current status of the construction of the angra ... · angra-cbpf - old 20´hc container placed...
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Current Status of the Construction of the Angra Antineutrino Detector
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15/09/11 J.C.Anjos-AAP-2011 2
ANGRA Collaboration:
CBPF J.C. Anjos, G.L. Azzi, A.F. Barbosa, R.M.O. Galvão, H. Lima Jr, M. Vaz
Graduate Students: Marcelo Nascimento Souza (PhD) Thamys Abrahão (MSc) Marcio Nunes (MSc) Andre G. Oliveira (MSc) Rafael Gama (MSc) Wallace R. Ferreira (MSc) Aridio Schiapazza (MSc)
Vitor Ferraz (MSc)
Undergraduate Students: Upiratan Beatriz
Brazilian Institutions:
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The ANGRA Collaboration:
PUC-RJ Hiroshi Nunokawa
UNICAMP E. Kemp, T. Bezerra, L. F. González, T. Junqueira
UFBA Iuri M. Pepe Paulo Farias
UEFS Germano P. Guedes
UFABC Marcelo Leigui, R. Da Maceno, P. Chimenti
UFJF Luciano M. Andrade, Rafael A. Nóbrega, Augusto S. Cerqueira
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The ANGRA Collaboration: International group
A. Bernstein, N. Bowden
L. Villaseñor, E. Casimiro Linares D. Reyna
Walter Fulgione, M.Aglietta
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Neutrinos Angra Project
Development of new techniques for nuclear reactor monitoring
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15/09/11 J.C.Anjos-AAP-2011 6
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15/09/11 J.C.Anjos-AAP-2011 7
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DETECTOR STATUS
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Existing Infrastructure at ANGRA
- Currently measuring background muon flux
- Remote data acquisition from Angra-CBPF
- Old 20´HC container placed next to reactor containment
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Top view of the container showing detector position
New container being prepared: size 40‘ High Cube model, for better shielding
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Central detector: Gd loaded water with 40 PMTs to detector Cherenkov radiation
external water shield
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Detector design (2011)
(detector + muon veto)
Central detector: Gd loaded water with 40 PMTs to detector Cherenkov radiation
Optimisation of number of PMTs:
Simulation with GEANT4 (2 MeV positrons at the center of the detector)
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13
Modeling of PMT fixture
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Prototype of the central detector Mechanical Project of “Sarcophage”
] External box: iron Internal box: Polypropilene
PMT test setup
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Setup for testing efficiency of PMT photo-cathode
Mounting of PMTs in the prototype tank
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Setup for testing efficiency of PMT photo-cathode
Mounting of the prototype tank
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Setup for testing efficiency of PMT photo-cathode
Mechanical project ”PMT Hat” Mounting of the PMT “hat”
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Single Photoelectron Charge Spectrum Nu-DAQ
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Construction of a 50 l prototype for neutron detection in Gd loaded water ( 1 PMT)
• 252Californium source donated by CDTN / MG (2010);
• Instalation of a small laboratory in the old CBPF linear accelerator tunnel;
• Authorization to use the neutron source given by CNEN in 2011;
• Some work still needs to be done
• Instalation of water purification station concluded;
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Muon outer veto project
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Testing Setup to test the multi-anode PMT H7546B
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ELECTRONICS STATUS
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Muon electronics - conceptual diagram (2007)
Front-end electronics
VME bus
PMT
ADC 125 MHz
trigger logic
control and status registers
data builder
TDC 81 ps
28 bits stop
start*
time encoding
FPGAs
* trigger pulse from previous event
leading-edge discriminator
control data addr
signal conditioning
10 bits
FIFO
DC level-1 trigger
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VII Encontro Neutrinos Angra – UFJF 1-3 de junho de 2011 Herman Lima Jr
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• Lay-out of VME board developed in
collaboration with Brazilian industry
CADSERVICE
• Ten units produced for tests
• Components mounted by
CADSERVICE (Campinas, SP)
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Luciano M. de A. Filho (UFJF) Augusto Santiago (UFJF)
A. F. Barbosa (CBPF)
26
Optimized Digital Detection for the Trigger System.
