The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients
Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1)...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Evans, M. W. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1995 |
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| Schlagwörter: |
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| Anmerkung: |
© Plenum Publishing Corporation 1995 |
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| Übergeordnetes Werk: |
Enthalten in: Foundations of physics - Kluwer Academic Publishers-Plenum Publishers, 1970, 25(1995), 2 vom: Feb., Seite 383-389 |
|---|---|
| Übergeordnetes Werk: |
volume:25 ; year:1995 ; number:2 ; month:02 ; pages:383-389 |
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| DOI / URN: |
10.1007/BF02055215 |
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10.1007/BF02055215 doi (DE-627)OLC2039091459 (DE-He213)BF02055215-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Evans, M. W. verfasserin aut The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients 1995 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1995 Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. Radiation Energy Density Power Density Density Dependence Electromagnetic Energy Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 25(1995), 2 vom: Feb., Seite 383-389 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:25 year:1995 number:2 month:02 pages:383-389 https://doi.org/10.1007/BF02055215 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_32 GBV_ILN_40 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2021 GBV_ILN_4012 GBV_ILN_4046 AR 25 1995 2 02 383-389 |
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10.1007/BF02055215 doi (DE-627)OLC2039091459 (DE-He213)BF02055215-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Evans, M. W. verfasserin aut The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients 1995 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1995 Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. Radiation Energy Density Power Density Density Dependence Electromagnetic Energy Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 25(1995), 2 vom: Feb., Seite 383-389 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:25 year:1995 number:2 month:02 pages:383-389 https://doi.org/10.1007/BF02055215 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_32 GBV_ILN_40 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2021 GBV_ILN_4012 GBV_ILN_4046 AR 25 1995 2 02 383-389 |
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10.1007/BF02055215 doi (DE-627)OLC2039091459 (DE-He213)BF02055215-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Evans, M. W. verfasserin aut The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients 1995 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1995 Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. Radiation Energy Density Power Density Density Dependence Electromagnetic Energy Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 25(1995), 2 vom: Feb., Seite 383-389 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:25 year:1995 number:2 month:02 pages:383-389 https://doi.org/10.1007/BF02055215 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_32 GBV_ILN_40 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2021 GBV_ILN_4012 GBV_ILN_4046 AR 25 1995 2 02 383-389 |
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10.1007/BF02055215 doi (DE-627)OLC2039091459 (DE-He213)BF02055215-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Evans, M. W. verfasserin aut The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients 1995 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1995 Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. Radiation Energy Density Power Density Density Dependence Electromagnetic Energy Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 25(1995), 2 vom: Feb., Seite 383-389 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:25 year:1995 number:2 month:02 pages:383-389 https://doi.org/10.1007/BF02055215 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_32 GBV_ILN_40 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2021 GBV_ILN_4012 GBV_ILN_4046 AR 25 1995 2 02 383-389 |
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10.1007/BF02055215 doi (DE-627)OLC2039091459 (DE-He213)BF02055215-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Evans, M. W. verfasserin aut The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients 1995 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1995 Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. Radiation Energy Density Power Density Density Dependence Electromagnetic Energy Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 25(1995), 2 vom: Feb., Seite 383-389 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:25 year:1995 number:2 month:02 pages:383-389 https://doi.org/10.1007/BF02055215 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_32 GBV_ILN_40 GBV_ILN_65 GBV_ILN_70 GBV_ILN_2006 GBV_ILN_2021 GBV_ILN_4012 GBV_ILN_4046 AR 25 1995 2 02 383-389 |
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The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients |
| abstract |
Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. © Plenum Publishing Corporation 1995 |
| abstractGer |
Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. © Plenum Publishing Corporation 1995 |
| abstract_unstemmed |
Abstract The role of the novel longitudinal vacuum fieldB(3)is discussed in relation to fundamental radiation laws: the Rayleigh-Jeans law, the Planck law, and the Einstein coefficients. The circular index (3) ofB(3)causes electromagnetic energy density to be redistributed from the other indices (1) and (2) of the circular basis, but the presence ofB(3)in the vacuum does not change the value of the Planck constant h. TheB(3)field does not affect, furthermore, the understanding of quantized radiation absorption first proposed by Einstein. Therefore, the experimental observableB(3) does not imply modification of these fundamental, radiation laws, and experimental isolation ofB(3) must take place through its characteristic square root power density dependence when used to magnetize an électron plasma. © Plenum Publishing Corporation 1995 |
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| title_short |
The $ B^{(3)} $ field: Its role in the Rayleigh-Jeans law, Planck law, and Einstein coefficients |
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https://doi.org/10.1007/BF02055215 |
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2024-07-03T21:31:05.844Z |
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