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Fundamental InteractionsPhysics & Instrumentation
Conclusions
Conveners:
P. Mueller, J. ClarkG. Savard, N. Scielzo
2
Short Term
Fully utilize low energy beams from CARIBU for mass measurements, laser spectroscopic studies and decay experiments. Ideally, the space available for low energy experiments at CARIBU should be expanded to fully exploit these possibilities (NA6).
3
Initial focus of measurements with the CPT at CARIBU
First measurements:
• 132Sn and neighbors
• 130Cd and neighbors
Future measurements:
• go as neutron-rich as possible
4
Moving the CPT to CARIBU
CARIBU
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Laser Lab Layout @ CARIBU
AC
H
EP
A
Laser Enclosure(~ 6’ x 10’)
Laser Table(~ 3’ x 7’)
Ion Trap
Collinear Beamline
Tape Station
Cf-252 source80 mCi -> 1Ci
High-resolutionmass separatorm/m > 1/20000
Gas catcher
RF Cooler & Buncher
… starting in fall 2010
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Beta-delayed neutron emission
Plastic scintillator
Plastic
scintillator
n
94Sr
95Rb+
95Rb 95Sr* 94Sr* n
• 1-mm3 trapped-ion sample and 1-ns timing resolution of detectors determines neutron momentum/energy to ~1% from time-of-flight of recoiling daughter ion
• intrinsic efficiency for MCP detectors can be ~100%
• many fission fragments available from the newly-developed CARIBU facility (an intense source of fission-fragment beams) at ANL
Novel approach: determine neutron energies and branching ratios by detecting beta particles and recoil ions that emerge from ion trapProvide reliable data for: r-process nucleosynthesis, nuclear structure, nuclear reactor performance, modeling of environments where fission fragments are produced
MCP ion detector
ExampleQ = 4.9 MeVt1/2 = 0.378 secPn ≈ 9%
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Short Term
Utilize ATLAS intensity upgrade (Phase I) for improved beta decay correlation experiments and weak interaction studies by increased production rate of light isotopes close to stability (e.g. 6He, 8Li, 14O, 18Ne ) (FI4). Phase II upgrade, in particular the recoil separator, would significantly improve production and separation of these isotopes.
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Beta-neutrino correlation in 8Li
DSSD Plastic scintillator
8Li+
8Li 8Be*
Neutrino momentum/energy can be determined from and recoiling 8Be momentum/energy
momentum/energy measured from DSSD and plastic scintillator detector
8Be momentum/energy determined from particle break-up… with no recoil, particles would have same energy and would be back-to-back. With recoil, energy difference can be up to 730 keV and the angle can deviate by as much as ±70
Low mass of 8Li and Q ≈ 13 MeV lead to large recoil energies of 12 keV which makes the correlation easier to measure. Other correlation measurements have had to deal with recoil energies of only 0.2-1.4 keV.
Beta-neutrino correlation measurement takes advantage of 1 mm3 trapped ion sample and position and energy resolution of double-sided silicon strip detectors to precisely reconstruct momentum vectors of all emitted particles (including neutrino!)
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MCPDSSD+ Scint.
MOTchamber
Atomtraps
Dipole traplaser
Atomic beam
Beta-Decay Study with Laser Trapped 6He
• 6He trapping rate: 1104 s-1,
• 2105 coincidence events in 15 min: a = ± 0.008
• 1 week: a/a = 0.1%
Cou
nts
500450400350300250200150Time of Flight (ns)
a = +1/3
a = -1/3
Simulated time-of-flight signal
Standard Model
New Physics
6He yields:• ATLAS: 1107 s-1
• CENPA: ~1109 s-1
• SARAF / SPIRAL2: ~11012 s-1
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Medium Term
Improve isotope separation and overall transmission of the ion transfer line after the gas catcher into the triangle room. This would enable mass measurements closer to the proton drip line (65As) once the CPT is moved back to its previous location (NA2). This upgrade also would improve correlation studies and decay experiments possible at that location (FI4).
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Moving the CPT to CARIBU
CARIBU
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Long Term
Add gas catcher and low-energy beam-line behind recoil separator for studies of very proton rich isotopes (e.g. around 100Sn, requires Phase II). Provide experimental area to accommodate low-energy beam experiments, e.g., in the ATSCAT area.
Support high precision measurements of basic nuclear properties of isotopes close to stability (on the proton rich side) to enable future high precision measurement far off stability at FRIB, e.g., measurements of T=2 superallowed beta decays.
13
Moving the CPT to CARIBU
CARIBU
RecoilSeparator
14
T=2 nuclei present an alternative way to check
Isospin breaking corrections
Bhattacharya et al., PRC 77, 065503 (2008)
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Long Term
Find a stronger source for 225Ra for improved EDM experiment that will be truly statistics limited (FI9).
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Search for EDM of 225Ra
Transversecooling
Oven:225Ra (+Ba)
Zeeman Slower
Opticaldipole trap
EDMprobe
Advantages:
•Large enhancement:
EDM(Ra) / EDM(Hg) ~ 200 – 2000
•Efficient use of 225Ra atoms
•High electric field (> 100 kV/cm)
•Long coherence times (~ 100 s)
•Negligible “v x E” systematic effect