Abstract

The ASACUSA (Atomic Spectroscopy And Collisions Using Slow Antipro- tons) collaboration of CERN is currently attempting to measure the antiproton-nucleus in-flight annihilation cross sections on thin target foils of C, Pd, and Pt at 130 keV of kinetic energy. The low-energy antiprotons were supplied by the Antiproton Decelera- tor (AD) and a radio-frequency quadrupole decelerator. For this measurement, a beam profile monitor based on secondary electron emission was developed. Data from this monitor was used to ensure that antiprotons were precisely tuned to the position of an 80- mm-diameter experimental target, by measuring the spatial profile of 200-ns-long beam pulses containing 10 5 10 6 antiprotons with an active area of 40 mm 40 mm and a spa- tial resolution of 4 mm. By using this monitor, we succeeded in finely tuning antiproton beams on the target, and observed some annihilation events originating from the target.

Highlights

  • Several groups have previously measured the cross sections of in-flight antiprotons annihilating on targets of various mass numbers at kinetic energies E > 600 keV, by using the Low Energy Antiproton Ring (LEAR) at CERN [1,2,3,4,5,6]

  • The 5.3-MeV antiprotons provided by the Antiproton Decelerator (AD) of CERN was allowed to pass through a radiofrequency quadrupole decelerator (RFQD), which reduced the kinetic energy of 30 % of the antiprotons to 130 keV

  • Despite the simplicity and low cost of this monitor, it had adequate sensitivity to measure the profiles of beams containing ∼104 antiprotons

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Summary

Introduction

Several groups have previously measured the cross sections of in-flight antiprotons annihilating on targets of various mass numbers at kinetic energies E > 600 keV, by using the Low Energy Antiproton Ring (LEAR) at CERN [1,2,3,4,5,6]. The ASACUSA (Atomic Spectroscopy And Collisions Using Slow Antiprotons) collaboration of CERN measured the antiproton-nucleus annihilation cross sections with targets of Mylar, Ni, Sn, and Pt at E = 5.3 MeV [7, 8] These experimental results were consistent with the prediction of a modified black-disk model, which implies that the antiproton is strongly absorbed near the nuclear surface, and that the real potential is weaker compared to the imaginary one [9]. In this experiment, the 5.3-MeV antiprotons provided by the Antiproton Decelerator (AD) of CERN was allowed to pass through a radiofrequency quadrupole decelerator (RFQD), which reduced the kinetic energy of 30 % of the antiprotons to 130 keV. This monitor was a secondary electron emission detector with an active area of 40 mm × 40 mm and a spatial resolution of 4 mm

Beam Profile Monitor
Findings
Conclusion
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