Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials

We used the nuclear magnetic resonance technique to study the evolution of the structural and magnetic properties of Fe-based melt-spun ribbons of Fe73.5Cu1Nb3Si13.5B9, Fe73.5Cu1Nb3Si18.5B4, and Fe86Zr7Cu1B6, as-cast and annealed at 500, 540, and 430 °C, respectively. Experiments were carried out at...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Journal of applied physics 2002-05, Vol.91 (10), p.8432-8434
Hauptverfasser: Barbatti, C. F., Sinnecker, E. H. C. P., Sarthour, R. S., Guimarães, A. P.
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 8434
container_issue 10
container_start_page 8432
container_title Journal of applied physics
container_volume 91
creator Barbatti, C. F.
Sinnecker, E. H. C. P.
Sarthour, R. S.
Guimarães, A. P.
description We used the nuclear magnetic resonance technique to study the evolution of the structural and magnetic properties of Fe-based melt-spun ribbons of Fe73.5Cu1Nb3Si13.5B9, Fe73.5Cu1Nb3Si18.5B4, and Fe86Zr7Cu1B6, as-cast and annealed at 500, 540, and 430 °C, respectively. Experiments were carried out at 4.2 K and zero-applied magnetic field, and in a controlled radio-frequency (rf) field. This type of measurement allows us to observe B and Nb sites, and makes it possible to distinguish signals associated with regions of different magnetic hardnesses. The results exhibit a high dependence of the spectra on rf power. For Fe–Si-based alloys, we observe well-defined Nb93 resonance signals from three distinct sites according to the concentration of Fe atoms in their neighborhood. In the Fe73.5Cu1Nb3Si18.5B4 spectra we also observe a peak around 34 MHz, connected to the B11 resonance in different Fe–B compounds, which remains as the rf power decreases, suggesting that the signals come from atoms inside a soft magnetic region. As for the Fe–Zr alloy, we also observe a peak around 36 MHz, identified as the B11 resonance, and a broad line around 62 MHz.
doi_str_mv 10.1063/1.1456388
format Article
fullrecord <record><control><sourceid>crossref</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_1456388</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1063_1_1456388</sourcerecordid><originalsourceid>FETCH-LOGICAL-c227t-4ee6f274eb060e0153ddd2c612e5cd345c362647ae64da976f508c85ca3d434f3</originalsourceid><addsrcrecordid>eNpFkLtOxDAURC0EEmGh4A_cUmS5fsYp0YqXtIIG6sjY12A2myDbW4SvJ8AKqinmzCmGkHMGSwZaXLIlk0oLYw5IxcC0daMUHJIKgLPatE17TE5yfgdgzIi2IpuHnevRJrq1rwOW6GjCPA52cEhz2fmJjoGWN6QuTbnYvo-ftsRxoJv4g2caB5rHUP4F83j8oweci4Ip2j6fkqMwB57tc0Geb66fVnf1-vH2fnW1rh3nTaklog68kfgCGhCYEt577jTjqJwXUjmhuZaNRS29bRsdFBhnlLPCSyGDWJCLX69LY84JQ_eR4tamqWPQfb_UsW7_kvgCkWxceA</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials</title><source>AIP Journals Complete</source><source>AIP Digital Archive</source><creator>Barbatti, C. F. ; Sinnecker, E. H. C. P. ; Sarthour, R. S. ; Guimarães, A. P.</creator><creatorcontrib>Barbatti, C. F. ; Sinnecker, E. H. C. P. ; Sarthour, R. S. ; Guimarães, A. P.</creatorcontrib><description>We used the nuclear magnetic resonance technique to study the evolution of the structural and magnetic properties of Fe-based melt-spun ribbons of Fe73.5Cu1Nb3Si13.5B9, Fe73.5Cu1Nb3Si18.5B4, and Fe86Zr7Cu1B6, as-cast and annealed at 500, 540, and 430 °C, respectively. Experiments were carried out at 4.2 K and zero-applied magnetic field, and in a controlled radio-frequency (rf) field. This type of measurement allows us to observe B and Nb sites, and makes it possible to distinguish signals associated with regions of different magnetic hardnesses. The results exhibit a high dependence of the spectra on rf power. For Fe–Si-based alloys, we observe well-defined Nb93 resonance signals from three distinct sites according to the concentration of Fe atoms in their neighborhood. In the Fe73.5Cu1Nb3Si18.5B4 spectra we also observe a peak around 34 MHz, connected to the B11 resonance in different Fe–B compounds, which remains as the rf power decreases, suggesting that the signals come from atoms inside a soft magnetic region. As for the Fe–Zr alloy, we also observe a peak around 36 MHz, identified as the B11 resonance, and a broad line around 62 MHz.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.1456388</identifier><language>eng</language><ispartof>Journal of applied physics, 2002-05, Vol.91 (10), p.8432-8434</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c227t-4ee6f274eb060e0153ddd2c612e5cd345c362647ae64da976f508c85ca3d434f3</citedby><cites>FETCH-LOGICAL-c227t-4ee6f274eb060e0153ddd2c612e5cd345c362647ae64da976f508c85ca3d434f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Barbatti, C. F.</creatorcontrib><creatorcontrib>Sinnecker, E. H. C. P.</creatorcontrib><creatorcontrib>Sarthour, R. S.</creatorcontrib><creatorcontrib>Guimarães, A. P.