Raman spectroscopy of amorphous silicon subjected to laser annealing

The effect of laser radiation power on the Raman spectra of amorphous silicon obtained by electron-beam evaporation has been revealed. The formation of nanocrystalline inclusions in the amorphous matrix under exposure to a laser with a power of more than 2.5 mW is established by Raman spectroscopy and photoluminescence. The influence of the fabrication conditions (substrate temperature and annealing in a vacuum) of source amorphous silicon films on the formation of nanocrystalline inclusions formed by subsequent laser treatment has been investigated. The features of silicon nanocrystal formation in cases when the original amorphous silicon film is obtained at a substrate temperature of ∼250°C have been revealed. These features may be associated with the presence of silicon-silicon multiple bonds.     

Interaction between rare-earth ions and amorphous silicon nanoclusters produced at low processing temperatures

Temperatures of 1000 °C and higher are a significant problem for the incorporation of erbium-doped silicon nanocrystal devices into standard silicon technology, and make the fabrication of contacts and reflectors in light emitting devices difficult. In the present work, we use energy-filtered TEM imaging techniques to show the formation of size-controlled amorphous silicon nanoclusters in SiO films annealed between 400 and 500 °C. The PL properties of such films are characteristic of amorphous silicon, and the spectrum can be controlled via a statistical size effect—as opposed to quantum confinement—that has previously been proposed for porous amorphous silicon. Finally, we show that amorphous nanoclusters sensitize the luminescence from the rare-earth ions Er, Nd, Yb, and Tm with excitation cross-sections similar in magnitude to erbium-doped silicon nanocrystal composites, and with a similar nonresonant energy transfer mechanism.     

镶嵌有纳米硅的氮化硅薄膜键合特性分析

采用螺旋波等离子体化学气相沉积(HWPCVD)技术制备了非化学计量比的氢化氮化硅薄膜,对所沉积样品及氮气环境中920 ℃退火样品的微观结构及键合特性进行了分析。Raman散射结果表明,薄膜中过量硅以非晶纳米粒子形式存在,退火样品呈现纳米晶硅和氮化硅的镶嵌结构。红外吸收和可见光吸收特性比较结果显示,薄膜样品的微观结构依赖于化学计量比以及退火过程,硅含量较低样品因高的键合氢含量而表现出低的纳米硅表面缺陷态密度;退火过程将引起Si—H和N—H键合密度的减少,因晶态纳米颗粒的形成,退火样品表现出更高的结构无序度。     

Synthesis and size differentiation of Ge nanocrystals in amorphous SiO2

Germanosilicate layers were grown on Si substrates by plasma enhanced chemical vapor deposition (PECVD) and annealed at different temperatures ranging from 700–1010 °C for durations of 5 to 60 min. Transmission electron microscopy (TEM) was used to investigate Ge nanocrystal formation in SiO₂:Ge films. High-resolution cross section TEM images, electron energy-loss spectroscopy and energy dispersive X-ray analysis (EDX) data indicate that Ge nanocrystals are present in the amorphous silicon dioxide films. These nanocrystals are formed in two spatially separated layers with average sizes of 15 and 50 nm, respectively. EDX analysis indicates that Ge also diffuses into the Si substrate. PACS 68.73.Lp; 61.46.Hk; 61.46.-w; 68.65.Hb; 61.82.Rx     

椭圆偏振光谱表征单晶硅衬底上生长的非晶硅和外延硅薄膜

本文采用射频等离子体增强化学气相沉积(rf-PECVD)技术在单晶硅衬底上沉积了两个系列的硅薄膜. 通过对样品进行固定角度椭圆偏振测试, 结果表明第一个系列硅薄膜为非晶硅, 形成了突变的a-Si:H/c-Si异质结构, 此结构在HIT电池中有利于形成好的界面特性, 对于非晶硅薄膜采用通常的Tauc-Lorentz摇摆模型(Genosc)拟合结果很好; 第二个系列硅薄膜为外延硅, 对于外延硅薄膜, 随着膜厚增加晶化率降低, 当外延硅薄膜厚度为46 nm时开始非晶硅生长. 对于外延硅通常采用EMA模型(即将硅薄膜体层看成由非晶硅和c-Si构成的混合层)拟合结果较好, 当硅薄膜中出现非晶硅生长时, 将体层分成混合层和非晶硅两层, 采用三层模型拟合结果很好. 本文证实了椭偏光谱分析采用不同的模型可对单晶硅衬底上不同结构的硅薄膜进行有效表征.     

