Title: Neutrino Masses and Mixings
1Neutrino Masses and Mixings Experiments Past,
Present, and Future
2ICHEP
02
For three neutrinos
? masses
and mixings
Dave Wark
University of Sussex/RAL
3ICHEP
02
For three neutrinos
? masses
Three Angles
and mixings
Dave Wark
University of Sussex/RAL
4ICHEP
02
For three neutrinos
? masses
- each has a sign
and mixings
Dave Wark
University of Sussex/RAL
5Matter Effects the MSW effect
In vacuum
6Matter Effects the MSW effect
7Matter Effects the MSW effect
8Matter Effects the MSW effect
9ICHEP
02
For three neutrinos
? masses
- each has a sign
and mixings
Dave Wark
University of Sussex/RAL
10ICHEP
02
For three neutrinos
? masses
and mixings
Dave Wark
University of Sussex/RAL
11So what do we have to measure?
- Three Angles
- Two mass differences
- Two signs of the mass differences
- One CP phase
- But Also
- The absolute mass scale
- Are neutrinos Dirac or Majorana (or both)?
- Are there more - sterile - neutrinos
(neuterinos)?
12So what do we have to measure?
- Most Importantly
- Is this the right model ?!?
- Many others have been proposed
- FCNC, extra dimensions, violations of the EP,
neutrino decay, neutrino magnetic moments, etc. - Must find signatures of oscillations
- Appearance of the wrong-flavour neutrinos
- Oscillation pattern
- Day/night or other matter effects
13Solar Neutrinos
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15ICHEP
02
? masses
and mixings
Dave Wark
University of Sussex/RAL
16ICHEP
02
? masses
and mixings
Dave Wark
University of Sussex/RAL
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1922,400 solar neutrino events!
2022,400 solar neutrino events!
21Super-Kamiokande Energy Spectrum
22Super-Kamiokande seasonal variation
23Day-night variation
Super Kamiokande
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28Energy Scale
Calibrations
Efficiency
Reconstruction
29SNO Backgrounds
30The energy spectrum?
31So subtract these backgrounds ?
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33Do they come from the sun?
34What does SuperK see?
16,700 electron type
5,700 mu or tau type!
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36How will we learn more?
- From SNO
- Currently running with NaCl in the D2O
- Shortly to install discrete neutron counters
- Stringent test of NC systematics
- From others
- Long term too many to discuss here
- Short term
- KamLAND
- BOREXINO
37KamLAND
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40KamLAND is taking data!
41Backgrounds are low!
First Results at PANIC?!?
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43Borexino Physics Target 7Be neutrinos
Fill to start November 2002, data spring 2003
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45SK can distinguish muons from electrons with
impressive precision
46SK data as a function of zenith angle
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48Excellent fit to nm?nt
Very poor fit to nm?ne
Also results from Soudan II, MACRO
49t-appearance in Super-K
50Consequences for Q13
51From Nakayas talk at n02
52The first LBL Experiment K2K
53This conference saw a detailed presentation of
systematics
54K2Ks statement of the significance
55The MINOS Experiment
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581st Supermodule (1/2 detector) done, other well
begun
Meanwhile first magnetized data on atmospheric n
59Beam construction is well advanced, first beams
in 2006
60OPERA Detector Emulsion
2 kTon (Pb) 0.04 kTon emulsion
56 emulsion films / brick
9 kt-yr
- Dm2 1.2 x 10-3 eV2 2.7 events
- Dm2 2.4 x 10-3 eV2 11 events
- Dm2 5.4 x 10-3 eV2 54 events
- To the full detector
- 2 supermodules
- 31 walls / supermodule
- 52 x 64 bricks /wall
- 200 000 bricks
613 kt to be in LNGS by 2005
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63Dashed lines MINOS Ph2le, Ph2me, Ph2he from
right (A.Para, hep-ph/0005012)
A European proto-collaboration is organizing,
interested parties should contact me
64- Off-Axis (0.5-10) NuMI beam to surface detector
- sites in Minnesota (700 km) Canada (900 km)
possible - 20 kTon detector, possibly H20, possibly RPC,
possibly scint. - Sensitivity to q13 at 1.5 x 10-3 level
- LOI (Fermilab P929)
- http//www-numi.fnal.gov/fnal_minos/new_initiative
s/ - Note 1-Day meeting at UC London, Monday
September 16
And beyond these lies the Neutrino Factory.
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66MiniBooNE
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68First beam in August 02
First results?
69Determining the absolute mass scale
- Kinematic limits If you believe the oscillation
results, all ?m21 eV, therefore only ne
measurements have useful sensitivity -gt current
best is Tritium Beta Decay - If neutrinos have Marjorana masses, then
zero-neutrino double-beta decay is allowed -gt
observation of 0vBB decay would be direct
evidence for neutrino mass - Neutrinos are the second most numerous particle
in the Universe -gt even a tiny neutrino mass
could have cosmological implications - All these have been used to set limits on
neutrino mass
70Model Independent!
State-of-the-art experiments in Mainz and INR
(Troitsk)
71How to reach sub-eV sensitivity?
Make em bigger! -gt KATRIN
Troitsk Anomaly?
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73Neutrinoless BB-decay limits
From Elliot and Vogel, hep-ph/0202264
74hep-ph/0201231
75Normal hierarchy
Inverted hierarchy
From Pascoli and Petcov, hep-ph/0205022
Need new experiments on much larger scale
76NEMO-3
100Mo at 1025 years
2.7m
Many many more, see Elliott and
Vogel hep-ph/0202264
77Cosmological studies of neutrino mass
- There are many cosmological consequences of
neutrino mass too many to discuss here - Specifically, however, neutrino mass will tend to
wash out intermediate scale structure during
galaxy formation - This has recently been studied by the 2dF Galaxy
Redshift Survey team (see astro-ph/0204152)
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80They derive mn,tot lt 2.2 eV
81- There is no time (and I havent really got the
expertise) to discuss this in detail here. - I think it is tremendously exciting that
cosmology and laboratory measurements are on the
same scale, and therefore the information flows
both ways. - The cosmological measurements will push to
greater sensitivity, down towards 0.1 eV. - In my opinion such measurements are no substitute
for good laboratory measurements, because they
are inherently dependent on cosmological models
we should be trying to test. - For instance, there is the bias b, and if this
is higher on small scales the 2dF analysis would
derive a non-zero mass - Laboratory limits therefore are potentially
measures of b, which is very hard to measure
otherwise!
82Conclusions!
- Neutrino mixing has moved from a speculation to
an observed property of nature. - For the simplest model we have measured 2 of the
3 angles, 3 of the 2 mass differences, and the
sign of one mass difference. - Results over the next few years will be of great
interest, with SNO, KamLAND, MiniBooNE, K2K,
BOREXINO, MINOS, CNGS, and others all
contributing new data - The farther future leads from Superbeams through
the Neutrino Factory, and we can look forward to
new discoveries at each step - Direct mass measurements, including double-beta
decay, must be a priority - There is much work to be done JOIN US!
- Thanks to everybody who I stole transparencies
from!
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85Signal PDFs for pure D2O
86CHOOZ / Palo Verde
Search for disappearance of reactor ne
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88Make intense, energetic, clean, sign-selected
neutrino beams from m- ? e - nm ne
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