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Journal ArticleDOI

A comparison of grain nucleation and grain growth during crystallization of HWCVD and PECVD a-Si:H films

15 Jan 2008-Thin Solid Films (Elsevier)-Vol. 516, Iss: 5, pp 529-532
TL;DR: In this article, the authors compare the crystallization kinetics of HWCVD and PECVD a-Si:H films, containing different initial film hydrogen contents (CH), by annealing at 600 °C.
About: This article is published in Thin Solid Films.The article was published on 2008-01-15 and is currently open access. It has received 25 citations till now. The article focuses on the topics: Crystallization & Nucleation.

Summary (2 min read)

1. Introduction

  • The crystallization of as deposited a-Si:H thin films is becoming increasingly important because of its potential use to produce higher mobility polycrystalline materials for use in solar cells and high performance thin film transistors.
  • This process is believed, at relatively low anneal temperatures (b 1000 °C), to follow a classical model of nucleation and grain growth [1], where an amorphous incubation time, a steady state nucleation rate, grain growth of these nuclei, and a characteristic time of crystallization can be identified.
  • Further, recent results have shown that the crystallization time, for a given film CH, can depend upon the a-Si:H deposition method [4].

2. Experimental

  • H films were deposited by HWCVD and PECVD, using deposition conditions described previously [6,7], also known as A-Si.
  • Regarding the latter, the width of the XRD diffraction peaks may result from a combination of grain size, defect density, or strain effects.
  • This thickness was chosen because no sample thinning was required.
  • TEM analysis was performed on a CM200 Scanning TEM using a Phillips single-slit holder and a Gatan Model 652 double-slit heating holder for in-situ annealing.

3. Results and discussion

  • Fig. 1 shows TEM images of partially crystallized HWCVD and PECVD a-Si:H films annealed at 600 °C, with the annealing times indicated in the figures.
  • From this figure, clear differences are seen not only in the anneal time, but also in the grain density and grain morphology between the different films.
  • These differences become even more pronounced when a low CH HWCVD film is included in the comparison compared to the PECVD film seen in Fig. 1(b) [8,9]; in these comparisons, the PECVD film showed much lower grain densities and larger grains overall.
  • In Table 3 the authors first present a review of the NMR data, from which the densities of the isolated and clustered hydrogen distributions can be obtained.
  • H calculation, the authors use an averaged value of the clustered/isolated hydrogen ratio, obtained for ‘standard’ (low deposition rate) films deposited using 100% silane and a moderate (∼ 200–250 C) substrate temperature, also known as For the PECVD a-Si.

4. Summary and conclusions

  • The authors have presented the crystallization kinetics when HWCVD films of different film CH and ‘standard’ PECVD aSi:H films have been annealed at a temperature of 600 °C to induce film crystallization.
  • The authors find that the low CH HWCVD film nucleates first, and that the incubation time increases with increasing film CH.
  • Not surprisingly, the films which nucleate the fastest contain the smallest grains when crystallization is complete.
  • The increase in short range disorder upon film hydrogen evolution does not seem to play a primary role in the crystallization process.
  • A tentative model relating the crystallization kinetics to the initial hydrogen spatial distribution in the film is presented.

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Citations
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Journal ArticleDOI
TL;DR: In this article, the width of the first X-ray diffraction (XRD) peak of amorphous silicon (a-Si:H) centered around 2θ =275° was analyzed.
Abstract: In recent years, it has been recognized that medium range ordering (MRO) in amorphous silicon (a-Si:H) plays a role in controlling its solid phase crystallization (SPC) behavior Information on the MRO can be obtained from the width of the first X-ray diffraction (XRD) peak of a-Si:H centered around 2θ = 275° The broader the full width half maximum (FWHM) of the first XRD peak, the less ordered the a-Si:H material in the medium range length scale (up to 5 nm) In this work, it was found that the FWHM of the first XRD peak changes with the pressure used during the deposition of a-Si:H A threshold SPC behavior was observed as a function of the a-Si:H deposition pressure and a good correlation between the SPC behavior and the a-Si:H XRD peak width was found Results in this study indicate that higher MRO in a-Si:H led to faster SPC rates and smaller grain sizes, suggesting the presence of relatively active and high density of nucleation sites High angle annular dark field scanning transmission electron microscopy and ultraviolet reflectance indicate that films with higher MRO yielded polycrystalline silicon (poly-Si) grains which were more defective and non-columnar in morphology Results suggest that a-Si:H material with lower MRO were preferred as a precursor for SPC, which forms a better quality poly-Si thin film material It was proposed that ion bombardment seems to play a role in altering the a-Si:H properties

4 citations

Journal ArticleDOI
TL;DR: In this paper, residual forms of hydrogen (H) atoms such as bonding configuration in poly-crystalline silicon (poly-Si) films formed by the flash-lamp-induced crystallization of catalytic chemical vapor deposited (Cat-CVD) a-Si films were investigated.

3 citations

Journal ArticleDOI
TL;DR: In this paper, the effect of film stress on crystallite nucleation was investigated in 0.11m thick, thermally annealed hydrogenated amorphous silicon films, using a recently developed optical method.
Abstract: The effect of film stress on crystallite nucleation is investigated in 0.11 μm thick, thermally annealed hydrogenated amorphous silicon films. Using a recently developed optical method, the crystallite density is measured as the films are isochronally annealed at 600 °C, which enables the determination of the crystallite nucleation rate. This rate is significantly suppressed around scratches, cleaved film edges, and laser ablated areas, extending laterally as much as 100–150 μm from these regions where the film connectivity is disrupted. μ-Raman measurements of the transverse optical mode of Si demonstrate an accompanying reduction in tensile stress in the regions where nucleation is suppressed. The first measurements of nucleation rate in stress and in stress relieved areas in the same film are presented.

