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Direct EDM search for charged hadrons at COSY
October 2, 2012 Frank Rathmann(on behalf of the BNL-EDM and JEDI collaborations)
EDM searches in Storage rings, ECT*, Trento, Italy
2
Topics
Introduction Search for Electric Dipole Moments Spin coherence time First direct measurement
Resonance Method with RF E(B)-fields Polarimetry Conclusion
Direct EDM search for charged hadrons at COSY [email protected]
Direct EDM search for charged hadrons at COSY 3
What caused the Baryon asymmetry?
Carina Nebula: Largest-seen star-birth regions in the galaxy
Observed 610-10 WMAP+COBE (2003)
SM expectation ~10-18
nnn BB /)(
What happened to the antimatter?
Sakharov (1967): Three conditions for baryogenesis
1. B number conservation violated sufficiently strongly2. C and CP violated, B and anti-Bs with different rates3. Evolution of universe outside thermal equilibrium
Permanent EDMs violate parity P and time reversal symmetry TAssuming CPT to hold,
combined symmetry CP violated as well.
Electric Dipole Moments (EDMs)
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EDMs are candidates to solve mystery of matter-antimatter asymmetry may explain why we are here!
5
History of neutron EDM limits
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Adopted from K. Kirch
• Smith, Purcell, Ramsey PR 108, 120 (1957)
• RAL-Sussex-ILL(dn 2.9 10-26 ecm) PRL 97,131801 (2006)
Sensitivity to NEW PHYSICS beyond the Standard Model
EDM searches - only upper limits (in )up to now:
Huge efforts underway to improve limits / find EDMs
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Limits for Electric Dipole Moments
Particle/Atom Current EDM Limit Future Goal equivalent
Neutron
Proton
Deuteron ?
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Why also EDMs of protons and deuterons?
Proton and deuteron EDM experiments may provide higher sensitivity.
In particular deuterons may provide a much higher sensitivity than protons.
Consensus in the theoretical community:Essential to perform EDM measurements on different targets with similar sensitivity:
• unfold the underlying physics,• explain the baryogenesis.
NEW: EDM search in time development of spin in a storage ring:
“Freeze“ horizontal spin precession; watchfor development of a vertical component !
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Search for Electric Dipole Moments
0G
Edts
dd
Frozen spin Method
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For transverse electric and magnetic fields in a ring ( ),anomalous spin precession is described by
0 EB
cE
pmGBG
mq
G
2
Magic condition: Spin along momentum vector
1. For any sign of , in a combined electric and magnetic machine
2. For (protons) in an all electric ring
2
2gG
222
2
1
GBc
GGBcE
x
Gmp
pmG
0
2
cMeV74.700 (magic)
NEW: EDM search in time development of spin in a storage ring:
A magic storage ring for protons (electrostatic), deuterons, …
“Freeze“ horizontal spin precession; watchfor development of a vertical component !
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Search for Electric Dipole Moments
particleproton
deuteronOne machine
with m
0G
Edts
dd
Two storage ring projects being pursued
(from R. Talman) (from A. Lehrach)
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BNL for protons all electric machine Jülich, focus on deuterons, or a combined machine
CW and CCW propagating beams
Most recent: Richard Talmans concept for a Jülich all-in-one machine
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Iron-free, current-only, magnetic bending, eliminates hysteresis
A
B
A B
2 beams simultaneously rotating in an all electric ring (cw, ccw)
Approved BNL-ProposalSubmitted to DOE 11/2012Goal for protons
Technological challenges !
Carry out proof of principle (demonstrator) experiments at COSY
• Spin coherence time • Beam positioning • Continuous polarimetry • E - field gradients
Circumference
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BNL Proposal
year)(onecme105.2 29 pd
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particleproton
deuteron
Parameters for Jülich all-in-one machine (R. Talmans concept )
𝒓=𝟏𝟎𝐦
• Fitting such a machine into the COSY building favors lower momenta.
Talman/Gebel give maximum achievable field of copper
magnets of ~ 0.15 T.
