Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution
Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obta...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Yang, Weimin [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2014 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media New York 2014 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of materials science / Materials in electronics - Springer US, 1990, 25(2014), 10 vom: 30. Juli, Seite 4517-4523 |
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| Übergeordnetes Werk: |
volume:25 ; year:2014 ; number:10 ; day:30 ; month:07 ; pages:4517-4523 |
| Links: |
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| DOI / URN: |
10.1007/s10854-014-2198-2 |
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| Katalog-ID: |
OLC2026279950 |
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| 245 | 1 | 0 | |a Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution |
| 264 | 1 | |c 2014 | |
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| 520 | |a Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. | ||
| 650 | 4 | |a Electron Paramagnetic Resonance | |
| 650 | 4 | |a Ferromagnetic Resonance | |
| 650 | 4 | |a Yttrium Iron Garnet | |
| 650 | 4 | |a Superexchange Interaction | |
| 650 | 4 | |a Yttrium Iron | |
| 700 | 1 | |a Wang, Lixi |4 aut | |
| 700 | 1 | |a Ding, Yujie |4 aut | |
| 700 | 1 | |a Zhang, Qitu |4 aut | |
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10.1007/s10854-014-2198-2 doi (DE-627)OLC2026279950 (DE-He213)s10854-014-2198-2-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Yang, Weimin verfasserin aut Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2014 Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron Wang, Lixi aut Ding, Yujie aut Zhang, Qitu aut Enthalten in Journal of materials science / Materials in electronics Springer US, 1990 25(2014), 10 vom: 30. Juli, Seite 4517-4523 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 https://doi.org/10.1007/s10854-014-2198-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_30 GBV_ILN_32 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 AR 25 2014 10 30 07 4517-4523 |
| spelling |
10.1007/s10854-014-2198-2 doi (DE-627)OLC2026279950 (DE-He213)s10854-014-2198-2-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Yang, Weimin verfasserin aut Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2014 Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron Wang, Lixi aut Ding, Yujie aut Zhang, Qitu aut Enthalten in Journal of materials science / Materials in electronics Springer US, 1990 25(2014), 10 vom: 30. Juli, Seite 4517-4523 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 https://doi.org/10.1007/s10854-014-2198-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_30 GBV_ILN_32 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 AR 25 2014 10 30 07 4517-4523 |
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10.1007/s10854-014-2198-2 doi (DE-627)OLC2026279950 (DE-He213)s10854-014-2198-2-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Yang, Weimin verfasserin aut Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2014 Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron Wang, Lixi aut Ding, Yujie aut Zhang, Qitu aut Enthalten in Journal of materials science / Materials in electronics Springer US, 1990 25(2014), 10 vom: 30. Juli, Seite 4517-4523 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 https://doi.org/10.1007/s10854-014-2198-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_30 GBV_ILN_32 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 AR 25 2014 10 30 07 4517-4523 |
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10.1007/s10854-014-2198-2 doi (DE-627)OLC2026279950 (DE-He213)s10854-014-2198-2-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Yang, Weimin verfasserin aut Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2014 Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron Wang, Lixi aut Ding, Yujie aut Zhang, Qitu aut Enthalten in Journal of materials science / Materials in electronics Springer US, 1990 25(2014), 10 vom: 30. Juli, Seite 4517-4523 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 https://doi.org/10.1007/s10854-014-2198-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_30 GBV_ILN_32 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 AR 25 2014 10 30 07 4517-4523 |
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10.1007/s10854-014-2198-2 doi (DE-627)OLC2026279950 (DE-He213)s10854-014-2198-2-p DE-627 ger DE-627 rakwb eng 600 670 620 VZ Yang, Weimin verfasserin aut Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution 2014 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2014 Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron Wang, Lixi aut Ding, Yujie aut Zhang, Qitu aut Enthalten in Journal of materials science / Materials in electronics Springer US, 1990 25(2014), 10 vom: 30. Juli, Seite 4517-4523 (DE-627)130863289 (DE-600)1030929-9 (DE-576)023106719 0957-4522 nnns volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 https://doi.org/10.1007/s10854-014-2198-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_30 GBV_ILN_32 GBV_ILN_70 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2015 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 AR 25 2014 10 30 07 4517-4523 |
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Enthalten in Journal of materials science / Materials in electronics 25(2014), 10 vom: 30. Juli, Seite 4517-4523 volume:25 year:2014 number:10 day:30 month:07 pages:4517-4523 |
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Yang, Weimin |
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Yang, Weimin ddc 600 misc Electron Paramagnetic Resonance misc Ferromagnetic Resonance misc Yttrium Iron Garnet misc Superexchange Interaction misc Yttrium Iron Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution |
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600 670 620 VZ Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution Electron Paramagnetic Resonance Ferromagnetic Resonance Yttrium Iron Garnet Superexchange Interaction Yttrium Iron |
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Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution |
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Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution |
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narrowing of ferromagnetic resonance linewidth in calcium substituted yig powders by $ zr^{4+} $/$ sn^{4+} $ substitution |
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Narrowing of ferromagnetic resonance linewidth in calcium substituted YIG powders by $ Zr^{4+} $/$ Sn^{4+} $ substitution |
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Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. © Springer Science+Business Media New York 2014 |
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Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. © Springer Science+Business Media New York 2014 |
| abstract_unstemmed |
Abstract $ Ca_{x+y} $$ Y_{3−x−y} $$ Sn_{x} $$ Zr_{y} $$ Fe_{5−x−y} $$ O_{12} $ powders were synthesized by a citric acid combustion method. The phase, microstructure and ferromagnetic resonance linewidth (ΔH) of the powders were analyzed. Pure garnet phase $ Y_{3} $$ Fe_{5} $$ O_{12} $ could be obtained at 1,200 °C, except for $ YFeO_{3} $ phase appearing in the sample with x = 0.5, y = 0.2. The addition of $ Zr^{4+} $ ion and $ Sn^{4+} $ ion could lower ΔH by replacing $ Fe^{3+} $ ion, which could change the a–d superexchange interaction in YIG lattice. Moreover, $ Zr^{4+} $ ion could promote this replacement by enlarging the lattice. However, too much addition of $ Zr^{4+} $ ion would bring the second phase $ YFeO_{3} $. The sample of $ Ca_{0.76} $$ Y_{2.24} $$ Sn_{0.7} $$ Zr_{0.06} $$ Fe_{4.34} $$ O_{12} $ shows excellent properties which are Ms = 6.4 emu/g, Hc = 10.9 Oe, ΔH = 113 Gs. © Springer Science+Business Media New York 2014 |
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