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Measuring the Electron EDM Using Ytterbium Fluoride (YbF) Molecules

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Presentation on theme: "Measuring the Electron EDM Using Ytterbium Fluoride (YbF) Molecules"β€” Presentation transcript:

1 Measuring the Electron EDM Using Ytterbium Fluoride (YbF) Molecules
β€œmeasuring the shape of the electron” Joe Smallman

2 The electron electric dipole moment (EDM)
Displacement of centre of charge from centre of mass 𝐸 βˆ’ βˆ’ 𝑑 𝑒 βˆ’ βˆ’ βˆ’ βˆ’ βˆ’ π‘ˆ=βˆ’ 𝑑 𝑒 βˆ™ 𝐸 𝑑 𝑒 ǁ 𝜎

3 Electron EDM estimates
David A. Aguilar Harvard-Smithsonian Center for AstrophysicsΒ  not enough CP violation |dethallium|< 1.6 x 10-27e.cm

4 How small is that? Assume: βˆ’ 𝑑 𝑒 βˆ™ 𝐸 β‰ˆ0.25 π‘šπ»π‘§
𝑑 𝑒 β‰ˆ 10 βˆ’27 𝑒.π‘π‘š=2Γ— 10 βˆ’19 𝑒. π‘Ž 0 =5Γ— 10 βˆ’19 𝐷 πΈβ‰ˆ1𝐺𝑉/π‘π‘š β‰‘βˆ’ πœ‡ 𝐡 βˆ™π΅ for β‰ˆ17𝑓𝑇 magnetic field β‰ˆ 10 βˆ’10 π‘π‘š βˆ’1 β‰ˆ 10 βˆ’18 𝑒𝑉 βˆ’ 𝑑 𝑒 βˆ™ 𝐸 β‰ˆ0.25 π‘šπ»π‘§ EDM interaction:

5 How atoms and molecules can help
Amplify the electron EDM interaction! βˆ’ 𝑑 𝑒 βˆ™ 𝐸 complicated special relativity βˆ’ 𝑑 𝑒 βˆ™ 𝐸 eff 𝑑 𝑒 𝐸 eff = 𝐸 eff max Ξ· 𝐸 app 𝑧 𝑛 𝐸 app 𝑧 structure dependent factor ~ 𝑍 3 polarisation factor 𝑛 βˆ™ 𝑧

6 YbF electric field enhancement
𝐸 eff =14.5 GV/cm for 𝐸 app =10 kV/cm Enhancement of ! Needs β€˜only’ nano-Gauss level of B-field control

7 YbF energy levels

8 EDM measurement πœ™ Ο•= (ΞΌBβˆ“d e E eff )T Δ§ 𝐸 eff
𝐡 πœ™ 𝐸 eff 𝐹 Torque: d 𝐹 dt = 𝑑 e Γ— 𝐸 𝐞𝐟𝐟 +( πœ‡ Γ— 𝐡 ) βˆ†πœ™<7 ΞΌrad Ο•= (ΞΌBβˆ“d e E eff )T Δ§ or βˆ†π‘ˆ<2 mHz

9 Measuring the electron EDM

10 Interference fringes 𝑆= cos 2 Ο• Ο•= (ΞΌBβˆ“d e E eff )T Δ§

11 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

12 Result d e = βˆ’2.4Β± 5.7 stat Β± 1.7 syst Γ— 10 βˆ’28 e.cm
2011 dataset: 6194 measurements (6min/measurement) d e = βˆ’2.4Β± 5.7 stat Β± 1.7 syst Γ— 10 βˆ’28 e.cm d e <1Γ— 10 βˆ’27 e.cm with 90% confidence J J Hudson et al. Nature (2011) D M Kara etal. New. J. Phys (2012)

13 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

14 YbF fountain 0.5s coherence time instead of 0.5ms
6Γ— 10 βˆ’31 e cm in 8hrs Tarbutt et al. New J. Phys (2013)

15 The YbF eEDM team Joe Smallman Ben Sauer Mike Tarbutt Ed Hinds
Jack Devlin Jony Hudson

16 EDM measurement Measure the EDM induced splitting + 𝑑 𝑒 𝐸 eff
mF=-1 nuclear spin electron spin mF=0 mF=+1 + 𝑑 𝑒 𝐸 eff - 𝑑 𝑒 𝐸 eff large tensor Stark shift


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