40% of ultrapure silicon is lost as kerf during slicing to produce wafers. Kerf is currently not being recycled due to engineering challenges and costs associated with removing its abundant impurities. Carbon left behind from the lubricant remains as one of the most difficult contaminants to remove in kerf without significant silicon oxidation. The present work enables to better understand the mechanism of carbon elimination in kerf which can aid the design of better processes for kef recycling and low cost photovoltaics. In this paper, we studied the kinetics of carbon elimination from silicon kerf in two atmospheres: air and N2, under a regime of no-diffusion-limitation. We report the apparent activation energy in both atmospheres using three methods: Kissinger, and two isoconversional approaches. In both atmospheres, a bimodal apparent activation energy is observed, suggesting a two stage process. A reaction mechanism is proposed in which (a) C-C and C-O bond cleavage reactions occur in parallel with polymer formation; (b) at higher temperatures, this polymer fully degrades in air but leaves a tarry residue in N2 that accounts for about 12% of the initial total carbon.
Silicon (Si) is the main semiconductor used in electronic and solar industries. Despite Si abundance in the earth’s crust, ultrapure silicon production is expensive as it goes through a myriad of industrial refining processes. These well-established processes1, developed and optimized for microchip needs, provide superior quality and purity at the cost of being highly energy intensive and wasteful, in that 68% of the initial silicon is converted to waste during the refining steps2. Microchips need only a few grams of silicon per chip, which comprise less than 1% of the final microchip cost. However, producing a solar module requires more than 400 g of silicon per m2, and silicon wafers add up to more than 45% of the total cost for installed modules1. This shows how silicon refining inefficiencies directly translate into high cost of solar modules, hindering its large scale implementation. Therefore, efficiency improvements in silicon manufacture are highly relevant.
A key point for improvement in ultrapure silicon processing is the production of wafers, consisting of slicing silicon ingots, which wastes 45% of the ultrapure material. Efforts such as ribbon technologies to avoid the need of axial slicing have been suggested3. Nevertheless, traditional wafer slicing techniques have shown higher efficiencies3,4, more reliability5 and better return on investment of the final solar panel6 compared to ribbon wafers. Thus, abrasive slicing from mono and polycrystalline ingots is still the dominant technology2. Wafers so produced are sliced from ingots using fixed abrasive or slurry methods7 that unavoidably produce silicon sawing dust (kerf) impregnated in lubricant.
Silicon carbide (SiC) was traditionally used in slurry slicing techniques, and its removal was the main concern in previous studies of kerf recycling8,9,10,11. However, recent advances in understanding of silicon ductile behavior in a narrow range of cutting speeds12 have enabled diamond wire sawing to produce better results than slurry slicing13. Further optimization of diamond wire slicing is still an ongoing effort14. Diamond wire kerf is a complex industrial residue containing numerous metallic contaminants15 and organics from the polymeric lubricant used during slicing. The exact composition of this lubricant is protected by proprietary rights. However, it is known to be mainly composed of polyethylene glycol (PEG)16 mass average molar mass (Mw) around 400–500 or combinations of PEG with diethylene glycol (DEG)17. To date, a few authors have reported methodologies for recycling kerf produced during diamond wire slicing. Their results point to the need for efficient removal of carbon. Tomono et al.16 reacted kerf with bromine forming bromosilanes for further distillation. Unfortunately, the carbon content in kerf reacted to form brominated organic compounds that behaved azeotropically and could not be separated via distillation. Dhamrin et al.17, on the other hand, melted kerf to make solar panels and showed the devastating effect that carbon contamination has on the efficiency of the so formed devices. Finally, Maeda et al.18 reported improvements in solar panel efficiency from recycled kerf by milling kerf and heating it in inert gas to remove carbon.
Previous efforts by Vazquez-Pufleau et al.19 demonstrated that carbon elimination from kerf was feasible using a furnace aerosol reactor (FuAR). In air, at high temperatures and low residence times, total carbon (TC) measurements below detection limits were achieved. To design an industrial reactor with more certainty, it is important to better understand the process and the kinetics of carbon elimination in a FuAR, including accurate activation energy (EA) values for the full range of conversion. To the best of our knowledge, the kinetics for the removal of organics for a metal recycling and particularly for silicon kerf, as well as the mechanistic understanding of the reaction paths, have not been systematically studied. Both will be required for industrial scale up of kerf recycling processes.
