2007
DOI: 10.1088/0022-3727/40/4/017
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Optical emission spectroscopic investigation of hydrogen plasma used for modification of electrical properties of multi-crystalline silicon

Abstract: Results of the treatment of multi-crystalline silicon with low-pressure inductive plasma are presented. Plasma treatment was found to increase silicon electrical conductivity to a greater value relative to its initial state; the time to reach this maximum was found to depend strongly on temperature between 120 and 400 °C. An effect of plasma parameters on collection efficiency and diffusion length was observed by EBIC measurements. An actinometry method based on optical emission spectroscopy measurements was u… Show more

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Cited by 22 publications
(7 citation statements)
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“…Using well established transition probability values of H atoms 28 and plotting I jfk λ jk /A jk g j against E j -E k , T e can be obtained. 29 The statistic weight of the higher energy levels of H R , H β , and H γ are 18, 32, and 50, corresponding to the principle quantum number 3, 4, and 5, respectively. The results were plotted in Figure 4b, showing a slight decrease with increasing Ar.…”
Section: Resultsmentioning
confidence: 99%
“…Using well established transition probability values of H atoms 28 and plotting I jfk λ jk /A jk g j against E j -E k , T e can be obtained. 29 The statistic weight of the higher energy levels of H R , H β , and H γ are 18, 32, and 50, corresponding to the principle quantum number 3, 4, and 5, respectively. The results were plotted in Figure 4b, showing a slight decrease with increasing Ar.…”
Section: Resultsmentioning
confidence: 99%
“…26,27 For the optical emission spectra (OES) of Ar plasma, the intense lines corresponding to Ar are observed in the range of 700nm to 800nm and Hydrogen species are at 410.2nm, 434nm and 656.5nm. 28 The presence of excited species in the cold atmospheric Ar plasma contributed to the deoxygenation of GO. When the GO deposited samples interacts with the ions, radicals and neutral molecules present in the plasma, deoxygenation starts.…”
Section: Resultsmentioning
confidence: 99%
“…We notice a progressive increase of the emission intensities of H α * with rising plasma power density and decreasing working pressure. Higher plasma power densities lead to an increase in the electronic temperature, favoring the excitation and then the dissociation of monatomic hydrogen . While at low pressures the energy of electrons is sufficient for H atom excitation leading to higher hydrogen emission intensity with high excitation temperatures .…”
Section: Resultsmentioning
confidence: 99%
“…Higher plasma power densities lead to an increase in the electronic temperature, favoring the excitation and then the dissociation of monatomic hydrogen . While at low pressures the energy of electrons is sufficient for H atom excitation leading to higher hydrogen emission intensity with high excitation temperatures . The reason for the reduction of the emission intensities at high pressures is that the molar fraction of atomic hydrogen drops and the recombination processes such as three‐body recombina‐ tion (H + + e + e → H* + e), dissociative recombination (H 2 + + e → H* + H), and mutual neutralization (H + + H – → H* + H) can be produced between atomic hydrogen and its excited state .…”
Section: Resultsmentioning
confidence: 99%
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