Gravitation and quantum mechanics of macroscopic objects
Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting unc...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Karolyhazy, F. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1966 |
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| Schlagwörter: |
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| Anmerkung: |
© Società Italiana di Fisica 1966 |
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| Übergeordnetes Werk: |
Enthalten in: Il Nuovo Cimento A (1965-1970) - Springer Berlin Heidelberg, 1971, 42(1966), 2 vom: März, Seite 390-402 |
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| Übergeordnetes Werk: |
volume:42 ; year:1966 ; number:2 ; month:03 ; pages:390-402 |
| Links: |
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| DOI / URN: |
10.1007/BF02717926 |
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| Katalog-ID: |
OLC2087109850 |
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| 520 | |a Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. | ||
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| 650 | 4 | |a Macroscopic Object | |
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10.1007/BF02717926 doi (DE-627)OLC2087109850 (DE-He213)BF02717926-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Karolyhazy, F. verfasserin aut Gravitation and quantum mechanics of macroscopic objects 1966 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Società Italiana di Fisica 1966 Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. Wave Function Wave Packet Pure State World Line Macroscopic Object Enthalten in Il Nuovo Cimento A (1965-1970) Springer Berlin Heidelberg, 1971 42(1966), 2 vom: März, Seite 390-402 (DE-627)130067792 (DE-600)441918-2 (DE-576)015602206 0369-3546 nnns volume:42 year:1966 number:2 month:03 pages:390-402 https://doi.org/10.1007/BF02717926 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 42 1966 2 03 390-402 |
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10.1007/BF02717926 doi (DE-627)OLC2087109850 (DE-He213)BF02717926-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Karolyhazy, F. verfasserin aut Gravitation and quantum mechanics of macroscopic objects 1966 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Società Italiana di Fisica 1966 Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. Wave Function Wave Packet Pure State World Line Macroscopic Object Enthalten in Il Nuovo Cimento A (1965-1970) Springer Berlin Heidelberg, 1971 42(1966), 2 vom: März, Seite 390-402 (DE-627)130067792 (DE-600)441918-2 (DE-576)015602206 0369-3546 nnns volume:42 year:1966 number:2 month:03 pages:390-402 https://doi.org/10.1007/BF02717926 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 42 1966 2 03 390-402 |
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10.1007/BF02717926 doi (DE-627)OLC2087109850 (DE-He213)BF02717926-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Karolyhazy, F. verfasserin aut Gravitation and quantum mechanics of macroscopic objects 1966 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Società Italiana di Fisica 1966 Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. Wave Function Wave Packet Pure State World Line Macroscopic Object Enthalten in Il Nuovo Cimento A (1965-1970) Springer Berlin Heidelberg, 1971 42(1966), 2 vom: März, Seite 390-402 (DE-627)130067792 (DE-600)441918-2 (DE-576)015602206 0369-3546 nnns volume:42 year:1966 number:2 month:03 pages:390-402 https://doi.org/10.1007/BF02717926 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 42 1966 2 03 390-402 |
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10.1007/BF02717926 doi (DE-627)OLC2087109850 (DE-He213)BF02717926-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Karolyhazy, F. verfasserin aut Gravitation and quantum mechanics of macroscopic objects 1966 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Società Italiana di Fisica 1966 Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. Wave Function Wave Packet Pure State World Line Macroscopic Object Enthalten in Il Nuovo Cimento A (1965-1970) Springer Berlin Heidelberg, 1971 42(1966), 2 vom: März, Seite 390-402 (DE-627)130067792 (DE-600)441918-2 (DE-576)015602206 0369-3546 nnns volume:42 year:1966 number:2 month:03 pages:390-402 https://doi.org/10.1007/BF02717926 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY 33.00 VZ AR 42 1966 2 03 390-402 |
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Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. © Società Italiana di Fisica 1966 |
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Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. © Società Italiana di Fisica 1966 |
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Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained. © Società Italiana di Fisica 1966 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2087109850</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230401103547.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230302s1966 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02717926</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2087109850</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02717926-p</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="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Karolyhazy, F.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Gravitation and quantum mechanics of macroscopic objects</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1966</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Società Italiana di Fisica 1966</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary The problem of the reduction of the wave function in quantum theory is treated from a new standpoint. First, by combining Heisenberg's uncertainty relations with gravitation, quantitative limi tations on the sharpness of the structure of space-time are derived. Second, the resulting uncertainty in space-time structure is incorporated into the equations for the propagation of the quantum-mechanical wave amplitudes. In the resulting theory an initially pure wave function generally develops in time into a mixture. A single pure wave function survives only as long as it corresponds to a sufficiently small spread in the position of any massive part of the system under investigation. Quantitative relations between the mass and the maximum coherent spread in the center-of-mass wave function of a single body are obtained.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Wave Function</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Wave Packet</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Pure State</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">World Line</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Macroscopic Object</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Il Nuovo Cimento A (1965-1970)</subfield><subfield code="d">Springer Berlin Heidelberg, 1971</subfield><subfield code="g">42(1966), 2 vom: März, Seite 390-402</subfield><subfield code="w">(DE-627)130067792</subfield><subfield code="w">(DE-600)441918-2</subfield><subfield code="w">(DE-576)015602206</subfield><subfield code="x">0369-3546</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:42</subfield><subfield code="g">year:1966</subfield><subfield code="g">number:2</subfield><subfield code="g">month:03</subfield><subfield code="g">pages:390-402</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02717926</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.00</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">42</subfield><subfield code="j">1966</subfield><subfield code="e">2</subfield><subfield code="c">03</subfield><subfield code="h">390-402</subfield></datafield></record></collection>
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