Abstract

Beam loss detection is essential for the machine protection and the fine-tuning of the accelerator to reduce the induced radioactivity. Monte Carlo simulations are also vital for the choice of beam loss monitor (BLM) type, for predicting and understanding the BLM response to beam losses. At the China Spallation Neutron Source (CSNS), the cylindrical ionization chamber (IC) filled with $\mathrm{Ar}/{\mathrm{N}}_{2}$ gas mixture is the main type of the BLM to detect the beam losses. This paper presents the detailed beam loss experiments and fluka simulations for the CSNS BLM system. It includes the response functions of the BLM detectors by taking into account the contributions of different secondary particles to the energy deposition in the sensitive volume of the BLM. Dedicated experiments were compared with fluka simulations. It was found that in the low energy section of the linac the usual ion chamber based BLMs are not sensitive enough. A BLM based on ${\mathrm{BF}}_{3}$ enclosed by a high-density polyethylene (PE) moderator is effective to detect the beam losses through detecting thermal neutrons. Its signal is about 3 orders of magnitude higher than that of $\mathrm{Ar}/{\mathrm{N}}_{2}$ BLM for a beam energy of 15 MeV. The simulations provide the results of the intrinsic delay time for the ${\mathrm{BF}}_{3}$ monitor and the thickness optimization for PE to reduce the delay. Finally, the simulated spatial resolution of loss location by detection of neutrons is also evaluated for a beam energy of 15 MeV, which presents a resolution of $\ensuremath{\sim}2\text{ }\text{ }\mathrm{m}$ in our experimental configuration.

Highlights

  • Neutron beams are created at the China Spallation Neutron Source (CSNS) through the spallation reaction of 1.6-GeV proton beams striking on the tungsten target, and widely utilized in various studies of material science and bioscience [1]

  • This paper presents detailed experimental and Monte Carlo studies for beam loss monitor (BLM) used in CSNS

  • Response functions of CSNS BLMs are investigated at the incident angle of 0°, 45°, 180°, and 90° for various secondary particles

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Summary

INTRODUCTION

Neutron beams are created at the China Spallation Neutron Source (CSNS) through the spallation reaction of 1.6-GeV proton beams striking on the tungsten target, and widely utilized in various studies of material science and bioscience [1]. There exist several types of beam loss monitors (BLMs) based on different detection principles such as ionization (e.g., IC, PIN diodes, and diamonds), scintillation (photomultipliers with scintillators), secondary emission, and. The facility for rare isotope beams (FRIB) has developed the loss monitor ring (LMR) type BLM for monitoring the beam loss in the low-energy heavy-ion accelerators [8]. For hadron machines, currently IC is still the main BLM type (SNS, LHC, RHIC, ESS, etc.) [6,12,13,14] due to its robustness to radiation damage, large dynamic range, little maintenance, and ease for calibration. The beam loss monitoring system in the CSNS mainly applies two types of monitors based on IC and plasticscintillator respectively.

Design parameter
Particle-matter interactions
Simulation considerations and methods
The response functions of the CSNS BLM
Beam loss measurement in the mixed radiation field and Monte Carlo validation
Findings
CONCLUSION
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