EDM at COSY – COoler SYnchrotron
Cooler and storage ring for (polarized) protons and deuterons
Phase space cooled internal & extracted beams
Injector cyclotron
COSY
… the spin-physics machinefor hadron physics
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EDM at COSY – COoler SYnchrotron
Injector cyclotron
COSY
… an ideal starting pointfor a srEDM search
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Cooler and storage ring for (polarized) protons and deuterons
Phase space cooled internal & extracted beams
AAS
one particle with magnetic moment
“spin tune”
“spin closed orbit vector”COn̂
s2AS
ring
makes one turn
stable polarizationS
if ║ COn̂
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Spin closed orbit
Spin coherence
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We usually don‘t worry about coherence of spins along COn̂
At injection all spin vectors aligned (coherent)
After some time, spin vectors get out of phase and fully populate the cone
Polarization not affected!
Situation very different, when you deal with S
COn̂
At injection all spin vectors aligned After some time, the spin vectors are all out of phase and in the horizontal plane
Longitudinal polarization vanishes!
COn̂
In an EDM machine with frozen spin, observation time is limited.
Crucial for srEDM searches is understanding and improving spin coherence times
Estimate of spin coherence times (Kolya Nikolaev)
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One source of spin coherence are random variations of the spin tune due to the momentum spread in the beam
and is randomized by e.g., phase space cooling
Estimate:
Spin coherence time for deuterons may be larger than for protons
𝛿𝜃=𝐺𝛿𝛾 𝛿𝛾
cos𝜔𝑡→cos (𝜔𝑡+𝛿𝜃 )
𝜏𝑠𝑐 ≈1
𝑓 rev𝐺2 ⟨𝛿𝛾 2 ⟩
≈ 1𝑓 rev𝐺
2𝛾2 𝛽4 ⟨ 𝛿𝑝𝑝2⟩
− 1
𝑇 kin=100 MeV 𝑓 rev=0.5 MHz
𝝉𝒔𝒄 (𝒑)≈𝟑 ∙𝟏𝟎𝟑𝐬 𝝉𝒔𝒄 (𝒅)≈𝟓 ∙𝟏𝟎𝟓𝐬𝑮𝒑=𝟏 .𝟕𝟗 𝑮𝒅=−𝟎 .𝟏𝟒 More details in
Kolya Nikolaev‘s talk
First measurement of spin coherence time
Polarimetry:
Spin coherence time:
[email protected] 20Direct EDM search for charged hadrons at COSY
from Ed Stephensonand Greta Guidoboni
decoherencetime
oscillationcapture
5 s 25 s 5 s
2011 Test measurements at COSY
21
Topics
Introduction Search for Electric Dipole Moments Spin coherence time First direct measurement
Resonance Method with RF E(B)-fields Polarimetry Conclusion
Direct EDM search for charged hadrons at COSY [email protected]
[email protected] Direct EDM search for charged hadrons at COSY 22
Resonance Method with „magic“ RF Wien filter
Avoids coherent betatron oscillations of beam. Radial RF-E and vertical RF-B fields to observe spin rotation due to EDMApproach pursued for a first direct measurement at COSY.
„Magic RF Wien Filter“ no Lorentz force
Statistical sensitivity for in the range to range possible.• Alignment and field stability of ring magnets• Imperfection of RF-E(B) flipper
Indirect EDM effect
Tilt of precession plane due to EDM
Observable:Accumulation of vertical polarization during spin coherence timePolarimeter (dp elastic)
stored d
RF E(B)-field In-plane polarization
Operation of „magic“ RF Wien filter
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Radial E and vertical B fields oscillate, e.g., with (here ).
Spin coherence time may depend on excitation and on chosen harmonics
beam energy
see Kolya Nikolaev‘s talk
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Simulation of resonance Method with „magic“ Wien filter for deuterons at COSYParameters: beam energy
assumed EDME-field
Linear extrapolation of for a time period of
EDM effect accumulates in .
𝜔=2𝜋 𝑓 𝑟𝑒𝑣𝐺𝛾=−3.402×105 Hz
turn number
𝑃 𝑥 𝑃 𝑧 𝑃 𝑦
Preliminary, based on Kolya Nikolaevs derivation of the combined rotation matrices of E/B flipper and ring
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Simulation of resonance Method with „magic“ Wien filter for deuterons at COSY
Linear extrapolation of for a time period of .
