Search for an Electric Dipole Moment of 199 Hg
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Transcript of Search for an Electric Dipole Moment of 199 Hg
Search for an Electric Dipole Moment of 199Hg
Blayne HeckelUniversity of Washington
Graduate students: Jennie Chen, Brent GranerScientific glassblower: Erik Lindahl
Support: NSF and DOE Low Energy Nuclear Physics
History of 199Hg EDM results
20142001 20091993 1995
Current sensitivity
LamoreauxJacobsKlipsteinFortson Griffith
SwallowsRomalisLoftusFortson
1.00E-30
1.00E-29
1.00E-28
1.00E-27
1.00E-26
1.00E-25
2 s
igm
a u
pp
er
lim
it
1987
wOT
wOB
BE
wMT
wMB
E Cancels up to 2nd order gradient noise
4-Cell, 199Hg Magnetometer
omc 3
1
dE
zz
Bc
4)
3
8( 3
3
3
EDM insensitive channels: ωOT - ωOB and (ωOT + ωOB) – (ωMT + ωMB) monitor for E field correlations odd and even in z, respectively.
EDM sensitive frequency combination
Improvements to the EDM Experiment
Vapor Cell development: Stable spin lifetimes of 800, 600, 500, and 270 secProblem of disappearance of Hg within the cells solved
Reduced magnetic field noise – less conducting materials near the cells
Light induced noise and systematic effects eliminated by precession in the dark
Reduced high voltage leakage currents:Measure separately the currents across the cell and to the ground plane
Commercial uv laser provides better stability
We are working on improving the beam pointing stability
Precession in the dark
Optical rotation angle of 240
Advantages: Longer spin coherence times Light induced noise and systematic errors eliminated Insensitive to common mode B field drift
A B
Frequency difference extractionBecause we are only interested in cell pair frequency differences during the light-off period, we need only the phase difference between cells at the end of the A period and start of the B period:
ABDark TT
AB
)()(
We find Δω by multiplying the signals from the 2 cells.
andtAetSFrom nt
nn )sin()( /
/2222 )2/()2/()()( ntnnnn eAtStStStN
andttNtStSgetwe nnnn )sin()(/)()( �
)cos(2/)]2/()2/([)( nnnn ttStStC���
)sin()()()()( nnMB
nMT
nMB
nMT ttStCtCtSFinally
����
ΔωMT-MB (mrad)
Photo-Diode (V)
2
4
6
8
10
Time (s)50 100 150 200 250
1.5
1.0
0.5
0
2.0
TA TB
ABDark TT
AB
)()(
Filtered Data
System Performance
Rad
/s
Run Number
Average angular frequency relative to first scan
This corresponds to a drift of ~1 µGauss/day
Rad
/sR
ad/s
Δω (MT-MB) Middle cell angular frequency difference
Δω (OT-OB) Outer cell angular frequency difference
0.3 nG/day
Rad
/sR
ad/s
Δω (OT-MT) + Δω (OB-MB) Quadratic field drift channel
ΔωC EDM sensitive frequency combination
80 pG/day
Rad
/s
ωedm(n) = (-1)n [ΔωC(n-1) - 2 ΔωC(n) + ΔωC(n+1)]/4
One day EDM signal
ωedm = xx ± 2.0 × 10-9 rad/s, a factor of 4 improvement over 2009
(3.5 × 10-29 e-cm/day for 10kV runs)
Data Sequences
EDM data is taken in ``sequences’’. Each sequence comprises:
• A defined set of cell orientations and ordering in the vessel• Equal number of day long runs at 6kV and 10kV• Equal number of runs with normal and reversed magnetic fields• Equal number of runs with fast and slow high voltage ramp rates• Typically 16 -20 runs total
We have completed 7 data sequences and have 5 to go for a complete EDM data set.
