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Hmotná neutrina Vít Vorobel, ÚČJF MFF UK. Úvod (milníky, pojmy) Kinematická měření m n Oscilace neutrin (mixování neutrin) Dvojný beta-rozpad (Majorana x Dirac ?) Experiment NEMO-3 – dvojný beta-rozpad Experiment SuperNEMO Experiment Daya Bay – oscilace reaktorových antineutrin. - PowerPoint PPT Presentation
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Seminář ÚČJF - Vít Vorobel 1
Hmotná neutrinaVít Vorobel, ÚČJF MFF UK
• Úvod (milníky, pojmy)– Kinematická měření mn
– Oscilace neutrin (mixování neutrin)– Dvojný beta-rozpad (Majorana x Dirac ?)
• Experiment NEMO-3 – dvojný beta-rozpad• Experiment SuperNEMO• Experiment Daya Bay – oscilace reaktorových antineutrin
24.03.2010
Seminář ÚČJF - Vít Vorobel 2
Neutrinové milníky• 1930 Pauli – neutrální částice v b-rozpadu• 1937 Majorana – co když n = anti-n ?• 1956 Reines, Cowan – pozorování reaktorových anti-n• 1957 Pontecorvo – hypotéza oscilací neutrin• 1968 Davis – pozorování slunečních n (deficit)
• množství experimentů a trpělivost
• 1998 Super-Kamiokande – pozorování oscilací atmosférických n
• .................................................................................
• 80 let poté• 2010 Hierarchie? Majorana? Hmotnost? Proč tak
malá? ...24.03.2010
Seminář ÚČJF - Vít Vorobel 3
i
iiii UU
*
100
00
00
100
0cossin
0sincos
cos0sin
010
sin0cos
cossin0
sincos0
0012/
2/
1212
1212
1313
1313
2323
23232
1
i
i
i
i
e
e
e
e
U
Základní formalizmus - mísení neutrin
• Slabé stavy• Hmotnostní stavy• Směšovací matice Pontecorvo-Maki-Nakagawa-Sakata
• Informace o hmotnosti neutrin (9 parametrů)– Hmotnosti (3)– Parametry PMNS matice
• Směšovací úhly (3)• Diracova fáze (1)• Majoranovy fáze (2)
24.03.2010
3,2,1,
,,
im
e
ii
21
132312
321
mmm
22222 2 mpmmmm
35 0
Kinematická měření .• Beta – rozpad 3H
– Mainz, Troick, mne < 2 eV/c2
– KATRINE, plánovaná citlivost 0.2 eV/c2
• Rozpad p – PSI, mnm < 170 keV/c2
• Rozpad t – OPAL, DELPHI,ALEPH• mnt < 18 MeV/c2
24.03.2010 Seminář ÚČJF - Vít Vorobel 4
22,e
mEQEQpEZEFEN
222i
ii mUm
Seminář ÚČJF - Vít Vorobel 5
E
cmEcmEpcctxcmE i
ii 2
424222
ii
iii
i
ii Ux
E
cmiUx
E
cmiUx
2exp
2exp
32*
32*
xE
cmUUUUx
E
cmUUUUxP ij
jijjii
ij
jijjii 2
sinIm24
sinRe432
**32
2**2
02
exp0exp0exp32
2i
iiiiiiii x
E
cmipxtE
icm
i
222jiij mmm
2232
22 48.24
sin2sineVm
MeVEm
cm
EL
L
xP
Oscilace neutrin .• Oscilace ve vakuu - Pontecorvo 1957
24.03.2010
• Oscilace v hmotném prostředí - Wolfenstein 1978, Mikheyev-Smirnov 1985 (MSW effect)– významný efekt pro sluneční a urychlovačová neutrina– Z0 : ne, nm, n t
– W+: pouze ne
– Efektivní mi jsou jiná v prostředí než ve vakuu
ijjiij mmm 2sin 2222
2 neutrina: oscilační délka
Seminář ÚČJF - Vít Vorobel 6
bb-rozpad
24.03.2010
i
ieie mUm 2
(A,Z)(A,Z+2) + 2e- + 2n (A,Z)(A,Z+2) + 2e-
2: proces dovolený v SM, T1/2 ~ 1020y 0: proces mimo SM, T1/2 1025y
22
0002/1
),(1
evvmMZQG
T
Seminář ÚČJF - Vít Vorobel 7
NEMO-3/SuperNEMO collaboration
Neutrino Ettore Majorana Observatory(Neutrino Experiment on MOlybdenum – historical name)
80 physicists / 30 institutions
24.03.2010
Seminář ÚČJF - Vít Vorobel 8
0nbb and neutrino fundamental properties
Probe of neutrino nature. Neutrinos are Majorana fermions (particle antiparticle) if 0 takes place See-Saw mechanism, Leptogenesis, Baryon asymmetry, CP violation
Neutrino mass hierarchy. 0 measurements might help to establish the right one.
