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Charged Particle Veto with CND & CTOF in CLAS Collaboration

This article discusses the development and implementation of a charged particle veto using the Central Neutron Detector (CND) and Central Time-of-Flight (CTOF) in the CLAS Collaboration. Results show the efficiency of the veto in detecting neutrons and differentiating them from protons and pions.

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Charged Particle Veto with CND & CTOF in CLAS Collaboration

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  1. CLAS Collaboration Meeting 18-21 June, 2019 A Charged Particle Veto in the Central Detector Using Only CND and CTOF Katheryne Price, IPN Orsayfor the CLAS Collaboration 20/06/2019

  2. Overview Charged Particle Veto for the CD Using CND & CTOF 1

  3. Background Central Neutron Detector Plastic scintillator 3 radial layers, total ~10 cm Angular coverage 40° < θ <120° Azimuthal coverage 2π Neutron detection efficiency ~10% Central Time-of-Flight Detector Plastic scintillator ~3 cm thick Angular coverage 35° < θ <125° Azimuthal coverage 2π Potential neutron detection efficiency ~3% Charged Particle Veto for the CD Using CND & CTOF 1

  4. Motivation (spoiler: yes!) Charged Particle Veto for the CD Using CND & CTOF 1

  5. Development and Evolution *RG-A shows we won’t see many above 800 MeV Charged Particle Veto for the CD Using CND & CTOF 1

  6. Development and Evolution We tried many different criteria... Charged Particle Veto for the CD Using CND & CTOF 1

  7. Development and Evolution Charged Particle Veto for the CD Using CND & CTOF 1

  8. Development and Evolution Charged Particle Veto for the CD Using CND & CTOF 1

  9. Development and Evolution for(int i=0; i<size; i++) { if(CND_hits_energy[i]>1) { counts++; if(CND_hits_layer[i]==1) { counts_l1++; } [...] } } for(int i=0; i<ctof_size; i++) { if(CTOF_hits_energy[i]>1) { ctof_counts++; } } if(counts>0 && ctof_counts==0) { for(int i=0; i<size; i++) { if(CND_hits_energy[i]>1) { total_event_energy += CND_hits_energy[i]; total_cnd_energy += CND_hits_energy[i]; cnd_only_counts++; } } } Charged Particle Veto for the CD Using CND & CTOF 1

  10. Development and Evolution Events only in CND else if(cnd_only_counts>0) { if(total_cnd_energy>10 && counts<3) { neutron++; cnd_only_neutron_counts++; } if(total_cnd_energy<=10 && counts<4) { neutron++; cnd_only_neutron_counts++; } } CND total event energy > 10 MeV, and hit multiplicity less than 3 Increment two counters – neutrons and CND only neutrons Charged Particle Veto for the CD Using CND & CTOF 1

  11. Development and Evolution 600 MeV neutrons 600 MeV π+ 600 MeV protons MeV MeV Charged Particle Veto for the CD Using CND & CTOF 1

  12. Results Baseline ~44% of 400 MeV protons detected in CND were detected only in CND; <1% of higher momentum protons But only 0.5% of 400 MeV protons detected in CND overall… Above 400 MeV, almost all protons detected were detected in both CND and CTOF Only about 15% of detected neutrons were detected in both CND and CTOF … almost all were detected in both CND and CTOF ~80% of neutrons detected in CND were detected only in CND ~55% of neutrons detected overall were detected only in CND Very few pions of all momenta were detected in only CND… ~60% of neutrons detected in CTOF were detected only in CTOF ~28% of neutrons detected overall were detected only in CND … because almost all of them stop in CTOF. A very small percentage of protons otherwise were detected only in CTOF …or only in CTOF… CND + CTOF + CND&CTOF All files: 100,000 particles φ = 0 θ = 60 Charged Particle Veto for the CD Using CND & CTOF 1

  13. Results 400 MeV neutrons 400 MeV protons 400 MeV π + ←n MeV ←p ←π+ Charged Particle Veto for the CD Using CND & CTOF 1

  14. Results 600 MeV neutrons 600 MeV protons 600 MeV π + ←n MeV ←p ←π+ Charged Particle Veto for the CD Using CND & CTOF <number>

  15. Further Testing Charged Particle Veto for the CD Using CND & CTOF <number>

  16. Implementation Charged Particle Veto for the CD Using CND & CTOF <number>

  17. Implementation Charged Particle Veto for the CD Using CND & CTOF <number>

  18. Summary

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