a new measurement of the electron’s electric dipole moment using ybf molecules mike tarbutt centre...

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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 Symposium on Molecular Spectroscopy, 23 rd June 2011

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Page 1: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

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, 23rd June 2011

Page 2: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Motivation

10-24

10-22

10-26

10-28

10-30

10-32

10-34

10-36

Multi Higgs

Left -Right

MSSM f ~ 1

MSSM f ~ /a p

Standard Model

Pred

icte

d va

lues

for

the

elec

tron

edm

de (

e.cm

)

The electron’s electric dipole moment (EDM) is sensitive to new physics

Page 3: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

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

Page 4: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Ground state YbF

-de Eeff

de Eeff

X 2S+ (n = 0, N = 0)

-1 +10F = 1

F = 0

170 MHz

MF

ElectricField

E

We measure the splitting 2deEeff between the MF = +1 and MF = -1 levels

Page 5: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Measurement scheme – a spin interferometer

Pulsed YbF beam

PumpA-X Q(0) F=1

ProbeA-X Q(0) F=0

PMT

3K beam

F=1

F=0

rf pulse

B HV+

HV-

Page 6: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Counts

BEE

Measuring the edm with the interferometer

Signal α cos2 [f] = cos2 [(mB B – de Eeff ) T / ћ]

Page 7: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

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

Page 8: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

F = 0

F = 1

rf

E

Sta

rk-s

hift

ed

hype

rfin

e in

terv

al

F = 0

F = 1

rf

E

Sta

rk-s

hift

ed

hype

rfin

e in

terv

al

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

Page 9: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Effect Systematic uncertainty (10-28 e.cm)

Electric field asymmetry 1.1

Electric potential asymmetry 0.1

Residual RF1 correlation 1.0

Geometric phase 0.03

Leakage currents 0.2

Shield magnetization 0.25

Motional magnetic field 0.0005

Systematic uncertainties

Page 10: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Result

10-24

10-22

10-26

10-28

10-30

10-32

10-34

10-36

Multi Higgs Left -

Right

MSSM f ~ 1

MSSM f ~ /a p

Standard Model

Pred

icte

d va

lues

for

the

elec

tron

edm

de (

e.cm

)

| de | < 10.5 × 10-28 e.cm (90% confidence)

Excluded region

(5 × 10-19 Debye)

de = (-2.4 ± 5.7stat ± 1.5syst) × 10-28 e.cm

Improvements planned to explore this region

Page 11: A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre for Cold Matter, Imperial College London. International

Joe Smallman Dhiren Kara

Jony Hudson Ben Sauer Ed Hinds