Absolute mass scale. 0 experiments are among the most sensitive ones.
Spreads are due to variations of unknown CP phases
24.03.2010
Seminář ÚČJF - Vít Vorobel 9
3 m
4 m
B (25 G)
Source: 10 kg of isotopes cylindrical, S = 20 m2, 60 mg/cm2
Tracking detector: drift wire chamber operating in Geiger mode (6180 cells)Gas: He + 4% ethyl alcohol + 1% Ar + 0.1% H2O
Calorimeter: 1940 plastic scintillators coupled to low radioactivity PMTs
The NEMO3 detector
Fréjus Underground Laboratory : 4800 m.w.e.
Magnetic field: 25 GaussGamma shield: Pure Iron (18 cm)Neutron shield: borated water (~30 cm) + Wood (Top/Bottom/Gaps between water tanks)
Able to identify e-, e+, g and -a delayed
20 sectors
24.03.2010
Seminář ÚČJF - Vít Vorobel 10
NEMO3 unique features
Multi-source detector Measurement of full bb-event pattern
Self-determination of ALL background components measuring independent channels
Multisource bb-detector
24.03.2010
Seminář ÚČJF - Vít Vorobel 11
Unique spectra from tracko-calo technique
100Mo 2 ResultsNEMO-3 ’’2n-factory’’ in action
Sum energy spectrum Angular distributionSingle electron energy spectrum
• Data- MC ββ2- background subtracted
100Mo
Latest results:
219 000 events389 daysS/B=40
100Mo 100Mo
24.03.2010
12
100Mo 2 ResultsSummary of NEMO-3 2n-results
IsotopeExpo-sure, days
Events S/B T1/2(2νββ), years
Published
100Mo 389 219000 40 (7.11 ± 0.02(stat)±0.54(syst))·1018 (SSD favored)
100Mo(0+1) 334.3 37,5 4 (5.7+1.3
-0.9(stat) )±0.8(syst))·1020
82Se 389 2750 4 (9.6± 0.3(stat)±1.0(syst))·1019
116Cd 168.4 1371 7.5 (2.8± 0.1(stat)±0.3(syst))·1019
150Nd 939 2018 2.8 (9.11+0.25-0.22(stat)±0.63(syst))·1018
New preliminary
130Te 1152 236 0.35 (6.9± 0.9(stat)±1.0(syst))·1020
96Zr 1221 428 1 (2.35± 0.14(stat)±0.16(syst))·1019
48Ca 943.2 116 6.8 (4.4+0.5-0.4(stat)±0.4(syst))·1019
Systematic studies of 2nbb process provide crucial knowledge for 0nbb search!
100Mo 2 Results0n-results
IsotopeT1/2(0νββ) limit,
×1024years <mn>, eV Experiment Year
76Ge > 15.7 <0.3-1.35 IGEX 2002
76Ge 15. 0.17-0.45 HM(KGC) 2004
76Ge > 15.5 <0.3-1.35 HM(Others) 2005
130Te >3 <0.2-0.7 CUORICINO 2008
100Mo >1.1 <0.45-0.93 NEMO-3 2009
From NEMO to SuperNEMO
SUPERNEMO R&D is in progress since 2006
NEMO-3 SuperNEMO
100Mo, 7kg Isotope, mass 82Se,100-200 kg208Tl: < 20 mBq/kg214Bi: < 300 mBq/kg
Backgroundin bb-foil
208Tl: < 2 mBq/kg214Bi: < 10 mBq/kg
8% Efficiency 30%
8% @ 3 MeV Energy resolution (FWHM) 4% @ 3 MeV
T1/2 > 2 x 1024 y<mn> < 0.3 – 0.8 eV
SensitivityT1/2 > 1-2 x 1026 y
<mn> < 40 – 100 meV
EN
tM
W
ayT
BGR
)(0
2/1
NEMO-3 successful experience allows to extrapolate tracko-calo technique on larger mass next generation detector to reach new sensitivity level.
