Calculation of hysteresis loops in face-centered cubic thin films
A total energy equation for a single-crystalline face-centered cubic thin film with its close-packed (111) plane parallel to the film plane is used to calculate in-plane and out-of-plane hysteresis loops at various values of the cubic magnetocrystalline anisotropy constant ( K 1). In-plane loops sho...
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description | A total energy equation for a single-crystalline face-centered cubic thin film with its close-packed (111) plane parallel to the film plane is used to calculate in-plane and out-of-plane hysteresis loops at various values of the cubic magnetocrystalline anisotropy constant (
K
1). In-plane loops show that the easy and hard axes are the and directions, respectively, and that the coercivities, which are nearly independent of the sign of
K
1, are quite low over the
K
1 values due to the small variation of the magnetocrystalline anisotropy energy during the field sweep. The out-of-plane loops are similarly shaped to those of typical thin films, except for the appearance of a small hysteresis loop near the origin, which is attributed to an irreversible magnetization jump from one easy axis to another in the (111) plane. The magnetic parameters such as
K
1 are estimated by comparing the theoretical results for in-plane and out-of-plane hysteresis loops with the experimental results measured for an epitaxial Co thin film. The value of
K
1 is estimated to be −
1.2
×
10
6
erg/cm
3, which is significantly higher than that of −
6×10
5
erg/cm
3 for bulk Co, but is in good agreement with the values of −
1.3 to −
1.6
×
10
6
erg/cm
3 reported for Co thin films. |
doi_str_mv | 10.1016/j.tsf.2011.03.106 |
format | Article |
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K
1). In-plane loops show that the easy and hard axes are the and directions, respectively, and that the coercivities, which are nearly independent of the sign of
K
1, are quite low over the
K
1 values due to the small variation of the magnetocrystalline anisotropy energy during the field sweep. The out-of-plane loops are similarly shaped to those of typical thin films, except for the appearance of a small hysteresis loop near the origin, which is attributed to an irreversible magnetization jump from one easy axis to another in the (111) plane. The magnetic parameters such as
K
1 are estimated by comparing the theoretical results for in-plane and out-of-plane hysteresis loops with the experimental results measured for an epitaxial Co thin film. The value of
K
1 is estimated to be −
1.2
×
10
6
erg/cm
3, which is significantly higher than that of −
6×10
5
erg/cm
3 for bulk Co, but is in good agreement with the values of −
1.3 to −
1.6
×
10
6
erg/cm
3 reported for Co thin films.</description><identifier>ISSN: 0040-6090</identifier><identifier>EISSN: 1879-2731</identifier><identifier>DOI: 10.1016/j.tsf.2011.03.106</identifier><identifier>CODEN: THSFAP</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>Analytical calculation ; Anisotropy ; Close-packed plane ; Coercive force ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Energy use ; Exact sciences and technology ; Face-centered cubic thin films ; Hysteresis loops ; Magnetic properties and materials ; Magnetic properties of monolayers and thin films ; Magnetic properties of surface, thin films and multilayers ; Magnetocrystalline anisotropy ; Mathematical analysis ; Physics ; Planes ; Single crystals ; Thin films</subject><ispartof>Thin solid films, 2011-09, Vol.519 (23), p.8256-8259</ispartof><rights>2011 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c359t-e40afce9267163f5793a0b2b3220f75fe3b91b92e7e419fb3901c828eaf8f13f3</citedby><cites>FETCH-LOGICAL-c359t-e40afce9267163f5793a0b2b3220f75fe3b91b92e7e419fb3901c828eaf8f13f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.tsf.2011.03.106$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>309,310,314,780,784,789,790,3549,23929,23930,25139,27923,27924,45994</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=24607314$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Nam, Yoon Jae</creatorcontrib><creatorcontrib>Lim, S.H.</creatorcontrib><title>Calculation of hysteresis loops in face-centered cubic thin films</title><title>Thin solid films</title><description>A total energy equation for a single-crystalline face-centered cubic thin film with its close-packed (111) plane parallel to the film plane is used to calculate in-plane and out-of-plane hysteresis loops at various values of the cubic magnetocrystalline anisotropy constant (
K
1). In-plane loops show that the easy and hard axes are the and directions, respectively, and that the coercivities, which are nearly independent of the sign of
K
1, are quite low over the
K
1 values due to the small variation of the magnetocrystalline anisotropy energy during the field sweep. The out-of-plane loops are similarly shaped to those of typical thin films, except for the appearance of a small hysteresis loop near the origin, which is attributed to an irreversible magnetization jump from one easy axis to another in the (111) plane. The magnetic parameters such as
K
1 are estimated by comparing the theoretical results for in-plane and out-of-plane hysteresis loops with the experimental results measured for an epitaxial Co thin film. The value of