空间限制与应变对发光多孔硅喇曼光谱的影响

发光多孔硅的喇曼光谱在５２０ｃｍ^－１附近呈现一锐峰，峰位的红移随多孔度的增大而增大采用微晶模型拟合喇曼谱的线形，发现除了光学声子的空间限制效应，硅单晶的应变对峰位的移动也有显著贡献。通过谱形的拟合估算了硅微粒的应变，与已报道的Ｘ射线衍射结果相一致。在多孔硅的喇曼光诸中没有观察到起源于非晶硅的光散射信号。 关键词：     

Trap states in oxidation layer of nanocrystal Si

The photoluminescence （PL） of nanocrystal present in porous silicon shifts from the near infrared to the ultraviolet depending on the size when the surface is passivated with Si-H bonds. After oxidation, the centre wavelength of PL band is pinned in a region of 700-750 nm and its intensity increases obviously. Calculation shows that trap electronic states appear in the band gap of a smaller nanocrystal when Si = O bonds or Si-O-Si bonds are formed. The changes in PL intensity and wavelength can be explained by both quantum confinement and trap states in an oxidation layer of nanocrystal. In the theoretical model, the most important factor in the enhancement and the pinning effects of PL emission is the relative position between the level of the trap states and the level of the photoexcitation in the silicon nanocrystal.     

Spatial versus quantum confinement in porous amorphous silicon nanostructures

Light-emitting porous amorphous silicon has been produced by anodization in HF of hydrogenated amorphous silicon films. The maximal thickness of the porous films is limited by the onset of an instability which results in the formation of large channels short-circuiting the amorphous layer. This is due to the high resistivity of the amorphous silicon films as compared to that of the electrolyte. Confinement effects on the electron wavefunction are analyzed in situ using photoluminescence measurements in hydrofluoric acid and compared to those observed in porous crystalline silicon. For crystalline silicon, a huge blue shift of the photoluminescence is observable upon reducing the size of the structures by photo-etch, showing clear evidence of quantum confinement effects in this material. No shift has been observed when carrying out the same experiment with amorphous silicon. This indicates that the extent of the wavefunction in the bandtail states involved in luminescence is too small to be sensitive to confinement down to the minimum sizes of our porous material ( 3 nm). Measurements of the width and the temperature dependence of the photoluminescence demonstrate that the Urbach energy does not change upon increasing the porosity, i.e., upon decreasing the size of the a-Si:H nanostructures, in contradiction with what has been reported in ultrathin a-Si:H multilayers. Received: 3 August 1998     

Optical Properties of Nonstoichiometric Silicon Oxide SiOx (x < 2)

Optics and Spectroscopy - The optical properties of amorphous nonstoichiometric silicon oxide (SiOx) films of variable composition (x = 0.62–1.92) formed by plasma-enhanced chemical vapor...     

Crystallization kinetics of amorphous SiC films: Influence of substrate

The crystallization kinetics of amorphous silicon carbide films was studied by means of X-ray diffractometry (XRD) and transmission electron microscopy (TEM). The films were deposited by radio frequency (r.f.) magnetron sputtering on glassy carbon and single crystalline silicon substrates, respectively. TEM micrographs and XRD patterns show the formation of nano-crystalline β-SiC with crystallite sizes in the order of 50 nm during annealing at temperatures between 1200 and 1600 °C. A modified Johnson-Mehl-Avrami-Kolmogorov (JMAK) formalism was used to describe the isothermal transformation of amorphous SiC into β-SiC as an interface controlled, three-dimensional growth processes from pre-existing small crystallites in the order of 10 nm. These pre-existing crystallites are formed in a transient process in the early stages of crystallization. For films deposited on the silicon substrate, the obtained rate constants of crystallite growth obey an Arrhenius behavior with an activation enthalpy of 4.1 ± 0.5 eV in accordance with literature data. Films deposited on glassy carbon show an increased stability of amorphous SiC films, which is reflected in smaller rate constants of crystallite growth of several orders of magnitude at low temperatures and a higher activation enthalpy of 8.9 ± 0.9 eV. A model is proposed, where the faster crystallization of films on silicon substrates can be explained with the presence of superabundant point defects, which diffuse from the substrate into the film and accelerate the incorporation of atoms from the amorphous into the crystalline phase.     