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Proposal
27
Digital Filter
Trigger Decision
Central FPGA of NDAQ
ADC
• Digital Filter to maximize signal/background ra8on before the trigger.
• Implementa8on → Filter FIR.
• Two methods tested
1. Joint Filter.
2. Op8mized Filter for amplitude es8mate.
• Similar results for both filters.
• Op8mized filter has advantage of output in Volts.
Increase signal/background
ra8o
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Optimal filter for amplitude estimate
28
Signal before the filter Signal aIer the filter
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Results
29
Peak/Valley = 2.5 Peak/Valley = 5.0
Variance of the measurement:
Error in the measurement:
ANTES DEPOIS
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15/09/11 J.C.Anjos-AAP-2011 30
Detector Simulation Studies
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Simulation Software for photon propagation in the Central Detector
Rafael Antunes Nóbrega Universidade Federal de Juiz de Fora - UFJF
Faculdade de Engenharia Elétrica
31
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Event Generation
32 32
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UP
DOWN
FRONT BACK
Configuration 1
< 55 55 – 60 60 – 65 65 – 70 70 – 75 75 – 80 80 – 85 > 85
Hits/100 Ev./PMT
77 (+19%)
Média / 100 Ev.
Detector Geometry Studies: With or without Winston cones?
Gustavo Valdiviesso (UFAlfenas)
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Conclusion of the Detector Geometry Studies
Geometric configuration of the 40 PMTs does not affect neutrino signal.
Final configuration to optimize muon rejection.
Better signal with Winston cones (16% more light), but technical difficulties to implement
(construction, cost... ).
Polyethilene Shielding generates at least the double of neutrons by spallation than water
Internal surface should be reflective but does not need to be polished.
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Data Analysis: simulation of expected signal and background
Signal and background Simulation:
• Positrons (from neutrino interaction) • Neutrons (from neutrino interaction) • Cosmic Muons • Cosmic Neutrons
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GEANT4: antineutrino signal
positron signal (prompt)
Neutron capture in Gd signal
Distribuition of total number of photo electrons (p.e.) observed
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15/09/11 J.C.Anjos-AAP-2011 37
GEANT4: muon background Cherenkov signal of a muon
in the target
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GEANT4: study of neutron shielding
Fluxo Experimental medido no LNGS (1000 m): En > 10 MeV
N_flux = 75 n/m2.s
Angra (nível do mar): redução 3x
N_flux = 25 n/m2.s
Atenuação da blindagem ( ~ 85% acima de 10 MeV)
N_flux = 4 n/m2.s ~ 5% de contaminação
10 MeV neutron
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39
µs
Counts
One day neutrino detection time
spectrum
Average ≈ 30µs
The time interval for both neutron capture in Gd and consecutive cosmic rays arrival
follow a Poisson distribution
The probability for an event to occur after a time interval ’t’ is:
1/λ = average time interval between events
1/λν ≈ 30µs = time average for n capture
1/λμ ≈ 1ms = time average for cosmic muons
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15/09/11 J.C.Anjos-AAP-2011 40
Data acquisition simulation
Simulated data for one day of data taking and data reduction by each selection criteria
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Data acquisition simulation
Simulated data for one day of data taking and data reduction by each selection criteria
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Data acquisition simulation
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15/09/11 J.C.Anjos-AAP-2011 43
Data acquisition simulation
Fit Result: Neutrino events estimated within ~ 8% uncertainty
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15/09/11 J.C.Anjos-AAP-2011 44
Conclusions • Previous experiments demonstrated a good capability of using antineutrinos for nuclear reactor distant monitoring.
• Neutrino laboratory already installed in Angra
• Muon detection (background estimate) and remote data acquisition (CBPF-Angra link) working.
• Simulation is running and guiding final detector design.
• Electronics is ready for production phase
• Expected data taking by beginning 2012
• Good opportunity to develop experimental neutrino physics in Brazil and to contribute to new safeguards techniques.
• Good opportunity to interact with local industry.
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Thank you!