measurement of the capture cross section of cm & cm€¦ · simon2 monitor •stable monitor...
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Measurement of the capture
cross section of 244Cm & 246Cm1V. Alcayne, 2A. Kimura, 1E. Mendoza, 1D. Cano Ott
and the n_TOF Collaboration
1CIEMAT– Spain2JAEA – Japan
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n_TOF CM | V. Alcayne | 27. Nov 2018 | 2
Introduction
Measurement during May-September 2017
Second smallest capture mass (177Tm ~0,3mg)
Second capture measurement in EAR2.
Precise background subtraction is needed
Sample ~1 mg with ~2 GBq activity
→Physics case for EAR2
TAC in EAR1TAC
Lower intensity / 185m flight
Better RF
Information EM cascade
C6D6 in EAR2 TED
High intensity / 20m flight path
Worse RF
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Data processing
• Reprocessed data
New Pulse Shape
Rebounds study
• New MC simulations
Full setup simulation
Energy Calibration
Energy Resolution
Gain Drift
Reproducing MC
simulationsLink to Analysis meeting talk
https://indico.cern.ch/event/735668/contributions/3047479/attachments/16834
68/2705906/PresentacionCm244NTOF7_18v05.pdf
n_TOF CM | V. Alcayne | 27. Nov 2018 | 3
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n_TOF CM | V. Alcayne | 27. Nov 2018 |
SiMon2 Monitor
• Stable monitor for 3 months
105 µg/cm2 ->Li6
4 silicon detectors 300µm
• New MC simulations
Full setup simulation
Energy Calibration
Energy Resolution
Gain Drift
Reproducing MC
simulations
4
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Normalization with SiMON2
WONDER 5th| V. Alcayne | 10. Oct. 2018| 3
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Flux calculated with SiMon2
n_TOF CM | V. Alcayne | 27. Nov 2018 | 6
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Small differences
1-2%
• Corrected by:
Detector efficiency
XS convoluted with RF
using Transport Code
Flux calculated with SiMon2
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Monitoring Run by Run
Differences sample position
Effective gain control of C6D6
Normalizing to SiMon2
Other effects
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Differences sample position
Effective gain control of C6D6
Normalizing to SiMon2
Other effects
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Small differences
1-2%
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n_TOF CM | V. Alcayne | 27. Nov 2018 | 11
244Cm EAR2
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246Cm EAR2
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n_TOF CM | V. Alcayne | 27. Nov 2018 |
Geant4 Simulations
Percentage of counts
lost below the threshold
(0.12 MeV)244Cm 7.2%246Cm 9.9%240Pu 4.4%197Au 4.1%
13
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Preliminary WF Det1
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Preliminary capture yields
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Outlook and Summary
TAC in EAR1
• Alpha discrimination
• Calibration
• Coincidences
• Reproduction Cascades
• Efficiency TAC (MC
Simulations)
• Resolution function and
corrections
• Normalize to neutron flux
• Analysis with Sammy
• ….
C6D6 in EAR2
• Calibrations
• Gain drift corrections
• PSA routine
• Background calculation
• Normalization to neutron flux
• WF
• Cascade Simulations
• Gain variation as a function of
the TOF
• Coincidences between detectors
• Resolution function and
corrections
• Resonance analysis
• ….
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Hola que tal
BACKUP SLIDES
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Hola que tal
BACKUP SLIDES
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Small differences
1-2%
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M. S. Moore and G. A.
Keyworth, Physical
Review C, 3, 1656 -
1667 (1971)
Experiment by Moore et al. Experiment by Kimura et al.
Only 2 sets of previous data
A. Kimura et al., J. Nucl.
Sci. Tech. 49, 708
(2012).
1969 Using underground nuclear
explosion
Moxon-Rae detectors
Accuracy questionable due to
systematic uncertainties
No data under 20eV
2010 at J-PARC
Two cluster-Ge detectors
Above100 eV, the measurement required
severe dead time corrections (up to 90%)
Resonance analysis up to 30 eV
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Samples
Two 244Cm sample
(%)246Cm sample (%)
244Cm 60.6±1.1 (~0.80 mg) 20.3±0.5 (~0.38mg)245Cm 2.38±0.30 (~0.02 mg) 1.03±0.29(~0.02 mg)246Cm 6.35±0.55 (~0.08 mg) 57.7±1.5 (~1.10mg)247Cm ----- 2.8±0.4 (~0.05mg)248Cm ----- 8.8±0.2 (~0.17mg)240Pu 31.1±0.6 (~0.40mg) 9.30±0.15 (~0.17mg)
9cm
Cm
9mm5mm
0,5mm 1,2mm
Cm
MylarKapton Al Ring
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C6D6 Setup EAR2 (~20 m)
Neutron Beam
Sample
• Experiment
3 months.
8·1018 protons of 20 GeV/c.
~ 50% of the beam measuring 244Cm and 246Cm rest dummy
measurements and check.
• Three detectors
Efficiency proportional to energy (egi∝Egi )
achieved using PHWT.
Good time resolution (~1ns).
• Analysis
Precise background subtraction.
Energy calibration (133Ba, 137Cs,60Co, 88Y, AmBe and CmC)
Gain drifts (12 sets)
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244Cm Experimental results EAR2
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246Cm Experimental results EAR2
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TAC Setup EAR1 (~185m) • TAC( Total Absorption Calorimeter).
Sphere of 40 BaF2 crystals, 95% solid angle.
Detecting almost all the gammas in the cascade.
• Experiment
2 weeks.
5·1017 protons of
20 GeV/c.
• Analysis
Coincidence between
the 40 detectors. Reject background.
Montecarlo simulations with Geant4.
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244Cm Experimental
results EAR1 TAC
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EM cascades TAC
• Background subtracted
• Different multiplicities
• Normalization
~60000 counts
~300000 counts
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Hola que tal
Motivation
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Neutrons per Pulse at n_TOF
~5*104 neutrons
~2.5*106 neutrons
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• 6 sources used( 133Ba,137Cs,60Co,88Y,AmBe,CmC)
• Fitting MC simulation with χ2
Energy calibrations
𝑓(𝑥) ቊ𝑎𝑥2 + 𝑏𝑥 + 𝑐 𝑥 < 𝑥0𝑑𝑥 + 𝑐 𝑥 ≥ 𝑥0
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• 6 sources used( 133Ba,137Cs,60Co,88Y,Ambe,CmC)
• Fitting MC simulation with χ2 method varying gain and
resolution.
Energy resolution
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n_TOF AM | V.Alcayne | 10. July. 2018 | 42
Gain Drifts
• 10 calibration measurements
• Source always in the same
position.
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MC Simulations Source Response
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44
CALIBRATIONS