Investigation of the dependence of the photoluminescence properties of silicon nanoclusters on their volume fraction in a silicon oxide matrix

The photoluminescence (PL) spectra and kinetics of amorphous and crystalline silicon nanoclusters are investigated. The given nanoclusters are formed by thermal annealing of thin suboxide silicon films with different volume fractions of silicon. It is demonstrated that the PL intensity and lifetime of the ensembles of silicon nanocrystals have a steplike dependence on the silicon volume fraction in the film. The influence of the percolation effect on the photoluminescence properties of the structures under study is discussed.     

低压下气流对激光沉积纳米硅晶化及尺寸的影响

纳米硅具有明显的光致发光效应和量子尺寸效应,广泛的应用在现代电子工业和太阳能光伏工业中.尺寸影响着纳米硅的实际用途,因此制备尺寸可控的纳米硅晶粒具有很重要的实际意义.本文采用脉冲激光沉积(PLD)技术,在烧蚀点水平方向、距靶2 cm处引入一束流量为5 sccm的氩(Ar)气流,在0.01-0.5 Pa的Ar气压下烧蚀高阻抗单晶硅(Si)靶.在管口正下方1 cm处水平放置衬底来沉积纳米Si薄膜;并用同一装置,在0.08 Pa的Ar气压下分别引入流量为0,2.5,5,7.5,10 sccm的Ar气流沉积纳米Si薄膜.利用原子力显微镜(AFM)、X射线衍射(XRD)、Raman散射对样品表面形貌和微观结构进行分析表征.结果表明:不引入气流时出现纳米Si晶粒的阈值气压是0.1Pa,引入气流后出现纳米Si晶粒的阈值气压为0.05 Pa.晶粒尺寸随着气流流量的增大而减小.     

Excitation of erbium in the heterogeneous nanocrystalline matrix of amorphous silicon

The erbium photoluminescence decay kinetics at a wavelength of 1.54 μm in amorphous hydrogenated silicon films obtained at high oxygen concentrations in a magnetron gas discharge is investigated. Optically active erbium is found to exist both in the semiconducting matrix of amorphous silicon and in dielectric nanocrystals of erbium silicate, which are formed in this case. The concentration ratio of excited erbium in amorphous silicon and in the nanocrystals is determined, as well as the time of excitation transfer from erbium in amorphous silicon to erbium in the nanocrystals. The mechanism of erbium excitation in this heterogeneous system is considered. The external quantum yield of erbium photoluminescence measured at a wavelength of 1.54 μm and room temperature is found to be 0.3–0.4%.     

氢化非晶硅叠层薄膜对单晶硅表面钝化研究

采用等离子体增强化学气相沉积法生长的单层本征氢化非晶硅薄膜对单晶硅片进行钝化,结果表明增加氢稀释比有利于减少薄膜中的缺陷,增强钝化效果,过量的氢稀释比会导致非晶硅在硅片表面的外延晶化生长,降低钝化效果。退火导致非晶硅晶化程度增加,降低了钝化效果,同时退火提升了薄膜的质量,改变了H键合方式,增强了钝化效果。因此,单层氢化非晶硅只有在合适的氢稀释比和退火温度才可以获得最佳钝化效果。为了提高非晶硅薄膜对硅片的钝化效果,采用具有高低氢稀释比的叠层本征非晶硅薄膜对硅片进行钝化。因此将高氢稀释比沉积的非晶硅薄膜叠层生长于低氢稀释比的薄膜之上,避免非晶硅在硅片表面的外延生长。在退火过程中,高氢稀释比薄膜中的氢扩散到低氢稀释比薄膜中,有效地钝化了非晶硅中和单晶硅表面的悬挂键,改善了非晶硅/硅片的界面质量,叠层钝化后硅片的少子寿命为7.36 ms,隐含开路电压为732 mV。     

Doping of evaporated amorphous silicon films

It is shown that evaporated amorphous silicon films can be doped interstitially by ion implantation and in-diffusion of lithium. The doping effect is smaller than for glow discharge silicon films, and the doped state is less stable at elevated temperature. This is explained by precipitation as well as out-diffusion effects in connection with the high defect concentration in evaporated films.     

