Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light
Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a typ...
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Gespeichert in:
| Autor*in: |
Mainland, G. B. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Schlagwörter: |
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| Anmerkung: |
© The Author(s) 2020 |
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| Übergeordnetes Werk: |
Enthalten in: Foundations of physics - Springer US, 1970, 50(2020), 5 vom: 27. März, Seite 457-480 |
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| Übergeordnetes Werk: |
volume:50 ; year:2020 ; number:5 ; day:27 ; month:03 ; pages:457-480 |
| Links: |
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| DOI / URN: |
10.1007/s10701-020-00339-3 |
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OLC2039116230 |
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| 520 | |a Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. | ||
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10.1007/s10701-020-00339-3 doi (DE-627)OLC2039116230 (DE-He213)s10701-020-00339-3-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Mainland, G. B. verfasserin aut Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2020 Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. Quantum vacuum Vacuum fluctuations Permittivity of the vacuum Speed of light in the vacuum Mulligan, Bernard aut Enthalten in Foundations of physics Springer US, 1970 50(2020), 5 vom: 27. März, Seite 457-480 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:50 year:2020 number:5 day:27 month:03 pages:457-480 https://doi.org/10.1007/s10701-020-00339-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 AR 50 2020 5 27 03 457-480 |
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10.1007/s10701-020-00339-3 doi (DE-627)OLC2039116230 (DE-He213)s10701-020-00339-3-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Mainland, G. B. verfasserin aut Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2020 Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. Quantum vacuum Vacuum fluctuations Permittivity of the vacuum Speed of light in the vacuum Mulligan, Bernard aut Enthalten in Foundations of physics Springer US, 1970 50(2020), 5 vom: 27. März, Seite 457-480 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:50 year:2020 number:5 day:27 month:03 pages:457-480 https://doi.org/10.1007/s10701-020-00339-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 AR 50 2020 5 27 03 457-480 |
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10.1007/s10701-020-00339-3 doi (DE-627)OLC2039116230 (DE-He213)s10701-020-00339-3-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Mainland, G. B. verfasserin aut Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2020 Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. Quantum vacuum Vacuum fluctuations Permittivity of the vacuum Speed of light in the vacuum Mulligan, Bernard aut Enthalten in Foundations of physics Springer US, 1970 50(2020), 5 vom: 27. März, Seite 457-480 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:50 year:2020 number:5 day:27 month:03 pages:457-480 https://doi.org/10.1007/s10701-020-00339-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 AR 50 2020 5 27 03 457-480 |
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10.1007/s10701-020-00339-3 doi (DE-627)OLC2039116230 (DE-He213)s10701-020-00339-3-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Mainland, G. B. verfasserin aut Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2020 Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. Quantum vacuum Vacuum fluctuations Permittivity of the vacuum Speed of light in the vacuum Mulligan, Bernard aut Enthalten in Foundations of physics Springer US, 1970 50(2020), 5 vom: 27. März, Seite 457-480 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:50 year:2020 number:5 day:27 month:03 pages:457-480 https://doi.org/10.1007/s10701-020-00339-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 AR 50 2020 5 27 03 457-480 |
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10.1007/s10701-020-00339-3 doi (DE-627)OLC2039116230 (DE-He213)s10701-020-00339-3-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Mainland, G. B. verfasserin aut Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Author(s) 2020 Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. Quantum vacuum Vacuum fluctuations Permittivity of the vacuum Speed of light in the vacuum Mulligan, Bernard aut Enthalten in Foundations of physics Springer US, 1970 50(2020), 5 vom: 27. März, Seite 457-480 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:50 year:2020 number:5 day:27 month:03 pages:457-480 https://doi.org/10.1007/s10701-020-00339-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 AR 50 2020 5 27 03 457-480 |
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Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. © The Author(s) 2020 |
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Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. © The Author(s) 2020 |
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Abstract There are two types of fluctuations in the quantum vacuum: type 1 vacuum fluctuations are on shell and can interact with matter in specific, limited ways that have observable consequences; type 2 vacuum fluctuations are off shell and cannot interact with matter. A photon will polarize a type 1, bound, charged lepton–antilepton vacuum fluctuation in much the same manner that it would polarize a dielectric, suggesting the method used here for calculating the permittivity $$\epsilon _{0}$$ of the vacuum. In a model that retains only leading terms, $$\epsilon _{0} \cong (6\mu _{0}/\pi )(8e^{2}/\hbar )^{2}= 9.10\times 10^{-12}$$ C/(Vm). The calculated value for $$\epsilon _{0}$$ is 2.7% more than the accepted value. The permittivity of the vacuum, in turn, determines the speed c of light in the vacuum. Since the vacuum is at rest with respect to every inertial frame of reference, c is the same in every inertial reference frame. © The Author(s) 2020 |
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Polarization of Vacuum Fluctuations: Source of the Vacuum Permittivity and Speed of Light |
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