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Effect of oxide film on nanoscale mechanical removal of pure iron

In this paper, the properties of an oxide film formed on a pure iron surface after being polished with an H 2 O 2 -based acidic slurry were investigated using an atomic force microscope (AFM), Auger electron spectroscopy (AES), and angle-resolved X-ray photoelectron spectroscopy (AR-XPS) to partly r...

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Published in:Friction 2018-09, Vol.6 (3), p.307-315
Main Authors: Liu, Jinwei, Jiang, Liang, Deng, Changbang, Du, Wenhao, Qian, Linmao
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creator Liu, Jinwei
Jiang, Liang
Deng, Changbang
Du, Wenhao
Qian, Linmao
description In this paper, the properties of an oxide film formed on a pure iron surface after being polished with an H 2 O 2 -based acidic slurry were investigated using an atomic force microscope (AFM), Auger electron spectroscopy (AES), and angle-resolved X-ray photoelectron spectroscopy (AR-XPS) to partly reveal the material removal mechanism of pure iron during chemical mechanical polishing (CMP). The AFM results show that, when rubbed against a cone-shaped diamond tip in vacuum, the material removal depth of the polished pure iron first slowly increases to 0.45 nm with a relatively small slope of 0.11 nm/μN as the applied load increases from 0 to 4 μN, and then rapidly increases with a large slope of 1.98 nm/μN when the applied load further increases to 10 μN. In combination with the AES and AR-XPS results, a layered oxide film with approximately 2 nm thickness (roughly estimated from the sputtering rate) is formed on the pure iron surface. Moreover, the film can be simply divided into two layers, namely, an outer layer and an inner layer. The outer layer primarily consists of FeOOH (most likely α-FeOOH) and possibly Fe 2 O 3 with a film thickness ranging from 0.36 to 0.48 nm (close to the 0.45 nm material removal depth at the 4 μN turning point), while the inner layer primarily consists of Fe 3 O 4 . The mechanical strength of the outer layer is much higher than that of the inner layer. Moreover, the mechanical strength of the inner layer is quite close to that of the pure iron substrate. However, when a real CMP process is applied to pure iron, pure mechanical wear by silica particles generates almost no material removal due to the extremely high mechanical strength of the oxide film. This indicates that other mechanisms, such as in-situ chemical corrosion-enhanced mechanical wear, dominate the CMP process.
doi_str_mv 10.1007/s40544-018-0238-2
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The AFM results show that, when rubbed against a cone-shaped diamond tip in vacuum, the material removal depth of the polished pure iron first slowly increases to 0.45 nm with a relatively small slope of 0.11 nm/μN as the applied load increases from 0 to 4 μN, and then rapidly increases with a large slope of 1.98 nm/μN when the applied load further increases to 10 μN. In combination with the AES and AR-XPS results, a layered oxide film with approximately 2 nm thickness (roughly estimated from the sputtering rate) is formed on the pure iron surface. Moreover, the film can be simply divided into two layers, namely, an outer layer and an inner layer. The outer layer primarily consists of FeOOH (most likely α-FeOOH) and possibly Fe 2 O 3 with a film thickness ranging from 0.36 to 0.48 nm (close to the 0.45 nm material removal depth at the 4 μN turning point), while the inner layer primarily consists of Fe 3 O 4 . The mechanical strength of the outer layer is much higher than that of the inner layer. Moreover, the mechanical strength of the inner layer is quite close to that of the pure iron substrate. However, when a real CMP process is applied to pure iron, pure mechanical wear by silica particles generates almost no material removal due to the extremely high mechanical strength of the oxide film. This indicates that other mechanisms, such as in-situ chemical corrosion-enhanced mechanical wear, dominate the CMP process.</description><identifier>ISSN: 2223-7690</identifier><identifier>EISSN: 2223-7704</identifier><identifier>DOI: 10.1007/s40544-018-0238-2</identifier><language>eng</language><publisher>Beijing: Tsinghua University Press</publisher><subject>Atomic force microscopes ; Atomic force microscopy ; Chemical-mechanical polishing ; Corrosion and Coatings ; Corrosive wear ; Diamonds ; Engineering ; Film thickness ; Hematite ; Hydrogen peroxide ; Iron oxides ; Mechanical Engineering ; nanoscale mechanical removal ; Nanotechnology ; Organic chemistry ; Oxide coatings ; oxide film ; Physical Chemistry ; pure iron ; Research Article ; Silicon dioxide ; Slurries ; Spectrum analysis ; Substrates ; Surfaces and Interfaces ; Tensile strength ; Thin Films ; Tribology ; Wear mechanisms ; X ray photoelectron spectroscopy</subject><ispartof>Friction, 2018-09, Vol.6 (3), p.307-315</ispartof><rights>The author(s) 2018</rights><rights>Friction is a copyright of Springer, (2018). