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Measurement of a false electric dipole moment signal from 199Hg atoms exposed to an inhomogeneous magnetic field
We report on the measurement of a Larmor frequency shift proportional to the electric-field strength for 199 Hg atoms contained in a volume permeated with aligned magnetic and electric fields. This shift arises from the interplay between the inevitable magnetic field gradients and the motional magne...
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Published in: | The European physical journal. D, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2015-10, Vol.69 (10), Article 225 |
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creator | Afach, S. Baker, C. A. Ban, G. Bison, G. Bodek, K. Chowdhuri, Z. Daum, M. Fertl, M. Franke, B. Geltenbort, P. Green, K. van der Grinten, M. G. D. Grujic, Z. Harris, P. G. Heil, W. Hélaine, V. Henneck, R. Horras, M. Iaydjiev, P. Ivanov, S. N. Kasprzak, M. Kermaïdic, Y. Kirch, K. Knowles, P. Koch, H.-C. Komposch, S. Kozela, A. Krempel, J. Lauss, B. Lefort, T. Lemière, Y. Mtchedlishvili, A. Naviliat-Cuncic, O. Pendlebury, J. M. Piegsa, F. M. Pignol, G. Prashant, P. N. Quéméner, G. Rebreyend, D. Ries, D. Roccia, S. Schmidt-Wellenburg, P. Severijns, N. Weis, A. Wursten, E. Wyszynski, G. Zejma, J. Zenner, J. Zsigmond, G. |
description | We report on the measurement of a Larmor frequency shift proportional to the electric-field strength for
199
Hg atoms contained in a volume permeated with aligned magnetic and electric fields. This shift arises from the interplay between the inevitable magnetic field gradients and the motional magnetic field. The proportionality to electric-field strength makes it apparently similar to an electric dipole moment (EDM) signal, although unlike an EDM this effect is P- and T-conserving. We have used a neutron magnetic resonance EDM spectrometer, featuring a mercury co-magnetometer and an array of external cesium magnetometers, to measure the shift as a function of the applied magnetic field gradient. Our results are in good agreement with theoretical expectations.
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doi_str_mv | 10.1140/epjd/e2015-60207-4 |
format | article |
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199
Hg atoms contained in a volume permeated with aligned magnetic and electric fields. This shift arises from the interplay between the inevitable magnetic field gradients and the motional magnetic field. The proportionality to electric-field strength makes it apparently similar to an electric dipole moment (EDM) signal, although unlike an EDM this effect is P- and T-conserving. We have used a neutron magnetic resonance EDM spectrometer, featuring a mercury co-magnetometer and an array of external cesium magnetometers, to measure the shift as a function of the applied magnetic field gradient. Our results are in good agreement with theoretical expectations.
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199
Hg atoms contained in a volume permeated with aligned magnetic and electric fields. This shift arises from the interplay between the inevitable magnetic field gradients and the motional magnetic field. The proportionality to electric-field strength makes it apparently similar to an electric dipole moment (EDM) signal, although unlike an EDM this effect is P- and T-conserving. We have used a neutron magnetic resonance EDM spectrometer, featuring a mercury co-magnetometer and an array of external cesium magnetometers, to measure the shift as a function of the applied magnetic field gradient. Our results are in good agreement with theoretical expectations.