20 modules, each of them hosts:
- 5 kg of source foil (82Se, 40mg/cm2)
- 2000-3000 Geiger channels
- 600 Calorimeter channels:
PVT Scintillator + 8’’ PMT
SuperNEMO basic design
SuperNEMO module
SuperNEMO is the favorite project to be hosted in the new LSM laboratory (hall A) planned to be opened at 2013
16
SuperNEMO demonstrator
SuperNEMO demonstrator (first module) being finalizing, which will: 1) Prove the concept2) Test 0nbb at level of KGC3) Start in 2012
Calorimeter R&DTracker R&D
Low background R&DSimulations
Source: 6.3 kg of 82Se
BiPo setup
24.03.2010
Seminář ÚČJF - Vít Vorobel 17
BiPo setup
24.03.2010
Aktivity MFF UK v NEMO-3/SuperNEMO• V úzké spolupráci s UTEF ČVUT
• NEMO-3• Simulace a návrh neutronového stínění• Koordinace výroby/dodávky nosné konstrukce detektoru (Transporta Chrudim)• Koordinace výroby/dodávky „Radon Trapping Facility“ (Hradec Králové)• Analýza dat 150Nd (excitovaný stav)
• SuperNEMO• Studie alternativní podoby kalorimetru (PD x PMT)• Optimalizace tvaru scintilátorů• Měření Rn• Testování scintilátorů
ecm
cMeVrqp
BBrqp5
/474.3
27.01.2009 NEMO3/SuperNEMO collaboration meeting, Prague
1911.9 12.5 13.7
13.9
14.113.811.8
12.7 11.5
20 mm
20 mm
Scintillator response vs irradiation position
91.5 88.6 85.5
87.3
89.9
91.988.7
90.6 92.5
Scintillatorposition scan Irradiated area 11.6 mm
FWHM @ 1 MeV, %
Peak position, ADC
Seminář ÚČJF - Vít Vorobel 20
Daya Bay Reactor Antineutrino Oscillation Experiment
24.03.2010
Seminář ÚČJF - Vít Vorobel 21
The Daya Bay Collaboration
North America (14)(54)BNL, Caltech, George Mason Univ., LBNL,
Iowa state Univ. Illinois Inst. Tech., Princeton, RPI, UC-Berkeley, UCLA, Univ. of Houston,
Univ. of Wisconsin, Virginia Tech., Univ. of Illinois-Urbana-Champaign
Asia (18) (88)IHEP, Beijing Normal Univ., Chengdu Univ. of Sci. and Tech., CGNPG, CIAE, Dongguan Polytech. Univ., Nanjing Univ.,Nankai Univ.,
Shandong Univ., Shenzhen Univ., Tsinghua Univ., USTC,
Zhongshan Univ., Hong Kong Univ.,Chinese Hong Kong Univ., National Taiwan Univ.,
National Chiao Tung Univ., National United Univ.
Europe (3) (9)JINR, Dubna, Russia
Kurchatov Institute, Russia
Charles University, Czech Republic
~ 150 collaborators
24.03.2010
Seminář ÚČJF - Vít Vorobel 22
?
13The Last Unknown Neutrino Mixing Angle
23 45
UMNSP MatrixMaki, Nakagawa, Sakata, Pontecorvo
1 0 0
0 cos23 sin23
0 sin23 cos23
cos13 0 e iCP sin13
0 1 0
e iCP sin13 0 cos13
cos12 sin12 0
sin12 cos12 0
0 0 1
1 0 0
0 e i / 2 0
0 0 e i / 2i
• What ise fraction of 3?• Ue3 is the gateway to CP violation in
neutrino sector:
U Ue1 Ue2 Ue 3
U1 U2 U 3
U1 U 2 U 3
0.8 0.5 Ue 3
0.4 0.6 0.7
0.4 0.6 0.7
?
atmospheric,accelerator
reactor,accelerator
0SNO, solar SK,KamLAND
12 ~ 32° 23 = ~ 45° 13 = ?
P( e) - P( e) sin(212)sin(223)cos2(13)sin(213)sinˉˉ
24.03.2010
Seminář ÚČJF - Vít Vorobel 23
ELm
ELm
Pdis 4sin2sincos
4sin2sin
2212
122
134
2132
132
Measuring 13 Using Reactor Anti-neutrinos
Electron anti-neutrino disappearance probability
Sin22q13 = 0.1Dm2
31 = 2.5 x 10-3 eV2
Sin22q12 = 0.825Dm2
21 = 8.2 x 10-5 eV2
Small oscillation due to q13
< 2 kmLarge oscillation due to q12
> 50 km
e disappearance at short baseline(~2 km): unambiguous measurement of 13
Osc. prob. (integrated over E n ) vs distance
24.03.2010
Seminář ÚČJF - Vít Vorobel 24Total length: ~3100 m
Daya BayNPP, 22.9 GW
Ling AoNPP, 22.9 GW
Ling Ao-ll NPP(under construction)
22.9 GW in 2011
295 m
81
0 m
465 m
900 m
Daya Bay Near site363 m from Daya BayOverburden: 98 m
Ling Ao Near site~500 m from Ling AoOverburden: 112 m
Far site1615 m from Ling Ao1985 m from DayaOverburden: 350 m
entrance
Filling hall
Mid site 873 m from Ling Ao1156 m from DayaOverburden: 208 m
Constructiontunnel
4 x 20 tons target mass at far site
Daya Bay: Powerful reactor close to mountains
24.03.2010
Seminář ÚČJF - Vít Vorobel 25
Detection of e
Time, space and energy-tagged signal suppress background events.
