Recent + future MEG results (and LFV implications) in the ... · H. Natori H. Nishiguchi ... ¥...
Transcript of Recent + future MEG results (and LFV implications) in the ... · H. Natori H. Nishiguchi ... ¥...
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Recent + future MEG results (and LFV implications)
in the “SuperB” era
Giovanni Signorelli INFN Sezione di Pisa
XVII SuperB Workshop and Kick-off Meeting
La Biodola (Isola d’Elba) 1 June 2011
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3
Lepton flavor violation• LFV decays in the SM is radiatively induced by neutrino masses and mixings at a negligible
level
• All SM extensions enhance the rate through mixing in the high energy sector of the theory (other particles in the loop...)
• Clear evidence for physics beyond the SM
- background-free • Restrict parameter space of SM extensions
! e!! !e
W
"
=3α
32π
�∆m2
23s13c13s23
M2W
�2
relative probability ~ 10–54
10-14
10-13
10-12
10-11
10-10
10-9
10-8
B.R.(!"
"e)
1.21.11.00.90.80.70.60.5The unified third generation Yukawa coupling (MG)
BR
(µ→
eγ)
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• LFV is related to a “new” lepton-lepton coupling
• A wide field of research
- LFV decays
- Anomalous magnetic moment for the µ, τ- Muon-to-electron conversion
- (LFV in B-meson decays)
Many processes
4
yij �̄iFµν�jσµν
γ
µ e
γ
τ µ,e
γ
µ µ
Ze
µ e
µ→ eγ τ → µγτ → eγ
(g − 2)µ µ−N → e−Nµ→ eee
µ,τ
b
γ
d l
l
e e
eNPNP NP NP NP
NP
B → ��̄�
B → ��̄�Xs
τ!"’# $%&'
(-$!)*&%+
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• LFV is related to a “new” lepton-lepton coupling
• A wide field of research
- LFV decays
- Anomalous magnetic moment for the µ, τ- Muon-to-electron conversion
- (LFV in B-meson decays)
Many processes
5
yij �̄iFµν�jσµν
γ
µ e
γ
τ µ,e
γ
µ µ
Ze
µ e
µ→ eγ τ → µγτ → eγ
(g − 2)µ µ−N → e−Nµ→ eee
µ,τ
b
γ
d l
l
e e
eNPNP NP NP NP
NP
B → ��̄�
B → ��̄�Xs
τ!"’# $%&'
(-$!)*&%+
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Processes are correlatedModel-dependent correlations
6
Barbieri et al,, Nucl. Phys B445 (1995) 225Hisano et al., Phys. Lett. B391 (1997) 341Masiero et al., Nucl. Phys. B649 (2003) 189Calibbi et al., Phys. Rev. D74 (2006) 116002Isidori et al., Phys. Rev. D75 (2007) 115019...
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The LFV wheel
7
µ→ eγ
µ→eee
µ−N → e−N τ →µγ
τ →eγ
�Zα
π
� �mτ
mµ
�2÷4
(g − 2)µ
LFV couplings
Bµeγ
10−12∝
�∆aµ
10−9
�2(αe.m.)
× tan2 β
≡ O(1)∝∝
∝
,&''&- .&/01#
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Present limits
8
µ→ eγ
µ→eee
µ−N → e−N τ →µγ
τ →eγ
(g − 2)µ
× tan2 β
1.2× 10−11
3.3÷ 4.5× 10−8
aexpµ − aSM
µ =(296± 81)× 10−11
B-factories
BNL E821
SINDRUMII
1× 10−12
B(µTi→ eTi) < 4.3× 10−12
B(µAu→ eAu) < 7× 10−13
SINDRUM
MEGA@BNL
5626
5667
2333
2344
566<
! 89-* $&% :;?
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Future prospects
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µ→ eγ
µ→eee
µ−N → e−N τ →µγ
τ →eγ
(g − 2)µ
× tan2 β
10−16 → 10−18
few × 10−13 2× 10−9
∼ 10−15÷16 ∆aµ = (XXX ± 34)× 10−11
3.6σ → 8σ
562?→
562?→
562?
