Specific heat and magnetization in dilute magnetic alloys
Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friede...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Souletie, J. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1969 |
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| Schlagwörter: |
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| Anmerkung: |
© Plenum Publishing Corporation 1969 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of low temperature physics - Kluwer Academic Publishers-Plenum Publishers, 1969, 1(1969), 2 vom: Apr., Seite 95-108 |
|---|---|
| Übergeordnetes Werk: |
volume:1 ; year:1969 ; number:2 ; month:04 ; pages:95-108 |
| Links: |
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| DOI / URN: |
10.1007/BF00628265 |
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OLC2036733794 |
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| 520 | |a Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. | ||
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10.1007/BF00628265 doi (DE-627)OLC2036733794 (DE-He213)BF00628265-p DE-627 ger DE-627 rakwb eng 530 VZ Souletie, J. verfasserin aut Specific heat and magnetization in dilute magnetic alloys 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1969 Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. Magnetic Property Magnetic Material Free Path Geometrical Characteristic Field Model Tournier, R. aut Enthalten in Journal of low temperature physics Kluwer Academic Publishers-Plenum Publishers, 1969 1(1969), 2 vom: Apr., Seite 95-108 (DE-627)129546267 (DE-600)218311-0 (DE-576)014996642 0022-2291 nnns volume:1 year:1969 number:2 month:04 pages:95-108 https://doi.org/10.1007/BF00628265 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2185 GBV_ILN_4046 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4323 GBV_ILN_4700 AR 1 1969 2 04 95-108 |
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10.1007/BF00628265 doi (DE-627)OLC2036733794 (DE-He213)BF00628265-p DE-627 ger DE-627 rakwb eng 530 VZ Souletie, J. verfasserin aut Specific heat and magnetization in dilute magnetic alloys 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1969 Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. Magnetic Property Magnetic Material Free Path Geometrical Characteristic Field Model Tournier, R. aut Enthalten in Journal of low temperature physics Kluwer Academic Publishers-Plenum Publishers, 1969 1(1969), 2 vom: Apr., Seite 95-108 (DE-627)129546267 (DE-600)218311-0 (DE-576)014996642 0022-2291 nnns volume:1 year:1969 number:2 month:04 pages:95-108 https://doi.org/10.1007/BF00628265 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2185 GBV_ILN_4046 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4323 GBV_ILN_4700 AR 1 1969 2 04 95-108 |
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10.1007/BF00628265 doi (DE-627)OLC2036733794 (DE-He213)BF00628265-p DE-627 ger DE-627 rakwb eng 530 VZ Souletie, J. verfasserin aut Specific heat and magnetization in dilute magnetic alloys 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1969 Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. Magnetic Property Magnetic Material Free Path Geometrical Characteristic Field Model Tournier, R. aut Enthalten in Journal of low temperature physics Kluwer Academic Publishers-Plenum Publishers, 1969 1(1969), 2 vom: Apr., Seite 95-108 (DE-627)129546267 (DE-600)218311-0 (DE-576)014996642 0022-2291 nnns volume:1 year:1969 number:2 month:04 pages:95-108 https://doi.org/10.1007/BF00628265 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2185 GBV_ILN_4046 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4323 GBV_ILN_4700 AR 1 1969 2 04 95-108 |
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10.1007/BF00628265 doi (DE-627)OLC2036733794 (DE-He213)BF00628265-p DE-627 ger DE-627 rakwb eng 530 VZ Souletie, J. verfasserin aut Specific heat and magnetization in dilute magnetic alloys 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1969 Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. Magnetic Property Magnetic Material Free Path Geometrical Characteristic Field Model Tournier, R. aut Enthalten in Journal of low temperature physics Kluwer Academic Publishers-Plenum Publishers, 1969 1(1969), 2 vom: Apr., Seite 95-108 (DE-627)129546267 (DE-600)218311-0 (DE-576)014996642 0022-2291 nnns volume:1 year:1969 number:2 month:04 pages:95-108 https://doi.org/10.1007/BF00628265 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2185 GBV_ILN_4046 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4323 GBV_ILN_4700 AR 1 1969 2 04 95-108 |
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10.1007/BF00628265 doi (DE-627)OLC2036733794 (DE-He213)BF00628265-p DE-627 ger DE-627 rakwb eng 530 VZ Souletie, J. verfasserin aut Specific heat and magnetization in dilute magnetic alloys 1969 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1969 Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. Magnetic Property Magnetic Material Free Path Geometrical Characteristic Field Model Tournier, R. aut Enthalten in Journal of low temperature physics Kluwer Academic Publishers-Plenum Publishers, 1969 1(1969), 2 vom: Apr., Seite 95-108 (DE-627)129546267 (DE-600)218311-0 (DE-576)014996642 0022-2291 nnns volume:1 year:1969 number:2 month:04 pages:95-108 https://doi.org/10.1007/BF00628265 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2185 GBV_ILN_4046 GBV_ILN_4126 GBV_ILN_4306 GBV_ILN_4323 GBV_ILN_4700 AR 1 1969 2 04 95-108 |
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Souletie, J. |
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10.1007/BF00628265 |
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530 |
| title_sort |
specific heat and magnetization in dilute magnetic alloys |
| title_auth |
Specific heat and magnetization in dilute magnetic alloys |
| abstract |
Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. © Plenum Publishing Corporation 1969 |
| abstractGer |
Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. © Plenum Publishing Corporation 1969 |
| abstract_unstemmed |
Abstract We have studied dilute alloys where interactions of the Ruderman-Kittel-Yosida type are assumed to exist between well-defined magnetic moments that are localized on impurities distributed at random in the matrix. Using a molecular field model, such as has been proposed by Blandin and Friedel,12 we show that, because of the geometrical characteristics of the interaction, simple correspondences are expected between the magnetic properties (specific heat and magnetization) of a given alloy for different values of the solute concentrationc. These quantities are expressed through concentration-independent functions of the “reduced temperature,”T/c, and the “reduced field,”h/c. The idea of “reduced diagrams,” where we plot both new and available data in terms ofT/c andh/c, follows from these functions. Generally good agreement is observed for the specific heat, the magnetization, the initial susceptibility, and the residual magnetization of a number of alloys. (The data used here are for theAu-Fe,Cu-Mn andAg-Mn systems.) Furthermore, discrepancies, due to other mechanisms, such as the Kondo effect, or the effect of a mean free path limitation may better appear in such diagrams. © Plenum Publishing Corporation 1969 |
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Specific heat and magnetization in dilute magnetic alloys |
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