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c425t-a19790e9c8be052db0bf703c262f855e3cb49d39df204b20f78935cf7234e0cb3</citedby><cites>FETCH-LOGICAL-c425t-a19790e9c8be052db0bf703c262f855e3cb49d39df204b20f78935cf7234e0cb3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2100181571/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2100181571?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,25753,27924,27925,37012,44590,75126</link.rule.ids></links><search><creatorcontrib>Liu, Jinwei</creatorcontrib><creatorcontrib>Jiang, Liang</creatorcontrib><creatorcontrib>Deng, Changbang</creatorcontrib><creatorcontrib>Du, Wenhao</creatorcontrib><creatorcontrib>Qian, Linmao</creatorcontrib><title>Effect of oxide film on nanoscale mechanical removal of pure iron</title><title>Friction</title><addtitle>Friction</addtitle><description>In this paper, the properties of an oxide film formed on a pure iron surface after being polished with an H 2 O 2 -based acidic slurry were investigated using an atomic force microscope (AFM), Auger electron spectroscopy (AES), and angle-resolved X-ray photoelectron spectroscopy (AR-XPS) to partly reveal the material removal mechanism of pure iron during chemical mechanical polishing (CMP). The AFM results show that, when rubbed against a cone-shaped diamond tip in vacuum, the material removal depth of the polished pure iron first slowly increases to 0.45 nm with a relatively small slope of 0.11 nm/μN as the applied load increases from 0 to 4 μN, and then rapidly increases with a large slope of 1.98 nm/μN when the applied load further increases to 10 μN. In combination with the AES and AR-XPS results, a layered oxide film with approximately 2 nm thickness (roughly estimated from the sputtering rate) is formed on the pure iron surface. Moreover, the film can be simply divided into two layers, namely, an outer layer and an inner layer. The outer layer primarily consists of FeOOH (most likely α-FeOOH) and possibly Fe 2 O 3 with a film thickness ranging from 0.36 to 0.48 nm (close to the 0.45 nm material removal depth at the 4 μN turning point), while the inner layer primarily consists of Fe 3 O 4 . The mechanical strength of the outer layer is much higher than that of the inner layer. Moreover, the mechanical strength of the inner layer is quite close to that of the pure iron substrate. However, when a real CMP process is applied to pure iron, pure mechanical wear by silica particles generates almost no material removal due to the extremely high mechanical strength of the oxide film. 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The AFM results show that, when rubbed against a cone-shaped diamond tip in vacuum, the material removal depth of the polished pure iron first slowly increases to 0.45 nm with a relatively small slope of 0.11 nm/μN as the applied load increases from 0 to 4 μN, and then rapidly increases with a large slope of 1.98 nm/μN when the applied load further increases to 10 μN. In combination with the AES and AR-XPS results, a layered oxide film with approximately 2 nm thickness (roughly estimated from the sputtering rate) is formed on the pure iron surface. Moreover, the film can be simply divided into two layers, namely, an outer layer and an inner layer. The outer layer primarily consists of FeOOH (most likely α-FeOOH) and possibly Fe 2 O 3 with a film thickness ranging from 0.36 to 0.48 nm (close to the 0.45 nm material removal depth at the 4 μN turning point), while the inner layer primarily consists of Fe 3 O 4 . The mechanical strength of the outer layer is much higher than that of the inner layer. Moreover, the mechanical strength of the inner layer is quite close to that of the pure iron substrate. However, when a real CMP process is applied to pure iron, pure mechanical wear by silica particles generates almost no material removal due to the extremely high mechanical strength of the oxide film. This indicates that other mechanisms, such as in-situ chemical corrosion-enhanced mechanical wear, dominate the CMP process.</abstract><cop>Beijing</cop><pub>Tsinghua University Press</pub><doi>10.1007/s40544-018-0238-2</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record>
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subjects Atomic force microscopes
Atomic force microscopy
Chemical-mechanical polishing
Corrosion and Coatings
Corrosive wear
Diamonds
Engineering
Film thickness
Hematite
Hydrogen peroxide
Iron oxides
Mechanical Engineering
nanoscale mechanical removal
Nanotechnology
Organic chemistry
Oxide coatings
oxide film
Physical Chemistry
pure iron
Research Article
Silicon dioxide
Slurries
Spectrum analysis
Substrates
Surfaces and Interfaces
Tensile strength
Thin Films
Tribology
Wear mechanisms
X ray photoelectron spectroscopy
title Effect of oxide film on nanoscale mechanical removal of pure iron
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