E Te+ + Tn + (mn - mp) + m e+ Te+ + 1.8 MeV
Inverse -decay in Gd-doped liquid scintillator:
0.3b® + Gd Gd* Gd + ’s(8 MeV) (t~30μs) + p D + (2.2 MeV) (t~180μs)
50,000b
nepe
24.03.2010
Seminář ÚČJF - Vít Vorobel 26
Antineutrino Detector
Cylindrical 3-Zone Structure separated by acrylic vessels:
I. Target: 0.1% Gd-loaded liquid scintillator, diameter=height= 3.1 m, 20 ton
II. g-catcher: liquid scintillator, 42.5 cm thick
III. Buffer shielding: mineral oil, 48.8 cm thick
vertex
14%~ , 14cm
(MeV)
E E
12.2%
13cm
With 192 PMT’s on circumference
and reflective reflectors on top and bottom:
24.03.2010
Seminář ÚČJF - Vít Vorobel 27
Inverse-beta SignalsAntineutrino Interaction Rate(events/day per 20 ton module)Daya Bay near site 840 Ling Ao near site 740 Far site 90
Delayed Energy SignalPrompt Energy Signal
MC statistics corresponds to a data taking with a single module at far site in 3 years.
Ee+(“prompt”) [1,8] MeVEn-cap (“delayed”) [6,10] MeV
tdelayed-tprompt [0.3,200] s
1 MeV 8 MeV
6 MeV 10 MeV
24.03.2010
Seminář ÚČJF - Vít Vorobel 28
Muon “Veto” System
Surround detectors with at least 2.5m of water, which shields the external radioactivity and cosmogenic background
Water shield is divided into two optically separated regions (with reflective divider, 8” PMTs mounted at the zone boundaries), which serves as two active and independent muon tagger
Augmented with a top muon tracker: RPCs
Combined efficiency of tracker > 99.5% with error measured to better than 0.25%
Resistive plate chamber (RPC)
Inner water shieldOuter water shield
24.03.2010
Seminář ÚČJF - Vít Vorobel 29
Backgrounds
DYB site LA site Far siteFast n / signal 0.1% 0.1% 0.1%
9Li-8He / signal 0.3% 0.2% 0.2%Accidental/signal <0.2% <0.2% <0.1%
Background = “prompt”+”delayed” signals that fake inverse-beta events
Three main contributors, all can be measured:
Background type Experimental Handle
Muon-induced fast neutrons (prompt recoil, delayed capture) from water or rock
>99.5% parent “water” muons tagged~1/3 parent “rock” muons tagged
9Li/8He (T1/2= 178 msec, b decay w/neutron emission, delayed capture)
Tag parent “showing” muons
Accidental prompt and delay coincidences Single rates accurately measured
Background/Signal:
24.03.2010
Seminář ÚČJF - Vít Vorobel 30
Daya Bay: Status and Plan• Ground Breaking Oct 07• CD-3 review comleted Spring 08• Surface Assembly Building occupancy March 09• Mini Dry Run Dec 09• Dry Run Spring 09• Daya Bay Near Hall ready for data taking 2010• All near and far halls ready for data taking 2011
0 1 2 3 4 5
0.01
0.02
0.03
0.04
Run Time (Years)
Se
nsi
tivity
Run Time (Years)
sin
2 2 1
30.01Goal:
sin2 2
13 (
90%
C.L
.)
24.03.2010
Seminář ÚČJF - Vít Vorobel 31
Testování RPC kosmickým zářením – IHEP Peking
24.03.2010
Kritéria testů: účinnost >95% singles (šum)< 0.8Hz/cm2 dark current< 10 μA/m2
Testováno 1600 ks RPC, odmítnuto 15%
Seminář ÚČJF - Vít Vorobel 32
谢谢你们 !Děkuji za pozornost !
24.03.2010