spin – physics, edm searches in storage rings
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SPIN – Physics, EDM searches in Storage Rings. August 14, 2012 Frank Rathmann 5 th GEORGIAN - GERMAN SCHOOL AND WORKSHOP IN BASIC SCIENCE. Topics. Introduction Search for Electric Dipole Moments - PowerPoint PPT PresentationTRANSCRIPT
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SPIN – Physics,EDM searches in Storage Rings
August 14, 2012 Frank Rathmann
5th GEORGIAN - GERMAN SCHOOL AND WORKSHOP IN BASIC SCIENCE
2
Topics
Introduction Search for Electric Dipole Moments Spin coherence time First direct measurement
Resonance Method with RF E(B)-fields Conclusion
SPIN – Physics, EDM searches in Storage [email protected]
SPIN – Physics, EDM searches in Storage Rings 4
Introduction: Four interactions (forces)
interaction couples to mediators(bosons) strength
strong color gluon 1038
electromagnetic electric charge photon 1036
weak weak charge W und Z 1025
gravitational mass graviton (?) 1
Matter consists of fermions, they attract or repel each other by exchanging bosons.
SPIN – Physics, EDM searches in Storage Rings 5
Introduction: Standard model of elementary particles
Fermions Bosons
• All particles (and their corresponding anti-particles) feature
1. mass2. charge, and3. spin
The spin vector of a particle is associated with a magnetic moment,
SPIN – Physics, EDM searches in Storage Rings 6
Burning questions http://particleadventure.org/beyond_start.html
• Why do we observe matter and almost no antimatter if we believe there is a symmetry between the two in the universe?
• What is this "dark matter" that we can't see that has visible gravitational effects in the cosmos?
• Why can't the Standard Model predict a particle's mass?• Are quarks and leptons actually fundamental, or made up
of even more fundamental particles? • Why are there exactly three generations of quarks and
leptons? How does gravity fit into all of this?
SPIN – Physics, EDM searches in Storage Rings 7
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?
SPIN – Physics, EDM searches in Storage Rings 8
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.
What caused the Baryon asymmetry?
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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
Carina Nebula: Largest-seen star-birth regions in the galaxy
Observed 610-10 WMAP+COBE (2003)
SM expectation ~10-18
nnn BB /)(
SPIN – Physics, EDM searches in Storage Rings 10
Dipole moments
Magnetic dipole moment
Electric dipole moment
Two electric charges separated by a distance
+𝑞−𝑞 𝑙
Two magnetic charges separated by a distance
SPIN – Physics, EDM searches in Storage Rings 11
Particles might have, besides mass, charge, and spin (magnetic moment ), an Electric Dipole Moment ?
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!
13
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 one order higher sensitivity.
In particular the deuteron 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
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 DOEGoal for protons
Technological challenges !
Carry out proof of principle experiments (demonstrators) at COSY
• Spin coherence time • Beam positioning • Continuous polarimetry • E - field gradients
Circumference
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BNL Proposal
year)(onecme105.2 29 pd
SPIN – Physics, EDM searches in Storage Rings 21
Magnetic moment, spin, g and G
𝜇𝑁=𝑒 ∙ h
2 ∙𝑚𝑝=5.05078324 J T −1
The nuclear magneton
particle spin charge proton
deuteron3He
𝜇=𝑔 ∙𝜇𝑁 ∙𝑚𝑝
𝑚 ∙𝑍 ∙𝑠
The 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)
Magic condition: Protons
Case 1: field only
23SPIN – Physics, EDM searches in Storage [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
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particleproton
deuteron
Parameters for Richard Talmans all-in-one machine
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”COn
s2AS
ring
makes one turn
stable polarizationS
if ║ COn
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Spin closed orbit
Spin coherence
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We usually don‘t worry about coherence of spins along COn
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
COn
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!
COn
In an EDM machine with frozen spin, observation time is limited.
Estimate of spin coherence times (N.N. 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., electron 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 ∙103 s 𝜏𝑠𝑐 (𝑑)≈5 ∙105 s
𝐺𝑝=1.79 𝐺𝑑=−0.14
First measurement of spin coherence time
Polarimetry:
Spin coherence time:
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from Ed Stephensonand Greta Guidoboni
decoherencetime
oscillationcapture
5 s 25 s 5 s
2011 Test measurements at COSY
Topics
Why EDMs? Search for EDMs using storage rings Two projects, at BNL and Jülich Spin coherence time First direct measurement
Resonance Method with RF E(B) –fields Polarimetry Summary
34SPIN – Physics, EDM searches in Storage [email protected]
[email protected] SPIN – Physics, EDM searches in Storage Rings 35
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
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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
Transverse 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
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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 K. 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
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
EDM effect accumulates in
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 eam1 ��=(𝑃 𝑥𝑃 𝑦𝑃 𝑧 )t arget (¿beam2)��=(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
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 could be tuned 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 𝑥𝑃 𝑦𝑃 𝑧) probingbeam ��=(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 IP should be rather small.• Advantage over suggestion 2. is that supports luminosity.• Disadvantage is that sensitivity comes mainly from terms with and .• Detailed estimates necessary.
𝜎𝜎0
=1+𝐴𝑦 [ (𝑃 𝑦+𝑄𝑦 ) cos𝜑− (𝑃 𝑥+𝑄𝑥 ) sin 𝜑 ]
cw beam𝑃=(𝑃𝑥𝑃𝑦𝑃𝑧 ) ccw beam��=(𝑄𝑥
𝑄𝑦𝑄𝑧
)
Luminosity estimate for the collider option
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𝐿(𝑇 , 𝛽 )=𝑁1𝑁2 𝑓 rev(𝑇 )𝑛𝑏
4𝜋 𝜎 (𝛽)2
𝜎 (𝛽)=√𝜖 ∙ 𝛽
Conditions:
k inetic energy(MeV )
Luminos
ity𝛽=10 m
𝛽=1m
𝛽=0.1m
T magic=232.8 MeV
Even under these very optimistic assumptions, event rate will be rather low.
Stepwise approach in the JEDI project
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
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, …
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EDM Workshop at ECT* (Trento)
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October 1-5, 2012
Organizing committee
Jülich Hans Ströher [email protected] Rathmann [email protected] Wirzba [email protected]
BrookhavenMei Bai [email protected] Marciano [email protected] Semertzidis [email protected]
http://www.ectstar.eu/
• Measurements of EDMs are extremely difficult, but the physics is fantastic!
• Two storage ring projects, at BNL and 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
• Polarimeter concepts to be addressed by simulations
• JEDI collaboration established
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Summary
SPIN – Physics, EDM searches in Storage Rings 53
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”