%"--9-=
→562>
562<→
562?→
mu2e COMET
MEG
HeidelbergGm2 FNAL
SuperB1÷
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The MEG collaboration
10
KEK
Tokyo U.Waseda U.
KEK
INFN & U PisaINFN & U Roma
INFN & U GenovaINFN & U Pavia
INFN & U Lecce
PSI UCIrvine JINR DubnaBINP Novosibirsk
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The MEG collaboration
11
Tokyo U.Waseda U.
KEK
INFN & U PisaINFN & U Roma
INFN & U GenovaINFN & U Pavia
INFN & U Lecce
PSI UCIrvine JINR DubnaBINP Novosibirsk
J. AdamM. Hildebrandt P.-R. Kettle O. KiselevA. Papa S. Ritt
X. Bai E. Baracchini T. DokeY. Fujii T. Haruyama T. Iwamoto A. Maki S. Mihara T. Mori H. Natori H. Nishiguchi Y. Nishimura W. Ootani R. Sawada Y. Uchiyama A. Yamamoto
A. Baldini C. Bemporad G. Boca P. W. Cattaneo G. Cavoto F. Cei C. Cerri A. De Bari M. De Gerone S. DussoniK. Fratini L. Galli F. Gatti M. GrassiD. Nicolò M. PanareoR. Pazzi† G. Piredda F. Renga M. Rossella
B. Golden G. LymmW. Molzon
F. Sergiampietri G. Signorelli F. TenchiniC. VoenaD. Zanello
D. N. Grigoriev F. Ignatov B. I. Khazin A. Korenchenko N. Kravchuk D. Mzavia†
A. Popov Yu. V. Yudin
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Time scale
• A experiment at the Paul Scherrer Institut (PSI)• The decay• The detector
• Overview of sub-detectors• Calibration methods
• Analysis of 2009 run• Status
• Run 2010 • 2011 and Next year(s)
12
µ→ eγµ→ eγ
Engineering
first limit (<2.8 x 10 -11)
This presentation
data under analysis
starting soon!
2012
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Signal and Background
13
“Signal” “RMD” “Accidental”
The accidental background is dominant and it is determined by the experimental resolutions
~~~~~µ+
!e+
"µ
"e µ+ e+
"µ
"e
~~~~~µ+
! e+
"µ
"e
~~~~~ µ+
!
e+
µ+
Ee = Eγ = 52.8 MeV
θeγ = 180ºteγ ~ 0
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14
MEG experimental method
Easy signal selection with μ+ at rest
• µ: stopped beam of 3 x 107 μ /sec in a 205 μm polyethylene target
- PSI !E5 beam line
• e+ detection
magnetic spectrometer composed by solenoidal magnet and drift chambers for momentum
plastic counters for timing
• γ detection
Liquid Xenon detector based on the scintillation light
- fast: 4 / 22 / 45 ns- high LY: ~ 0.8 * NaI- short X0: 2.77 cm
~~~~~ µ+
!
e+
µ+
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Some detector pictures
15
LXe detectorDC system
Beam Line
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16
The photon detector• γ Energy, position, timing
• Homogeneous 0.8 m3 volume of liquid Xe
• 10 % solid angle
• 65 < r < 112 cm
• |cosθ| < 0.35 |ϕ| < 60o
• Only scintillation light
• Read by 848 PMT
• 2’’ photo-multiplier tubes
• Maximum coverage FF (6.2 cm cell)
• Immersed in liquid Xe
• Low temperature (165 K)
• Quartz window (178 nm)
• Thin entrance wall
• Singularly applied HV
• Waveform digitizing @2 GHz
• Pileup rejection
Liq. Xe
H.V.
