Improving the electrong-2 measurement
Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet...
Ausführliche Beschreibung
Autor*in: |
Mittleman, R. K. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1993 |
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Schlagwörter: |
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Anmerkung: |
© J.C. Baltzer AG, Science Publishers 1993 |
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Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 81(1993), 1-4 vom: März, Seite 105-113 |
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Übergeordnetes Werk: |
volume:81 ; year:1993 ; number:1-4 ; month:03 ; pages:105-113 |
Links: |
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DOI / URN: |
10.1007/BF00567254 |
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Katalog-ID: |
OLC2076375880 |
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520 | |a Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. | ||
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10.1007/BF00567254 doi (DE-627)OLC2076375880 (DE-He213)BF00567254-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Mittleman, R. K. verfasserin aut Improving the electrong-2 measurement 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer AG, Science Publishers 1993 Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. Magnetic Field Thin Film Trap Electron Anomalous Magnetic Moment Stringent Test Palmer, F. L. aut Dehmelt, H. G. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 81(1993), 1-4 vom: März, Seite 105-113 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:81 year:1993 number:1-4 month:03 pages:105-113 https://doi.org/10.1007/BF00567254 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 33.00 VZ AR 81 1993 1-4 03 105-113 |
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10.1007/BF00567254 doi (DE-627)OLC2076375880 (DE-He213)BF00567254-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Mittleman, R. K. verfasserin aut Improving the electrong-2 measurement 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer AG, Science Publishers 1993 Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. Magnetic Field Thin Film Trap Electron Anomalous Magnetic Moment Stringent Test Palmer, F. L. aut Dehmelt, H. G. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 81(1993), 1-4 vom: März, Seite 105-113 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:81 year:1993 number:1-4 month:03 pages:105-113 https://doi.org/10.1007/BF00567254 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 33.00 VZ AR 81 1993 1-4 03 105-113 |
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10.1007/BF00567254 doi (DE-627)OLC2076375880 (DE-He213)BF00567254-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Mittleman, R. K. verfasserin aut Improving the electrong-2 measurement 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer AG, Science Publishers 1993 Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. Magnetic Field Thin Film Trap Electron Anomalous Magnetic Moment Stringent Test Palmer, F. L. aut Dehmelt, H. G. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 81(1993), 1-4 vom: März, Seite 105-113 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:81 year:1993 number:1-4 month:03 pages:105-113 https://doi.org/10.1007/BF00567254 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 33.00 VZ AR 81 1993 1-4 03 105-113 |
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10.1007/BF00567254 doi (DE-627)OLC2076375880 (DE-He213)BF00567254-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Mittleman, R. K. verfasserin aut Improving the electrong-2 measurement 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer AG, Science Publishers 1993 Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. Magnetic Field Thin Film Trap Electron Anomalous Magnetic Moment Stringent Test Palmer, F. L. aut Dehmelt, H. G. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 81(1993), 1-4 vom: März, Seite 105-113 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:81 year:1993 number:1-4 month:03 pages:105-113 https://doi.org/10.1007/BF00567254 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 33.00 VZ AR 81 1993 1-4 03 105-113 |
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10.1007/BF00567254 doi (DE-627)OLC2076375880 (DE-He213)BF00567254-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Mittleman, R. K. verfasserin aut Improving the electrong-2 measurement 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer AG, Science Publishers 1993 Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. Magnetic Field Thin Film Trap Electron Anomalous Magnetic Moment Stringent Test Palmer, F. L. aut Dehmelt, H. G. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 81(1993), 1-4 vom: März, Seite 105-113 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:81 year:1993 number:1-4 month:03 pages:105-113 https://doi.org/10.1007/BF00567254 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 33.00 VZ AR 81 1993 1-4 03 105-113 |
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Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. © J.C. Baltzer AG, Science Publishers 1993 |
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Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. © J.C. Baltzer AG, Science Publishers 1993 |
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Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”. © J.C. Baltzer AG, Science Publishers 1993 |
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K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Improving the electrong-2 measurement</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1993</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">© J.C. Baltzer AG, Science Publishers 1993</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The measurement and calculation of the anomalous magnetic moment of the electron currently provides the most stringent test of QED. In the past, one of the limitations in the experiment has been the small inhomogeneous component of the magnetic field which has been used to detect the magnet resonances of the trapped electron. We have developed a technique which allows us to reduce this inhomogeneous field by as much as two orders of magnitude and have demonstrated the technique with a factor of fifteen reduction, virtually eliminating the broadening of the magnetic lines in our “geonium atom”.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Magnetic Field</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Thin Film</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Trap Electron</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Anomalous Magnetic Moment</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Stringent Test</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Palmer, F. L.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dehmelt, H. G.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Hyperfine interactions</subfield><subfield code="d">Kluwer Academic Publishers, 1975</subfield><subfield code="g">81(1993), 1-4 vom: März, Seite 105-113</subfield><subfield code="w">(DE-627)129438685</subfield><subfield code="w">(DE-600)194471-X</subfield><subfield code="w">(DE-576)014809028</subfield><subfield code="x">0304-3843</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:81</subfield><subfield code="g">year:1993</subfield><subfield code="g">number:1-4</subfield><subfield code="g">month:03</subfield><subfield code="g">pages:105-113</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF00567254</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="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2279</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4046</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">81</subfield><subfield code="j">1993</subfield><subfield code="e">1-4</subfield><subfield code="c">03</subfield><subfield code="h">105-113</subfield></datafield></record></collection>
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