Kinetics of solid phase crystallization in amorphous silicon

G.L. Olson, J.A. Roth
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We showed that solid phase, transformations can occur in a-Si at temperatures far in excess of the a-Si melting point, <em>T</em><sub>al</sub>, and that the competition between solid phase crystallization and melting is a function of heating conditions (thermal rise-time, heating duration) and properties of the sample (amorphous film thickness). We evaluated kinetics of random nucleation and growth over a temperature range from 650 to 1380°C and showed that the random crystallization process is a well-behaved function of temperature over that temperature range with an activation energy of 4 eV. We found that random nucleation and growth becomes the dominant solid phase crystallization process at high temperatures ( &gt; 1330 °C) in agreement with predictions based on differences between the activation energies for random crystallization and SPE.</p><p>The effects of doping and non-doping impurities on the kinetics of SPE and randomcrystallization were investigated as a function of temperature and impurity concentration. We showed that a variety of phenomena, including precipitation and impurity segregation can alter the intrinsic crystallization kinetics, and we identified time-temperature-concentration windows in which specific processes dominate. We concentrated on the investigation of crystallization behavior in layers containing impurities which illustrate the wide range of temperature- and concentration-dependent phenomena that can occur during heating of an amorphous thin film. Simple rate-enhancement and -retardation processes produced by doping (B and P) and non-doping impurities (F) were contrasted with the complex rate changes that can occur when processes such as impurity clustering and phase separation compete either individually or collectively with SPE in layers containing As, In and Au. We showed that random crystallization rates can be enhanced enormously by the presence of certain impurities and that impurity-enhanced nucleation can give rise to strong competition between random crystallization and SPE at temperatures much lower than observed in intrinsic layers. In the case of certain impurities (e.g. fluorine) the effects due to enhanced random crystallization in the high-temperature regime can be predicted from nucleation rate measurements performed at low temperatures. In other cases (e.g. arsenic), a different enhancement mechanism must be invoked to rationalize the experimental observations.</p><p>The competition between melting and solid phase crystallization was investigated at <em>T</em> ≥ <em>T</em><sub>al</sub>. We showed that melting at temperatures near <em>T</em><sub>al</sub> (1200°C) can be observed under microsecond duration heating conditions in thick (2600 A) films, whereas solid phase crystallization at temperatures in excess of 1300 °C is observed in thin (1000 Å) films. The differences in observed melting behavior have not yet been fully reconciled. A model which rationalizes the melting behavior in terms of amorphous phase relaxation during heating has been proposed [138], but more quantitative information concerning the thermodynamics of a-Si and 1-Si in the very high temperature regime is required before this model can be fully tested. Taken together with the results of nanosecond duration heating experiments, the results obtained using cw Ar and fl-pumped dye laser heating suggest that the kinetics of melt nucleation may play a pivotal role in determining the conditions under which melting of a-Si at <em>T</em><sub>al</sub> will occur.</p><p>We have shown that the interplay among solid phase crystallization and competitive processes in a-Si depends strongly on temperature. The combination of laser heating and in situ diagnostics provides a powerful capability for investigating crystallization behavior at temperatures that are inaccessible with conventional techniques. The ability to access the high-temperature regime has allowed us to obtain new information concerning the kinetics and thermodynamics of phase transformations and to characterize the competition that can occur among the various solid phase processes during heating of amorphous silicon.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"3 1","pages":"Pages 1-77"},"PeriodicalIF":0.0000,"publicationDate":"1988-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0920-2307(88)80005-7","citationCount":"568","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Science Reports","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0920230788800057","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 568

Abstract

In this review we have examined the crystallization behavior of a-Si over the temperaturerange from 500 °C to ∼ 1380°C. We have shown that SPE is a thermally activated process which is characterized by a single activation energy (2.7 eV) over the temperature range from ∼ 470 °C to ∼ 1350 °C. The activation energies for intrinsic SPE in ion-implanted and e-beam deposited layers on Si(100) substrates were found to be the same, implying that the interfacial bond breaking and rearrangement processes responsible for SPE in those layers is the same in spite of possible differences in microstructure. We showed that solid phase, transformations can occur in a-Si at temperatures far in excess of the a-Si melting point, Tal, and that the competition between solid phase crystallization and melting is a function of heating conditions (thermal rise-time, heating duration) and properties of the sample (amorphous film thickness). We evaluated kinetics of random nucleation and growth over a temperature range from 650 to 1380°C and showed that the random crystallization process is a well-behaved function of temperature over that temperature range with an activation energy of 4 eV. We found that random nucleation and growth becomes the dominant solid phase crystallization process at high temperatures ( > 1330 °C) in agreement with predictions based on differences between the activation energies for random crystallization and SPE.