Vacuum
for thermal insulation
Al Honeycomb
window
PMT
Refrigerator
Cooling pipe
Signals
fillerPlastic
0 100 cm50
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17
Xe properties• Liquid Xenon was chosen because of its unique properties among radiation
detection active media
• Z=54, ρ=2.95 g/cm3 (X0=2.7 cm), RM=4.1 cm
• High light yield (similar to NaI)
• 40.000 phe/MeV
• Fast response of the scintillation decay time
•τsinglet= 4.2 ns
•τtriplet= 22 ns
•τrecomb= 45 ns
• Particle ID is possible
• α ~ singlet+triplet, γ ~ recombination
• Large refractive index n = 1.65
• No self-absorption (λAbs=")
α-particle
electron
Xe Xe
Xe Xe
e e
e
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Calibrations
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LEDPMT Gain
Higher V with
light att.
Alpha on wires
PMT QE & Att. L
Cold GXe
LXe
Laser
Laser
relative
timing calib.
Nickel ! Generator
9 MeV Nickel _-line
NaI
quelle
onoff
Illuminate Xe from
the back
Source (Cf)
transferred by
comp air ! on/off
Proton Accelerator Li(p,!)Be
LiF target at
COBRA center
17.6MeV !
~daily calib.
also for initial
setup
KBi
Tl
F
Li(p, !0) at 17.6 MeV
Li(p, !1) at 14.6 MeV
µ radiative decay
"0! !!"- + p ! "0 + n
"0 ! !! (55MeV, 83MeV)
"- + p ! ! + n (129MeV)
LH2 target
!
e+
e-
ee!!
##µµ
##Lower beam intensity < 107
Is necessary to reduce pile-
ups
A few days ~ 1 week to get
enough statistics
Xenon
Calibration
18
[MeV]!E0 5 10 15 20
Num
ber
of e
vent
s
0
200
400
600
800
1000
1200
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!"#$%&#'(!! )*+*,%-./01)232 9
!"#$%&"'(
454
!' !65"
77
89
!':
• The precise knowledge of the calorimeter energy scale is crucial for the experiment
• constant check of Xe light yield and purity
- trigger threshold
- systematic error on energy scale
• Different calibrations have different time-scales
19
γ-energy scale calibration
Process Energy Frequency
Charge exchange 55, 83, 129 MeV year - month
Proton accelerator 14.8, 17.6 MeV week
Nuclear reaction 9 MeV daily
Radioactive source 1.1 -4.4 MeV daily
!!
p ! !0n
!0! ""
7Li(p, !17.6)8Be
58Ni(n, !9)59Ni En
ergy
Freq
uenc
y
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2009: efficient physics run
20
- 2008 run BR<2.8 x 10-11
Nucl. Phys. B834, 1–12 (Apr. 2010)
January - October - detector dismantling - improvement (after run 2008)
-DCH-Electronic
- re – installation - LXe purification - CW calibration - another experiment in the area had
“exciting results” (µp)
October - !º calibration
November – December - MEG run
Running conditionsMEG run period
– Live time ∼84% of total time– Total time ~ 7 weeks– μ stop rate: 3x107 μ/s– Trigger rate 6.5 ev/s ;– Total data taken: 93 TB
Programmed beam shutdowns
Beam line tests and Maintenance
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Analysis principle• A µ→eγ event is described by 5 kinematical variables
• Ee, Eγ, (Δϑ, Δφ), teγ
• Likelihood function is built in terms of Signal, radiative Michel decay RMD and
background BG number of events and their probability density function PDFs
• Extended unbinned likelihood fit
- fit (Nsig, NRMD, NBG) in a wide region
• PDFs taken from
- data
- MC tuned on data
21
• 48 ≤ Eγ ≤ 58 MeV• 50 ≤ Ee ≤ 56 MeV• | Teγ | ≤ 0.7 ns• | φeγ |, | θeγ | ≤ 50 mrad
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22
(nsec)e t-2 0 2
(MeV
)E
44464850525456586062
Right Sideband
Left Sideband
E Sideband
Blind box
RMD
• We adopt a blind-box likelihood analysis
strategy
• The blinding variables are Eγ and teγ
- Hidden until analysis is fixed
• Three independent analyses
- different pdf implementation
- Fit or input NRMD, NBG
- Different statistical treatment (Freq. or Bayes)
• Use of the sidebands
- our main background comes from accidental
coincidences
- RMD can be studied in the low Eγ sideband
Analysis principle
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Pdfs and resolutions
23
µ→eγ runs
• Average upper tail for deep conversions• σR = (2.1 ± 0.15) %
• Systematic uncertainty on energy scale < 0.6%
• Resolution functions of core and tail components• core = 390 keV (0.74%)
• Positron angle resolution measured using multi-loop tracks• σ(φ) = 7.1 mrad (core)• σ(ϑ) = 11.2 mrad
• Overall angular resolution combining • XEC+DCH+target
• σ(φ) = 12.7 mrad (core)• σ(ϑ) = 14.7 mrad
Eγ Ee+ teγ
(nsec)e t-1 0 1
Num
ber
of e
vent
s /(0
.080
nse
c)
0200400600800
10001200140016001800200022002400
(MeV)eE50 51 52 53 54 55 56
Num
ber
of e
vent
s (0.
