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1.
280-nm-thick silicon-on-insulator films are implanted with high doses of hydrogen with the energy 24 keV and the dose 5 × 1017 cm?2. Peaks corresponding to optical phonons localized in the silicon nanocrystals 1.9?C2.5 nm in size are observed in the Raman spectra. The fraction of the nanocrystal phase is ??10%. A photoluminescence band with a peak at about 1.62 eV is detected. The intensity of the 1.62 eV band nonmonotonically depends on the measurement temperature in the range from 88 to 300 K. An increase in the radiative recombination intensity at temperatures <150 K is interpreted in the context of a two-level model for the energy of strongly localized electrons and holes. The activation energy of photoluminescence enhancement is 12.4 meV and corresponds to the energy of splitting of the excited state of charge carriers localized in the silicon nanocrystals.  相似文献   

2.
The special features of photoluminescence spectra of silicon-on-insulator structures implanted with hydrogen ions are studied. An increase in the photoluminescence intensity with increasing hydrostatic pressure P during annealing and the formation of narrow periodic photoluminescence peaks in the spectral range from ~500 to 700 nm are revealed for the structures annealed at P > 6 kbar. It is shown that the fine structure of the photoluminescence spectra correlates with the slowing-down of hydrogen effusion from the implanted samples and with the suppression of the formation of hydrogen microbubbles in the surface layer. These processes promote the formation of an optical resonator, with the mirrors formed by the “silicon-on-insulator-air” and “silicon-on-insulator-SiO2” interfaces and with the optically active layer formed by hydrogen ion implantation and subsequent annealing.  相似文献   

3.
The properties of silicon-on-insulator films implanted with high hydrogen-ion doses (~50 at %) and annealed under a pressure of 10.5 kbar are studied using the Raman scattering (RS) method. A high degree of optical-phonon localization is detected in the films under study, which is retained to an annealing temperature of ~1000°C and is explained by the formation of silicon nanocrystals. It is found that the activation energy of annealing of the structural relaxation of dangling bonds in films with a high hydrogen content is independent of the annealing pressure. The activation energy of growth of the crystalline phase, calculated from RS spectra is ~1.5 eV and is independent of pressure. The effect of hydrostatic pressure consists only in a decrease in the frequency factor limiting Si-Si bond relaxation during ordering.  相似文献   

4.
GaAs samples were implanted with 100–400 keV, 1012–1014/cm2Se+ ions and annealed using undiffused and diffused pulsed ruby-laser beams with the samples held at various temperatures.

The resulting surface and structural defects as observed by various microscopic and spectroscopic methods are related to measured electrical properties of implanted GaAs, and the causes of the observed poor and lack of electrical activation of samples identified.

Laser irradiation of samples (T ≈ 516°C) induces surface damage in the form of regular parallel broken lines with a periodicity of about 0.69 μm, the wavelength of the ruby laser.

A diffused laser beam (0.5 J/cm2) reduces surface vaporisation and eliminates periodic surface structures. The measured electrical properties are still poor.  相似文献   


5.
Sulfur ions were implanted into semi-insulating GaAs. A SiO2 film was deposited by either of two methods onto the implanted surface. The samples were then subjected to either rapid thermal annealing (using halogen lamps) for 10–12 s at 805°C or to conventional thermal annealing for 30 min at 800°C. The content of GaAs components in the film was determined from the spectra of Rutherford backscattering. The electron-concentration profiles were plotted using the measurements of the capacitance-voltage characteristics. It is shown that sulfur diffuses in two directions, i.e., towards the surface and into the GaAs bulk. The former process is stimulated by vacancies formed near the semiconductor surface during the deposition of SiO2. The coefficients of the “volume” diffusion of S and of the diffusion of S towards the surface are two orders of magnitude larger upon rapid thermal annealing than upon conventional thermal annealing, with the degree of S activation also being higher.  相似文献   