The effects of doping and non-doping impurities on the kinetics of SPE and randomcrystallization were investigated as a function of temperature and impurity concentration. We showed that a variety of phenomena, including precipitation and impurity segregation can alter the intrinsic crystallization kinetics, and we identified time-temperature-concentration windows in which specific processes dominate. We concentrated on the investigation of crystallization behavior in layers containing impurities which illustrate the wide range of temperature- and concentration-dependent phenomena that can occur during heating of an amorphous thin film. Simple rate-enhancement and -retardation processes produced by doping (B and P) and non-doping impurities (F) were contrasted with the complex rate changes that can occur when processes such as impurity clustering and phase separation compete either individually or collectively with SPE in layers containing As, In and Au. We showed that random crystallization rates can be enhanced enormously by the presence of certain impurities and that impurity-enhanced nucleation can give rise to strong competition between random crystallization and SPE at temperatures much lower than observed in intrinsic layers. In the case of certain impurities (e.g. fluorine) the effects due to enhanced random crystallization in the high-temperature regime can be predicted from nucleation rate measurements performed at low temperatures. In other cases (e.g. arsenic), a different enhancement mechanism must be invoked to rationalize the experimental observations.

The competition between melting and solid phase crystallization was investigated at TTal. We showed that melting at temperatures near Tal (1200°C) can be observed under microsecond duration heating conditions in thick (2600 A) films, whereas solid phase crystallization at temperatures in excess of 1300 °C is observed in thin (1000 Å) films. The differences in observed melting behavior have not yet been fully reconciled. A model which rationalizes the melting behavior in terms of amorphous phase relaxation during heating has been proposed [138], but more quantitative information concerning the thermodynamics of a-Si and 1-Si in the very high temperature regime is required before this model can be fully tested. Taken together with the results of nanosecond duration heating experiments, the results obtained using cw Ar and fl-pumped dye laser heating suggest that the kinetics of melt nucleation may play a pivotal role in determining the conditions under which melting of a-Si at Tal will occur.

We have shown that the interplay among solid phase crystallization and competitive processes in a-Si depends strongly on temperature. The combination of laser heating and in situ diagnostics provides a powerful capability for investigating crystallization behavior at temperatures that are inaccessible with conventional techniques. The ability to access the high-temperature regime has allowed us to obtain new information concerning the kinetics and thermodynamics of phase transformations and to characterize the competition that can occur among the various solid phase processes during heating of amorphous silicon.

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非晶硅固相结晶动力学
在这篇综述中,我们研究了a-Si在500°C到~ 1380°C的温度范围内的结晶行为。我们已经证明SPE是一个热激活过程,其特征是在~ 470°C至~ 1350°C的温度范围内具有单一活化能(2.7 eV)。在Si(100)衬底上,离子注入层和电子束沉积层的本态SPE活化能是相同的,这意味着尽管微观结构可能存在差异,但导致这些层中SPE的界面键断裂和重排过程是相同的。我们发现,在远超过a- si熔点Tal的温度下,a- si可以发生固相转变,并且固相结晶和熔化之间的竞争是加热条件(热上升时间、加热持续时间)和样品性质(非晶膜厚度)的函数。在650 ~ 1380°C的温度范围内,我们评估了随机成核和生长的动力学,结果表明,在该温度范围内,随机结晶过程是温度的良好函数,活化能为4 eV。我们发现,在高温下,随机形核和生长成为主要的固相结晶过程(>1330°C),与基于随机结晶活化能和SPE之间差异的预测一致。研究了掺杂和非掺杂杂质对固相萃取和随机结晶动力学的影响,并将其作为温度和杂质浓度的函数。我们发现了多种现象,包括沉淀和杂质偏析可以改变本征结晶动力学,我们确定了特定过程占主导地位的时间-温度-浓度窗口。我们集中研究了含杂质层的结晶行为,这说明了在非晶薄膜加热过程中可能发生的广泛的温度和浓度依赖现象。对比了掺杂(B和P)和非掺杂杂质(F)产生的简单速率增强和-延迟过程,以及杂质聚类和相分离等过程单独或共同与含有as, in和Au的层中SPE竞争时可能发生的复杂速率变化。我们发现,某些杂质的存在可以极大地提高随机结晶速率,并且杂质增强的成核可以在远低于内在层观察到的温度下引起随机结晶和SPE之间的激烈竞争。在某些杂质(如氟)的情况下,可以通过在低温下进行的成核速率测量来预测高温状态下增强的随机结晶的影响。在其他情况下(如砷),必须调用不同的增强机制来使实验观察合理化。在T≥Tal时,研究了熔融和固相结晶之间的竞争。我们表明,在微秒持续加热条件下,厚膜(2600 A)在接近Tal(1200°C)的温度下可以观察到熔化,而薄膜(1000 Å)在超过1300°C的温度下可以观察到固相结晶。观察到的熔化行为的差异尚未完全调和。已经提出了一个模型,该模型根据加热过程中的非晶相松弛来合理化熔化行为[138],但在对该模型进行充分测试之前,需要更多关于A - si和1-Si在高温状态下的热力学的定量信息。结合纳秒持续加热实验的结果,用连续氩和流泵染料激光加热得到的结果表明,熔体成核动力学可能在决定a- si在Tal处熔化的条件中起关键作用。我们已经证明,在a-Si中,固相结晶和竞争过程之间的相互作用很大程度上取决于温度。激光加热和原位诊断的结合为研究传统技术无法达到的温度下的结晶行为提供了强大的能力。进入高温状态的能力使我们能够获得有关相变动力学和热力学的新信息,并表征非晶硅加热过程中各种固相过程之间可能发生的竞争。
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