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Journal ArticleDOI

Influence of post-hydrogenation upon electrical, optical and structural properties of hydrogen-less sputter-deposited amorphous silicon

TL;DR: In this article, an intrinsic and doped, hydrogen-less amorphous silicon films are RF magnetron sputter deposited and post-hydrogenated in a remote hydrogen plasma reactor at a temperature of 370°C.
About: This article is published in Thin Solid Films.The article was published on 2016-01-01 and is currently open access. It has received 9 citations till now. The article focuses on the topics: Amorphous solid & Amorphous silicon.

Summary (1 min read)

2.2. Passivation quality

  • Passivation quality and evaluation during post hydrogenation of RFS deposited a Si:H is done by means of effective minority carrier lifetime (τ eff ) measurements.
  • These are carried out at room temperature (~25 °C) via microwave detected photo conductance decay measure ments (μPCD) using a Semilab WT 2000 with a spatial resolution of 250 μm and bias light of 1 sun.
  • Spatially resolved τ eff data are providing detailed information about the local influence of the post hydrogenation and the homogeneity of the film.
  • Measurements are cross checked via τ eff deduction from transient and quasi steady state photo conductance decay (WCT 120, Sinton Instruments), also at ~25 °C.

3.4. Structural stability

  • Raman investigations demonstrate that there is no crystallization occurring during post hydrogenation (4>, = 0%).
  • Moreover, it is shown that the (i) and (p) a Sl surfaces investigated by AFM (Fig. 6 ) and the discussed nano sized structures are also amorphous.

4. Conclusions

  • The investigations in this study demonstrated that initially hydrogen less and non passivating intrinsic as well as doped a Si layers develop surface passivation properties during a post hydrogenation step in a MIRHP reactor at 370 °C.
  • These optimal lifetime values are achieved with layer thicknesses of ~40 nm deposited at a temperature of 325 °C.
  • This can be related to a decrease of localized states within the band gap.
  • The surface roughness of the initially rough RFSD a Si decreases up to 25% during post hydrogenation while the Raman crystallinity remains at 0%, indicating the stability of the amorphous network.
  • This suggests a columnar growth of the RFS deposited a Si.

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Citations
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Book ChapterDOI
09 Sep 2014

152 citations

Journal ArticleDOI
TL;DR: In this article, the porosity of underdense a-Si:H layer enables H penetration into the amorphous network and the Si:H/c-Si interface.
Abstract: Underdense hydrogenated amorphous silicon (a-Si:H) prepared by plasma-enhanced chemical vapor deposition was used as a passivation layer in silicon heterojunction (SHJ) solar cells. By reducing the thickness of the underdense a-Si:H passivation layer from 15 nm to 5 nm, the open circuit voltage (Voc) of the corresponding SHJ solar cell increased significantly from 724.3 mV to 738.6 mV. For comparison, a widely used transition-zone a-Si:H passivation layer was also examined, but reducing its thickness from 15 nm to 5 nm resulted in a continuous Voc reduction, from 724.1 mV to 704.3 mV. The highest efficiency was achieved using a 5-nm-thick underdense a-Si:H passivation layer. We propose that this advantageous property of underdense a-Si:H reflects its microstructural characteristics. While the porosity of a-Si:H layer enables H penetration into the amorphous network and the a-Si:H/c-Si interface, a high degree of disorder inhibits the formation of the epitaxial layer at the a-Si:H/c-Si interface during pos...

45 citations

Journal ArticleDOI
M. Grdeń1
TL;DR: The manuscript reviews several selected applications of Activation Analysis that differ from classical laboratory measurements by the fact that they do not require sampling of the analysed object and/or measurements under analytical laboratory conditions.
Abstract: The manuscript reviews several selected applications of Activation Analysis that differ from classical laboratory measurements by the fact that they do not require sampling of the analysed object and/or measurements under analytical laboratory conditions. One of great advantages of the Activation Analysis lies in its versatility that allows it to be applied under conditions not available for other analytical techniques.

15 citations

Journal ArticleDOI
TL;DR: In this paper, bias-plasma assisted radio frequency magnetron sputter deposition (RFSD) is used to flatten the a-Si surface of the film, resulting in an amorphous network with only few vacancies and related defects.

7 citations


Cites background or methods from "Influence of post-hydrogenation upo..."