6.
利用Kr准分子激光器晶化非晶硅薄膜, 研究了不同的激光能量密度和脉冲次数对非晶硅薄膜晶化效果的影响.利用X 射线衍射(XRD)和扫描电子显微镜(SEM)对晶化前后的样品的物相结构和表面形貌进行了表征和分析.实验结果表明, 在激光频率为1 Hz 的条件下, 能量密度约为180 mJ/cm2时,准分子激光退火处理实现了薄膜由非晶结构向多晶结构的转变;当大于晶化阈值180 mJ/cm2小于能量密度230 mJ/cm2时, 随着激光能量密度增大, 薄膜晶化效果越来越好;激光能量密度为230 mJ/cm2时, 晶化效果最好、晶粒尺寸最大, 约60 nm, 并且此时薄膜沿Si(111)面择优生长;脉冲次数50 次以后对晶化的影响不大.  相似文献   

7.
Luminescent and structural properties of n-FZ-Si and n-Cz-Si implanted with Si ions at amorphizing doses and annealed at 1100°C in a chlorine-containing atmosphere have been studied. An analysis of proton Rutherford backscattering spectra of implanted samples demonstrated that an amorphous layer is formed, and its position and thickness depend on the implantation dose. An X-ray diffraction analysis revealed that defects of the interstitial type are formed in the samples upon annealing. Photoluminescence spectra measured at 78 K and low excitation levels are dominated by the dislocation-related line D1, which is also observed at 300 K. The peak position of this line, its full width at half-maximum, and intensity depend on the conduction type of Si and implantation dose. As the luminescence excitation power is raised, a continuous band appears in the spectrum. A model is suggested that explains the fundamental aspects of the behavior of the photoluminescence spectra in relation to the experimental conditions.  相似文献   

8.
The physical and electrical properties of BF 2 + implanted polysilicon films subjected to rapid thermal annealing (RTA) are presented. It is found that the out diffusion ofF and its segregation at polysilicon/silicon oxide interface during RTA are the major causes ofF anomalous migration. Fluorine bubbles were observed in BF 2 + implanted samples at doses of 1×1015 and 5×1015 cm−2 after RTA.  相似文献   

9.
Changes induced by annealing the spectrum of states on a Si/SiO2 interface obtained by direct bonding and on a Si(substrate)/〈thermal SiO2〉 interface in silicon-on-insulator (SOI) structures were investigated by charge-related deep-level transient spectroscopy. The structures were formed by bonding silicon wafers and slicing one of the wafers along a plane weakened by hydrogen implantation. The SOI structures were annealed at 430°C for 15 min in hydrogen, which corresponded to the conventional mode of passivation of the Si/SiO2-interface states. The passivation of interface states by hydrogen was shown to take place for the Si/〈thermal SiO2〉 interface, as a result of which the density of traps substantially decreased, and the continuous spectrum of states was replaced by a band of states in the energy range E c=0.1–0.35 eV within the entire band. For the traps on the bonded Si/SiO2 interface, the transformation of the centers occurs; namely, a shift of the energy-state band is observed from E c=0.17–0.36 to 0.08–0.22 eV. The trapping cross section decreases by about an order of magnitude, and the density of traps observed increases slightly.  相似文献   

10.
Crystalline Si implanted with the 380-keV cobalt ions with the dose Φ = 1014?1016 cm?2 is studied. The method of Rutherford backscattering is used to determine the Si amorphization threshold (Φ = 3 × 1014 cm?2). A quasi-resonance anisotropic line with a width of approximately 170 mT is observed at a temperature of T = 78 K in the spectrum of the electron spin resonance of silicon implanted with Co+ ions with Φ ≥ 3 × 1014) cm?2. A resonance signal of paramagnetic centers in amorphous Si regions (g = 2.0057 and δB = 0.74 mT) is observed against the background of the above line. A quasi-resonance line of the electron spin resonance related to Co atoms and intrinsic Si defects was not observed at T = 300 K.  相似文献   

11.
Rapid thermal processing utilizing microwave energy has been used to anneal N, P, and Al ion-implanted 6H-SiC. The microwaves raise the temperature of the sample at a rate of 200°C/min vs 10°C/min for conventional ceramic furnace annealing. Samples were annealed in the temperature range of 1400-1700°C for 2-10 min. The implanted/annealed samples were characterized using van der Pauw Hall, Rutherford backscattering, and secondary ion mass spectrometry. For a given annealing temperature, the characteristics of the microwave-annealed material are similar to those of conventional furnace anneals despite the difference in cycle time.  相似文献   

