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Neutrino 2012 June 3-9, 2012 Kyoto, Japan. Reactor antineutrinos in the world. V. Chubakov 1 , F. Mantovani 1 , B. Ricci 1 , J. Esposito 2 , L. Ludhova 3 and S. Zavatarelli 4. 1 Dip. di Fisica, Università degli Studi di Ferrara and INFN-Ferrara, Italy - PowerPoint PPT Presentation
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Reactor antineutrinos Reactor antineutrinos in the in the
worldworldV. Chubakov1, F. Mantovani1, B. Ricci1, J. Esposito2, L. Ludhova3 and S. Zavatarelli4
1Dip. di Fisica, Università degli Studi di Ferrara and INFN-Ferrara, Italy2INFN, Laboratori Nazionali di Legnaro, Padova, Italy
3INFN- Milano, Italy 4INFN- Genova, Italy
The High Energy Region (HER) has to be controlled by studying the different contributions from the nuclear reactors, if one wants to disentangle Ngeo- and Nreact in the Low Energy Region (LER)
Signal Calculations
Result: a world wide map
Total uncertainties on predicted signal is about 5%, coming from mixing, anti-spectrum, fuel composition and thermal power
Reactor signal in Low Energy Region, for different sites.React. signal and geo neutrino detection
Conclusions and perspectives
We calculated reactor anti-e signal all over the world, by taking into account updated data on nuclear plants, anti-e
spectrum and e oscillation parameters.
We compare reactor signal with geo-neutrino signal for different places in the world.
Study of time variation of reactor signal is also possible (± 10% variation in summer/winter).
Detailed study on the effect of exhausted fuel must be completed (we estimate a 2% increase in the signal).
1
3
5
6
Reactor antineutrinos are the main source of background in the detection of geo-neutrinos (i.e. anti-e from 238U and 232Th decay chains, present in the Earth interior)
3.31.8 [MeV]
E 8
Why reactor antineutrinos ?
reactorN
iiee
Nfuel
kk
k
ki
i
ipTOT EdEPE
QpdELF
dP
NN1 1
2 )(),()(4
ddii =reactor distance =reactor distance PPii=thermal power=thermal power LFLF= Load Factor = Load Factor [1] [1] ppkk= power fraction = power fraction
QQkk = =energy released energy released for fission for fission [4][4]
kk =reactor anti- =reactor anti-neutrino spectrum neutrino spectrum [5][5]
PPeeee = = oscillation oscillation survival probability survival probability [2][2]
(E(E))= cross section = cross section anti-anti-e e +p -> e+p -> e++ +n +nEEthth=1.806 MeV =1.806 MeV [3][3]
PH
YSI
CS
DET
ECTO
REA
CTO
R
Many ingredients: neutrino physics, nuclear physics, reactor properties…
SitesSites React. LER React. LER [TNU][TNU]
Geo Geo (G)(G) [6] [6] [TNU][TNU]
RRLERLER/G/G
FREJUSFREJUS 138 138 (1±5%)(1±5%)
43±1343±13 3.23.2
SUDBURYSUDBURY 47 “47 “ 51±1051±10 0.920.92GRAN SASSOGRAN SASSO 23 “23 “ 41±841±8 0.560.56PYHASALMIPYHASALMI 19 “19 “ 51±851±8 0.370.37BAKSANBAKSAN 9.8 “9.8 “ 51±851±8 0.190.19DUSELDUSEL 8.0 “8.0 “ 53±853±8 0.150.15KAMIOKAKAMIOKA 6.7 “6.7 “ 34±634±6 0.200.20CURACAOCURACAO 2.5 “2.5 “ 32±632±6 0.0780.078HAWAIIHAWAII 0.90 “0.90 “ 12±412±4 0.0730.073
Bibliography:[1] courtesy by J. Mandula ,IAEA, International Atomic Energy Agency 2012. [4] M. Apollonio et al., Eur. Phys. J. C27, 331 (2003)[2]G.L. Fogli et al., Phys. Rev. D 84, 053007 (2011) [5]Th. A Mueller et al., Phys.Rev.C83:054615 (2011)[3]F.Vissani and A. Strumia, Phys.Lett.B564:42-54 (2003) [6]G. Fiorentini et al., Phys.Rept.453:117-172 (2007)
NU
CLE
AR
k = 235U, 238U, 239Pu , 241Pu (nuclear fuel)
4
Frejus requires a detailed knowledge of closeby reactors.
Kamioka is at the moment a very good site.
Hawaii and Curacao are ‘wonderful’ places also for geo- study.
Neutrino 2012 June 3-9, 2012 Kyoto, Japan
R.B
.
=100% efficiency=100% efficiency = 1 year= 1 year NNpp=10=103232 target protons target protons
(1kton kton liquid liquid scintillator)scintillator)
reactorN
iiee
kk
k
ki
i
ipTOT EdEPE
QpdELF
dP
NN1
4
12 )(),()(
4
DET
ECTO
R Reactor antineutrino events all over the world[1 TNU=1 event/ 103232 target protons /year]
Current status
http://pris.iaea.org/public/
Japan cores switched off
394333 215
Nuclear power plants in the world 2Total Thermal Power =1023 GW
265; 60%
94; 21%
44; 10%18; 4% 16; 4%
2; < 1%0
100
200
300
PWR BWR PHWR GCR LWGR FBR
Core type
Num
ber o
f cor
es
0.0
20.0
40.0
60.0
%
PWR BWR PHWR GCR LWGR FBR
% Total Thermal Power
63; 17%
249; 69%
47; 7.7%18; 2.6% 15; 3.5% 2; 1 %
PWR Pressurized (light) Water Reactor
BWR Boiling Water Reactor
PHWR Pressurized Heavy Water Reactor
GCRGCR Gas Cooled ReactorGas Cooled Reactor
LWGRLWGR Light Water Graphite mod.Light Water Graphite mod.
FBRFBR Fast Breeder ReactorFast Breeder Reactor