  • ...Furthermore, analyzing formerly hydrogen-less a-Si during a post-hydrogenation step allows determining hydrogen related influences on electrical, optical and structural characteristics [3]....

    [...]

  • ...Bias-plasma assisted as well as standard RFS-deposition takes place in an “AJA ATC 2200” RF magnetron sputtering system....

    [...]

  • ...The abrasive process of BPA-RFS-deposition smoothening the surface of the growing (i) a-Si layer can be used for surface preparation prior to deposition....

    [...]

  • ...[3], the investigation of the progress of hydrogen based saturation of defects like dangling bonds and the related reduction of surface recombination velocity with post-hydrogenation duration can be evaluated by effective minority carrier lifetime measurements ( eff)....

    [...]

  • ...2 (a) shows i. a. the evolution of eff after the mentioned post-hydrogenation step of (i) a-Si layers, RFS-deposited with ( ) and without ( ) bias-plasma assistance and as a function of RFS-deposition temperature....

    [...]

Book ChapterDOI
01 Jan 2019
TL;DR: In this article, the main focus is on physical vapor deposition techniques, with special emphasis on plasma processing techniques, i.e., sputter deposition and pulsed laser deposition, as well as ion plating and ion beam-assisted deposition.
Abstract: This chapter is devoted to the description of available experimental methods which are used for the fabrication of glassy and amorphous thin films or coatings on glass. Current deposition techniques offer great flexibility for the fabrication of such thin films with specific chemistry and microstructure leading to films and coatings with distinctive properties. After a brief introduction to amorphous thin films' processing, general information regarding film nucleation and growth, its microstructure and films' characterization techniques, the main focus is on physical vapor deposition techniques, with special emphasis on plasma processing techniques, i. e., sputter deposition and pulsed laser deposition. The classical vapor deposition techniques as well as ion plating and ion beam-assisted deposition are also briefly described. The chapter then describes the exploitation of chemical vapor deposition, after which a comparison of physical vapor deposition processes with chemical vapor deposition is given. Amorphous thin film fabrication via liquids is shortly reviewed, and finally an outlook regarding the contribution of amorphous thin films and coatings to societal development in the 21st century closes the chapter.

6 citations

References
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Journal ArticleDOI
TL;DR: The atomic force microscope as mentioned in this paper is a combination of the principles of the scanning tunneling microscope and the stylus profilometer, which was proposed as a method to measure forces as small as 10-18 N. As one application for this concept, they introduce a new type of microscope capable of investigating surfaces of insulators on an atomic scale.
Abstract: The scanning tunneling microscope is proposed as a method to measure forces as small as 10-18 N. As one application for this concept, we introduce a new type of microscope capable of investigating surfaces of insulators on an atomic scale. The atomic force microscope is a combination of the principles of the scanning tunneling microscope and the stylus profilometer. It incorporates a probe that does not damage the surface. Our preliminary results in air demonstrate a lateral resolution of 30 A and a vertical resolution less than 1 A.