The most important parameter for determining the kinetic behavior of a reacting system with Arrhenius behavior is the EA20. The k0 parameter, or pre-exponential factor, can then be determined via compensation effect21, which depends on the reaction model employed. However, the EA remains unaffected even if the kinetic model employed is incorrectly chosen. Therefore, the focus of kinetics has historically been EA determinations20. The Kissinger method is a simple and well known technique to obtain EA, but this value is determined based on limited information, i.e. the peak values of the reaction rate. The values obtained are more meaningful after comparing and contrasting with isoconversional analysis, which provides reliable EA values for the entire range of conversion22. Reliable EA for the entire range of conversion is needed because a single value of EA is not enough to describe the full process for polymeric decomposition, as the apparent EA might be different from the intrinsic EA due to competition among radical polymerization, homolysis and volatilization23.
In general, the elimination of residual polymer contamination from powders has not been widely studied, even less so in the case of kerf. Nevertheless, kinetic studies for pure PEG have been executed experimentally23,24,25,26,27,28,29 and theoretically30. A detail discussion on the PEG literature is provided in the supplementary section. The reported PEG literature needs to be analyzed carefully to extrapolate the findings under ideal conditions to conditions of real kerf recycling systems full of other contaminants. As Lin et al.31 have observed, the presence of nanoparticles significantly alters the degradation kinetics for PEG which follows a different degradation process when combined with Ni and Al nanoparticles. Ni accelerated the decomposition whereas Al was a retardant at the beginning but accelerated the decomposition at a later stage. This indicates that the kinetics and mechanism of removal of slicing lubricant (composed of PEG and additives) from kerf (made of silicon nanoparticles and metallic contaminants) might differ compared to pure PEG degradation.
In this work, based on thermogravimetric analysis (TGA) results, we determine the activation energy (EA) of carbon removal in kerf using the Kissinger method and Ozawa-Flynn-Wall (OFW) and Kissinger-Akahira-Sunose (KAS) isoconversional analysis. Additionally, we present characterization results from samples thermally treated by TGA in either air or N2 using Fourier transformed infrared (FTIR) spectroscopy, gas chromatography mass spectroscopy (GCMS), total carbon (TC) determination, Brunauer–Emmett–Teller (BET) surface area measurement and scanning electron microscopy (SEM). At the end, we provide an overall reaction mechanism for the elimination of carbon from kerf based on the instrumental evidence.
Results and Discussion
Kerf was initially characterized by BET, and had a surface area of 9.6 m2/g, a pore volume of 0.052 cm3/g and a pore radius of 15.6 Å, proving its large surface area and flake-like morphology. In this section the results of each technique are presented separately followed by a brief discussion of direct implications for the individual instrumental observations summarized in Table 1. Finally, in the mechanism section, the implications for all results and individual instrument discussions are combined. Under the complexity of kerf composition and carbon elimination kinetics, a qualitative reaction mechanism is provided.
Total carbon content
The conversion of carbon calculated using traditional TGA weight loss method was compared with a TGA-TC method (using TGA and stopping the run to determine its remaining total carbon (TC) content at various temperatures). The heating rate chosen of 20 °C/min is sufficiently high to emulate real aerosol reactor conditions and at the same time, low enough to guarantee mass and heat transfer. Thus, providing an accurate thermogravimetric reading. Figure 1 shows that the conversion using the two methods differs. A discussion of differences in conversion using TGA and TC is provided in the supplementary section.
Gas chromatography mass spectroscopy
Based on their chemical composition, detected peaks were classified into different categories as: CnHm (aliphatic compounds containing only carbon and hydrogen with m ~ 2n), Unsat. HC (unsaturated hydrocarbons CnHm with m ~ n), CnHmNl, CnHmOl and CnHmOlSik. The chromatogram area corresponding to all components assigned to each category were summed and normalized with respect to the total area, a relative abundance value was assigned for each category. See Fig. 2(a) for samples treated in air and Fig. 2(b) for samples treated in N2. A discussion follows for each atmosphere based on observations for each category except for CnHmOlSik, whose consistent presence in most samples is explained in a separate paragraph.
In Fig. 2(a), for samples treated in air, GCMS shows that the highest rate of all volatiles formation occurs around 300 °C and no unsaturated CnHm compounds are observed at any temperature. CnHmOl compounds seem to be present in the same ratio (around 20%) at all temperatures except at the peak of volatile formation where its presence becomes more abundant. Elimination of nitrogenated compounds peak at 450 °C, showing that they are more difficult to remove than oxygenated compounds or aliphatic compounds that have an absolute peak at 300 °C.
