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P. Harris IoP 2011 Measurement principle BE BB Measure Larmor spin precession freq in parallel & antiparallel B and E fields d makes precession faster... Reverse E relative to B, look for freq shift.... or slower.
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Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London
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Page 1: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Electric dipole moment searches

E.A. Hinds

Birmingham 11th July 2011

Centre for Cold MatterImperial College London

Page 2: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

YbF

atom/moleculelevel

EDM: from particles to atoms and molecules

nuclearlevel

NNNN Schiffmoment

mercury

HiggsSUSY

Left/Right

StrongCP

field theoryCP model

qGG

neutron

nucleonlevel

electron/quark level

de

dq

dcq

~

Page 3: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

Measurement principle

B E

mB

Measure Larmor spin precession freq in parallel & antiparallel B and E fields

d makes precessionfaster...

Reverse E relative to B, look for freq shift.... or slower.

Page 4: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

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-

eEDM in practice (Imperial)Ch 15 Cold Molecules, eds. Krems, Stwalley and Friedrich, (CRC Press 2009)

Page 5: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

nEDM in practice

N S

Magnetic shielding

Storage cell

Magnet & polarizing foil Ultracold

neutrons(UCN)

UCN detector

Approx scale 1 m

Magnetic field coil

B

High voltage lead

E

/analysingfoil

Page 6: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Status of eEDM and nEDM

de = (-2.4 5.7 1.5) ×10-28 e.cm

68% statisticalsystematic - limited by statistical noise

• New eEDM result – YbF – Hudson et al. (Nature 2011)

• Previous eEDM result - Tl atoms de < 2.0 × 10-27 e.cm with 90% confidence

Regan et al. (PRL 2002)Nataraj et al. (PRL 2011)

de < 1 × 10-27 e.cm with 90% confidence dn < 3 × 10-26 e.cm with 90% confidence

Current upper limits

Page 7: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Left -Right MSSM

f ~ a/p

Multi Higgs

MSSM f ~ 1

10-24

10-22

10-26

10-28

10-30

10-32

10-34

10-36

eEDM (e.cm)

Imperial eEDM starting to explore

this region

Standard Model

de < 1.0 x 10-27 e.cm

Imperial eEDM (2011)Excluded region

e.g. Pospelov and RitzarXiv:hep-ph/0504231(2005)

Page 8: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

Constraints on SUSY parameters

Pospelov & Ritz, hep-ph/0504231

MSUSY = 500 GeVtan b = 3

e

Page 9: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

SUSY again Lebedev et al., hep-ph/0402023

n

Tl YbF (2011)n (2006)

Page 10: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Where do we go from here?nEDM Better polarisation

Higher E field Longer spin coherence time More neutrons

10 x betterCryoEDM

eEDM Better field control Longer spin coherence time More YbF molecules

10 x betterCryoYbF

Page 11: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Cryogenic YbF experiment (Imperial)

YbF beam

YAGablationlaser3K He gas cell

Yb+AlF3target

New J. Phys. 11 123026 (2009) Physical Review A (2011)S. M. Skoff et al.

Uses new molecular beam source

Page 12: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

eEDM prospects with new source15 more molecules

3 longer interaction time

=> access to few x 10-29 e.cm range

=> 10 better signal:noise ratiowill improve systematics as well as statistics

Page 13: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

+-+-

+-

+-

+-

garnet

E+-

squid magnetometer

GGG (LANL), GIG (Amherst)Gadolinium Garnets

Huge number of electrons

Other electron EDM searches+-

+-

+-

+-

+- E+-

Cs atomsFountain (LBL), Trapped (Penn State), Trapped (Texas) Long coherence time

Molecules Large effective E field

PbF beam (Oklahoma) similar to YbFMetastable ThO beam (Yale/Harvard) similar to YbF

Trapped HfF+ ions (JILA) 1 molecule; very long coh.time

none competitive with YbF in the immediate future

Page 14: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

Cryogenic nEDM experiment

• Neutrons produced, transported, & stored. Need lower losses.

• 10 kV/cm applied; aiming for 20-30 kV/cm

• Polarisation observed, but must improve

• Detector efficiency set to improve significantly

• Magnetic field stability to be improved by factor 1000

Sussex, RAL, Oxford, ILL,Kure

Page 15: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

Other nEDM experiments PSI (50 people) aim 5 10-27 by 2015 ORNL (90 people) construction 2017;

aims eventually for 5 10-28

e.cm

ILL: Russian group. Reinstating system from 1990 measurement. Perhaps 1 10-26 e.cm eventually.

FRM, Munich: hoping to install UCN source. Nothing firm yet

Masuda, Japan: observed resonance, but very low stats. Move to TRIUMF?

Page 16: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

P. HarrisIoP 2011

... and other particles Muon EDM: from g-2

(7E-19 e.cm; proposed upgrades could reach ~10-24 e.cm by ~2020)

Deuterium EDM: similarprinciple (claimed potential reach ~10-29 e.cm)

Tau weak dipole moment – look for CP-odd observables in diff. x-sec at Z res.(6E-18 e.cm from LEP data)Sensitivity to physics BSM depends on source of CPv

Page 17: Electric dipole moment searches E.A. Hinds Birmingham 11 th July 2011 Centre for Cold Matter Imperial College London.

Conclusions

These place strong constraints onCP-violation beyond std model

de < 1 × 10-27

e.cm dn < 3 × 10-26

e.cm

Current upper limits

UK leads the world in both

Will continue to do so if projects funded.


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