12,344 citations

Book
04 Jul 1990
TL;DR: In this article, the authors present a characterization of the resistivity of a two-point-versus-four-point probe in terms of the number of contacts and the amount of contacts in the probe.
Abstract: Preface to Third Edition. 1 Resistivity. 1.1 Introduction. 1.2 Two-Point Versus Four-Point Probe. 1.3 Wafer Mapping. 1.4 Resistivity Profiling. 1.5 Contactless Methods. 1.6 Conductivity Type. 1.7 Strengths and Weaknesses. Appendix 1.1 Resistivity as a Function of Doping Density. Appendix 1.2 Intrinsic Carrier Density. References. Problems. Review Questions. 2 Carrier and Doping Density. 2.1 Introduction. 2.2 Capacitance-Voltage (C-V). 2.3 Current-Voltage (I-V). 2.4 Measurement Errors and Precautions. 2.5 Hall Effect. 2.6 Optical Techniques. 2.7 Secondary Ion Mass Spectrometry (SIMS). 2.8 Rutherford Backscattering (RBS). 2.9 Lateral Profiling. 2.10 Strengths and Weaknesses. Appendix 2.1 Parallel or Series Connection? Appendix 2.2 Circuit Conversion. References. Problems. Review Questions. 3 Contact Resistance and Schottky Barriers. 3.1 Introduction. 3.2 Metal-Semiconductor Contacts. 3.3 Contact Resistance. 3.4 Measurement Techniques. 3.5 Schottky Barrier Height. 3.6 Comparison of Methods. 3.7 Strengths and Weaknesses. Appendix 3.1 Effect of Parasitic Resistance. Appendix 3.2 Alloys for Contacts to Semiconductors. References. Problems. Review Questions. 4 Series Resistance, Channel Length and Width, and Threshold Voltage. 4.1 Introduction. 4.2 PN Junction Diodes. 4.3 Schottky Barrier Diodes. 4.4 Solar Cells. 4.5 Bipolar Junction Transistors. 4.6 MOSFETS. 4.7 MESFETS and MODFETS. 4.8 Threshold Voltage. 4.9 Pseudo MOSFET. 4.10 Strengths and Weaknesses. Appendix 4.1 Schottky Diode Current-Voltage Equation. References. Problems. Review Questions. 5 Defects. 5.1 Introduction. 5.2 Generation-Recombination Statistics. 5.3 Capacitance Measurements. 5.4 Current Measurements. 5.5 Charge Measurements. 5.6 Deep-Level Transient Spectroscopy (DLTS). 5.7 Thermally Stimulated Capacitance and Current. 5.8 Positron Annihilation Spectroscopy (PAS). 5.9 Strengths and Weaknesses. Appendix 5.1 Activation Energy and Capture Cross-Section. Appendix 5.2 Time Constant Extraction. Appendix 5.3 Si and GaAs Data. References. Problems. Review Questions. 6 Oxide and Interface Trapped Charges, Oxide Thickness. 6.1 Introduction. 6.2 Fixed, Oxide Trapped, and Mobile Oxide Charge. 6.3 Interface Trapped Charge. 6.4 Oxide Thickness. 6.5 Strengths and Weaknesses. Appendix 6.1 Capacitance Measurement Techniques. Appendix 6.2 Effect of Chuck Capacitance and Leakage Current. References. Problems. Review Questions. 7 Carrier Lifetimes. 7.1 Introduction. 7.2 Recombination Lifetime/Surface Recombination Velocity. 7.3 Generation Lifetime/Surface Generation Velocity. 7.4 Recombination Lifetime-Optical Measurements. 7.5 Recombination Lifetime-Electrical Measurements. 7.6 Generation Lifetime-Electrical Measurements. 7.7 Strengths and Weaknesses. Appendix 7.1 Optical Excitation. Appendix 7.2 Electrical Excitation. References. Problems. Review Questions. 8 Mobility. 8.1 Introduction. 8.2 Conductivity Mobility. 8.3 Hall Effect and Mobility. 8.4 Magnetoresistance Mobility. 8.5 Time-of-Flight Drift Mobility. 8.6 MOSFET Mobility. 8.7 Contactless Mobility. 8.8 Strengths and Weaknesses. Appendix 8.1 Semiconductor Bulk Mobilities. Appendix 8.2 Semiconductor Surface Mobilities. Appendix 8.3 Effect of Channel Frequency Response. Appendix 8.4 Effect of Interface Trapped Charge. References. Problems. Review Questions. 9 Charge-based and Probe Characterization. 9.1 Introduction. 9.2 Background. 9.3 Surface Charging. 9.4 The Kelvin Probe. 9.5 Applications. 9.6 Scanning Probe Microscopy (SPM). 9.7 Strengths and Weaknesses. References. Problems. Review Questions. 10 Optical Characterization. 10.1 Introduction. 10.2 Optical Microscopy. 10.3 Ellipsometry. 10.4 Transmission. 10.5 Reflection. 10.6 Light Scattering. 10.7 Modulation Spectroscopy. 10.8 Line Width. 10.9 Photoluminescence (PL). 10.10 Raman Spectroscopy. 10.11 Strengths and Weaknesses. Appendix 10.1 Transmission Equations. Appendix 10.2 Absorption Coefficients and Refractive Indices for Selected Semiconductors. References. Problems. Review Questions. 11 Chemical and Physical Characterization. 11.1 Introduction. 11.2 Electron Beam Techniques. 11.3 Ion Beam Techniques. 11.4 X-Ray and Gamma-Ray Techniques. 11.5 Strengths and Weaknesses. Appendix 11.1 Selected Features of Some Analytical Techniques. References. Problems. Review Questions. 12 Reliability and Failure Analysis. 12.1 Introduction. 12.2 Failure Times and Acceleration Factors. 12.3 Distribution Functions. 12.4 Reliability Concerns. 12.5 Failure Analysis Characterization Techniques. 12.6 Strengths and Weaknesses. Appendix 12.1 Gate Currents. References. Problems. Review Questions. Appendix 1 List of Symbols. Appendix 2 Abbreviations and Acronyms. Index.