Parameters: beam energy assumed EDME-field
EDM effect accumulates in
𝑃 𝑦
turn number
𝑃 𝑦
EDM effect accumulates in
Simulation of resonance Method with Magic Wien filter for deuterons at COSY
Linear extrapolation of for a time period of .
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Parameters: beam energy assumed EDME-field
𝑃 𝑦
turn number
Some polarimetry issuespC and dC polarimetry is the currently favored approach for the pEDM experiment at BNL
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srEDM experiments use frozen spin mode, i.e., beam mostly polarized along direction of motion,
most promising ring options use cw & ccw beams.
• scattering on C destructive on beam and phase-space,• scattering on C determines polarization of mainly
particles with large betatron amplitudes, and• is not capable to determine . • For elastic scattering longitudinal analyzing powers are tiny (violates parity).
Ideally, use a method that would determine .
Exploit observables that depend on beam and target polarization
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b eam1𝑃=(𝑃 𝑥
𝑃 𝑦𝑃 𝑧
)t arget (¿beam2)𝑄=(𝑄𝑥
𝑄𝑦𝑄𝑧
)
𝜎𝜎0
=1+𝐴𝑦 [ (𝑃 𝑦+𝑄𝑦 ) cos𝜑− (𝑃 𝑥+𝑄𝑥 ) sin 𝜑 ]
Spin-dependent differential cross section for
Analyzing powerSpin correlations
In scattering, necessary observables are well-known in the range MeV (not so for or ).
𝑥 (sideways)
𝑦 (up)
𝑧 (along beam)𝜑
𝜃
(see David Chiladze‘s talk)
How could one do that, determine ?
Suggestion 1: Use a polarized storage cell target
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Detector
• Detector determines of cw & ccw beams separately, based on kinematics.• Alignment of target polarization along axes by magnetic fields. Leads to
unwanted MDM rotations absolute no-go in EDM experiments.
cell
CW CCW
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Suggestion 2: Use colliding beam from external source
• Collide two external beams with cw and ccw stored beams.• Energy tunable to match detector acceptance.• Polarization components of probing low-energy beam can be made large, would
be selected by spin rotators in the transmission lines.• Luminosity estimates necessary.
Detector
Polarized ion source(~10 MeV)
How could one do that, determine ?
𝜎𝜎0
=1+𝐴𝑦 [ (𝑃 𝑦+𝑸𝒚 )cos𝜑− (𝑃𝑥+𝑸 𝒙 ) sin 𝜑 ]
cw beam𝑃=(𝑃 𝑥
𝑃 𝑦𝑃 𝑧) probingbeam𝑄=(𝑄𝑥
𝑄𝑦𝑄𝑧
)=(𝑄𝑥
00 ) ,( 0
𝑄𝑦0 ) ,∨( 0
0𝑄𝑧
)
How could one do that, determine ?
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Suggestion 3: Use directly reactions from colliding beams
Detector
CW CCW
Requires luminosity, -functions at IPs should be rather small.• Advantage over suggestion 2.: supports luminosity.• Disadvantage: Sensitivity mainly from terms with and .• Detailed estimates necessary.
𝜎𝜎0
=1+𝐴𝑦 [ (𝑃 𝑦+𝑄𝑦 ) cos𝜑− (𝑃 𝑥+𝑄𝑥 ) sin 𝜑 ]
cw beam𝑃=(𝑃𝑥
𝑃𝑦𝑃𝑧) ccw beam𝑄=(𝑄𝑥
𝑄𝑦𝑄𝑧
)
Luminosity estimate for the collider option
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𝐿(𝑇 , 𝛽 )=𝑁1𝑁2 𝑓 rev(𝑇 )𝑛𝑏4𝜋 𝜎 (𝛽)2
𝜎 (𝛽)=√𝜖 ∙ 𝛽
Conditions: (, , , )
k inetic energy(MeV )Lu
mino
sity
𝛽=10 m
𝛽=1m
𝛽=0.1m
T magic=232.8 MeV
Even under these optimistic assumptions, event rate might be sufficient.
4 polarimeters allow one to collect interactions from all bunch combinations.
