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Neutrino Factory Activities Glasgow

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Weak eigenstates do not have to coincide with mass eigenstates. Neutrino mixing matrix (Pontecorvo-Maki-Nakagawa-Sakata, ... The octant of the atmospheric angle ... – PowerPoint PPT presentation

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Title: Neutrino Factory Activities Glasgow


1
Neutrino Factory Activities Glasgow
PPE-PPT meeting 29 April 2008 Paul Soler
2
Neutrino 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.
  • where
  • and
  • States

3
Neutrino oscillations
  • Matter oscillation results for three neutrinos

(MSW effect)
Minakata Nunokawa JHEP 2001
4
Neutrino oscillations
  • Matter oscillation results for three neutrinos

Only one term in equation
(MSW effect)
Magic baseline
Clean determination of q13
5
Degeneracies
Two expts., diff. L/E n and anti-n
  • Intrinsic degeneracy

One expt., n and anti-n
One expt, only n
Golden ne-gtnm and Silver ne-gtnt channels
6
Degeneracies
  • Eightfold degeneracy
  • The sign of the atmospheric mass difference
  • The octant of the atmospheric angle

Strategies different experiments to resolve
degeneracy problem
7
Unknown 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.

8
Neutrino 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)

9
Magnetised 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

10
Magnetised 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

11
Magnetised 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

12
Magnetised 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)

13
Totally 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)

14
Hybrid 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.

17
Flux 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
18
Near 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.
19
Charm 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!)

20
Other 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)
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