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Published byRosamund Horton Modified over 9 years ago
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Measuring the Electron EDM Using Ytterbium Fluoride (YbF) Molecules
βmeasuring the shape of the electronβ Joe Smallman
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The electron electric dipole moment (EDM)
Displacement of centre of charge from centre of mass πΈ β β π π β β β β β π=β π π β πΈ π π Η π
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Electron EDM estimates
David A. Aguilar Harvard-Smithsonian Center for AstrophysicsΒ not enough CP violation |dethallium|< 1.6 x 10-27e.cm
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How small is that? Assume: β π π β πΈ β0.25 ππ»π§
π π β 10 β27 π.ππ=2Γ 10 β19 π. π 0 =5Γ 10 β19 π· πΈβ1πΊπ/ππ β‘β π π΅ βπ΅ for β17ππ magnetic field β 10 β10 ππ β1 β 10 β18 ππ β π π β πΈ β0.25 ππ»π§ EDM interaction:
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How atoms and molecules can help
Amplify the electron EDM interaction! β π π β πΈ complicated special relativity β π π β πΈ eff π π πΈ eff = πΈ eff max Ξ· πΈ app π§ π πΈ app π§ structure dependent factor ~ π 3 polarisation factor π β π§
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YbF electric field enhancement
πΈ eff =14.5 GV/cm for πΈ app =10 kV/cm Enhancement of ! Needs βonlyβ nano-Gauss level of B-field control
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YbF energy levels
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EDM measurement π Ο= (ΞΌBβd e E eff )T Δ§ πΈ eff
π΅ π πΈ eff πΉ Torque: d πΉ dt = π e Γ πΈ πππ +( π Γ π΅ ) βπ<7 ΞΌrad Ο= (ΞΌBβd e E eff )T Δ§ or βπ<2 mHz
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Measuring the electron EDM
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Interference fringes π= cos 2 Ο Ο= (ΞΌBβd e E eff )T Δ§
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Lots of other parameter modulations
E-field direction B-field direction B-field magnitude rf pulse frequency (independently) rf pulse amplitude (independently) rf pulse phase difference laser frequency demonstrated in last slide
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Result d e = β2.4Β± 5.7 stat Β± 1.7 syst Γ 10 β28 e.cm
2011 dataset: 6194 measurements (6min/measurement) d e = β2.4Β± 5.7 stat Β± 1.7 syst Γ 10 β28 e.cm d e <1Γ 10 β27 e.cm with 90% confidence J J Hudson et al. Nature (2011) D M Kara etal. New. J. Phys (2012)
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Upgrades since 2011 3rd layer of magnetic shielding
Less magnetic field noise Longer inner magnetic shield Reduce end effects Separate rf transmission line from HV plates Reduce end effects, higher applied E-field, less leakage Shorten rf pulses Reduce systematics associated with rf detuning old scheme new scheme
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YbF fountain 0.5s coherence time instead of 0.5ms
6Γ 10 β31 e cm in 8hrs Tarbutt et al. New J. Phys (2013)
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The YbF eEDM team Joe Smallman Ben Sauer Mike Tarbutt Ed Hinds
Jack Devlin Jony Hudson
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EDM measurement Measure the EDM induced splitting + π π πΈ eff
mF=-1 nuclear spin electron spin mF=0 mF=+1 + π π πΈ eff - π π πΈ eff large tensor Stark shift
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