The signature of II is: Ec?EII = 0.031 eV, K = 4 × 107 cm?2s?1; level I is about half as deep. In addision, the excitation spectrum of I is recorded by PTIS. It is composed of three hydrogenic donor series Ia, b, c with activation energies 17.25, 17.6 and 18.1 meV. The donors I and II are thought to correspond with the well known thermal oxygen donors. Energies for the latter were determined at 0.017 and 0.04 eV from Hall effect by Fuller and Doleiden. The possibility of double donors is examined, in analogy with the case of oxygen donors in silicon. 相似文献
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Abstract The nature of the irradiation induced defects in germanium single crystal doped with tellurium was studied by DLTS and electrical measurements. The Ec-0.21 eV level produced by irradiation with 1.5 MeV electrons was studied by DLTS technique. It was found that the defect associated with the Ec-0.21 eV level is divacancy. The E-center like defect (group V impurity-vacancy pair) introduces the Ec-0.20 eV level in samples doped with group V impurity. The level introduced by tellurium (group VI impurity)-vacancy pair is located at deeper than Ec-0.21 eV. The Ec-0.16 eV level was generated by the annealing at 430 K. A model for the defect associated with the level is proposed to be a tellurium-vacancies complex. 相似文献
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J. Bartoš E. Pinčík I. Thurzo O. E. Balvinskij J. Ivančo 《Czechoslovak Journal of Physics》1993,43(9-10):875-879
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
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Deep-level transient spectroscopy (D.L.T.S.) has been applied to the determination of defects in ion implanted silicon. Preliminary
results concerning defects introduced by 130 KeV phosphorous ion implantation are described. Four electron traps are found:
atE
c
-0.21 eV,E
c
-0.39 eV,E
c
-0.52 eV andE
c
-0.58 eV and their cross-sections estimated. The annealing behaviour in the range 450–800°C of these traps is described.
Work supported in part by the Institute of Physics, Polish Academy of Science, Warsaw.
Laboratoire associé au C.N.R.S. 相似文献
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The temperature dependent visible photoluminescence (PL) property of a-SiOx:H (x<2) samples prepared in a PECVD system by using SiH4+CO2 gas mixture is investigated at a temperature range of 20 K-400 K. One of the two explicitly distinguished PL bands, with varying peak photon energies between 1.70 and 2.05 eV, can be detected at only low temperatures below 200 K, which is attributed to tail-to-tail radiative recombination. Thermal quenching parameter (TL) of the tail-to-tail PL band is calculated as varying between 120 and 280 K as the atomic oxygen concentration ([O]at.%) of the samples increases. Stokes shift (ΔEStokes) of the tail-to-tail PL band is found to change from 85 meV to 420 meV due to band tail widening. The other PL band emerges at 2.1 eV and can be detected at higher temperatures with thermal activation behavior. The activation energies calculated about room temperature vary in the range of 8 meV-50 meV with oxygen concentration. Thermal activation of the 2.1 eV PL band is attributed to the behavior of thermally activated incoherent hopping migration of electrons. These electrons combine with self trapped holes (STHs) to form self trapped excitons (STEs). STEs are localized at intrinsic defects of SiO2 structure such as oxygen vacancies (E′ centers) and non-bridging oxygen hole centers (NBOHC). 相似文献
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We present the first investigation of the stress-induced coupling between X1c and X3c conduction band minima in zincblende type semiconductors. The high uniaxial stress values achieved in this work (X= 19 kbar) enable us to observe a nonlinear behavior of the X1c minima due to the stress-induced X1c-X3c coupling. This coupling is described by a single deformation potential 6E36 = 13 eV. 相似文献
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The photoluminescence of the 1.55 eV band of Ge doped A?xGa1?xAs, with x=0.30–0.33, grown by liquid phase epitaxy is presented. The broad shape was found to be due to a lattice relaxation upon optical transitions. Resonant modes with ?ωq = 35±2 meV and ?ωq = 45±2 meV are found for the optical band, yielding a zero phonon transition energy = 1.73±0.02 eV and a Franck-Condon shift = 0.17–0.20 eV for the optical center. The activation energy of thermal quenching yields an associated donnor binding energy of 0.17±0.04 eV. Possible mechanisms for the radiative transitions are discussed. 相似文献