2007
DOI: 10.1016/j.apsusc.2007.02.008
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Control of reactive plasmas for low- k /Cu integration

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Cited by 36 publications
(18 citation statements)
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“…7(a) for positive ions and (b) for negative ions, for P ¼ 500 W, p ¼ 5 mTorr, and Ar flow of 1 sccm. While up to 6 positive ion species were detected ( 6 . The same behavior was observed for p ranging from 1 up to 10 mTorr and for discharge powers below 1600 W. This result is well correlated with the fact that SF À 5 and SF À 6 are formed for T e 0.7 eV while F À formation peaks around 1 eV.…”
Section: Resultsmentioning
confidence: 99%
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“…7(a) for positive ions and (b) for negative ions, for P ¼ 500 W, p ¼ 5 mTorr, and Ar flow of 1 sccm. While up to 6 positive ion species were detected ( 6 . The same behavior was observed for p ranging from 1 up to 10 mTorr and for discharge powers below 1600 W. This result is well correlated with the fact that SF À 5 and SF À 6 are formed for T e 0.7 eV while F À formation peaks around 1 eV.…”
Section: Resultsmentioning
confidence: 99%
“…[1][2][3][4][5][6][7] So far, only positive ions at low pressure and high plasma densities are used to ensure good anisotropy and high etching rates. [8][9][10][11][12][13][14][15][16][17][18][19] The continuous decreasing of the node size (now below 100 nm) at an increased devices density bring new challenges that need to be solved, including: charging-induced gate breakdown; 20,21 dependence of the etching rate on the pattern size (low RIE-lag effect 22 or aspect-ratio-dependence etching effect) and on the laid-out pattern density (microloading effect); 23 and handling of new materials such as low-k and high-k. 1 In particular, the notch phenomenon 24 induced by side etching with positive ions deflected by the positive space charge accumulated at the bottom of patterns has pointed to the possibility to reduce the charge build-up effect by etching with negative ions that induce lower charging potentials for similar ion fluxes and ion energy.…”
Section: Introductionmentioning
confidence: 99%
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“…This value is within the experimental error, revealing that the penetration depth that is caused by the plasma treatment depends less on the NH 3 /N 2 gas ratio than on the plasma treatment time, power, and method. 17 Additionally, the total thicknesses shrink after performing the plasma treatment, suggesting that the porous low-k films were densified by vacuum ultraviolet radiation, radical etching, and ion bombardment in the plasma with NH 3 /N 2 mixed gas. Furthermore, the sample was treated with pure NH 3 gas exhibited slightly higher thickness shrinkage than the others.…”
Section: Methodsmentioning
confidence: 99%
“…4,80,81) Because of this, a new technology for the prediction and control of these properties is required for the next generation of CMOS devices, in addition to the conventional waferless auto clean (WAC) process with SF 6 = O 2 plasma and the process of chamber wall coating with fluorocarbon plasma before etching. Specifically, hydrogen is normally included in various etching processes, such as those for the Si gate, SiN side wall (SW), and SiO 2 contact hole, and it has a high reactivity with other species.…”
Section: Plasma-chamber Wall Interactionmentioning
confidence: 99%