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Neutrino Masses and Mixings

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Title: Neutrino Masses and Mixings


1
Neutrino Masses and Mixings Experiments Past,
Present, and Future
2
ICHEP
02
For three neutrinos
? masses
and mixings
Dave Wark
University of Sussex/RAL
3
ICHEP
02
For three neutrinos
? masses
Three Angles
and mixings
Dave Wark
University of Sussex/RAL
4
ICHEP
02
For three neutrinos
? masses
- each has a sign
and mixings
Dave Wark
University of Sussex/RAL
5
Matter Effects the MSW effect
In vacuum
6
Matter Effects the MSW effect
7
Matter Effects the MSW effect
8
Matter Effects the MSW effect
9
ICHEP
02
For three neutrinos
? masses
- each has a sign
and mixings
Dave Wark
University of Sussex/RAL
10
ICHEP
02
For three neutrinos
? masses
and mixings
Dave Wark
University of Sussex/RAL
11
So 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)?

12
So 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

13
Solar Neutrinos
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15
ICHEP
02
? masses
and mixings
Dave Wark
University of Sussex/RAL
16
ICHEP
02
? masses
and mixings
Dave Wark
University of Sussex/RAL
17
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19
22,400 solar neutrino events!
20
22,400 solar neutrino events!
21
Super-Kamiokande Energy Spectrum
22
Super-Kamiokande seasonal variation
23
Day-night variation
Super Kamiokande
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28
Energy Scale
Calibrations
Efficiency
Reconstruction
29
SNO Backgrounds
30
The energy spectrum?
31
So subtract these backgrounds ?
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33
Do they come from the sun?
34
What does SuperK see?
16,700 electron type
5,700 mu or tau type!
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How 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

37
KamLAND
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40
KamLAND is taking data!
41
Backgrounds are low!
First Results at PANIC?!?
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43
Borexino Physics Target 7Be neutrinos
Fill to start November 2002, data spring 2003
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45
SK can distinguish muons from electrons with
impressive precision
46
SK data as a function of zenith angle
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Excellent fit to nm?nt
Very poor fit to nm?ne
Also results from Soudan II, MACRO
49
t-appearance in Super-K
50
Consequences for Q13
51
From Nakayas talk at n02
52
The first LBL Experiment K2K
53
This conference saw a detailed presentation of
systematics
54
K2Ks statement of the significance
55
The MINOS Experiment
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58
1st Supermodule (1/2 detector) done, other well
begun
Meanwhile first magnetized data on atmospheric n
59
Beam construction is well advanced, first beams
in 2006
60
OPERA 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

61
3 kt to be in LNGS by 2005
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Dashed 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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66
MiniBooNE
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68
First beam in August 02
First results?
69
Determining 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

70
Model Independent!
State-of-the-art experiments in Mainz and INR
(Troitsk)
71
How to reach sub-eV sensitivity?
Make em bigger! -gt KATRIN
Troitsk Anomaly?
72
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73
Neutrinoless BB-decay limits
From Elliot and Vogel, hep-ph/0202264
74
hep-ph/0201231
75
Normal hierarchy
Inverted hierarchy
From Pascoli and Petcov, hep-ph/0205022
Need new experiments on much larger scale
76
NEMO-3
100Mo at 1025 years
2.7m
Many many more, see Elliott and
Vogel hep-ph/0202264
77
Cosmological 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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80
They 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!

82
Conclusions!
  • 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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85
Signal PDFs for pure D2O
86
CHOOZ / Palo Verde
Search for disappearance of reactor ne
87
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88
Make intense, energetic, clean, sign-selected
neutrino beams from m- ? e - nm ne
89
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