Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics
Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe...
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| Autor*in: |
Hou, Ruiting [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2023 |
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© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: Journal of sol gel science and technology - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993, 107(2023), 2 vom: 15. Mai, Seite 474-482 |
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| Übergeordnetes Werk: |
volume:107 ; year:2023 ; number:2 ; day:15 ; month:05 ; pages:474-482 |
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| DOI / URN: |
10.1007/s10971-023-06134-6 |
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SPR052238792 |
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| 245 | 1 | 0 | |a Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
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| 520 | |a Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract | ||
| 650 | 4 | |a La |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Ca |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Sr |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Mn |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Fe |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a O |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a : Ag |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a A-site |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Temperature coefficient of resistivity |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Magnetoresistance |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Wang, Haishan |4 aut | |
| 700 | 1 | |a Zhu, Xiangxiang |4 aut | |
| 700 | 1 | |a Chen, Qingming |4 aut | |
| 700 | 1 | |a Zhang, Hui |4 aut | |
| 700 | 1 | |a Li, Yule |0 (orcid)0000-0002-1978-5544 |4 aut | |
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10.1007/s10971-023-06134-6 doi (DE-627)SPR052238792 (SPR)s10971-023-06134-6-e DE-627 ger DE-627 rakwb eng Hou, Ruiting verfasserin aut Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 Wang, Haishan aut Zhu, Xiangxiang aut Chen, Qingming aut Zhang, Hui aut Li, Yule (orcid)0000-0002-1978-5544 aut Enthalten in Journal of sol gel science and technology Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993 107(2023), 2 vom: 15. Mai, Seite 474-482 (DE-627)268757607 (DE-600)1472726-2 1573-4846 nnns volume:107 year:2023 number:2 day:15 month:05 pages:474-482 https://dx.doi.org/10.1007/s10971-023-06134-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 107 2023 2 15 05 474-482 |
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10.1007/s10971-023-06134-6 doi (DE-627)SPR052238792 (SPR)s10971-023-06134-6-e DE-627 ger DE-627 rakwb eng Hou, Ruiting verfasserin aut Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 Wang, Haishan aut Zhu, Xiangxiang aut Chen, Qingming aut Zhang, Hui aut Li, Yule (orcid)0000-0002-1978-5544 aut Enthalten in Journal of sol gel science and technology Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993 107(2023), 2 vom: 15. Mai, Seite 474-482 (DE-627)268757607 (DE-600)1472726-2 1573-4846 nnns volume:107 year:2023 number:2 day:15 month:05 pages:474-482 https://dx.doi.org/10.1007/s10971-023-06134-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 107 2023 2 15 05 474-482 |
| allfields_unstemmed |
10.1007/s10971-023-06134-6 doi (DE-627)SPR052238792 (SPR)s10971-023-06134-6-e DE-627 ger DE-627 rakwb eng Hou, Ruiting verfasserin aut Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 Wang, Haishan aut Zhu, Xiangxiang aut Chen, Qingming aut Zhang, Hui aut Li, Yule (orcid)0000-0002-1978-5544 aut Enthalten in Journal of sol gel science and technology Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993 107(2023), 2 vom: 15. Mai, Seite 474-482 (DE-627)268757607 (DE-600)1472726-2 1573-4846 nnns volume:107 year:2023 number:2 day:15 month:05 pages:474-482 https://dx.doi.org/10.1007/s10971-023-06134-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 107 2023 2 15 05 474-482 |
| allfieldsGer |
10.1007/s10971-023-06134-6 doi (DE-627)SPR052238792 (SPR)s10971-023-06134-6-e DE-627 ger DE-627 rakwb eng Hou, Ruiting verfasserin aut Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 Wang, Haishan aut Zhu, Xiangxiang aut Chen, Qingming aut Zhang, Hui aut Li, Yule (orcid)0000-0002-1978-5544 aut Enthalten in Journal of sol gel science and technology Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993 107(2023), 2 vom: 15. Mai, Seite 474-482 (DE-627)268757607 (DE-600)1472726-2 1573-4846 nnns volume:107 year:2023 number:2 day:15 month:05 pages:474-482 https://dx.doi.org/10.1007/s10971-023-06134-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 107 2023 2 15 05 474-482 |