(see David Chiladze‘s talk)
Stepwise approach for all-in-one machine for JEDI
Step Aim / Scientific goal Device / Tool Storage ring
1Spin coherence time studies Horizontal RF-B spin flipper COSY
Systematic error studies Vertical RF-B spin flipper COSY
2COSY upgrade Orbit control, magnets, … COSYFirst direct EDM measurement at RF-E(B) spin flipper Modified
COSY
3 Built dedicated all-in-one ring for p, d, 3He
Common magnetic-electrostatic deflectors
Dedicated ring
4 EDM measurement of p, d, 3He at
Dedicated ring
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Time scale: Steps 1 and 2: < 5 yearsSteps 3 and 4: > 5 years
• Measurements of EDMs are extremely difficult, but the physics is fantastic!
• Two storage ring projects, at BNL and Jülich
• Jülich all-in-one machine with copper-only magnets
• Pursue spin coherence time measurements at COSY
• First direct EDM measurement at COSYResonance Method with RF E(B) -fields
• Optimize beam-beam polarimeter concept
• JEDI collaboration established
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Summary
35
Georg Christoph Lichtenberg (1742-1799)
“Man muß etwas Neues machen, um etwas Neues zu sehen.”“You have to make (create) something new,
if you want to see something new”
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Direct EDM search for charged hadrons at COSY 37
Two years R&D/preparationOne year final ring designTwo years ring/beam-line constructionTwo years installationOne year “string test”
12 13 14 15 16 17 18 19 20 21
Technically driven timeline for all-electric pEDM at BNL
srEDM cooperations
Institutional (MoU) and Personal (Spokespersons …) Cooperation, Coordination
International srEDM Network
srEDM Collaboration (BNL)(spokesperson Yannis Semertzidis)
JEDI Collaboration (FZJ)(spokespersons: A. Lehrach, J. Pretz, F.R.)
Common R&DRHIC EDM-at-COSY
Beam Position Monitors Polarimetry (…) Spin Coherence Time
Cooling Spin Tracking (…)
DOE-Proposal (submitted)
Study Group
First direct measurement Ring Design
JEDI pEDM Ring at BNL
HGF Application(s) CD0, 1, …
[email protected] 38Direct EDM search for charged hadrons at COSY
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Resonance Method with RF E-fields
Polarimeter (dp elastic)
stored d
RF E-fieldvertical
polarization
spin precession governed by: (* rest frame)
Two situations:
1. EDM effect2. no EDM effect
This way, the EDM signal is accumulated during the cycle. • Statistical improvement over single turn effect is about: . • Brings us in the range for .
5101/1000 ss
• But: Flipping fields will lead to coherent betatron oscillations, with hard to handle systematics.
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Simulation of resonance Method with RF E-fields for deuterons at COSY
Parameters: beam energy assumed EDME-field
Constant E-field
Number of turns
E-field reversed every
Number of turns
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Simulation of resonance Method with RF E-fields for deuterons at COSY
Parameters: beam energyassumed EDME-field
Linear extrapolation of for a time period of
Number of turns
EDM effect accumulates
Polarimeter determines
22zx PPP
Direct EDM search for charged hadrons at COSY 42
Symmetries
Parity:
𝑷 :(𝒙𝒚𝒛 )→(− 𝒙−𝒚− 𝒛 )
C-parity (or Charge parity): Changes sign of all quantized charges• electrical charge,• baryon number,• lepton number,• flavor charges, • Isospin (3rd-component)
T-Symmetry: 𝑻 :𝒕→− 𝒕
Physical laws are invariant under certain transformations.
Magic condition: Protons
Case 1: field only
43Direct EDM search for charged hadrons at COSY [email protected]
5 10 15 20 25 30 350
20
40
60
80
100Proton EDM
E-field (MV/m)
radi
us (m
)
r1 E( )
E
r2 250 md 0.48 Gd Zd 8.44
r2 280 m3He 0.0575 G3He Z3He 21.959
𝐸=17 MV /m
𝑟=24.665m
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Magic condition: Protons
Case 2: and fields
magic energy
𝐵>0 𝐵<0magic energy
𝐵>0 𝐵<0
Magic condition: Deuterons
and fields
45Direct EDM search for charged hadrons at COSY [email protected]
Magic condition: Helions
46Direct EDM search for charged hadrons at COSY [email protected]
and fields
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