Figure 2(b) summarizes the GCMS data for samples treated in N2 atmosphere. There, the peak of volatiles formation occurs at a higher temperature than in air; at about 350 °C and, beyond this temperature, a significant amount of unsaturated compounds gets released. CnHmOl compounds are abundant at the beginning, but their abundance drops after 350 °C. A significant fraction of saturated compounds is visible at 450 °C, and at 550 °C all of the CnHm compounds are already saturated. This can be interpreted as the lack of available O2 causes any remaining polymer in kerf to undergo saturation reactions, leaving a carbonaceous residue that is hard to pyrolyze (tar). This agrees with the TC results from Fig. 1, where not all the carbon can be eliminated. In contrast, in the air atmosphere, the availability of O2 permits virtually full polymer decomposition into volatiles and thus no saturated CnHm compounds are formed. Nitrogenated compounds in N2 atmosphere become more abundant in terms of total signal as temperatures rise. Based on XPS evidence (See supplementary information), the nitrogen source of the nitrogenated compounds is the lubricant itself. Finally, the total GCMS signal for the pyrolysis is 6 times more intense than the one for air atmosphere (combustion) indicating that, during the combustion process, a significant fraction of volatiles fully reacts into CO2.
During TGA thermal operations, siloxanes seem always to be present in trace amounts. This is due to the presence of silicon nanoparticles in contact with the lubricant. Its total abundance seems to be constant, but due to large differences in the abundance of other compounds, its fraction is highly diluted on the peaks of signal and conversely overshadows other components especially at the beginning of the TGA thermal run and at the end when most of the organics have already been released.
Fourier transformed infrared spectroscopy
The results of FTIR for different temperatures are displayed in Fig. 3(a) for kerf treated in air atmosphere and Fig. 3(b) for kerf treated in N2 atmosphere. The peak assignment with references is presented in Supplementary Table 1. The peaks can be classified into molecular motion of three groups: silicon and SiOx, organics, and Al. Insights into sample composition are gained through analyzing the molecular motion characteristics of the most important peaks.
Regarding silicon, the peak at ~1230 cm−1 is attributed to the silicon longitudinal optical (LO) mode. The peak at ~1050 cm−1 is attributed to transverse optical (TO) mode of the silicon asymmetric stretching vibrations32. It is well known that the exact peak of TO in cm−1 is proportional to the thickness of the alpha-SiO2 layer with an interface region of about 1.6 nm and corresponds to a simplified chemical formula of SiO33. Both the outer layer of SiO2 and the interface with Si include effects such as compressive stress and roughness that change the LO and TO mode. Furthermore, the peak intensity of TO and LO is directly correlated with the degree of silicon oxidation34. In our case TO for air is evidently larger than the one for N2, evidencing a higher degree of oxidation in the first scenario.
Organic peaks are small due to their low mass fraction in the sample. Before thermal treatment, total organics account for 4% of the sample, TC is 1.3%. After thermal treatment, TC approaches 0% for air and 0.15% in N2, imposing instrumental detection challenges. The peak at 960 cm−1 corresponds to hydrocarbon CH2 motion in the C axis25. A C-O stretching characteristic peak25 appears at 1149 cm−1 in the region between TO and LO altering its shape. CH2 scissoring is attributed to the peak at 1460 cm−1 25. Depending on the molecular weight (MW) of PEG, a difference of up to 10 cm−1 in the peaks of characteristic bonds can be expected35. Finally, in the region between 1300 and 1600 cm−1 several peaks are observed at low temperatures. These peaks are attributed to stretching and bending of modes of aromatic hydrocarbons36. Most of these peaks disappear at high temperatures, indicating decomposition. However, above 700 °C in N2 atmosphere, a small differentiated peak can be observed that does not appear in air atmosphere. This peak is attributed to aromatic hydrocarbons37 that are believed to be the tarry residue following pyrolysis of the polymer mixture. This is in agreement with TC measurements.
The third most abundant contaminant in kerf after oxygen and carbon, see Table 2, is aluminum (0.3%). The peak at 1612 cm−1 of the kerf sample is similar for both atmospheres and is assigned to be due to Al2-O3 vibration38. It originates from the beam supporting the ingot during slicing.
