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INDIABASED NEUTRINO OBSERVATORY

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Title: INDIABASED NEUTRINO OBSERVATORY


1
INDIA-BASED NEUTRINO OBSERVATORY
I N O
Naba K Mondal TIFR
2
Neutrino Physics in India
Physics Letters 18, (1965) 196, dated 15th Aug
1965
Atmospheric neutrino detector at Kolar Gold
Field 1965
PRL 15, (1965), 429, dated 30th Aug. 1965
3
KGF Continued
KGF Proton Decay Experiment
KGF collaboration contributed immensely to the
cosmic ray and particle physics. The KGF mine
was closed in early 90s
4
INO initiative
  • Multi Institutional Collaborative approach from
    beginning
  • MOU Signed by Directors of 7 institutes under DAE
    in a meeting attended by Chairman, AEC on August
    30th 2002
  • Two phase approach

R D and Construction Phase I Detector R
D, Physics studies, Site survey, Human resource
development Phase II Construction of the
detector
Operation of the Detector Phase I Physics with
Atmospheric Neutrinos Phase II Physics with
Neutrino beam from a factory
5
Physics using atmospheric neutrinos during Phase I
  • Reconfirm atmospheric neutrino oscillation
  • Improved measurement of oscillation parameters
  • Octant degeneracy for q23
  • Search for potential matter effect in neutrino
    oscillation
  • Determining the sign of Dm23 using matter effect
  • Discrimination between nm ? nt and nm ? ns
    oscillation
  • Probing CP and CPT violations
  • Constraining long range leptonic forces
  • Ultra high energy neutrinos and muons
  • Kolar events

6
Physics with Neutrino beam from NUFACT Phase II
  • Determination of q13
  • Sign of d32
  • Probing CP violation in leptonic sector
  • Matter effect in nm ? nt oscillation

7
Choice of Neutrino Source and Detector
  • Neutrino Source
  • Need to cover a large L/E range
  • Large L range
  • Large En range
  • Use Atmospheric neutrinos as source
  • Detector Choice
  • Should have large target mass ( 50-100 KT)
  • Good tracking and Energy resolution ( tracking
    calorimeter)
  • Good directionality ( lt 1 nsec time resolution
    )
  • Ease of construction
  • Modularity
  • Complimentarity with other existing and proposed
    detectors
  • Use magnetised iron as target mass and RPC as
    active detector medium

8
INO Detector Concept
9
The Magnet
10
Construction of RPC
Two 2 mm thick float Glass Separated by 2 mm
spacer
2 mm thick spacer
Pickup strips
Glass plates
Graphite coating on the outer surfaces of glass
11
ICAL Detector Specifications
12
RPC R D
  • Built RPCs of different sizes
  • 30 cm X 30 cm 25
  • 120 cm X 90 cm 2

13
RPC Test facilities
Cosmic Muon test setup at TIFR
Gas mixing unit developed at SINP
14
RPC Efficiencies and Timing
RPC working in Streamer mode
15
RPC in Avalanche mode
CMS bakelite RPC 73 cm X 42.5 cm
120 cm X 90 cm Glass RPC Built at TIFR
CMS RPC on test stand
16
Performance in Avalanche mode
Efficiency plots of RPCs in Avalanche mode
Noise Rates of RPCs operating in Avalanche mode
17
Magnet R D
  • Two independent Studies
  • Using Poisson Code at VECC
  • with solenoidal coil
  • Using MagNet 6.0 at BARC/TIFR
  • with Helmholtz coil

18
Magnet Simulation
19
Magnet Prototype
20
Electronics for ICAL
21
Detector Simulation
  • Used NUANCE Neutrino Event Generator
  • Generate atmospheric neutrino events inside INO
    detector
  • Used Atmospheric Neutrino Flux of Honda et. al.
  • GEANT3 detector simulation package
  • Simulate the detector response for the neutrino
    event
  • Generated 5 years of simulated data equivalent to
    5 years of running the experiment.
  • Analysed oscillation data at two levels
  • Using NUANCE output and kinematic resolution
    function
  • Using full detector simulation
  • Obtained preliminary results so far. Detailed
    simulation is underway.

22
Results using NUANCE
n
m
23
Matter effects Sign of D32
Preliminary With 500 kton yr exposure
24
Location of the Underground Laboratory
  • Studies were performed on two potential sites.
  • Pykara Ultimate Stage Hydro Electric Project
    (PUSHEP) at Masinagudi, Tamilnadu
  • Rammam Hydro Electric Project Site at Darjeeling
    District in West Bengal
  • INO Site Selection Committee after thorough
    evaluation have now recommended PUSHEP at
    Tamilnadu as the preferred site for the
    underground lab.

25
Possible tunnel alignments at PUSHEP
4 possible alignments of INO tunnel at PUSHEP
26
Underground Cavern
Layout of the Underground Cavern
Experimental Hall
Size of the experimental hall 150 m X 22 m X 30 m
Parking Storage
Access tunnel
Experimental Hall
Electronics
27
Preliminary Cost Estimate
  • Three components
  • Cost of building the facility
  • Underground Tunnel
  • Cavern
  • Surface laboratory and INO Center
  • Cost of Iron
  • Cost of the Active Detector Modules
  • RPCs
  • Gas System
  • Electronics
  • Magnetisation

28
Cost breakup
29
Time Scale
  • Phase 1 12-18 months
  • Draw up detailed design report for tunnel and
    cavern
  • Detailed design report on detector structure,
    RPCs, pickup electrodes, electronics power
    supply system
  • Phase II 22-40 months
  • Tunnel cavern construction
  • RPC construction
  • Tendering and procurement of iron, magnet coil
  • Electronics and gas mixing unit procurement and
    fabrication
  • Phase III 12-18 months
  • Laboratory outfitting
  • Transporting of materials
  • Assembly
  • Data taking of first module start early while
    assembly of other modules continue

30
INO as a Facility for the Future
  • Low Energy neutrinos
  • Reactor neutrinos
  • Supernova neutrinos
  • Global radioactivity in the earth
  • Double beta decay
  • Nucleon decay
  • Neutrino astronomy
  • Low energy accelerator for nuclear astrophysics

31
Documentation produced so far
32
Status of the project
  • Recent Important Steps
  • Presentation to Funding agencies in May, 2005
  • Presentation to SAC, PM in October, 2005
  • Site Selection complete
  • Task force for DPR report on site is being
    constituted now
  • A committee setup jointly by DAE DST to discuss
    the future projects on HEP in india to meet soon.

33
Summary
  • Neutrino physics is key to our understanding of
    physics beyond standard model.
  • A large magnetised detector of 50-100 Kton is
    needed to achieve some of the very exciting
    physics goals using atmospheric neutrinos.
  • Physics case for such a detector is strong as
    evident from recent publications.
  • It will complement the existing and planned
    water cherenkov detectors.
  • Can be used as a far detector during neutrino
    factory era.
  • We have started a very active R D work towards
    building such a detector.
  • Looking for participation from international
    neutrino community.
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