neda (neutron detector array)
DESCRIPTION
NEDA (NEutron Detector Array). J.J. Valiente Dobon (LNL-INFN) on behalf of the NEDA collaboration. Organization. Spokeperson: J.J. Valiente Dobon (LNL-INFN) GANIL Liason: M. Tripon (GANIL) Steering committee: -B. Wadsworth (U. of York) -N. Erduram (U. of Istanbul) - PowerPoint PPT PresentationTRANSCRIPT
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NEDA (NEutron Detector Array)
J.J. Valiente Dobon (LNL-INFN)
on behalf of the NEDA collaboration
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Organization
Spokeperson: J.J. Valiente Dobon (LNL-INFN)
GANIL Liason: M. Tripon (GANIL)
Steering committee:
-B. Wadsworth (U. of York)
-N. Erduram (U. of Istanbul)
-L. Sttugge (IRES – Strasbodurg)
-J. Nyberg (U. of Uppsala)
-M. Palacz (U. of Warsaw)
-A. Gadea (IFIC - Valencia)
Members of the collaboration:
U. of Ankara (Turkey), COPIN (Poland), CSIC-IFIC (Spain), Daresbury Laboratory (U.K.), GANIL (France), U. of Istanbul (Turkey), INFN (Italy), IRES (France), U. of Nidge (Turkey), U. of Uppsala (Sweeden), U. of York (U.K.) and Kolkata, India (under discussion)
FP7-INFRASTRUCTURES-2007-1
SPIRAL2 PREPARATORY PHASE
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Working groups
•Detector characteristics (Physics interests of NEDA to define the detector specifications).
•Responsible: B. Wadsworth•Geometry (Make a full study of geometry to determine (materials) efficiency, reduce cross-talk, ... Comparison between different codes: Geant4, MCNP-X. Simulate effect of other ancillaries, neutron scattering.).
•Responsible: M. Palacz•Study New Materials (Exploring new materials, solid scintillators, deuterated liquid scintillators).
•Responsible: L. Stuttgé•Digital Electronics (Flash ADCs, GTS, EXOGAM2 electronics, ..)
•Responsible: A. Gadea•PSA (Pulse shapes analysis, PSA algorithms, ...).
•Responsible: J. Nyberg•Synergies other detectors (Detectors that can be considered in synergy with NEDA: EXOGAM2, PARIS, AGATA, FAZIA, GASPARD, DIAMANT, DESCANT, Neutron spectroscopy at DESIR, DESPEC/HISPEC, NEUTROMANIA, ... ).
•Responsible: P. Bednarczyk
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Physics with NEDA
• Nuclear Structure– Probe of the T=0 correlations in N=Z nuclei: The structure beyond 92Pd
(Uppsala, LNL, GANIL, Stockholm, York)– Coulomb Energy Differences in isobaric multiplets: T=0 versus T=1 states
(Warsaw, LNL, GANIL, York)– Coulomb Energy Differences and Nuclear Shapes (York, Padova, GANIL)– Low-lying collective modes in proton rich nuclei (Valencia, Istanbul, Milano, LNL,
Krakow)• Nuclear Astrophysics
– Element abundances in the Inhomogeneous Big Bang Model (Weizmann, Soreq, GANIL)
– Isospin effects on the symmetry energy and stellar collapse (Naples, Debrecen, LNL, Florence)
• Nuclear Reactions– Level densities of neutron-rich nuclei (Naples, LNL, Florence)– Fission dynamics of neutron-rich intermediate fissility systems (Naples,
Debrecen, LNL, GANIL)
NEDA will address the physics of neutron-rich as well as neutron deficient nuclei, mainly in conjunction with gamma-ray detectors arrays like AGATA, EXOGAM2, GALILEO and PARIS.
AGATA: A. GadeaEXOGAM2: G. de FranceGALILEO: C. UrPARIS: D. Jenkins
AGATA: A. GadeaEXOGAM2: G. de FranceGALILEO: C. UrPARIS: D. Jenkins
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First day experiment
Nuclear structure N=Z beyond 92Pd : 96Cd, etc
AGATA/EXOGAM2 + NEDA
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Low-lying collective modes in proton rich nuclei
Second day experiment
Transition densities
PARIS + NEDA
N=20
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NEDA+PARIS experiment
34Ar + 16O → 44Cr + 2n (34Ar 108 pps)
The reaction to study the Pigmy resonance in 44Cr
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Physics themes
• G de Angelis – Physics with NEDA• G. de France - Results on the 92Pd experiment • A. Gottardo - Study of proton-rich nuclei with NEDA around A=100 • A. Pipidis - NEDA: At the service of n-p correlations • M. Palacz - Spectroscopy next to 100Sn: 3n gating and where is
100In? • A. Di Nitto – The role of isospin in fusion-evaporation reactions• G. Verde - The Farcos project and access to the symmetry energy
with proton-neutron measurements
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-NEDA: Neutron detector to be used coupled to AGATA/EXOGAM2/GALILEO/PARIS
-Previous experience with the NWall (BC501) currently at GANIL
-High efficiency 25% for one neutron.
