How to Build a Neutrino Oscillations Detector - Why MINOS is like it is! - PowerPoint PPT Presentation

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How to Build a Neutrino Oscillations Detector - Why MINOS is like it is!

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... baseline Neutrino Oscillation Experiment. What do we want to measure? ... Look for appearance of ?e. beam & NC contamination. range, B field. calorimetric. ?m2 ... – PowerPoint PPT presentation

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Title: How to Build a Neutrino Oscillations Detector - Why MINOS is like it is!


1
How to Build a Neutrino Oscillations
Detector-Why MINOS is like it is!
  • Alfons Weber
  • March 2005

2
Neutrino Oscillations
  • MINOS is a long baseline Neutrino Oscillation
    Experiment
  • What do we want to measure?
  • We want to see, how one type of Neutrino
    transforms itself into another.
  • There is a characteristic pattern, if this is
    transformation is due to neutrino mass
    eigenstates
  • Simplified two neutrino scenario

3
How are Neutrinos produced?
4
NuMI The Main Injector
Fermilab Main Injector 120 GeV protons
2.5 x 1013 protons/pulse 1.9 sec
rep rate (8 msec spill)
? 0.25 MW NuMI Beam Graphite
target Two magnetic horns 675 m.
vac. decay pipe hadron absorber
designed for 4 x 1013 ppp Beam Monitoring
muon detectors hadron detectors
Near Detector !
5
NuMI Beam Layout
6
Neutrino Production
120 GeV primary Main Injector beam Target readily
movable in beam direction 2-horn beam adjusts
for variable energy ranges 675 meter decay pipe
for p decay
7
MINOS Physics Reach
  • Intense nm beam from FNAL
  • - initially 2.5 x 1020 p.o.t./year,
  • (being commisioned now !!)

Nominal Beam Configurations
?µ CC Events/year (with no oscillations) Low
Medium High 1,600 4300 9250
Beam spectra M. Messier
8
Neutrino Interactions
  • Charge current
  • electron
  • muon
  • tau
  • Can measure neutrino energy
  • Neutral Current
  • electron
  • muon
  • tau

hadrons
? µ
µ
5 m
hadrons
? µ
? µ
1.5 m
9
Oscillation Pattern
No Effect!
10
MINOS Analysis
  • Select ?µ charge current events and reconstruct
    neutrino energy
  • Energy resolution
  • Compare energy spectrum in near and far detector
  • Measure ?m2 and sin22?
  • Look for appearance of ?e
  • beam NC contamination

range, B field
calorimetric
?m2
sin22?
11
Where should the Experiment be?
  • ?m2 0.002-0.003 eV2 (from SK)
  • In oscillation Minimum L/E 400 - 800 km /
    GeV
  • Larger distance ? shorter distance
  • High energy ? low energy
  • Flux 1/L2
  • Cross section E
  • Event size E

12
The MINOS Experiment
  • NuMI beam travels 735 km to Soudan (MN)
  • Sagitta10 km
  • 1 km wide at destination

13
How many detectors?
Where?
Why?
W I C H T Y P E?
14
Detector
  • Design requirements
  • High Mass
  • High segmentation
  • Affordable

Pick any 2!
15
MINOS Detectors
  • There are 3 MINOS Detectors
  • Near Detector _at_ FNAL (ND)
  • Far Detector _at_ Soudan (FD)
  • Calibration Detector _at_ CERN (CalDet)
  • Magnetised steel scintillator tracking
    calorimeter
  • Alternating planes of steel and scintillator
    strips

12 ton
0.9 kton
5.4 kton
16
Soudan Underground Laboratory
  • former iron mine, now a state park,
  • home of Soudan-1 2 , CDMS-II , and MINOS expts

17
MINOS Construction Challenge

18
MINOS Plane
2-m wide, 0.5-inch thick steel plates
Bottom steel plane layer
Scintillator plane Orientations alternate ?90o in
successive planes
Top steel plane layer
19
Far Detector
  • In old iron mine
  • Was already there
  • Soudan 1 2
  • Right distance from FNAL

20
MINOS Scintillator Module
  • 4-8m scintillator modules
  • 24-28 strips
  • double sided readout
  • multi anode PMTs (16/64)

21
PMT
  • Light is detected bymulti-anode PMTs
  • 230x 64-pixel in ND
  • 1500x 16-pixel in FD
  • pixel to pixel variations

22
FD Front End Electronics
  • MINOS developed an ASIC chip for PMT readout
  • 32 channels
  • shaping
  • amplification
  • sample hold
  • output driver to ADC
  • Excellent product
  • fast shaping 500 nsec
  • noise lt 2 fC
  • lineargt 20 pC
  • 6 ASICs multiplexed onto 1 ADC

23
Signal Amplification
24
Output of Pre-amplifier
25
Signal Digitisation
26
DAQ System
  • Trigger-less DAQ system
  • ASIC close to PMT
  • ADC in VME crate
  • fast PVIC-bus to PC trigger farm
  • search for hits correlated in space and time
  • Timing System
  • Absolute time from GPS(?tabs 200 nsec)
  • optical distribute along large detector (?trel
    4 nsec)

27
Near Detector Event
Low-energy track from fiducial region
MINOS Preliminary Etrack approx. 1.5 GeV
28
Additional Near Detector Events
Medium energy track from near peak in
pseudo-medium beam
MINOS Preliminary Etrack approx. 3.1 GeV
29
Additional Near Detector Events
One snarl (beam pulse) in near detector,
showing multiple events.
MINOS Preliminary
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