12.
本文对不同衬底制备的VO2 薄膜进行了表面形貌测试 ,对其红外透射光谱和Raman光谱进行了研究 ,并进行 370nm -90 0nm波段的光透射测试以及 90 0nm波长的热滞回线特性测试 ,表明所制备VO2 薄膜具有优良的热致相变光学特性 ,薄膜为纳米结构 ,并且结晶状态不同的薄膜其Raman谱位置有明显改变 ,室温时的红外光谱表现出较好的红外振动特性。讨论了薄膜结晶状态对Raman位移的影响以及VO2 薄膜的红外光谱  相似文献   

13.
High concentrations (0.1–5 at.%) of Mn or Fe were introduced into the near-surface region (≤2000 Å) of 6H-SiC substrates by direct implantation at ~300°C. After annealing at temperatures up to 1000°C, the structural properties were examined by transmission electron microscopy (TEM) and selected-area diffraction pattern (SADP) analysis. The magnetic properties were examined by SQUID magnetometry. While the Mn-implanted samples were paramagnetic over the entire dose range investigated, the Fe-implanted material displayed a ferromagnetic contribution present at <175 K for the highest dose conditions. No secondary phases were detected, at least not to the sensitivity of TEM or SADP.  相似文献   

14.
The formation of silicon nanocrystals in SiO2 layers implanted with Si ions was investigated by Raman scattering, X-ray photoelectron spectroscopy, and photoluminescence. The excess Si concentration was varied between 3 and 14 at. %. It was found that Si clusters are formed immediately after implantation. As the temperature of the subsequent annealing was raised, the segregation of Si accompanied by the formation of Si-Si4 bonds was enhanced but the scattering by clusters was reduced. This effect is attributed to the transformation of loosely packed clusters into compact, separate-phase nanoscale Si precipitates, with the Raman peak observed at 490 cm?1 being related to surface scattering. The process of Si segregation was completed at 1000°C. Nevertheless, characteristic nanocrystal photoluminescence was observed only after annealing at 1100°C. Simultaneously, scattering in the range 495–520 cm?1, typical of nanocrystals, appeared; however, the “surface-related” peak at 490 cm?1 persisted. It is argued that nanocrystals are composed of an inside region and a surface layer, which is responsible for their increased formation temperature.  相似文献   

15.
The properties of silicon implanted with boron ions through thermal SiO2 films were studied using sheet resistivity measurements (corroborated by Hall data). Electrical properties for implants through 0.1 μm of SiO2, as compared to bare silicon, showed no unusual behavior as a function of anneal temperature. Sheet resistivity measurements as a function of SiO2 thickness for fixed ion energy, and as a function of energy for fixed oxide thickness were made after 525 and 925°C anneals, for boron doses of 1013, 1014 and 1015 ions/cm2. The profile of boron ions in SiO2 is near Gaussian for the energy range investigated and the stopping power is 0 to 20% lower than the theoretical value currently in the literature. Considerations for device manufacture are discussed in light of the results.  相似文献   

16.
The short-wavelength (400–700 nm) photoluminescence (PL) spectra of SiO2 layers implanted with Si+, Ge+, and Ar+ ions in the dose range 3.2×1016–1.2×1017 cm−2 are compared. After Ar+ implantation an extremely weak luminescence, which vanishes completely after annealing for 30 min at 400 °C or 20 ms at 1050 °C, was observed. After implantation of group-IV elements the luminescence intensities were 1 to 2 orders of magnitude higher, and the luminescence remained not only with annealings but it could also increase. The dose and heating dependences of the luminescence show that it is due to the formation of impurity clusters and this process is more likely to be of a percolation than a diffusion character. For both group-IV impurities an intense blue band and a weaker band in the orange part of the spectrum were observed immediately after implantation. The ratio of the excitation and emission energies of the blue luminescence is characteristic of oxygen vacancies in SiO2; its properties are determined by the direct interaction of group-IV atoms. On this basis it is believed that the centers of blue PL are chains of Si (or Ge) atoms embedded in SiO2. The orange luminescence remained after annealings only in the case of Si+ implantation. This is attributed directly to the nonphase precipitates of Si in the form of strongly developed nanometer-size clusters. Fiz. Tekh. Poluprovodn. 32, 439–444 (April 1998)  相似文献   