Graphical abstract</description><subject>Applications of Nonlinear Dynamics and Chaos Theory</subject><subject>Atomic</subject><subject>Molecular</subject><subject>Optical and Plasma Physics</subject><subject>Physical Chemistry</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Information Technology</subject><subject>Quantum Physics</subject><subject>Regular Article</subject><subject>Spectroscopy/Spectrometry</subject><subject>Spintronics</subject><issn>1434-6060</issn><issn>1434-6079</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kMFOwzAQRC0EEqXwA5z8A6G248T2EVVAKxVxgbPlxuuQKrYjO5Xg70lTxJHT7kozs5qH0D0lD5RysoLhYFfACK2KmjAiCn6BFpSXfDqFuvzba3KNbnI-EEJYxesFGl7B5GMCD2HE0WGDnekzYOihGVPXYNsNsQfs46zIXRtMj12KHlOlNi02Y_QZw9cQM1g8RmwC7sJn9LGFAPGYsTdtgHGKch309hZdzR_ufucSfTw_va83xe7tZbt-3BUNY3QsaCVZWRppa1sb4iogag-cOy5KoYiUDpiRkgvF2Z4Ty8TeMQeybhTQprKiXCJ2zm1SzDmB00PqvEnfmhJ9YqZPzPTMTM_MNJ9M5dmUJ3FoIelDPKapcf7P9QNPxHKP</recordid><startdate>20151006</startdate><enddate>20151006</enddate><creator>Afach, S.</creator><creator>Baker, C. A.</creator><creator>Ban, G.</creator><creator>Bison, G.</creator><creator>Bodek, K.</creator><creator>Chowdhuri, Z.</creator><creator>Daum, M.</creator><creator>Fertl, M.</creator><creator>Franke, B.</creator><creator>Geltenbort, P.</creator><creator>Green, K.</creator><creator>van der Grinten, M. G. D.</creator><creator>Grujic, Z.</creator><creator>Harris, P. G.</creator><creator>Heil, W.</creator><creator>Hélaine, V.</creator><creator>Henneck, R.</creator><creator>Horras, M.</creator><creator>Iaydjiev, P.</creator><creator>Ivanov, S. N.</creator><creator>Kasprzak, M.</creator><creator>Kermaïdic, Y.</creator><creator>Kirch, K.</creator><creator>Knowles, P.</creator><creator>Koch, H.-C.</creator><creator>Komposch, S.</creator><creator>Kozela, A.</creator><creator>Krempel, J.</creator><creator>Lauss, B.</creator><creator>Lefort, T.</creator><creator>Lemière, Y.</creator><creator>Mtchedlishvili, A.</creator><creator>Naviliat-Cuncic, O.</creator><creator>Pendlebury, J. 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N.</au><au>Quéméner, G.</au><au>Rebreyend, D.</au><au>Ries, D.</au><au>Roccia, S.</au><au>Schmidt-Wellenburg, P.</au><au>Severijns, N.</au><au>Weis, A.</au><au>Wursten, E.</au><au>Wyszynski, G.</au><au>Zejma, J.</au><au>Zenner, J.</au><au>Zsigmond, G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measurement of a false electric dipole moment signal from 199Hg atoms exposed to an inhomogeneous magnetic field</atitle><jtitle>The European physical journal. D, Atomic, molecular, and optical physics</jtitle><stitle>Eur. Phys. J. D</stitle><date>2015-10-06</date><risdate>2015</risdate><volume>69</volume><issue>10</issue><artnum>225</artnum><issn>1434-6060</issn><eissn>1434-6079</eissn><abstract>We report on the measurement of a Larmor frequency shift proportional to the electric-field strength for
199
Hg atoms contained in a volume permeated with aligned magnetic and electric fields. This shift arises from the interplay between the inevitable magnetic field gradients and the motional magnetic field. The proportionality to electric-field strength makes it apparently similar to an electric dipole moment (EDM) signal, although unlike an EDM this effect is P- and T-conserving. We have used a neutron magnetic resonance EDM spectrometer, featuring a mercury co-magnetometer and an array of external cesium magnetometers, to measure the shift as a function of the applied magnetic field gradient. Our results are in good agreement with theoretical expectations.
Graphical abstract</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjd/e2015-60207-4</doi></addata></record> |
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subjects | Applications of Nonlinear Dynamics and Chaos Theory Atomic Molecular Optical and Plasma Physics Physical Chemistry Physics Physics and Astronomy Quantum Information Technology Quantum Physics Regular Article Spectroscopy/Spectrometry Spintronics |
title | Measurement of a false electric dipole moment signal from 199Hg atoms exposed to an inhomogeneous magnetic field |
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