-Relatively good gamma/neutron discrimination.
-Problems with cross talk.
-Low efficiency for 2n (1-2%).
-Analogic electronics.
Problem definition
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Neutron Wall
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Neutron Wall
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Neutron Wall: N=Z-2
A. Gadea et al., PRL97, 152501 (2006)S. Lenzi et al., PRL87, 122501 (2001)
24Mg(32S,2n)54Ni28Si(28Si,2nα)50Fe
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Cross talk – low 2n cross section
•High cross talk between neighboring detectors
•It is not possible to differenciate between 2n real events or just 1n scattered.
•Therefore neighbouring detectors are dismiss in the analysis and the efficiency decreases to 1-2%.
One aim of NEDA is to be able to distinguish between real 2n events and scattered neutrons → Increase of the 2n efficiency.
J. Ljungvall et al., NIMA528 471 (2004)
Possible to improve 2n efficiency using TOF among detectors
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Strategy of NEDA
-Optimization of the geometry: unitary cell size, spherical, planar, zig-zag, granularity, distance, versatile.
-FEE: GTS integrated in the motherboard and FADC in a mezzanine. Fully compatible with AGATA, GALILEO and EXOGAM2
-Use of the TOF information in addition to the measured energy to disentangle the 1n scattered events from the real 2n channels
-Use of the deuterated scintillator BC537
-Pulse height seems to be proportional to incident neutron energy (reported by DESCANT collaboration)
-Provides another method of determinig neutron energy beyond TOF
-Can lead to a better discrimination of high multiplicity neutron events and scattered events.
-New solid scintillators Lawrence Livermore National Laboratory
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BC501 vs. BC537 response
Courtesy of P. Garrett, University of Guelph.
BC537BC501A
En = 4.3 MeV
En = 2.5 MeV
BC501 BC537
DESCANT
Presented by P. GarrettPresented by P. Garrett
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Solid scintillators for neutron detection
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Simulations
Neutron HP model in G4.9.2.p01 (rel. March 2009) much improved comparing to earlier versions
Total cross sections and angular distributions for elastic scattering on p, d, and 12C reasonable
Correct (high energy) γ-ray lines produced Wrong kinematics (angular distributions?) in the
12C(n,α)9Be reaction. Important reactions still missing, like 12C(n,n’)3α
Existing defficiencies not significant in the <~10MeV energy range, which if interest for
NEDA
Presented by M. PalaczPresented by M. Palacz
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Light output of liquid scintillator
•The light-output L is usually given in MeVee: the particle energy required to generate 1 MeVee of light is defined as 1 MeV for fast electrons •L is generally less for heavier particles such as protons, deuterons, alphas, beryllium, carbon…• Therefore, the light output L in a certain path dx is a function of the deposited energy E in dx: L(E)
Dekempeneer et Liskien NIM A 256 (1987) 489-498
Deposited energy Light output
Presented by A. GottardoPresented by A. Gottardo
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Geometry study
Definition of the unitary cell dimensions
Presented by G. JaworskiPresented by G. Jaworski
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Geometries
There are two possible main geometries, either spherical or planar.
•The spherical geometry presents the full symmetry.
•The planar has some advantages, than the spherical does not present.
-Flexibility – different arrangements of the detectors, e.g. zig-zag
-Different focal posistions (500cm, 1000cm, 2000cm)
-Budget issues
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Performance of diff. geometries
Flat Zig-zag Spherical
BC501ABC537
Presented by T. HüyükPresented by T. Hüyük
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Discriminating neutron/gamma
Pulse shapes from the detector differs between neutrons and gamma rays.
