Loading…

Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings

In the field of hard protective coatings, nano-crystalline Ti-B-N films are of great importance due to the adjustable microstructure and mechanical properties through their B content. Here, we systematically study this influence of B on Ti-B-N during reactive as well as non-reactive DC magnetron spu...

Full description

Saved in:
Bibliographic Details
Published in:Surface & coatings technology 2021-08, Vol.420, p.127327, Article 127327
Main Authors: Hahn, R., Tymoszuk, A., Wojcik, T., Kirnbauer, A., Kozák, T., Čapek, J., Sauer, M., Foelske, A., Hunold, O., Polcik, P., Mayrhofer, P.H., Riedl, H.
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3
cites cdi_FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3
container_end_page
container_issue
container_start_page 127327
container_title Surface & coatings technology
container_volume 420
creator Hahn, R.
Tymoszuk, A.
Wojcik, T.
Kirnbauer, A.
Kozák, T.
Čapek, J.
Sauer, M.
Foelske, A.
Hunold, O.
Polcik, P.
Mayrhofer, P.H.
Riedl, H.
description In the field of hard protective coatings, nano-crystalline Ti-B-N films are of great importance due to the adjustable microstructure and mechanical properties through their B content. Here, we systematically study this influence of B on Ti-B-N during reactive as well as non-reactive DC magnetron sputtering. The different deposition routes allow for an additional, very effective key parameter to modify bond characteristics and microstructure. Plasma analysis by mass spectroscopy reveals that for comparable amounts of Ti+, Ti2+, Ar+, and Ar2+ ions, the count of N+ ions is about 2 orders of magnitude lower during non-reactive sputtering. But for the latter, the N+/N2+ ratio is close to 1, whereas during reactive sputtering this ratio is only 0.1. This may explain why during reactive deposition of Ti-B-N, the BN bonds dominate (as suggested by X-ray photoelectron spectroscopy), whereas the BB and TiB bonds dominate for non-reactively prepared Ti-B-N. Chemically, reactively versus non-reactively sputtered Ti-B-N coatings follow the TiN-BN versus TiN-TiB2 tie line, respectively. Detailed X-ray diffraction and transmission electron microscopy studies reveal, that up to 10 at.% B can be dissolved in the fcc-TiN lattice when prepared by non-reactive sputtering, whereas already for a B content of 4 at.% a BN-rich boundary phase forms when reactively sputtered. Thus, we could not only observe a higher hardness (35 GPa instead of 25 GPa) as well as a higher indentation modulus (480 GPa instead of 260 GPa), but also a higher fracture energy (0.016 instead of 0.009 J/m during cube-corner indentations) for Ti-B-N coatings with 10 at.% B, when prepared non-reactively. •Major differences in plasma species between reactive and non-reactive sputtering•The elemental composition also varies with the deposition route.•Significant differences in mechanical properties at higher boron contents
doi_str_mv 10.1016/j.surfcoat.2021.127327
format article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2569688486</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0257897221005016</els_id><sourcerecordid>2569688486</sourcerecordid><originalsourceid>FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3</originalsourceid><addsrcrecordid>eNqFkMtOwzAQRS0EEqXwC8gS6wQ_mtjeARUvqQIWZW05zoQ6auNgO5X696QUJHasRjO6c-fOQeiSkpwSWl63eRxCY71JOSOM5pQJzsQRmlApVMb5TByjCWGFyKQS7BSdxdgSQqhQswlybysTATc-bExyvsOmq_EG7Mp0zpo17oPvISQHEfsGBzA2uS2sd9-6znfZn1Hsh5QgQI2XLrvLXvDKhBrvg7nuI56jk8asI1z81Cl6f7hfzp-yxevj8_x2kVkuZcqashTAVVUZWzBRV5SIiksONRGKclFKWVS8ZKqmoEAqMIqSqgAjxNhbaPgUXR18x-ifA8SkWz-EbjypWVGq0WAmy1FVHlQ2-BgDNLoPbmPCTlOi91h1q3-x6j1WfcA6Lt4cFmH8Yesg6GgddBZqF8AmXXv3n8UXmUiF8A</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2569688486</pqid></control><display><type>article</type><title>Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings</title><source>ScienceDirect Freedom Collection 2022-2024</source><creator>Hahn, R. ; Tymoszuk, A. ; Wojcik, T. ; Kirnbauer, A. ; Kozák, T. ; Čapek, J. ; Sauer, M. ; Foelske, A. ; Hunold, O. ; Polcik, P. ; Mayrhofer, P.H. ; Riedl, H.