17.
Zirconia (8 mol% yttria) (YSZ) amorphous layers were deposited by spray pyrolysis on Si oxidized substrates and crystallized by rapid thermal treatment in a home-made halogen lamps furnace. Uniform films were obtained by depositing up to six layers, followed by the thermal treatment. X-ray analysis showed that the cubic phase is obtained during the initial stage of the annealing process. No significant differences with increasing annealing time nor interaction between the YSZ film and the substrate were observed. Ionic conduction in air, with activation energies comparable to those of bulk YSZ ceramics, was observed. The electrical characteristics of the films make them suitable for microelectronics applications.  相似文献   

18.
Bonding and thermal stability of implanted hydrogen in silicon   总被引:1,自引:0,他引:1  
The behavior of implanted hydrogen in Si has been investigated by differential infrared transmittance measurements using multiple-internal-reflection (MIR) plates. Si-H bonding of implanted hydrogen is detected by seven absorption bands between 4.5 and 5.5 μm after implantation with 1016 H+/cm2 at ion energies between 70 and 400 keV. The absorption bands are close in frequency to those for SiH stretching modes for silane, and they are produced only by hydrogen implantation. Implantation with deuterium gave absorption bands shifted to lower frequencies in accord with the square root of the reduced mass ratio for Si-H relative to Si-D. The multiplicity of hydrogen-associated bands is apparently a consequence of defects in the implanted layer. A dependence of the hydrogen-associated bands on the disorder is suggested by the annealing loss of five of the initial seven bands, and a growth of the other two, for the same temperatures (100–300°C) as those for annealing out the broad divacancy band at 1.8 μm. A disorder dependence of the Si-H vibrational frequencies is further demonstrated by a regeneration of the bands annealing below 300°C when a hydrogen-implanted MIR plate annealed at 300°C was subsequently bombarded with neon. In addition to the seven resolved bands after H+ implantation, five other bands in the same range of frequencies grow in and anneal out between 100 and 700°C. Annealing at 700°C eliminates all SiH bands, and they cannot be regenerated by bombardment with other ions. It is suggested that implanted hydrogen in Si is bonded at defect sites, and that a loss of an SiH band is caused by either a change in charge state of a defect or by the loss of a defect. This work was supported by the United States Atomic Energy Commission  相似文献   

19.
Photoluminescence (PL), Raman scattering, and the Rutherford backscattering of α-particles were used to study the formation of the centers of radiative-recombination emission in the visible region of the spectrum on annealing of the SiO2 layers implanted with Ge ions. It was found that the Ge-containing centers were formed in the as-implanted layers, whereas the stages of increase and decrease in the intensities of PL bands were observed following an increase in the annealing temperature to 800°C. The diffusion-related redistribution of Ge atoms was observed only when the annealing temperatures were as high as 1000°C and was accompanied by formation of Ge nanocrystals. However, this did not give rise to intense PL as distinct from the case of Si-enriched SiO2 layers subjected to the same treatment. It is assumed that, prior to the onset of Ge diffusion, the formation of PL centers occurs via completion of direct bonds between the neighboring excess atoms, which gives rise to the dominant violet PL band (similar to the PL of O vacancies in SiO2) and a low-intensity long-wavelength emission from various Ge-containing complexes. The subsequent formation of centers of PL with λm~570 nm as a result of anneals at temperatures below 800°C is explained by agglomeration of bonded Ge atoms with formation of compact nanocrystalline precipitates. The absence of intense PL following the high-temperature anneals is believed to be caused by irregularities in the interfaces between the formed Ge nanoc-rystals and the SiO2 matrix.  相似文献   

20.
真空还原制备的VO2热致相变薄膜光学性质研究   总被引:2,自引:0,他引:2  
卢勇  林理彬 《激光杂志》2001,22(3):8-10
本文对不同衬底制备的VO2薄膜进行了表面形貌测试,对其红外透射光谱和Raman光谱进行了研究,并进行370mm-900nm波段的光透射测试以及900nm波长的热滞回线性测试,表明所制备VO2薄膜具有优良的热致相变光学特性,薄膜为纳米结构,并且结晶状态不同的薄膜其Raman谱位置有改变,室温时的红外光谱表现出较好的红外振动特性。讨论了薄膜结晶状态对Raman位移的影响以及VO2薄膜的红外光谱。  相似文献   

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