10/ M
eV)
0
1000
2000
3000
4000
5000
0.048 0.05 0.052 0.054 0.056 0.058
Num
ber
of e
vent
s (0.
5 / M
eV)
0
200
400
600
800
1000
1200
1400
(MeV)E50 52 54 56 58 60
Num
ber
of e
vent
s / (0
.64
MeV
)
0
100
200
300
400
500
600
700
48 50 52 54 56 58
• 40 MeV < Eγ < 48 MeV• σt is corrected for a
small energy-dependence• (142 ± 15) ps• stable within 15 ps
along the run• MEGA had on RMD
• 700 ps resolution
!º
γ bck
RMD
Michel
!"#$%&'()(*+%,
!"#$%&'()(*+%,
!"#$%&'()(*+%,
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Normalization• The normalization factor is obtained from the number of observed Michel
positrons taken simultaneously (pre-scaled) with the µ→eγ trigger• Cancel at first order
- Absolute e+ efficiency and DCH instability
- Instantaneous beam rate variations
24B.R. = Nsig x (1.01 ± 0.08) # 10-12
theory
resolution
acceptance
O(1)
~18k107
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Likelihood fit result• Nsig < 14.5 @ 90% C.L., Nsig best–fit value = 3.0• Nsig = 0 is in 90% confidence region
- C.L @0: 40÷60% depending on the statistical approach
-
25
(sec)eT-0.5 0 0.5
-910!
Even
ts /
( 5.6
e-11
sec
)
0
5
10
15
20
25
30
(sec)eT-0.5 0 0.5
-910!
Even
ts /
( 5.6
e-11
sec
)
0
5
10
15
20
25
30
(GeV)eE0.05 0.051 0.052 0.053 0.054 0.055
Even
ts /
( 0.0
0024
GeV
)
0
5
10
15
20
25
30
35
40
45
(GeV)eE0.05 0.051 0.052 0.053 0.054 0.055
Even
ts /
( 0.0
0024
GeV
)
0
5
10
15
20
25
30
35
40
45
(GeV)E0.048 0.05 0.052 0.054 0.056 0.058
Even
ts /
( 0.0
004
GeV
)
0
10
20
30
40
50
60
70
(GeV)E0.048 0.05 0.052 0.054 0.056 0.058
Even
ts /
( 0.0
004
GeV
)
0
10
20
30
40
50
60
70
(rad)-0.04 -0.02 0 0.02 0.04
Even
ts /
( 0.0
04 )
0
5
10
15
20
25
(rad)-0.04 -0.02 0 0.02 0.04
Even
ts /
( 0.0
04 )
0
5
10
15
20
25
(rad)-0.04 -0.02 0 0.02 0.04
Even
ts /
( 0.0
04 )
0
5
10
15
20
25
(rad)-0.04 -0.02 0 0.02 0.04
Even
ts /
( 0.0
04 )
0
5
10
15
20
25 Accidental BGRMDSignalTotal
Dashed lines : 90% C.L. UL of Nsig
Fitting was done by three groups with different parametrization, analysis window and statistical approaches, and confirmed to be consistent (Nsig best fit = 3.0-4.5, UL = 1.2-1.5×10-11)
!"#$%&'()(*+%,!"#$%&'()(*+%, !"#$%&'()(*+%,
!"#$%&'()(*+%, !"#$%&'()(*+%,
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Upper limit• From the analysis of the 2009 data our limit on the BR is the following:
- cfr. MEGA limit BR < 1.2 x 10–11 @ 90% C.L.