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利用微波电子回旋共振等离子体增强型化学气相沉积(ECR-PECVD)采用一步法直接在K9玻璃上低温沉积制备了多晶硅薄膜.研究了不同实验参数对薄膜沉积的影响,采用X射线衍射(XRD)、拉曼光谱、扫描电子显微镜(SEM)等实验分析方法对不同条件下制备的样品进行了晶体结构和表面形貌分析,并讨论了多晶硅薄膜沉积的最佳条件.实验结果表明,玻璃衬底上多晶硅薄膜呈柱状生长,并有一定厚度的非晶孵化层;较高氢气比例和衬底温度有利于结晶,薄膜的结晶率达到了62％;晶粒团簇的最大尺寸约为500nm.     

氢化非晶硅薄膜退火形成的纳米硅及其光致发光

本文报道对氢化非晶硅(a-Si:H)薄膜在600～620℃温度下快速退火10s可以形成纳米晶硅(nc-Si),其Raman散射表明,在所形成的nc-Si在薄膜中的分布是随机的,直径在1.6～15nm范围内,并且在强激光辐照下观察了nc-Si在薄膜中的结晶和生长情况.经退火所形成的nc-Si可见光辐射较弱,不能检测到它们的光致发光(PL),但用氢氟酸腐蚀钝化后则可检测到较强的红PL,并且钝化后的nc-Si在空气中暴露一定的时间后,其辐射光波长产生了蓝移.文中就表面钝化和量子限制对可见光辐射的重要性作了讨论.     

PROPERITES OF HYDROGENATED AMORPHOUS SILICON CARBIDE FILMS IRRADIATED BY EXCIMER PULSE LASER

A series of hydrogenated amorphous silicon carbide film (a-SiC:H) were prepared by rf plasma-enhanced chemical vapor deposition method. The optical band gap(E^opt_g) of the films can be extended to 2.6eV. The as-deposited alma were then irradiated by a KrF excimer laser. During the irradiation process, hydrogen escaped out of the films, and the structure of the films was changed from an amorphous phase to mixed phases of nanocrystallites of silicon and amorphous silicon carbide. The room-temperature dark conductivity of the laser irradiated films is 6-7 orders of magnitude larger than that of the as-deposited films, which was attributed to the modification of the conductivity mechanism resulting from the structural change.     

Gibbs free energy and equilibrium states in the Si/Si oxide systems

In this paper, the equilibrium states in the Si/Si oxide systems formed as a result of the phase separation of nonstoichiometric silicon oxide films are studied. The expressions for the Gibbs free energy of Si oxide and Si/Si oxide systems are derived thermodynamically. The transformations of the Gibbs free energy in the amorphous Si/Si oxide and the crystalline Si/Si oxide systems with the change in the amount of separated silicon and the composition of the silicon oxide phase are analyzed. By minimizing the Gibbs free energy of these systems, the equilibrium stoichiometry indices of silicon oxide are calculated as functions of its initial stoichiometry and the temperature. The solubility limits of Si in SiO(2) in equilibrium with amorphous and crystalline Si are determined. The obtained results form the basis for the development of a complete thermodynamic theory of phase separation in nonstoichiometric silicon oxide films with the formation of Si nanoinclusions in the silicon oxide matrix.     

Study on phase separation in a-SiOx for Si nanocrystal formation through the correlation of photoluminescence with structural and optical properties

The phase separation in amorphous silicon suboxide (a-SiO_x) films upon thermal annealing for the formation of light emitting silicon nanocrystals (Si-NCs) was studied through the correlation of photoluminescence (PL) and photoluminescence excitation (PLE) with structural and optical properties. The PL and PLE features and the structural and optical properties show a strong dependence on the annealing process and reveal that the precipitation of the excess Si in a-SiO_x and the formation of Si-NCs from the precipitated Si are two separate processes which should be distinguished in the phase separation in a-SiO_x. They proceed at different temperatures and the formation of Si-NCs is a slow process compared with the precipitation of the excess Si. The nanocrystal size and size distribution evolve with annealing time at the initial stages and are mainly dependent on annealing temperature for a certain O content in the initial a-SiO_x with the density of the formed Si-NCs increasing with longer annealing duration.