</creator><creatorcontrib>Hahn, R. ; Tymoszuk, A. ; Wojcik, T. ; Kirnbauer, A. ; Kozák, T. ; Čapek, J. ; Sauer, M. ; Foelske, A. ; Hunold, O. ; Polcik, P. ; Mayrhofer, P.H. ; Riedl, H.</creatorcontrib><description>In the field of hard protective coatings, nano-crystalline Ti-B-N films are of great importance due to the adjustable microstructure and mechanical properties through their B content. Here, we systematically study this influence of B on Ti-B-N during reactive as well as non-reactive DC magnetron sputtering. The different deposition routes allow for an additional, very effective key parameter to modify bond characteristics and microstructure. Plasma analysis by mass spectroscopy reveals that for comparable amounts of Ti+, Ti2+, Ar+, and Ar2+ ions, the count of N+ ions is about 2 orders of magnitude lower during non-reactive sputtering. But for the latter, the N+/N2+ ratio is close to 1, whereas during reactive sputtering this ratio is only 0.1. This may explain why during reactive deposition of Ti-B-N, the BN bonds dominate (as suggested by X-ray photoelectron spectroscopy), whereas the BB and TiB bonds dominate for non-reactively prepared Ti-B-N. Chemically, reactively versus non-reactively sputtered Ti-B-N coatings follow the TiN-BN versus TiN-TiB2 tie line, respectively. Detailed X-ray diffraction and transmission electron microscopy studies reveal, that up to 10 at.% B can be dissolved in the fcc-TiN lattice when prepared by non-reactive sputtering, whereas already for a B content of 4 at.% a BN-rich boundary phase forms when reactively sputtered. Thus, we could not only observe a higher hardness (35 GPa instead of 25 GPa) as well as a higher indentation modulus (480 GPa instead of 260 GPa), but also a higher fracture energy (0.016 instead of 0.009 J/m during cube-corner indentations) for Ti-B-N coatings with 10 at.% B, when prepared non-reactively. •Major differences in plasma species between reactive and non-reactive sputtering•The elemental composition also varies with the deposition route.•Significant differences in mechanical properties at higher boron contents</description><identifier>ISSN: 0257-8972</identifier><identifier>EISSN: 1879-3347</identifier><identifier>DOI: 10.1016/j.surfcoat.2021.127327</identifier><language>eng</language><publisher>Lausanne: Elsevier B.V</publisher><subject>Deposition ; Fracture toughness ; Indentation ; Magnetron sputtering ; Mechanical properties ; Microstructure ; Non-reactive magnetron sputtering ; Parameter modification ; Photoelectrons ; Physical vapor deposition ; Protective coatings ; Spectrum analysis ; Ti-B-N</subject><ispartof>Surface &amp; coatings technology, 2021-08, Vol.420, p.127327, Article 127327</ispartof><rights>2021 The Authors</rights><rights>Copyright Elsevier BV Aug 25, 2021</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3</citedby><cites>FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Hahn, R.</creatorcontrib><creatorcontrib>Tymoszuk, A.</creatorcontrib><creatorcontrib>Wojcik, T.</creatorcontrib><creatorcontrib>Kirnbauer, A.</creatorcontrib><creatorcontrib>Kozák, T.</creatorcontrib><creatorcontrib>Čapek, J.</creatorcontrib><creatorcontrib>Sauer, M.</creatorcontrib><creatorcontrib>Foelske, A.</creatorcontrib><creatorcontrib>Hunold, O.</creatorcontrib><creatorcontrib>Polcik, P.</creatorcontrib><creatorcontrib>Mayrhofer, P.H.</creatorcontrib><creatorcontrib>Riedl, H.</creatorcontrib><title>Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings</title><title>Surface &amp; coatings technology</title><description>In the field of hard protective coatings, nano-crystalline Ti-B-N films are of great importance due to the adjustable microstructure and mechanical properties through their B content. Here, we systematically study this influence of B on Ti-B-N during reactive as well as non-reactive DC magnetron sputtering. The different deposition routes allow for an additional, very effective key parameter to modify bond characteristics and microstructure. Plasma analysis by mass spectroscopy reveals that for comparable amounts of Ti+, Ti2+, Ar+, and Ar2+ ions, the count of N+ ions is about 2 orders of magnitude lower during non-reactive sputtering. But for the latter, the N+/N2+ ratio is close to 1, whereas during reactive sputtering this ratio is only 0.1. This may explain why during reactive deposition of Ti-B-N, the BN bonds dominate (as suggested by X-ray photoelectron spectroscopy), whereas the BB and TiB bonds dominate for non-reactively prepared Ti-B-N. Chemically, reactively versus non-reactively sputtered Ti-B-N coatings follow the TiN-BN versus TiN-TiB2 tie line, respectively. Detailed X-ray diffraction and transmission electron microscopy studies reveal, that up to 10 at.