K
1 is estimated to be −
1.2
×
10
6
erg/cm
3, which is significantly higher than that of −
6×10
5
erg/cm
3 for bulk Co, but is in good agreement with the values of −
1.3 to −
1.6
×
10
6
erg/cm
3 reported for Co thin films.</description><subject>Analytical calculation</subject><subject>Anisotropy</subject><subject>Close-packed plane</subject><subject>Coercive force</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Energy use</subject><subject>Exact sciences and technology</subject><subject>Face-centered cubic thin films</subject><subject>Hysteresis loops</subject><subject>Magnetic properties and materials</subject><subject>Magnetic properties of monolayers and thin films</subject><subject>Magnetic properties of surface, thin films and multilayers</subject><subject>Magnetocrystalline anisotropy</subject><subject>Mathematical analysis</subject><subject>Physics</subject><subject>Planes</subject><subject>Single crystals</subject><subject>Thin films</subject><issn>0040-6090</issn><issn>1879-2731</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp9kE9LxDAQxYMouK5-AG-9iKfWSdJNGzwti_9gwYueQ5qdsFm67ZppBb-9Kbt49DTw5r03zI-xWw4FB64edsVAvhDAeQEySeqMzXhd6VxUkp-zGUAJuQINl-yKaAcAXAg5Y8uVbd3Y2iH0Xdb7bPtDA0akQFnb9wfKQpd56zB32E2LTebGJrhs2E6L0O7pml142xLenOacfT4_faxe8_X7y9tquc6dXOghxxKsd6iFqriSflFpaaERjRQCfLXwKBvNGy2wwpJr30gN3NWiRutrz6WXc3Z_7D3E_mtEGsw-kMO2tR32I5nULHRZKUhOfnS62BNF9OYQw97GH8PBTLTMziRaZqJlQCZJpczdqd2Ss62PtnOB_oKiVJBAlsn3ePRhevU7YDTkAnYONyGiG8ymD_9c-QUm9X7o</recordid><startdate>20110930</startdate><enddate>20110930</enddate><creator>Nam, Yoon Jae</creator><creator>Lim, S.H.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20110930</creationdate><title>Calculation of hysteresis loops in face-centered cubic thin films</title><author>Nam, Yoon Jae ; Lim, S.H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c359t-e40afce9267163f5793a0b2b3220f75fe3b91b92e7e419fb3901c828eaf8f13f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Analytical calculation</topic><topic>Anisotropy</topic><topic>Close-packed plane</topic><topic>Coercive force</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Energy use</topic><topic>Exact sciences and technology</topic><topic>Face-centered cubic thin films</topic><topic>Hysteresis loops</topic><topic>Magnetic properties and materials</topic><topic>Magnetic properties of monolayers and thin films</topic><topic>Magnetic properties of surface, thin films and multilayers</topic><topic>Magnetocrystalline anisotropy</topic><topic>Mathematical analysis</topic><topic>Physics</topic><topic>Planes</topic><topic>Single crystals</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nam, Yoon Jae</creatorcontrib><creatorcontrib>Lim, S.H.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Thin solid films</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nam, Yoon Jae</au><au>Lim, S.H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Calculation of hysteresis loops in face-centered cubic thin films</atitle><jtitle>Thin solid films</jtitle><date>2011-09-30</date><risdate>2011</risdate><volume>519</volume><issue>23</issue><spage>8256</spage><epage>8259</epage><pages>8256-8259</pages><issn>0040-6090</issn><eissn>1879-2731</eissn><coden>THSFAP</coden><abstract>A total energy equation for a single-crystalline face-centered cubic thin film with its close-packed (111) plane parallel to the film plane is used to calculate in-plane and out-of-plane hysteresis loops at various values of the cubic magnetocrystalline anisotropy constant (
K
1). In-plane loops show that the easy and hard axes are the and directions, respectively, and that the coercivities, which are nearly independent of the sign of
K
1, are quite low over the
K
1 values due to the small variation of the magnetocrystalline anisotropy energy during the field sweep. The out-of-plane loops are similarly shaped to those of typical thin films, except for the appearance of a small hysteresis loop near the origin, which is attributed to an irreversible magnetization jump from one easy axis to another in the (111) plane. The magnetic parameters such as
K
1 are estimated by comparing the theoretical results for in-plane and out-of-plane hysteresis loops with the experimental results measured for an epitaxial Co thin film. The value of
K
1 is estimated to be −
1.2
×
10
6
erg/cm
3, which is significantly higher than that of −
6×10
5
erg/cm
3 for bulk Co, but is in good agreement with the values of −
1.3 to −
1.6
×
10
6
erg/cm
3 reported for Co thin films.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.tsf.2011.03.106</doi><tpages>4</tpages></addata></record> |
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source | ScienceDirect Journals (5 years ago - present) |
subjects | Analytical calculation Anisotropy Close-packed plane Coercive force Condensed matter: electronic structure, electrical, magnetic, and optical properties Energy use Exact sciences and technology Face-centered cubic thin films Hysteresis loops Magnetic properties and materials Magnetic properties of monolayers and thin films Magnetic properties of surface, thin films and multilayers Magnetocrystalline anisotropy Mathematical analysis Physics Planes Single crystals Thin films |
title | Calculation of hysteresis loops in face-centered cubic thin films |
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