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10.1007/s10971-023-06134-6 doi (DE-627)SPR052238792 (SPR)s10971-023-06134-6-e DE-627 ger DE-627 rakwb eng Hou, Ruiting verfasserin aut Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 Wang, Haishan aut Zhu, Xiangxiang aut Chen, Qingming aut Zhang, Hui aut Li, Yule (orcid)0000-0002-1978-5544 aut Enthalten in Journal of sol gel science and technology Dordrecht [u.a.] : Springer Science + Business Media B.V, 1993 107(2023), 2 vom: 15. Mai, Seite 474-482 (DE-627)268757607 (DE-600)1472726-2 1573-4846 nnns volume:107 year:2023 number:2 day:15 month:05 pages:474-482 https://dx.doi.org/10.1007/s10971-023-06134-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 107 2023 2 15 05 474-482 |
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Hou, Ruiting @@aut@@ Wang, Haishan @@aut@@ Zhu, Xiangxiang @@aut@@ Chen, Qingming @@aut@@ Zhang, Hui @@aut@@ Li, Yule @@aut@@ |
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Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. 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Hou, Ruiting |
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Hou, Ruiting misc La misc Ca misc Sr misc Mn misc Fe misc O misc : Ag misc A-site misc Temperature coefficient of resistivity misc Magnetoresistance Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
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Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics La (dpeaa)DE-He213 Ca (dpeaa)DE-He213 Sr (dpeaa)DE-He213 Mn (dpeaa)DE-He213 Fe (dpeaa)DE-He213 O (dpeaa)DE-He213 : Ag (dpeaa)DE-He213 A-site (dpeaa)DE-He213 Temperature coefficient of resistivity (dpeaa)DE-He213 Magnetoresistance (dpeaa)DE-He213 |
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Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
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Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
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Hou, Ruiting Wang, Haishan Zhu, Xiangxiang Chen, Qingming Zhang, Hui Li, Yule |
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studying near room-temperature magnetoresistance of a-site sr-doped into $ la_{0.67} %$ ca_{0.33} %$ mn_{0.98} %$ fe_{0.02} %$ o_{3} $: $ ag_{0.15} $ ceramics |
| title_auth |
Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
| abstract |
Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. Graphical Abstract © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">SPR052238792</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230714064802.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230714s2023 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10971-023-06134-6</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR052238792</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10971-023-06134-6-e</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="100" ind1="1" ind2=" "><subfield code="a">Hou, Ruiting</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Studying near room-temperature magnetoresistance of A-site Sr-doped into $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ ceramics</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2023</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Perovskite $ La_{1-x} %$ Ca_{x} %$ MnO_{3} $ (LCMO) has attracted extensive attention due to its high-temperature coefficient of resistivity (TCR) and large magnetoresistance (MR), which can be used in infrared measurements, magnetic refrigeration, magnetic storage and other applications. Doping Fe on the b-site of LCMO can provide larger TCR and MR. The $ La_{0.67} %$ Ca_{0.33} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (LCMFO: Ag) obtained by compounding with Ag showed that these properties were further improved. However, the temperature points at which peak TCR and peak MR occur for LCMO are not practical for applications. Sr doping at the a-site of LCMO is an effective means to control the insulation-metal transition temperature of the system. In this study, the temperature corresponding to the peak TCR and peak MR shifted to room temperature by Sr doping at the a-site of LCMFO: Ag to create $ La_{0.67} %$ Ca_{0.33-x} %$ Sr_{x} %$ Mn_{0.98} %$ Fe_{0.02} %$ O_{3} $: $ Ag_{0.15} $ (x = 0–0.09) ceramics. For x = 0.09, the peak TCR reached 10.8%·$ K^{−1} $ at 280.1 K and the peak MR reached 41.7% at 282.5 K. These results are beneficial to enhancing the application potential of LCMO-based systems. 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