% B can be dissolved in the fcc-TiN lattice when prepared by non-reactive sputtering, whereas already for a B content of 4 at.% a BN-rich boundary phase forms when reactively sputtered. Thus, we could not only observe a higher hardness (35 GPa instead of 25 GPa) as well as a higher indentation modulus (480 GPa instead of 260 GPa), but also a higher fracture energy (0.016 instead of 0.009 J/m during cube-corner indentations) for Ti-B-N coatings with 10 at.% B, when prepared non-reactively. •Major differences in plasma species between reactive and non-reactive sputtering•The elemental composition also varies with the deposition route.•Significant differences in mechanical properties at higher boron contents</description><subject>Deposition</subject><subject>Fracture toughness</subject><subject>Indentation</subject><subject>Magnetron sputtering</subject><subject>Mechanical properties</subject><subject>Microstructure</subject><subject>Non-reactive magnetron sputtering</subject><subject>Parameter modification</subject><subject>Photoelectrons</subject><subject>Physical vapor deposition</subject><subject>Protective coatings</subject><subject>Spectrum analysis</subject><subject>Ti-B-N</subject><issn>0257-8972</issn><issn>1879-3347</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNqFkMtOwzAQRS0EEqXwC8gS6wQ_mtjeARUvqQIWZW05zoQ6auNgO5X696QUJHasRjO6c-fOQeiSkpwSWl63eRxCY71JOSOM5pQJzsQRmlApVMb5TByjCWGFyKQS7BSdxdgSQqhQswlybysTATc-bExyvsOmq_EG7Mp0zpo17oPvISQHEfsGBzA2uS2sd9-6znfZn1Hsh5QgQI2XLrvLXvDKhBrvg7nuI56jk8asI1z81Cl6f7hfzp-yxevj8_x2kVkuZcqashTAVVUZWzBRV5SIiksONRGKclFKWVS8ZKqmoEAqMIqSqgAjxNhbaPgUXR18x-ifA8SkWz-EbjypWVGq0WAmy1FVHlQ2-BgDNLoPbmPCTlOi91h1q3-x6j1WfcA6Lt4cFmH8Yesg6GgddBZqF8AmXXv3n8UXmUiF8A</recordid><startdate>20210825</startdate><enddate>20210825</enddate><creator>Hahn, R.</creator><creator>Tymoszuk, A.</creator><creator>Wojcik, T.</creator><creator>Kirnbauer, A.</creator><creator>Kozák, T.</creator><creator>Čapek, J.</creator><creator>Sauer, M.</creator><creator>Foelske, A.</creator><creator>Hunold, O.</creator><creator>Polcik, P.</creator><creator>Mayrhofer, P.H.</creator><creator>Riedl, H.</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>6I.</scope><scope>AAFTH</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20210825</creationdate><title>Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings</title><author>Hahn, R. ; Tymoszuk, A. ; Wojcik, T. ; Kirnbauer, A. ; Kozák, T. ; Čapek, J. ; Sauer, M. ; Foelske, A. ; Hunold, O. ; Polcik, P. ; Mayrhofer, P.H. ; Riedl, H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Deposition</topic><topic>Fracture toughness</topic><topic>Indentation</topic><topic>Magnetron sputtering</topic><topic>Mechanical properties</topic><topic>Microstructure</topic><topic>Non-reactive magnetron sputtering</topic><topic>Parameter modification</topic><topic>Photoelectrons</topic><topic>Physical vapor deposition</topic><topic>Protective coatings</topic><topic>Spectrum analysis</topic><topic>Ti-B-N</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hahn, R.</creatorcontrib><creatorcontrib>Tymoszuk, A.</creatorcontrib><creatorcontrib>Wojcik, T.</creatorcontrib><creatorcontrib>Kirnbauer, A.</creatorcontrib><creatorcontrib>Kozák, T.</creatorcontrib><creatorcontrib>Čapek, J.</creatorcontrib><creatorcontrib>Sauer, M.</creatorcontrib><creatorcontrib>Foelske, A.</creatorcontrib><creatorcontrib>Hunold, O.</creatorcontrib><creatorcontrib>Polcik, P.</creatorcontrib><creatorcontrib>Mayrhofer, P.H.</creatorcontrib><creatorcontrib>Riedl, H.