6,573 citations


"Influence of post-hydrogenation upo..." refers methods in this paper

  • ...6 Ω cm (in house measured by the 4 Point Probe method [23])....

    [...]

BookDOI
01 Jan 1996
TL;DR: The client would like to get a larger, approximately 3 cm in diameter, well fixed tissue sample, together with a detailed report of the clinical presentation, gross, and microscopic lesions, along with the submission of samples prepared in a similar manner by the client for processing.
Abstract: We wrote it to be read by, and taught to, senior undergraduates and starting graduate students, rather than studied in a research laboratory. We wrote it using the same style and sentence construction that we have used in countless classroom lectures, rather than how we have written our countless (and much-less read) formal scientificpapers. In this respect particularly, wehave been deliberate in notreferencing the sources of every experimental fact or theoretical concept (although we do include some hints and clues in the chapters). However, at the end of each chapter we have included groups of references that should lead you to the best sources in the literature and help you go into more depth as you become more confident about what you are looking for. We are great believers in the value of history as the basis for under- standing the present and so the history of the techniques and key historical references are threaded throughout the book. Just because a reference is dated in the previous century (or even the antepenultimate century) doesn’t mean it isn’t useful! Likewise, with the numerous figures drawn from across the fields of materials science and engineering and nanotechnology, we do not reference the source in each caption. But at the very end of the book each of our many generous colleagues whose work we have used is clearly acknowledged.

4,412 citations

Journal ArticleDOI
TL;DR: EDS results confirmed a systematic increase of Eu content in the as-prepared samples with the increase of nominal europiumcontent in the reaction solution, and crystallinity and crystallite size of the titania particles decreased gradually.
Abstract: Uniform, spherical-shaped TiO2:Eu nanoparticles with different doping concentrations have been synthesized through controlled hydrolysis of titanium tetrabutoxide under appropriate pH and temperature in the presence of EuCl3·6H2O. Through air annealing at 500°C for 2 h, the amorphous, as-grown nanoparticles could be converted to a pure anatase phase. The morphology, structural, and optical properties of the annealed nanostructures were studied using X-ray diffraction, scanning electron microscopy, energy-dispersive X-ray spectroscopy [EDS], and UV-Visible diffuse reflectance spectroscopy techniques. Optoelectronic behaviors of the nanostructures were studied using micro-Raman and photoluminescence [PL] spectroscopies at room temperature. EDS results confirmed a systematic increase of Eu content in the as-prepared samples with the increase of nominal europium content in the reaction solution. With the increasing dopant concentration, crystallinity and crystallite size of the titania particles decreased gradually. Incorporation of europium in the titania particles induced a structural deformation and a blueshift of their absorption edge. While the room-temperature PL emission of the as-grown samples is dominated by the 5D0 - 7Fj transition of Eu+3 ions, the emission intensity reduced drastically after thermal annealing due to outwards segregation of dopant ions.

2,378 citations

Journal ArticleDOI
TL;DR: In this article, a monotone piecewise bicubic interpolation algorithm was proposed for data on a rectangular mesh, where the first partial derivatives and first mixed partial derivatives are determined by the mesh points.
Abstract: In a 1980 paper [SIAM J. Numer. Anal., 17 (1980), pp. 238–246] the authors developed a univariate piecewise cubic interpolation algorithm which produces a monotone interpolant to monotone data. This paper is an extension of those results to monotone $\mathcal{C}^1 $ piecewise bicubic interpolation to data on a rectangular mesh. Such an interpolant is determined by the first partial derivatives and first mixed partial (twist) at the mesh points. Necessary and sufficient conditions on these derivatives are derived such that the resulting bicubic polynomial is monotone on a single rectangular element. These conditions are then simplified to a set of sufficient conditions for monotonicity. The latter are translated to a system of linear inequalities, which form the basis for a monotone piecewise bicubic interpolation algorithm.

2,174 citations