n Physics at UCL MINOS and NEMO-III Ruben Saakyan UCL Sheffield Particle Physics seminar 12 November 2003

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Transcript n Physics at UCL MINOS and NEMO-III Ruben Saakyan UCL Sheffield Particle Physics seminar 12 November 2003

n Physics at UCL
MINOS and NEMO-III
Ruben Saakyan
UCL
Sheffield Particle Physics seminar
12 November 2003
Motivation
Neutrino Mixing Observed !
 ne    Ue1
 n    U1
  
 n    U1
Ue2
U 2
U 2
Ue3  n1  
U 3  n2  
 
U 3  n3  
From KamLAND, solar n and atmospheric n
 0.5

U  0.61

 0.61
VERY approximately
0.87
0.35
0.35
0 

0.71

0.71
2
mLMA
 5x10 5 eV 2  (7 meV)2
2
matm
 3x10 3 eV 2  (55 meV)2
Neutrino MASS
What do we want to know?
• Relative mass scale (n-osc)
• Mass hierarchy (n-osc and bb)
• Absolute mass scale (bb+3Hb)
mmin ~ 0 - 0.01 eV
mmin ~ 0.03 - 0.06 eV
Dirac or Majorana
n 
preferred by
 
n  theorists
n 
n 
 (see-saw)
n  or 
  
 
 
n 
Only from bb
ne
n1
n2
n3
Ue12
Ue22
Ue32
From n-osc
Mixing
MINOS outline




MINOS basics
Construction status and schedule
Atmospheric n’s
Physics reach
Why ?




Confirm SuperK with controlled n beam
(K2K is first here)
Demonstrate oscillatory behaviour
Make first ever precise (10%)
measurement of oscillation parameters
Dm232, sin2 2q23
Improving existing result (CHOOZ) on
subdominant n ne (Ue3)
Who ?
Main Injector Neutrino Oscillation Study
32 institutions
175 physicists
Where and How ?
NearDet
~1kT
735km
FarDet
~5.4kT
Two functionally identical
magnetized steel/scintillator
sandwich calorimeters
How ? (Part II)
Expected event spectrum
(from NearDet)
Observed event spectrum
(from FarDet)
Ratio: survival probability as a
Function of energy
Shape: Oscillations? Decay?
Other?
Mixing angle
Dm2
NuMI beam
# protons on target 5 year plan
Year
2005 2006 2007 2008 2009 Total
Protons 2.5 3.8 5.0 6.5 7.2 25
( × 1020)
Lots of work to make it possible
n CC events/8×1020 pot
(~2.5 yr)
Low
5,080
Medium High
13,800 29,600
Construction @ Fermilab. The Beam
Decay pipe is finished
Horns in fabrication
Tunneling is finished
and encased in concrete
• NuMI beamline completed Dec 2004
• Jan-Mar 2005 – Beam commissioning
• Apr 2005 – Start of physics running
October’03:
Target Hall outfitting complete
Beneficial occupancy of Near
Detector hall – January 2004
677 m decay pipe
Target
Near
Detector
Detector Technology
• 1” thick steel planes
• Extruded plastic scintillator strips
• XY orientation of scint planes
• WLS fiber + Hamamatsu multianode
PMTs: M16 (Far) and M64 (Near)
• <B> = 1.5 Tl (Far and Near)
• Front-ends
VA(IDE) – M16
QIE – M64
• Software trigger
MINOS Far Detector
•8
m octagonal 1” steel plates
• 2 Supermodules 15 m each
• 5.4 kT total mass
• 484/485 scintillator/steel planes
• 2-ended readout
• 8X optical multiplexing
• ~1000 Km of scintillator
~2000km of WLS + clear fiber
~26000m2 of active detector planes
• <B> ~ 1.5 Tl
• DE/Ehadronic  55%/E
DE/Eem  22%/E
• DP/P  12% (by curvature)
 6% (by range)
Far Detector at Soudan
Completed July 2003
Magnetized and
running
Half the detector has
been running since
mid 2002
Fully commissioned
Taking atmospheric
neutrino data, Soudan
2 exposure by the end
of next year
Cosmic ray muons
Reconstructed front view
Cosmic ray muons
are used for calibration
(and physics!)
2.6ns/plane timing
resolution permits
direction determination
Veto shield tags
incoming “parallel”
muons which can
mimic neutrino events
Timing
Atmospheric n’s at FarDet
Veto Shield
Veto shield to veto vertical muons
and reduce background
Veto shield
Upward muons
Downward
Timing allows
measurement of 1/b
Good separation of
downward (cosmic
ray) and upward
(neutrino induced)
muons
Upward
Atmospheric n events at FarDet
• Atmospheric n interactions
have been observed
• B-field allows to measure
muons up to 70 GeV
• B-field gives charge info:
distinguish n and nbar
• Potential to test CPT
Num of events in 5 years n
Contained vertex with  620
Upgoing 
280
nbar
400
120
700 MeV muon
Near Detector
n target
• ~1 kT
• High rates ~ 3 MHz
• 3.8 x 4.8 “squeezed” octagon
• 1-end readout
• no-multiplexing
• 220 M64s QIE-based front-end
•282 steel planes
•153 scintillator planes
• Use events with R<30cm
EnNear  EnFar
ninteractions in ND
~10 – 100 n events/spill

