Abstract

The 3 GeV rapid cycling synchrotron (RCS) at Japan Proton Accelerator Research Complex is already in user operation stage, delivering a stable and relatively high power beam to the Material and Life Science Experimental Facility as well as to the main ring. RCS utilizes multiturn ${\mathrm{H}}^{\ensuremath{-}}$ charge-exchange injection for which a hybrid-type boron doped carbon stripper foil known as HBC foil with a thickness of around $200\text{ }\text{ }\ensuremath{\mu}\mathrm{g}/{\mathrm{cm}}^{2}$ is used at the present injection beam energy of 181 MeV. It will be changed to $290\text{ }\text{ }\ensuremath{\mu}\mathrm{g}/{\mathrm{cm}}^{2}$ at the near future upgrade and design injection beam energy of 400 MeV. The stripping efficiencies are expected to be 99.6% and 99.7% in the present and the later case, respectively. The remaining 0.4% or 0.3% of the beam is called the waste beam and is transported to the injection beam dump with a capacity of only 4 kW. The full power of the injected beam at 400 MeV is 133 kW, while the waste beam power is calculated to be about 0.4 kW. The raw signal measured by a current transformer placed downstream of the waste beam dump line contains a large noise and it is practically very hard to identify the beam signal. However, a fast Fourier transformation analysis of the raw signal made it possible to clearly identify the beam signal. The power spectrum is calibrated with respect to the known injected beam current. The absolute error of the monitor system is 0.2 mV, which gives the ratio of the waste beam to the injected beam as $(0.38\ifmmode\pm\else\textpm\fi{}0.03)%$. Such an accurate and realtime monitoring system provides quite an efficient method to know the conditions of the stripper foil and the incoming linac beam during the user operation.

Highlights

  • The 3 GeV rapid cycling synchrotron (RCS) at Japan Proton Accelerator Research Complex (J-PARC) is in user operation stage, delivering a stable and high power beam of 200 kW to the neutron target in the Material and Life Science Experimental Facility (MLF) as well as an equivalent beam power of more than 250 kW to the main ring (MR)

  • The remaining 0.4% or 0.3% of the unstripped beam is mostly partially stripped particles and it is neutral and is called H0 beam. They are further stripped to a proton beam by the secondary stripper foil placed about 2 m downstream from the primary stripper foil and transported to the injection beam dump

  • In the injection beam dump mode, the 1st foil is removed and all of the incoming HÀ beam is stripped to proton beam by using the 3rd foil and driven to the injection beam dump, whereas in the single-pass extraction mode the 1st foil is put in the right position so that most of the incoming HÀ beam is stripped to proton beam and is injected into the RCS ring but travels only one-third of the RCS circumference before being driven to the extraction beam dump [10]

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Summary

INTRODUCTION

The 3 GeV rapid cycling synchrotron (RCS) at Japan Proton Accelerator Research Complex (J-PARC) is in user operation stage, delivering a stable and high power beam of 200 kW to the neutron target in the Material and Life Science Experimental Facility (MLF) as well as an equivalent beam power of more than 250 kW to the main ring (MR). The primary stripper foil will be changed to a thickness of 290 g=cm at the upgraded injection energy of 400 MeV, where the stripping efficiency is expected to be. The remaining 0.4% or 0.3% of the unstripped beam is mostly partially stripped particles (single electron detachment) and it is neutral (uncharged) and is called H0 beam They are further stripped to a proton beam by the secondary stripper foil (named 2nd foil) placed about 2 m downstream from the primary stripper foil and transported to the injection beam dump. Data was taken with several experimental conditions and from the offline analysis a precise value of the measured stripping efficiency was given, which was found to be very consistent with the expectation Through such a precise measurement of the waste beam in the injection beam dump, the present idea is being used for online monitoring of the waste beam during RCS operation

H0CT AND THE EXPERIMENTAL SETUP
EXPERIMENTAL MEASUREMENT
ONLINE MONITORING
Findings
SUMMARY

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