Title: Neutrino Factory Activities Glasgow
1Neutrino Factory Activities Glasgow
PPE-PPT meeting 29 April 2008 Paul Soler
2Neutrino mixing
- Weak eigenstates do not have to coincide with
mass eigenstates
- Neutrino mixing matrix (Pontecorvo-Maki-Nakagawa-S
akata, PMNS matrix) - similar to CKM matrix of quark sector.
3Neutrino oscillations
- Matter oscillation results for three neutrinos
(MSW effect)
Minakata Nunokawa JHEP 2001
4Neutrino oscillations
- Matter oscillation results for three neutrinos
Only one term in equation
(MSW effect)
Magic baseline
Clean determination of q13
5Degeneracies
Two expts., diff. L/E n and anti-n
One expt., n and anti-n
One expt, only n
Golden ne-gtnm and Silver ne-gtnt channels
6Degeneracies
- Eightfold degeneracy
- The sign of the atmospheric mass difference
- The octant of the atmospheric angle
Strategies different experiments to resolve
degeneracy problem
7Unknown parameters
- Global fit to all neutrino oscillation
experiments give q23, q12, Dm122 and Dm232 - q13, sign of Dm132 (mass hierarchy) and CP
violation phase d not known. -
8Neutrino Factory
- Baseline for a Neutrino Factory for the
International Design Study (Jan 08) - Muons accelerated to 25 GeV and fires neutrino
beams to two 50 kton iron detectors at two
different baselines (4000 km and 7500 km) -
9Magnetised Iron Neutrino Detector (MIND)
- Golden channel signature wrong-sign muons in
magnetised calorimeter
(Cervera et al. 2000)
Magnetic Iron Neutrino Detector (MIND)
- Far detector (3000-7000 km) can search for
wrong-sign muons in appearance mode (for
example, Large Magnetic Detector)
- Background charm production, charge
misidentification.
QtPmsin2 q
- Eliminates background
- at 10-6
10Magnetised Iron Neutrino Detector (MIND)
- Golden paper (Cervera et al, 2000) defined
analysis and efficiency for discovery of CP
violation at low values of q13 - New analysis (Cervera, 2007)
- Efficiency plateau between 5 and 8 GeV
- Baseline Lm gt 150 cm
- Ensures charge mis-ID
- below 10-3
11Magnetised Iron Neutrino Detector (MIND)
- Collaboration Valencia-Glasgow improvements MIND
- analysis with full GEANT4 reconstruction
- Demonstrate that for En lt 10 GeV
- Backgrounds are below 10-3
- The efficiency can be increased with respect to
fast analysis - Compute
- Signal and backgrounds efficiency as a function
of energy - Energy resolution as a function of energy
- Optimise segmentation and B field based on the
above parameters and taking into account
feasibility and cost - Add Quasi-Elastic (QE) and Resonance (RES)
production to Deep Inelastic (DIS) events
12Magnetised Iron Neutrino Detector (MIND)
- Performance of IDS-NF baseline detectors (two
MIND detectors, one at 4000 km and one at 7500
km) at 3s (Huber, Winter, ISS 2007) - Phenomenology of detector efficiency vs baseline
(M-project,McLachlan)
13Totally Active Scintillating Detectors (TASD)
Improvement Totally Active Scintillating
Detector (TASD) using Nona and Minerna concepts
Ellis, Bross
Main problem magnetisation huge volume
- Momenta between 100 MeV/c to 15 GeV/c
- Magnetic field considered 0.5 T
- Reconstructed position resolution 4.5 mm
Reduction threshold second oscillation maximum
and electron identification
- TASD opens up possibility of running low energy
neutrino factory (4 GeV)
14Hybrid detectors MINDTASD?
- Compromise between MIND and TASD concepts?
Optimisation of geometry not done - Iron free regions improve momentum and charge
determination
- Combining MINDTASD and iron-free regions
15 Other detector technologies
- Liquid argon TPC for ne (platinum channel) and
nt appearance (silver channel). ICARUS-like.
Simultaneous fit to all wrong and right sign
distributions.
- Hybrid Emulsion-Magnetised Iron simultaneous nm
(golden channel) and nt appearance (silver
channel). ICARUS-like.
16 Near detector
What needs to be measured
- Near detectors should be able to measure flux and
energy of and - Calibration and flux control (inverse muon
decay) -
- High event rate 109 CC events/year in 50 kg
detector
- Measure charm x-section in near detector to
control systematics of far detector (main
background)
- Other physics neutrino cross-sections, PDF,
electroweak measurements, ... - Possible technology fully instrumented silicon
target in a magnetic detector.
17Flux Measurement at Near Detector for NF
- Best possibility Inverse Muon Decay scattering
off electrons in the near detector. Known
cross-sections
Kharadzov, Tsenov
- Rates in 1 ton Near Detector for 1021 muons/yr
1.7x106 evts/yr
6.9x105 evts/yr
5.8x105 evts/yr
7x104 evts/yr
18Near Detector used to extract Pnenm
- Matrix method with Near Detector data (even if
spectrum not identical in near and far detector!)
to extract oscillation probability - Where M1matrix relating event rate and flux of
ne at ND - M2matrix relating event rate and flux of nm
at FD - Mmatrix relating measured ND ne rate and FD
nm rate - MnOscmatrix relating expected ne flux from
ND to FD - Proof of principle works
- for Neutrino Factory near
- detector but need to extract
- syst errors of method
PS, Laing
q138o
Probability of oscillation determined by matrix
method under simplistic conditions. Need to
give more realism to detector and matter effects.
19Charm measurement for NF
- Motivation measure charm cross-section to
validate size of charm background in wrong-sign
muon signature - Charm cross-section and branching fractions
poorly known
- Semiconductor vertex detector only viable option
in high intensity environment (emulsion too slow!)
20Other measurements Near Detector
- Near detector neutrino physics
- Cross-section measurements DIS, QES, RES
scattering - sin2?W - ?sin2?W 0.0001
- Parton Distribution Functions (polarised and
unpolarised), nuclear shadowing - ?S from xF3 - ??S0.003
- L polarization spin transfer from quarks to L
21 Future Outlook and EU Funding
- EuroNu four year EU Design Study for A High
Intensity Neutrino Oscillation Facility in
Europe (Super-beam, Neutrino Factory, Beta-beam,
neutrino detectors and physics performance). 1
PDRA Glasgow - DevDet is a new Integrating Activity proposal
across Europe to coordinate Detector Development
Infrastructures for Particle Physics Experiments - It is a 37.8 M proposal to the European Union
(EU) with a requested EU contribution of 11.0 M.
It has 87 participants from 21 different
countries - It includes the luminosity-upgraded LHC (SLHC),
future Linear Colliders (ILC/CLIC), future
accelerator-driven neutrino facilities and
B-physics facilities - Scope for collaboration with PPT phenomenology
of neutrino oscillations, optimal strategy for
measurements, how accurate do we need to know
mixing angles, mass differences and CP phase?,
hints for higher symmetries from neutrino
oscillations?, near detector physics (ie. PDFs,
neutrino cross-sections, electroweak
measurements)