Usually both pulse shape analysis and the time-of-flight information is used for discrimination neutron-gamma discrimination.
neutrons
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Digital electronics: PSA
It is possible to obtain better quality using same algorithms but digital electronics
Analog zero-crossover method
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Applying an artificial neural network can increase the quality even further
Digital electronics: Neural Network
P=sqrt(εn2+εγ
2)
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GTS supervisor
Event Builder
PSA
Pre-processing
Digitizer
TrackingOnline analysis
GTS local
prompt trigger
REQ
VAL
REQ
VAL
Global Merger
GA
MM
A-A
RR
AY
GTS local
Event Builder
PSA
Pre-processing
Digitizer
NE
DA
NEDA coupled to AGATA/EXOGAM2
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ADC Logic- FADC samples collection- Digital Processing
- Trigger- Data formatting- Inspection control
PPC
Common Logic
GTS Fanin ADC Logic Interface
Clocks(Local &
Recovered)
Delay Line
OpticalLink
Flash (Linux)
SRAM(Oscilloscope)
PROM(VHDL)
PROM(VHDL)
DPRAM(Physics, ADONIS)
Ethernet 100
Ethernet Gigabit
PCIe(Adonis)
8*FADC14 bits
100MHz
DACs(Test, control,
inspection)
Seriallink
SDRAM
Mux
MGTClocks
Fast serial links
Parallel linksSlow control
Serial link
Digital electronics: EXOGAM2-NEDA
Basic diference EXOGAM2/NEDA is the ADC: 200-300 MHz 12-14bit
Presented by M. TriponPresented by M. Tripon
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Silicon Photo multipliers readout
Direct replacement for photomultiplier tube
Insensitive to magnetic fields Can operate in vacuum Large sizes possible Attractive for simultaneous PET and
MRI scanning
SPMPlus
Synergy with PARIS – D. Jenkins
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BC501A and BC537 detectors
Currently bought commercial detectors from Saint Gobain
•Two detectors 5”x5” BC537 (LNL-INFN)
•Two detectors 5”x5” BC501A (York-Valencia)
A. Pipidis (founded SP2PP) working on the characterization of the detectors.
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Summary
• Currently bought BC537 and BC501A commercial detectors to test:
– cross talk – light production – FADC – frecuency and number of bits– PSA – neutron-gamma discrimination
• First contacts with Livermore – Start up collaboration solid scintillators?
• Test of SPMPlus from York in BC537 and BC501A • Development of electronics in synergy with EXOGAM2• Optimal geometry
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Workshop program
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Phases of NEDA
The current development on new materials and readout systems for neutron detection makes necessary to build NEDA in four different phases:
• Phase 0: Upgrade of Neutron Wall with digital electronics.• Phase 1: R&D on new material and light readout systems for a
highly segmented neutron detector array.• Phase 3: Construction of a limited size Demonstrator • Phase 4: Final construction of NEDA
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With current technological status …
• Three main options:– 200 detectors BC501A – PM readout –Digital electronics
• Total cost: 600K€ (BC501A) + 200K€(Elec.) + 40K€ (mechanics) = 840 K€
– 200 detectors BC536 – PM readout – Digital electronics• Total cost: 2000K€ (BC537) + 200K€(Elec.) + 40K€ (mechanics) = 2240 K€
– Upgrade Neutron Wall - Phase 0 (Digital electronics)• Total cost (50 channels) = 40K€
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Collaborating Institutes
• Centro Superior de Investigaciones Cientificas (CSIC) – Valencia• Grand Accelerateur National d’Ions Lourds (GANIL)• Istituto Nazionale di Fisica Nucleare – Laboratori Nazionale di
Legnaro• Royal Institute of Technology - KTH• University of Istanbul• University of Lund• University of Nidge• University of Uppsala• University of Warsaw• University of York
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Summary and future work
• NEDA – Looks at improving efficiency for 2n channels – BC537, geometry• Validated simulatons – realistic results for BC501 and BC537• Included model for light production.• PSA algorithms to discriminate neutron-gamma – Neural Network great perspectives.• Synergies
– PARIS (A. Maj): SPMPlus, electronics?– EXOGAM (G. De France): electronics– Neutron Spectroscopy at DESIR (D. Cano & N. Orr): Simulations, FADC
FUTURE WORK• Currently bought BC537 and BC501 commercial detectors to test:
– cross talk – light production – PSA – neutron-gamma discrimination
• Test of SPMPlus from York in BC537 and BC501 • Development of electronics in synergy with EXOGAM2• Design of FADC mezzanines• Optimal geometry
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NEDA possible geometries
Step-spherical Spherical
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Neutron-γ discrimination
BC537 n-γ discrimination
BC501A(D) n-γ discrimination
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Light output
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Time scale
2008 2009 2010
Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3
Validation GEANT4 neutron simulations
Geometry definition
Digital algorithms for PSA
Detector prototype
Test prototype
Electronics
Negoziations MoU
MoU signature
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Silicon PM
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Synergies
EXOGAM array
PARIS
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Commercial electronics: Struck
4 channel VME digitizer/transient recorder with a sampling rate of up to 500 MS/s (for the individual channel) and 12-bit resolution
Programmable FPGAs
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Intrinsic efficiency of BC501A and BC537