• Sensitivity: • 6.1 x 10-12 average 90% upper limit on null-signal toy experiments • BR < (4 ÷ 6) x 10-12 from the SideBands
• On going activity• better understanding of the spectrometer• reduction of systematics on back-to-back alignment• better usage of sideband information in the likelihood
• We plan to present a combined 2009/2010 analysis this summer26
!"#$%&'()(*+%,
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27
(MeV)eE50 51 52 53 54 55 56
(MeV
)E
48
49
5051
52
53
54
5556
5758
(MeV)eE50 51 52 53 54 55 56
(MeV
)E
48
49
5051
52
53
54
5556
5758
ecos-1 -0.9995 -0.999 -0.9985
(nse
c)et
-3.5
-3
-2.5
-2
-1.5
-1
-0.5
0
ecos-1 -0.9995 -0.999 -0.9985
(nse
c)et
0
0.5
1
1.5
2
2.5
3
3.5
(MeV)eE50 51 52 53 54 55 56
(MeV
)E
48
49
5051
52
53
54
5556
5758
8152 3
ecos-1 -0.9995 -0.999 -0.9985
(nse
c)et
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
12 3
56 7
8 9
10
!"#$%&'()(*+%,
!"#$%&'()(*+%, !"#$%&'()(*+%,
!"#$%&'()(*+%,
!"#$%&'()(*+%,
!"#$%&'()(*+%,
Blue lines are 1(39.3 % included inside the region w.r.t. analysis window), 1.64(74.2%) and 2(86.5%) sigma regions.For each plot, cut on other variables for roughly 90% window is applied.
Event distibution
ecos-1 -0.9995 -0.999 -0.9985
(nse
c)et
0
0.5
1
1.5
2
2.5
3
3.5
!"#$%&'()(*+%,
Signal region
RightSB
LeftSB
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Event display• Events in the signal region were checked carefully• An event in the signal region
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-80 -60 -40 -20 0 20 40
-40
-20
0
20
40
xy
-80 -70 -60 -50 -40 -30 -20 -10 0
-50
-40
-30
-20
-10
0
-100 0 100 200 300-100
-80
-60
-40
-20
0
20
40
60
80
100
1
3
12
42
148
517
1806
6304
21999
z
0
20
40
60
80
100
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What’s next?• Data taking was restarted from Aug. 5 to Nov. 6 2010
- !º calibration from 23/8 to 9/9
- accident to the beam transport solenoid on Nov. 6
- ~ 2 x 2009 statistics
• An accident on Nov. 6 put a premature end to the 2010 run• Analysis ongoing
- 2009 & 2010 data together
• Run 2011 soon starting
- physics data taking from June to December
29
2009 run
2010
!º
µ on target
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Sensitivity prospect• Data from the two months of stable data taking of the MEG experiment in 2009 give
a result competitive with the previous limit
• Plans to reach its design sensitivity (few x 10–13) within 2013
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Back to the wheel...
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µ→ eγ
µ→eee
µ−N → e−N τ →µγ
τ →eγ
(g − 2)µ
× tan2 β
10−16 → 10−18
few × 10−13 2× 10−9
∼ 10−15÷16 ∆aµ = (XXX ± 34)× 10−11
3.6σ → 8σ
562?→
562?→
562?
%"--9-=
→562>
5627→
562?→
mu2e COMETMEG
HeidelbergGm2 FNAL
SuperB
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Thank you
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Back-up slides