~108 – 109 events/yr
Unique opportunity
for n-scattering physics
 spectrometer
Construction @ Fermilab
Near Detector
• All NearDet planes assembled
and ready to install
• Beneficial occupancy of
NearDet Hall – Jan 04
• Installation starts January 04
• Installation complete – Oct 04
Calibration Detector
at CERN
• Both ND and FD too big to
be calibrated in test beam
• CalDet is the same but smaller
• T7 and T11 beamlines at CERN PS
in 2001, 2002, 2003
• October 2003: Data taking
programme complete
 Understand detector response to
 p, e, , p of 0.5 – 10 GeV (particle ID)
 Calibrate out Near/Far readout
 differences
 Debug detector subsystems
 Refine topology and pattern recognition
 software
 60 planes (1m×1m) 12 ton
 24 strips/plane, XY orientation in
consecutive planes
 FarDet and/or NearDet readout
Calibration Detector Events
Pion
2 GeV
1 GeV
Strip
Strip
Plane
Even Plane view
3.5 GeV
Plane
2 GeV
1 GeV
Odd Plane view
Relative Pulse Height
3.5 GeV
Odd Plane view
Relative Pulse Height
Even Plane view
Proton
Calibration Detector Results
Very preliminary
MINOS:
Physics Reach
n   n
2.3 yr*
3.7 yr*
5.0 yr*
*
Times according to
5 year proton intensity
plan
MINOS:
Physics Reach
n  ne
Summary




The MINOS Far Detector is complete and
taking cosmic and atmospheric n data
Beam work and Near Detector construction at
FNAL is on schedule. First beam – end 2004.
Calibration Detector programme at CERN
complete
Physics running with NuMI n’s – April 2005
NEMO
NEMO Outline





bb decay basics
The NEMO-III detector
First results
Sensitivity by 2008
Towards NEMO-NEXT
bb decay basics
In many even-even nuclei
b-decay is energetically forbidden
n
SM
Requires Majorana
mn ≠ 0
e
e
p
n
n
p
2-
n
76
n
As
e
n
0+
p
e
n
p
76
Ge
Two Neutrino Spectrum
Zero Neutrino Spectrum
1% resolution
(2 n) = 100 *
(0 n)
0+
bb
Qbb
2+
0+
76
Se
This leaves bb as the allowed
decay mode
0.0
0.5
1.0
1.5
Sum Energy for the Two Electrons (MeV)
2.0
Qbb
bb Decay Basics. Rates
2n
1/ 2
T
0n
1/ 2
(0  0 ) 
+
+
1
1
2n
 G ( E0 , Z ) M
0n
T (0  0 )   G ( E0 , Z ) M
+
+
2n 2
0n 2
 mn 2
G – phase space, exactly calculable; G0n ~ Qbb5, G2n ~ Qbb11
M – nuclear matrix element. Hard to calculate.
Uncertainties factor of 2-10 (depending on isotope)
Must investigate several different isotopes!
<mn> is effective Majorana neutrino mass
Isotopes of Interest
48Ca, 76Ge, 100Mo, 150Nd,136Xe, 116Cd, 96Zr, 82Se,130Te
Currently Active Experiments
NEMO-3
(Tracking calorimeter)
CUORICINO
(bolometer)
<mn> = 0.4 eV ???
Heidelberg-Moscow exp is still running ???
Neutrino Ettore Majorana Observatory
40 physicists and engineers

13 Laboratories/Universities

7 Countries
UK NEMO team (so far)
 Phil Adamson,
Leo Jenner, Ruben Saakyan,
Jenny Thomas (all UCL)
 Received approval from PPRP 27 Jan 03
 Main involvement: data analysis..
 ..and some hardware tasks: PMT helium
tests, light injection optimization
 Expect to participate in shifts at Frejus
• From scintil detector:
s = 250 ps
• From tracker:
s||= 1cm s = 0.45mm
(using timing information
on plasma propagation)
Calibration:
• Laser survey
• neutron Am/Be for
s||, s, e+ signature
• e- 207Bi, 90Sr for
energy calibration
•  60Co for time alignment
Trigger:
1 scintillator hit > 150 keV
+
1 track: few Geiger planes
(flexible  3 – 7 Hz)
How it works
NEMO bb events
3D pictures
 study single electron spectra
 study angular distributions