Kinetics of carbon elimination in kerf were evaluated using three thermogravimetric analysis methods: OFW, KAS and Kissinger. The three methods are used in conjunction as their combined results provide more certainty on the accuracy of the obtained activation energy22. The raw quadruplet data at four different heating rates and its derivatives are shown for air in Fig. 4(a) and for N2 in Fig. 4(b). For information on determination of OFW and KAS EA refer to the supplementary section. The EA determined with the Kissinger method was obtained by computing the peak values of the derivatives from insets of Fig. 4(a) and (b). The apparent EA determination results from the three methods are compared in Fig. 5(a) for air and Fig. 5(b) for N2. The OFW and KAS methods provide a similar plot as they are both isoconversional methods, yet the KAS determined EA is considered to be a more accurate method22. The first peak for both gases shows a rather similar behavior even though in air the EA is about 10 kJ/mol lower than in N2. However, the second peak for EA is significantly more elevated in N2 than in air, suggesting a radically different mechanism for this second stage.
Stages of the process
Carbon elimination in kerf is a two stage process
The rate of weight loss as a function of temperature exhibits two peaks, both in air, and in N2 (Fig. 4). The similar two-peak dependence is observed for the apparent activation energy as a function of conversion. Two peak phenomenon is the first fingerprint that our process is characterized by two stages. These stages are well distinguished by the products which are observed within the different temperature domains. (See Fig. 2 with the elemental characterization of corresponding volatiles).
GCMS for both air atmospheres and N2 shows two differentiated processes. In air, CnHm compounds are observed up to 350 °C and not above this temperature. In the case of N2, saturated CnHm compounds at temperatures above 450 °C, become less abundant, and unsaturated CnHm compounds become more dominant. This comes in accordance with Arisawa et al.23, who reported that below this temperature, PEG forms both volatiles and a higher MW residue. Above this temperature, both PEG and its higher MW residue begin to decompose. Similar observations have been made for PEG decompositions at low pressure28. All of these facts provide evidence that carbon elimination in kerf is a two stage process.
Apparent activation energy and stages of the process
Apparent activation energies, both for air and N2 atmospheres, as a function of conversion are not constant. Moreover, they are not constant even within the stages selected. This is consistent with observations of EA behavior on PEG at comparable conditions by Arisawa et al.23. The two-peak apparent energy dependence is observed for the N2 atmosphere. Also the similar dependence is presented for the air atmosphere. For both cases, one can distinguish the clear ‘volcano-shape’ peculiarities of these dependences.
In the kinetic and catalytic literature, the observed increase in the apparent activation energy is typically attributed to the endothermic reactions, while the decrease is attributed to exothermic reactions39,40,41. The decrease in EA between the two peaks for either air or N2 shows the point where the exothermic process (likely, polymerization) provides energy for volatiles to evolve but also diminishes the rate of total volatiles being released at that particular temperature. Then, in the second stage, the endothermic process (cleavage of molecules) produces the increase in EA and releases more mass in the gas phase. Generally, two stages of our process present an interplay between the endothermic and exothermic factors.
All these facts provide evidence that our process is complex, displays at least two stages, and every stage is not an elementary reaction.
Chemical reactions. Preliminary considerations
Evolution of chemical composition in the course of the TGA provides vast information about the complexity of our process within each stage.
Both atmospheres display a qualitatively analogous first stage, yet with different magnitudes. Based on GCMS (Fig. 2), oxygenated compounds, released as volatiles in the N2 atmosphere are abundant at the beginning of the 1st peak (Fig. 4), but become scarce after 350 °C. On the other hand, in air for the same temperature domains, the oxygenated compounds ratio remains constant. This suggests that for the first stage, volatiles are evolving from comparably analogous mechanisms where the polymer cleaves itself using its own oxygen atoms to favor bond rupture. This holds true for both atmospheres (air and N2), although the magnitude of the effect is different. Moisture and low MW volatiles can be ruled out as the kerf sample was heated up to 120 °C for 1 hr and TGA showed a plateau in weight loss.
Furthermore, the results for the formation of CnHm aliphatic compounds for pyrolysis (N2 atmosphere) conditions show firstly an increasing degree of polymerization with progressively increasing chain length. At temperatures below 350 °C, highly saturated linear chains form and volatize, and above that temperature more unsaturated compounds become prevalent. This is in agreement with Lattimer et al.27 who report that up to their tested temperature of 325 °C, in pyrolysis, no unsaturated compounds were found on volatilized products.
