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A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International.

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Presentation on theme: "A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International."— Presentation transcript:

1 A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International Symposium on Molecular Spectroscopy, 23 rd June 2011

2 Motivation 10 -24 10 -22 10 -26 10 -28 10 -30 10 -32 10 -34 10 -36 Multi Higgs Left - Right MSSM  ~ 1 MSSM  ~  Standard Model Predicted values for the electron edm d e (e.cm) The electron’s electric dipole moment (EDM) is sensitive to new physics

3 Measuring the EDM – spin precession Electron precessing in a magnetic field Electron precessing in parallel magnetic and electric fields Electron precessing in anti-parallel magnetic and electric fields Measure change in precession rate when electric field direction is reversed We use the valence electron in the YbF molecule Effective electric field >> Applied electric field

4 Ground state YbF -d e E eff d e E eff X 2  + ( = 0, N = 0) +10 F = 1 F = 0 170 MHz MFMF Electric Field E We measure the splitting 2d e E eff between the M F = +1 and M F = -1 levels

5 Measurement scheme – a spin interferometer Pulsed YbF beam Pump A-X Q(0) F=1 Probe A-X Q(0) F=0 PMT 3K beam F=1 F=0 rf pulse B HV+ HV-

6 Counts B E E Measuring the edm with the interferometer Signal α cos 2 [  ] = cos 2 [(  B B – d e E eff ) T / ћ]

7 Dataset  6194 measurements of the EDM, each derived from 4096 beam pulses  Each measurement takes 6 minutes

8 F = 0 F = 1 rf E Stark-shifted hyperfine interval F = 0 F = 1 rf E Stark-shifted hyperfine interval rf detuning phase shift: ~100 nrad/Hz Imperfect E-reversal Changes detuning via Stark shift Phase correlated with E-direction Correction to EDM: (5.5 ± 1.5) × 10 -28 e.cm Correcting a systematic error

9 EffectSystematic uncertainty (10 -28 e.cm) Electric field asymmetry1.1 Electric potential asymmetry0.1 Residual RF1 correlation1.0 Geometric phase0.03 Leakage currents0.2 Shield magnetization0.25 Motional magnetic field0.0005 Systematic uncertainties

10 Result 10 -24 10 -22 10 -26 10 -28 10 -30 10 -32 10 -34 10 -36 Multi Higgs Left - Right MSSM  ~ 1 MSSM  ~  Standard Model Predicted values for the electron edm d e (e.cm) | d e | < 10.5 × 10 -28 e.cm (90% confidence) Excluded region (5 × 10 -19 Debye) d e = (-2.4 ± 5.7 stat ± 1.5 syst ) × 10 -28 e.cm Improvements planned to explore this region

11 Joe Smallman Dhiren Kara Jony Hudson Ben Sauer Ed Hinds


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