For seq. 1-6: at 10kV, dHg = -(13.4 ± 5.6) × 10-30 e-cm at 6kV, dHg = -(15.6 ± 9.3) × 10-30 e-cm
combined, dHg = -(14.0 ± 4.8) × 10-30 e-cm
(blind offset in place)
-25
-20
-15
-10
-5
0
5
10
15
20
EDM data by Sequence
Seq.3Seq.2 Seq.4 Seq.5 Seq.6Seq.1
10 kV χ2 = 1.22
ωc
× 1
0-10
rad/
s
-25
-20
-15
-10
-5
0
5
10
15
6 kV χ2 = 0.98
ω c
× 1
0-10
rad/
s
Seq.3Seq.2 Seq.4 Seq.5 Seq.6Seq.1
B field up
B field down
χ2
Systematic Uncertainties
2009 Error Budget
X (no sparks observed) X (precession in the dark)
-- Scale with frequency precision
IGas= 0.4 pA (2009)
ICell = 0.08 pA (2009)
10 kV
0 Volts
Leakage Currents
We now measure separately the currents flowing down the cell walls and through the dry air.
2014: With tin oxide coated ground planes (rather than gold), we see 10 times less leakage current -- no photo-electrons:Igas = 0.04 pA (2014), Icell = ?
Issues to address
• Better understanding of the long time constants associated with the leakage currents
• Identification of the dominant source of excess noise(simulated data with Gaussian photon shot noise added results in 40% smaller EDM values)
• Identification of the source for occasional runs with 2-3 sigmacorrelations between the outer cell frequency difference and high voltage
Summary
• We anticipate a 199Hg EDM result with a factor of roughly 4 improvement in statistical precision by the end of 2014.
• The data, so far, looks reasonable but there remains work to do concerning systematic errors.
• We are constructing shorter vapor cells to allow us to increase the applied electric field in our current EDM apparatus.
Transverse Pumping / Optical Rotation
B
254 nm s+
Pump Phase
B
254 nm Linear
Probe Phase wL
Linear Polarizer
Detector
Systematic Errors and Tests for Systematic Effects
No Statistically Significant Dependence on:• The Vapor Cells or Electrodes (or their orientation)• The DAQ Channel Ordering• The Vessels
99% of Total Error
Systematic Error Budget
Statistical Error 12.90
Bounds on CP Violating Parameters
d(199Hg) = (0.49 ± 1.29stat ± 0.76sys ) x 10-29 e cm
| d(199Hg) | < 3.1 x 10-29 e cm (95% CL)
Confidence Levels: 199Hg (95%), 205TI (90%), TIF (95%)
Quark Chromo EDMs
Proton EDM
Semi-Leptonic Interactions:
QCD Phase
Neutron EDM
Electron EDM
Current Status
• More uniform and stable magnetic field• Detection of both polarization states of transmitted light• ``In the Dark’’ elimination of uv light induced noise and systematic error
Six-fold Reduction of Noise
``In the Dark’’ Old Analysis
Current Status
Improved Hg Vapor Cells: so far, natural Hg test cells
• Hydroxy bonded rather than glued – should last forever• 600 sec spin lifetime (distilled wax + smaller magnetic field gradients)
Remaining Tasks: • Construct enriched Hg vapor cells• Acquire a new uv laser source
Summary
Our 2009 Result led to a New Limit on the EDM of 199Hg
| d(199Hg) | < 3.1 x 10-29 e cm (95% CL)
• Factor of 7 Reduction in Previous Upper Limit• Improved Bounds on CP Violating Parameters
• Expect Factor of 5 improvement in Experimental Sensitivity• Expect to begin data collection later this year
Upgrading the Current Apparatus
Among his many accomplishments, Norman Ramsey founded the research field of EDM measurements and developed many of the techniques needed to do such precise measurements. He will always be an inspiration to us.
Reasons to Expect more T (CP) Violation
• The observed matter-antimatter asymmetry: CP violation in the SM is too small to
account for Baryogenesis.• The Strong CP problem:
Why is QCD so small?• The Standard Model is incomplete:
Extensions to the SM, such as SUSY, introduce new phases that lead to new sources of CP violation often
106 times larger than the SM for EDMs.
From the 199Hg EDM to Models for CP Violation
199Hg Atomic EDM
Atomic Physics
199Hg Schiff Moment
Nuclear Physics
CP-Violating Pion-Nucleon Coupling
QCD
CP-Violating QCD Term, Quark Chromo-EDMs
Model-Dependent CP-Violating Parameters
SUSY, etc …
Contributions to S from p, n EDMs
d(n)d(p)
Hyperfine Coupling: d(e)
Semileptonic Interactions: CS CP CT
Naturalness Parameters