In the second stage domain, a larger fraction of oxygenated compounds is found via GCMS in air rather than in N2. This indicates that in the air atmosphere, either oxygen reacts with the polymer and gets incorporated into the volatile chains as part of the reaction mechanism or the evolved gases oxidize in the gas phase. For N2, a relative lower abundance of oxygenated compounds indicates that as oxygen becomes less abundant in the remaining polymeric chain, C-C cleavage turns more dominant, yet not the sole reaction pathway. In the case of air atmosphere, CnHm saturated compounds are not detected beyond 350 °C, and unsaturated CnHm compounds were not found at any temperature.
Higher MW polymer formation
Based on the FTIR results in N2, as shown in Fig. 3(b), a small peak visible above 700 °C, is attributable to tar. Additionally, 12% of the original TC cannot be removed. This proves that pyrolysis is not enough for full carbon elimination of kerf lubricant. Lattimer et al.27 similarly observed a dark colored PEG residue attributable to highly unsaturated organics. In the case of N2, this higher MW PEG residue strongly influences the second peak decomposition features. Furthermore C-O and C-C bond cleavage (volatile formation) competes with radical recombination generating an even higher MW residue (tar), in agreement with previous studies23,42,43.
Analysis of apparent EA dependences
As indicated, the apparent EA dependence on temperature is characterized by two peaks similar to the rate of volatiles elimination. We considered it as a fingerprint of the two stage process. However even within one stage this apparent energy is not constant. Obviously it is the strong kinetic fingerprint that each stage is not an elementary reaction. Moreover, the maximum of the apparent energy for each stage can be interpreted as a result of the complicated interplay between at least two reactions, endothermic for decomposition reactions and exothermic for polymerization reactions. This interplay can be attributed both to the first and second stage.
Based on the presented composition and kinetic data and supported by the literature for PEG, a mechanism for the elimination of carbon from the slicing lubricant in kerf is presented graphically in Fig. 6.
The reduction of mass during TGA in air can be explained by the formation of species with lower MW due to thermal degradation released to the gas phase upon formation. For the first stage, there are two competing types of reactions during thermal oxidation of PEG: oxidative degradation of PEG by a chain scission mechanism, and polymerization of PEG by loose crosslinking. The process of degradation consists primarily of competing C-C and C-O bond cleavage occurring in parallel at arguably comparable rates28. This is not different for the decomposition of polypropylene Glycol (PPG) or its related compounds24. During TGA in air, PEG undergoes thermal degradation forming lower MW species which are released into the gas phase, causing weight loss.
The second stage consists of the higher MW PEG undergoing full degradation into volatiles, with a peak in the formation of volatiles around 280 °C. No remaining carbon could be measured after exposing the sample up to 900 °C using a heating rate of 20 °C/min.
The proposed mechanism for kerf lubricant degradation in N2 involves also two types of reaction as in air, each comprising different mechanisms. In the first stage, the two overall processes occur in parallel. Competing C–C and C–O scissions take place to form volatiles, while at the same time, a higher MW polymer is formed at the same temperature as in the case of air (230 °C) hinting that the process might be the same in both atmospheres. Whereas in air the formation of volatiles dominates, in N2, the conditions favor the formation of high MW residue.
In the second stage in N2, the same two processes occur as in the first stage, C–O and C–C bond scissions compete to form volatiles. Those volatiles include a large fraction of saturated hydrocarbons in the gas phase that are not seen in the corresponding second stage in air. In N2, similar to the first stage, the polymerization continues and forms a tarry residue. This residue accounts for about 12% of the original TC content even after heating up to 900 °C using a heating rate of 20 °C/min. and shows that C elimination is not achievable under inert atmospheres. Tar was not observed in air.
Interpretation of ‘volcano-shape’ energetic dependences
Our activation energy curves are similar to volcano-shape energetic dependences (volcano curves) which have been found in many heterogeneous chemical systems, particularly in gas-solid catalytic systems Typically, the interpretation of these interesting effects is presented based on linear correlations between the activation energy and the reaction enthalpy, Broensted-Evans-Polyani correlations, with the different sign, positive or negative, for endothermic and exothermic reactions, respectively44. In a simple way, the volcano curve can be explained by the compromise between endothermic and exothermic reactions.