Detailed 2ninformation
 O (105) 2n 100Mo events/yr !
 7 isotopes

NEMO background events
 e+e-
e- (~7 MeV) from n
Data taking
 June
2002: start with all 20 sectors, iron
shielding, neutron shielding but…
 …still a lot of debugging (both tracking
detector and calorimeter)
 14 February 2003: start of routine data
taking
NEMO-3 First Results
100Mo 1200 h
2n:
T1/2=[7.4±0.05(stat)±0.8(sys)]×1018yr
(19000 events; S/B  50)
0n:
1 event in 2.8 – 3.2 MeV region
T1/2 > 1023 yr
90% CL
<mn> < 0.9 – 2.1 eV
World’s best result for 100Mo
Very preliminary (and conservative) from 3800h: T1/2 > 2.3×1023 yr
<mn> < 0.6 – 1.4 eV
Single State Dominance (SSD)
VS
Higher order State Dominance (HSD)
Simkovic, Domin, Semenov
nucl-th/0006084, Phys. Rev. C
HSD
1+
100Tc
0+
SSD
100Mo
0+
1.
2.
3.
4.
100Ru
single e- spectrum
Shape of
Shape of 2b spectrum
Angular distribution
~ 20% difference in T1/2
100Mo
+ NEMO-like detector can test it
experimentally !
NEMO-3 First Results
100Mo 1200 h
single e- spectrum
Angular distribution
between two e-
Preliminary:
SSD is preferred
NEMO-3 First Results
Other Isotopes
150Nd
116Cd
T1/2=[8.2±0.4(stat)±0.8(sys)]×1019
T1/2=[7.0±0.7(stat)±0.7(sys)]×1018
T1/2=[3.9±0.3(stat)±0.4(sys)]×1019
T1/2 > 4 × 1022 y
90% CL
World’s best result !
T1/2 > 7.7 × 1020 y
T1/2 > 1.0 × 1022 y
82Se
90% CL
90% CL
NEMO-3 0nbb sensitivity
5 years
100Mo
E = 2.8 – 3.2 MeV
7 kg Qbb =3.034 MeV
External BG: 0
Internal BG:
radioactivity < 0.04 event/y/kg
2nbb= 0.11 event/y/kg

T1/2 > 3 × 1024 yr

<mn> < 0.2 – 0.5 eV
82Se
1 kg Qbb =2.995 MeV
External BG: 0
Internal BG:
radioactivity < 0.01 event/y/kg
2nbb= 0.01 event/y/kg

T1/2 > 1 × 1024 yr

<mn> < 0.6 – 1.2 eV
In case of full load of 82Se (~14kg) <mn> < 0.1 – 0.3 eV
T1/2(2n) and Energy Resolution
T1/2n2 ( 82Se)
~ 10
2n 100
T1/ 2 ( Mo)
82Se
looks most promising
candidate
F ~ (sE/E)6
SuperNEMO
~ 100 kg 82Se (or other)
Sensitivity
<mn> ~ 0.03 eV in 5 yr
4 supermodules,
planar geometry
Feasible if:
a) BG only from 2n
(NEMO3)
b) DE/E = 5-6%
at 3 MeV (Qbb 82Se)
(R&D needed)
Future bb projects comparison
5yr exposure
*
Experiment
Source and
Mass
Sensitivity
to
T1/2 (y)
3×1027
Sensitivity to
<mn> (eV)*
Majorana
$50M
CUORE
$25M
EXO
$50M-100M
SuperNEMO
$20M
76Ge,
2×1026
0.03 – 0.10
136Xe
8×1026
0.03 – 0.10
1 ton
82Se(or other)
100 kg
2×1026
0.03 – 0.07
500kg
130Te,
0.02 – 0.06
750kg(nat)
5 different latest NME calculations
Concluding Remarks

First (preliminary) results from NEMO-III:



<mn> ≤ 0.6 eV after 3800h
2n: SSD is preferred
NEMO-III to reach 0.1 – 0.3 eV with
10 – 14 kg 82Se upgrade



UK involvement: 1000cm3 HP Ge detector
bb excited states physics with this Ge detector
Happy to collaborate with Sheffield and Boulby
Concluding Remarks II





SuperNEMO sounds very promising.
Sensitivity ~ 0. 03 eV with 100kg 82Se
Feasibility tested with NEMO-III
Boulby is a great potential site for SuperNEMO
Opportunity for UK leadership
3-5 December in Orsay: 1st meeting to form
SuperNEMO collaboration – ALL WELCOME
BACKUP
n beam systematics
Pointing at right place ?
• Beam Monitors
• GPS and laser survey
Do we know the n spectrum
and rates ?
Near Det
What about spectra differences
at Near and Far sites ?
Far Det
MIPP – a hadron
production expt
MINOS Calibration
Cosmic muons
• strip-to-strip calibration 
 Muon Energy Unit (MEU)
• relative calibration between ND
and FD (stopping muons)
Energy Calibration goal:
• 5%
absolute
Light
Injection
• PMT gain drift
• 2% relative between
ND and FD
• PMT/electronic
non-linearity
Calibration Detector
• Converts MEU to GeV
• Topology and pattern recognition
Pure materials:
Source foils
measured with the
NEMO-3 detector
• 208Tl < 2 Bq/kg
• 214Bi < 2 Bq/kg
• neutrons < 10-9 n cm-2s-1
Radon in the detector
• 222Rn ~ 20 mBq/m3
• 220Rn ~ 1.6 mBq/m3
to be improved with new
anti-radon system