A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre...
-
Upload
elvin-wright -
Category
Documents
-
view
216 -
download
1
Transcript of A new measurement of the electron’s electric dipole moment using YbF molecules Mike Tarbutt Centre...
![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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/1.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/2.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/3.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/4.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/5.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/6.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/7.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/8.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/9.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/10.jpg)
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.](https://reader035.fdocuments.us/reader035/viewer/2022062517/56649f225503460f94c3a79f/html5/thumbnails/11.jpg)
Joe Smallman Dhiren Kara
Jony Hudson Ben Sauer Ed Hinds