In summary, we studied the carbon elimination from kerf and defined it as a two stage process based on TGA analysis. The activation energy for carbon elimination from kerf and its evolution was obtained in air and N2 atmosphere from room temperature to 900 °C. We developed a mechanistic model based on characterization tools including TC, FTIR, and GCMS and supported the model by the PEG decomposition literature. This mechanism is proposed as the skeleton of the actual reaction mechanism for the thermal decomposition of slicing lubricant in kerf in air and N2. In the first stage of our proposed model, the reaction rate is dominated by long hydrocarbon chains undergoing depolymerization by rupture of C-C and C–O bonds in competition with further polymerization. This happens in both atmospheres, but with different output ratios. The second stage is radically different for each atmosphere. In the case of air, this second stage is less energy demanding and the carbonaceous compounds polymerize to a lesser extent facilitating the removal of organics during the second stage. Complete carbon elimination in N2 atmosphere was not achieved under the temperatures and heating rates tested. The reaction rate is slower compared to air and yields a tarry byproduct (12% of original TC content) that cannot be easily eliminated by further heating.
We observe a higher rate of carbonaceous compound removal from kerf in air than in N2 atmosphere; however, this comes at the cost of oxidizing the silicon which is undesirable for kerf purification. The kinetics of carbon elimination should be linked with a model for silicon oxidation in kerf. A first approximation can be obtained from the Deal and Grove model45. However, the development of more accurate models for silicon oxidation from kerf is desirable. Further research on different concentrations of O2 and N2 could provide optimum conditions to maximize carbonaceous compound elimination while minimizing silicon oxidation. Such models will help to design processes to more effectively recycle and re-use kerf so as to bring down costs of Si wafers.
Kerf was provided by SunEdison, Inc. (Saint Louis, MO) along with its elemental analysis determined by combustion infrared, inert gas fusion non dispersive infrared, and glow discharge mass spectrometry shown in Table 2. The surface area determination was performed using a Nova 200e BET instrument (Quantachrome Instruments, Boynton Beach, FL). Surface morphology and structural analysis were obtained by SEM in a FEI Nova 2300 SEM (FEI, Hillsboro, OR). Kerf was dried and its volatiles were removed by keeping the sample at 120 °C for 60 min before the experiments. Kerf was heated to various temperatures using TGA in a Q5000 IR thermogravimetric analyzer (TA Instruments, New Castle, DE) using a heating rate of 20 °C/min up to various temperatures at intervals of around 200 °C in either air (Airgas, St. Louis, MO) or ultra-high purity (99.999%) N2 (Airgas, St. Louis, MO). Samples were then quickly cooled down by shutting off the TGA furnace and characterized using TC determinations (Shimadzu SSM-5000, Schimadzu, Columbia, MD) with a solid sample module and FTIR spectroscopy (Nicolette Nexus 470 GMI, Ramsey, MN). The volatiles, evolved from kerf at different temperatures and atmospheres, were extracted from the TGA exhaust at the desired temperature using a gas tight 0.5 mL Luer syringe (Restek, Bellefonte, PA) and were immediately injected into a RTX 50 gas chromatography (GC) column equipped with mass spectroscopy (MS) (Agilent 5975 C Series GC/MSD, Santa Clara, CA). Peaks were integrated using Agilent Mass Hunter Quantitative Analysis Software and identified using the NIST library.
TGA for kinetic analysis
TGA was used to determine the kinetics of carbon elimination in kerf. Each kerf sample was heated up to 120 °C and kept at that temperature for 60 min to remove water and volatiles from the sample. DEG as a component of the lubricant has a vapor pressure of 5.6 Torr at 120 °C46 and would be removed from the sample within this time (1 hr). Dried kerf samples were then subjected to four heating rates: 2, 5, 10 and 20 °C/min. under combustion (air) or pyrolysis (ultrapure N2, 99.999%). The experiments were run in triplicate. A detailed discussion of the thermal analysis methods to determine EA is provided in the supplementary section.
How to cite this article: Vazquez-Pufleau, M. et al. Carbon elimination from silicon kerf: Thermogravimetric analysis and mechanistic considerations. Sci. Rep. 7, 40535; doi: 10.1038/srep40535 (2017).
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This work was partially supported by the Solar Energy Research Institute for India and the United States (SERIIUS), funded jointly by the U.S. Department of Energy (Office of Science, Office of Basic Energy Sciences, and Energy Efficiency and Renewable Energy, Solar Energy Technology Program, under Subcontract DE-AC36-08GO28308 to the National Renewable Energy Laboratory, Golden, Colorado) and the Government of India, through the Department of Science and Technology under Subcontract IUSSTF/JCERDC-SERIIUS/2012. The Nano Research Facility (NRF) at Washington University in St. Louis, a member of the National Nanotechnology Infrastructure Network (NNIN) was used for SEM analysis.
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