Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $
Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a te...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zinovik, E. V. [verfasserIn] |
|---|
| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2005 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media, Inc. 2005 |
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| Übergeordnetes Werk: |
Enthalten in: Powder metallurgy and metal ceramics - Kluwer Academic Publishers-Consultants Bureau, 1993, 44(2005), 9-10 vom: Sept., Seite 481-488 |
|---|---|
| Übergeordnetes Werk: |
volume:44 ; year:2005 ; number:9-10 ; month:09 ; pages:481-488 |
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| DOI / URN: |
10.1007/s11106-006-0013-1 |
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OLC2061148573 |
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| 520 | |a Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. | ||
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10.1007/s11106-006-0013-1 doi (DE-627)OLC2061148573 (DE-He213)s11106-006-0013-1-p DE-627 ger DE-627 rakwb eng 670 VZ Zinovik, E. V. verfasserin aut Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $ 2005 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2005 Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. solid solution tetragonal phase cubic phase free energy Curie point magnetic moment lattice parameter Zinovik, M. A. aut Enthalten in Powder metallurgy and metal ceramics Kluwer Academic Publishers-Consultants Bureau, 1993 44(2005), 9-10 vom: Sept., Seite 481-488 (DE-627)171221524 (DE-600)1167195-6 (DE-576)038719614 1068-1302 nnns volume:44 year:2005 number:9-10 month:09 pages:481-488 https://doi.org/10.1007/s11106-006-0013-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_32 GBV_ILN_70 GBV_ILN_2014 AR 44 2005 9-10 09 481-488 |
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10.1007/s11106-006-0013-1 doi (DE-627)OLC2061148573 (DE-He213)s11106-006-0013-1-p DE-627 ger DE-627 rakwb eng 670 VZ Zinovik, E. V. verfasserin aut Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $ 2005 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2005 Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. solid solution tetragonal phase cubic phase free energy Curie point magnetic moment lattice parameter Zinovik, M. A. aut Enthalten in Powder metallurgy and metal ceramics Kluwer Academic Publishers-Consultants Bureau, 1993 44(2005), 9-10 vom: Sept., Seite 481-488 (DE-627)171221524 (DE-600)1167195-6 (DE-576)038719614 1068-1302 nnns volume:44 year:2005 number:9-10 month:09 pages:481-488 https://doi.org/10.1007/s11106-006-0013-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_32 GBV_ILN_70 GBV_ILN_2014 AR 44 2005 9-10 09 481-488 |
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10.1007/s11106-006-0013-1 doi (DE-627)OLC2061148573 (DE-He213)s11106-006-0013-1-p DE-627 ger DE-627 rakwb eng 670 VZ Zinovik, E. V. verfasserin aut Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $ 2005 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2005 Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. solid solution tetragonal phase cubic phase free energy Curie point magnetic moment lattice parameter Zinovik, M. A. aut Enthalten in Powder metallurgy and metal ceramics Kluwer Academic Publishers-Consultants Bureau, 1993 44(2005), 9-10 vom: Sept., Seite 481-488 (DE-627)171221524 (DE-600)1167195-6 (DE-576)038719614 1068-1302 nnns volume:44 year:2005 number:9-10 month:09 pages:481-488 https://doi.org/10.1007/s11106-006-0013-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_32 GBV_ILN_70 GBV_ILN_2014 AR 44 2005 9-10 09 481-488 |
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10.1007/s11106-006-0013-1 doi (DE-627)OLC2061148573 (DE-He213)s11106-006-0013-1-p DE-627 ger DE-627 rakwb eng 670 VZ Zinovik, E. V. verfasserin aut Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $ 2005 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2005 Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. solid solution tetragonal phase cubic phase free energy Curie point magnetic moment lattice parameter Zinovik, M. A. aut Enthalten in Powder metallurgy and metal ceramics Kluwer Academic Publishers-Consultants Bureau, 1993 44(2005), 9-10 vom: Sept., Seite 481-488 (DE-627)171221524 (DE-600)1167195-6 (DE-576)038719614 1068-1302 nnns volume:44 year:2005 number:9-10 month:09 pages:481-488 https://doi.org/10.1007/s11106-006-0013-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_32 GBV_ILN_70 GBV_ILN_2014 AR 44 2005 9-10 09 481-488 |
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10.1007/s11106-006-0013-1 doi (DE-627)OLC2061148573 (DE-He213)s11106-006-0013-1-p DE-627 ger DE-627 rakwb eng 670 VZ Zinovik, E. V. verfasserin aut Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $ 2005 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, Inc. 2005 Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. solid solution tetragonal phase cubic phase free energy Curie point magnetic moment lattice parameter Zinovik, M. A. aut Enthalten in Powder metallurgy and metal ceramics Kluwer Academic Publishers-Consultants Bureau, 1993 44(2005), 9-10 vom: Sept., Seite 481-488 (DE-627)171221524 (DE-600)1167195-6 (DE-576)038719614 1068-1302 nnns volume:44 year:2005 number:9-10 month:09 pages:481-488 https://doi.org/10.1007/s11106-006-0013-1 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_32 GBV_ILN_70 GBV_ILN_2014 AR 44 2005 9-10 09 481-488 |
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Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. © Springer Science+Business Media, Inc. 2005 |
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Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. © Springer Science+Business Media, Inc. 2005 |
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Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me. © Springer Science+Business Media, Inc. 2005 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2061148573</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504011019.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2005 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11106-006-0013-1</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2061148573</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s11106-006-0013-1-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">670</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Zinovik, E. V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Structure and Properties of Ferrites Based on $ CuFe_{2} $$ O_{4} $</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2005</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Springer Science+Business Media, Inc. 2005</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We have studied the magnetic and structural properties of the solid solutions Mx2+Cu1−x2+Fe23+$ O_{4} $, where M = Mg, Ni, Co, Zn, Mn, Me0.5x+Cu1−x2+Fe2+0.5x3+$ O_{4} $, were Me = Li, Cu, and ($ Mn_{3} $$ O_{4} $)x($ CuFe_{2} $$ O_{4} $)1−x. We have developed a new method for detecting a tetragonal phase and have used this method to determine the range of existence for solutions with a tetragonal structure. We explain the dependence of these ranges on the nature of M and Me.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">solid solution</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">tetragonal phase</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">cubic phase</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">free energy</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Curie point</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">magnetic moment</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">lattice parameter</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zinovik, M. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Powder metallurgy and metal ceramics</subfield><subfield code="d">Kluwer Academic Publishers-Consultants Bureau, 1993</subfield><subfield code="g">44(2005), 9-10 vom: Sept., Seite 481-488</subfield><subfield code="w">(DE-627)171221524</subfield><subfield code="w">(DE-600)1167195-6</subfield><subfield code="w">(DE-576)038719614</subfield><subfield code="x">1068-1302</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:44</subfield><subfield code="g">year:2005</subfield><subfield code="g">number:9-10</subfield><subfield code="g">month:09</subfield><subfield code="g">pages:481-488</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s11106-006-0013-1</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">44</subfield><subfield code="j">2005</subfield><subfield code="e">9-10</subfield><subfield code="c">09</subfield><subfield code="h">481-488</subfield></datafield></record></collection>
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