</creatorcontrib><title>Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials</title><title>Journal of applied physics</title><description>We used the nuclear magnetic resonance technique to study the evolution of the structural and magnetic properties of Fe-based melt-spun ribbons of Fe73.5Cu1Nb3Si13.5B9, Fe73.5Cu1Nb3Si18.5B4, and Fe86Zr7Cu1B6, as-cast and annealed at 500, 540, and 430 °C, respectively. Experiments were carried out at 4.2 K and zero-applied magnetic field, and in a controlled radio-frequency (rf) field. This type of measurement allows us to observe B and Nb sites, and makes it possible to distinguish signals associated with regions of different magnetic hardnesses. The results exhibit a high dependence of the spectra on rf power. For Fe–Si-based alloys, we observe well-defined Nb93 resonance signals from three distinct sites according to the concentration of Fe atoms in their neighborhood. In the Fe73.5Cu1Nb3Si18.5B4 spectra we also observe a peak around 34 MHz, connected to the B11 resonance in different Fe–B compounds, which remains as the rf power decreases, suggesting that the signals come from atoms inside a soft magnetic region. As for the Fe–Zr alloy, we also observe a peak around 36 MHz, identified as the B11 resonance, and a broad line around 62 MHz.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><recordid>eNpFkLtOxDAURC0EEmGh4A_cUmS5fsYp0YqXtIIG6sjY12A2myDbW4SvJ8AKqinmzCmGkHMGSwZaXLIlk0oLYw5IxcC0daMUHJIKgLPatE17TE5yfgdgzIi2IpuHnevRJrq1rwOW6GjCPA52cEhz2fmJjoGWN6QuTbnYvo-ftsRxoJv4g2caB5rHUP4F83j8oweci4Ip2j6fkqMwB57tc0Geb66fVnf1-vH2fnW1rh3nTaklog68kfgCGhCYEt577jTjqJwXUjmhuZaNRS29bRsdFBhnlLPCSyGDWJCLX69LY84JQ_eR4tamqWPQfb_UsW7_kvgCkWxceA</recordid><startdate>20020515</startdate><enddate>20020515</enddate><creator>Barbatti, C. F.</creator><creator>Sinnecker, E. H. C. P.</creator><creator>Sarthour, R. S.</creator><creator>Guimarães, A. P.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20020515</creationdate><title>Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials</title><author>Barbatti, C. F. ; Sinnecker, E. H. C. P. ; Sarthour, R. S. ; Guimarães, A. P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c227t-4ee6f274eb060e0153ddd2c612e5cd345c362647ae64da976f508c85ca3d434f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2002</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Barbatti, C. F.</creatorcontrib><creatorcontrib>Sinnecker, E. H. C. P.</creatorcontrib><creatorcontrib>Sarthour, R. S.</creatorcontrib><creatorcontrib>Guimarães, A. P.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Barbatti, C. F.</au><au>Sinnecker, E. H. C. P.</au><au>Sarthour, R. S.</au><au>Guimarães, A. P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials</atitle><jtitle>Journal of applied physics</jtitle><date>2002-05-15</date><risdate>2002</risdate><volume>91</volume><issue>10</issue><spage>8432</spage><epage>8434</epage><pages>8432-8434</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>We used the nuclear magnetic resonance technique to study the evolution of the structural and magnetic properties of Fe-based melt-spun ribbons of Fe73.5Cu1Nb3Si13.5B9, Fe73.5Cu1Nb3Si18.5B4, and Fe86Zr7Cu1B6, as-cast and annealed at 500, 540, and 430 °C, respectively. Experiments were carried out at 4.2 K and zero-applied magnetic field, and in a controlled radio-frequency (rf) field. This type of measurement allows us to observe B and Nb sites, and makes it possible to distinguish signals associated with regions of different magnetic hardnesses. The results exhibit a high dependence of the spectra on rf power. For Fe–Si-based alloys, we observe well-defined Nb93 resonance signals from three distinct sites according to the concentration of Fe atoms in their neighborhood. In the Fe73.5Cu1Nb3Si18.5B4 spectra we also observe a peak around 34 MHz, connected to the B11 resonance in different Fe–B compounds, which remains as the rf power decreases, suggesting that the signals come from atoms inside a soft magnetic region. As for the Fe–Zr alloy, we also observe a peak around 36 MHz, identified as the B11 resonance, and a broad line around 62 MHz.</abstract><doi>10.1063/1.1456388</doi><tpages>3</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0021-8979
ispartof Journal of applied physics, 2002-05, Vol.91 (10), p.8432-8434
issn 0021-8979
1089-7550
language eng
recordid cdi_crossref_primary_10_1063_1_1456388
source AIP Journals Complete; AIP Digital Archive
title Nuclear magnetic resonance study of the crystallization kinetics in soft magnetic nanocrystalline materials
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-11T23%3A12%3A38IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Nuclear%20magnetic%20resonance%20study%20of%20the%20crystallization%20kinetics%20in%20soft%20magnetic%20nanocrystalline%20materials&rft.jtitle=Journal%20of%20applied%20physics&rft.au=Barbatti,%20C.%20F.&rft.date=2002-05-15&rft.volume=91&rft.issue=10&rft.spage=8432&rft.epage=8434&rft.pages=8432-8434&rft.issn=0021-8979&rft.eissn=1089-7550&rft_id=info:doi/10.1063/1.1456388&rft_dat=%3Ccrossref%3E10_1063_1_1456388%3C/crossref%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true