3 citations

Journal ArticleDOI
TL;DR: In this article, the authors investigated the crystallization in amorphous silicon doped with B2H6 for varing doping levels under ǫ-field and found that the rate is saturated at around 10μm/h after 2min doping time.

2 citations

Dissertation
07 May 2015

1 citations


Cites background from "A comparison of grain nucleation an..."

  • ...X-ray Diffraction (XRD), UV-reflectance, Raman [33] [42], and ellipsometry are non-destructive, whereas transmission electron microscopy (TEM), Rutherford...

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References
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Journal ArticleDOI
TL;DR: In this paper, it was shown that hydrogenated amorphous silicon containing as little as 1/10 the bonded H observed in device-quality glow discharge films have been deposited by thermal decomposition of silane on a heated filament.
Abstract: Device‐quality hydrogenated amorphous silicon containing as little as 1/10 the bonded H observed in device‐quality glow discharge films have been deposited by thermal decomposition of silane on a heated filament. These low H content films show an Urbach edge width of 50 mV and a spin density of ∼1/100 as large as that of glow discharge films containing comparable amounts of H. High substrate temperatures, deposition in a high flux of atomic H, and lack of energetic particle bombardment are suggested as reasons for this behavior.

464 citations

Journal ArticleDOI
TL;DR: It is shown that the width of the ``optic peak'' increases roughly linearly with the rms bond-angle distortion of the network, consistent with model-building experience which shows that it is impossible to construct fully bonded amorphous networks with \ensuremath{\Delta}${\ensureMath{\theta}}_{b}$.
Abstract: The Raman scattering from various model structures for amorphous silicon is computed. It is shown that the width of the ``optic peak'' increases roughly linearly with the rms bond-angle distortion \ensuremath{\Delta}${\ensuremath{\theta}}_{b}$ of the network. The experimentally observed linewidths lead to 7.7\ifmmode^\circ\else\textdegree\fi{}\ensuremath{\le}\ensuremath{\Delta}${\ensuremath{\theta}}_{b}$\ensuremath{\le}10.5\ifmmode^\circ\else\textdegree\fi{}. The smaller linewidths (and hence angles) correspond to networks that have been annealed at higher temperatures. These results are consistent with model-building experience which shows that it is impossible to construct fully bonded amorphous networks with \ensuremath{\Delta}${\ensuremath{\theta}}_{b}$\ensuremath{\le}6.6\ifmmode^\circ\else\textdegree\fi{}.

392 citations

Journal ArticleDOI
TL;DR: In this paper, the morphological evolution of the amorphous towards the polycrystalline phase is investigated by transmission electron microscopy and it is interpreted in terms of a physical model containing few free parameters related to the thermodynamical properties of ammorphous silicon and to the kinetical mechanisms of crystal grain growth.
Abstract: The solid phase crystallization of chemical vapor deposited amorphous silicon films onto oxidized silicon wafers, induced either by thermal annealing or by ion beam irradiation at high substrate temperatures, has been extensively developed and it is reviewed here. We report and discuss a large variety of processing conditions. The structural and thermodynamical properties of the starting phase are emphasized. The morphological evolution of the amorphous towards the polycrystalline phase is investigated by transmission electron microscopy and it is interpreted in terms of a physical model containing few free parameters related to the thermodynamical properties of amorphous silicon and to the kinetical mechanisms of crystal grain growth. A direct extension of this model explains also the data concerning the ion-assisted crystal grain nucleation.

332 citations

Journal ArticleDOI
TL;DR: In this paper, a theoretical and experimental study of the recrystallization behavior of polycrystalline silicon films amorphized by self-implantation was carried out and the crystallization behavior was found to be similar to the crystallisation behavior of films deposited in the amorphous state, however, a transient time was observed, during which negligible crystallization occurs.
Abstract: This paper presents a theoretical and experimental study of the recrystallization behavior of polycrystalline silicon films amorphized by self‐implantation. The crystallization behavior was found to be similar to the crystallization behavior of films deposited in the amorphous state, as reported in the literature; however, a transient time was observed, during which negligible crystallization occurs. The films were prepared by low‐pressure chemical vapor deposition onto thermally oxidized silicon wafers and amorphized by implantation of silicon ions. The transient time, nucleation rate, and characteristic crystallization time were determined from the crystalline fraction and density of grains in partially recrystallized samples for anneal temperatures from 580 to 640 °C. The growth velocity was calculated from the nucleation rate and crystallization time and is lower than values in the literature for films deposited in the amorphous state. The final grain size, as calculated from the crystallization param...

329 citations

Journal ArticleDOI
TL;DR: Using the fact that multiple-quantum excitation is limited by the size of the dipolar-coupled spin system, it is shown that the predominant bonding environment for hydrogen is a cluster of four to seven atoms.
Abstract: Multiple-quantum nuclear-magnetic-resonance techniques are used to study the distribution of hydrogen in hydrogenated amorphous silicon. Using the fact that multiple-quantum excitation is limited by the size of the dipolar-coupled spin system, we show that the predominant bonding environment for hydrogen is a cluster of four to seven atoms. For device quality films, the concentration of these cluster defects increases with increasing hydrogen content. At very high hydrogen content, the clusters are replaced with a continuous network of silicon-hydrogen bonds.

174 citations

Frequently Asked Questions (1)
Q1. What contributions have the authors mentioned in the paper "A comparison of grain nucleation and grain growth during crystallization of hwcvd and pecvd a-si:h films" ?

Even though the bonded hydrogen evolves very early from the film during annealing, the authors suggest that the initial spatial distribution of hydrogen plays a critical role in the crystallization kinetics, and they propose a preliminary model to describe this process.