Title: The Experimental Program
1The ???Experimental Program
2An exciting experimental program
- Experimental techniques
- General requirements
- Discovery vs. measurement
- Required number of measurements and their
precision - If we see ??, the qualitative physics results are
profound, but next well want to quantify the
underlying physics.
3Past Results
Elliott Vogel Annu. Rev. Part. Sci. 2002 52115
4A Recent Claimhas become a litmus test for
future efforts
??? is the search for a very rare peak on a
continuum of background. 70 kg-years of
data 13 years The feature at 2039 keV is
arguably present.
NIM A522, 371 (2004)
5Future Data Requirements
- Why wasnt this claim sufficient to avoid
controversy? - Low statistics of claimed signal - hard to repeat
measurement - Background model uncertainty
- Unidentified lines
- Insufficient auxiliary handles
- Result needs confirmation or repudiation
6Various Levels of Confidence
- A preponderance of the evidence a combination of
- Correct peak energy
- Single-site energy deposit
- Proper detector distributions (spatial, temporal)
- Rate scales with isotope fraction
- Open and shut case include the following
- Observe the two-electron nature of the event
- Measure kinematic dist. (energy sharing, opening
angle) - Observe the daughter
- Observe the excited state decay
- Beyond a reasonable doubt the smoking gun
- See the process in several isotopes
7Discovery vs. Measurementa future decision point
These two goals may require different technical
approaches.
As yet, there is no viable proposal for an
experiment sensitive to the solar scale.
8Solar Scale showstoppers
- Need 100 tons of isotope
- Enrichment costs and production rates are not
sufficient yet - Will need RD to improve capability
- Need excellent energy resolution
- Better than 1 FWHM
- Perhaps an experiment with 106 solid state
detectors is possible - Cost/detector will need to be greatly reduced
- Large multi-element detector electronics are
improving - Metal loaded liquid scintillator or Xe techniques
scale more easily and cost effectively, but
resolution requires RD
9Need several, precise experiments
- Values of the double beta decay rate from several
nuclei will help untangle the underlying physics - 3-4 experiments
- Several values are only useful, if the
measurements are precise - 10-20 uncertainty
- Different techniques are also required
- No one technique can provide all the
characteristics of a perfect experiment
10Our White Paper
- Science (draft could be written beforehand) 1-2
pages - Priority for first suite of experiments 1/2 page
- science goals, not specific experiment technology
- Proof-of-principle RD vs. ready-to-go
technologies - Roadmap (rough order of magnitude of cost time
frame) 1 page - A rough guess as to the cost and schedule of any
first-suite experimental program. - RD needs 1/2 page
- An estimate of the cost to determine
engineering/costing/scheduling for the initial
suite of experiments proposed for DUSEL itself in
time for the MRE-FC submission in addition, we
also need to know ongoing proof-of-principle RD
costs. - How to arrive at realistic cost and schedules 1/2
page - If an experiment (or goal) clearly can not make
the MRE-FC timescale, we should indicate so. - Education and Outreach 1/2 page
- What is our subfields opportunities
11Our Plan
- Hear from the community about various ideas for
double beta decay - Discuss these proposals in context of our white
paper - Begin work on the white paper in public to
maximize community input - Hopefully well have at least a good outline by
days end
12Underlying ??(0?) Mechanisms
- There are many physics models that lead to Lepton
Number Violation (?), M can change with the
model - Light neutrino exchange
- Heavy neutrino exchange
- R-parity violating supersymmetry
- RHC
- etc.
13SignalBackground 11Its all about the
background
Degenerate
To reach atmospheric scale need BG on order 1/t-y.
Atmospheric
Solar
14KKDC Claim
50 meV Or 1027 yr
Atmospheric Scale
Inverted
Solar Scale
Normal
15An Ideal ExperimentMaximize Rate/Minimize
Background
- Large Mass ( 1 ton)
- Large Q value, fast bb(0n)
- Good source radiopurity
- Demonstrated technology
- Ease of operation
- Natural isotope
- Small volume, source detector
- Good energy resolution
- Slow bb(2n) rate
- Identify daughter in real time
- Event reconstruction
- Nuclear theory
16Great Number of Proposed Experiments
- Calorimeter
- Semi-conductors
- Bolometers
- Crystals/nanoparticles immersed in scintillator
- Tracking
- Liquid or gas TPCs
- Thin source with wire chamber or scintillator