</creatorcontrib><collection>ScienceDirect Open Access Titles</collection><collection>Elsevier:ScienceDirect:Open Access</collection><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Surface &amp; coatings technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hahn, R.</au><au>Tymoszuk, A.</au><au>Wojcik, T.</au><au>Kirnbauer, A.</au><au>Kozák, T.</au><au>Čapek, J.</au><au>Sauer, M.</au><au>Foelske, A.</au><au>Hunold, O.</au><au>Polcik, P.</au><au>Mayrhofer, P.H.</au><au>Riedl, H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings</atitle><jtitle>Surface &amp; coatings technology</jtitle><date>2021-08-25</date><risdate>2021</risdate><volume>420</volume><spage>127327</spage><pages>127327-</pages><artnum>127327</artnum><issn>0257-8972</issn><eissn>1879-3347</eissn><abstract>In the field of hard protective coatings, nano-crystalline Ti-B-N films are of great importance due to the adjustable microstructure and mechanical properties through their B content. Here, we systematically study this influence of B on Ti-B-N during reactive as well as non-reactive DC magnetron sputtering. The different deposition routes allow for an additional, very effective key parameter to modify bond characteristics and microstructure. Plasma analysis by mass spectroscopy reveals that for comparable amounts of Ti+, Ti2+, Ar+, and Ar2+ ions, the count of N+ ions is about 2 orders of magnitude lower during non-reactive sputtering. But for the latter, the N+/N2+ ratio is close to 1, whereas during reactive sputtering this ratio is only 0.1. This may explain why during reactive deposition of Ti-B-N, the BN bonds dominate (as suggested by X-ray photoelectron spectroscopy), whereas the BB and TiB bonds dominate for non-reactively prepared Ti-B-N. Chemically, reactively versus non-reactively sputtered Ti-B-N coatings follow the TiN-BN versus TiN-TiB2 tie line, respectively. Detailed X-ray diffraction and transmission electron microscopy studies reveal, that up to 10 at.% B can be dissolved in the fcc-TiN lattice when prepared by non-reactive sputtering, whereas already for a B content of 4 at.% a BN-rich boundary phase forms when reactively sputtered. Thus, we could not only observe a higher hardness (35 GPa instead of 25 GPa) as well as a higher indentation modulus (480 GPa instead of 260 GPa), but also a higher fracture energy (0.016 instead of 0.009 J/m during cube-corner indentations) for Ti-B-N coatings with 10 at.% B, when prepared non-reactively. •Major differences in plasma species between reactive and non-reactive sputtering•The elemental composition also varies with the deposition route.•Significant differences in mechanical properties at higher boron contents</abstract><cop>Lausanne</cop><pub>Elsevier B.V</pub><doi>10.1016/j.surfcoat.2021.127327</doi><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0257-8972
ispartof Surface & coatings technology, 2021-08, Vol.420, p.127327, Article 127327
issn 0257-8972
1879-3347
language eng
recordid cdi_proquest_journals_2569688486
source ScienceDirect Freedom Collection 2022-2024
subjects Deposition
Fracture toughness
Indentation
Magnetron sputtering
Mechanical properties
Microstructure
Non-reactive magnetron sputtering
Parameter modification
Photoelectrons
Physical vapor deposition
Protective coatings
Spectrum analysis
Ti-B-N
title Phase formation and mechanical properties of reactively and non-reactively sputtered Ti-B-N hard coatings
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-06T19%3A52%3A34IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Phase%20formation%20and%20mechanical%20properties%20of%20reactively%20and%20non-reactively%20sputtered%20Ti-B-N%20hard%20coatings&rft.jtitle=Surface%20&%20coatings%20technology&rft.au=Hahn,%20R.&rft.date=2021-08-25&rft.volume=420&rft.spage=127327&rft.pages=127327-&rft.artnum=127327&rft.issn=0257-8972&rft.eissn=1879-3347&rft_id=info:doi/10.1016/j.surfcoat.2021.127327&rft_dat=%3Cproquest_cross%3E2569688486%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c388t-f667e39bbac527db107b383ed0791376885b3629d1e9e89ea910b5ea77e9ecef3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2569688486&rft_id=info:pmid/&rfr_iscdi=true