Abstract

Thin carbon foils are used as strippers for charge exchange injection into high intensity proton rings. However, the stripping foils become radioactive and produce uncontrolled beam loss, which is one of the main factors limiting beam power in high intensity proton rings. Recently, we presented a scheme for laser stripping an ${\mathrm{H}}^{\ensuremath{-}}$ beam for the Spallation Neutron Source (SNS) ring. First, ${\mathrm{H}}^{\ensuremath{-}}$ atoms are converted to ${\mathrm{H}}^{0}$ by a magnetic field, then ${\mathrm{H}}^{0}$ atoms are excited from the ground state to the upper levels by a laser, and the excited states are converted to protons by a magnetic field. In this paper we report on the proof-of-principle demonstration of this scheme to give high efficiency (around 90%) conversion of ${\mathrm{H}}^{\ensuremath{-}}$ beam into protons at SNS in Oak Ridge. The experimental setup is described, and comparison of the experimental data with simulations is presented.

Highlights

  • Hÿ ion laser stripping was initially proposed by Zelensky et al in a paper [1] describing a 3-step stripping method: Hÿ conversion to H0, H0 excitation from ground to upper state, and H0to p conversion using photoionization

  • A variety of methods have been proposed to overcome this difficulty. Two of these proposals have become foundations for proofof-principle (POP) experiments: (i) the frequency sweep excitation [4]; (ii) the broadening of the upper levels by a magnetic field, which is Lorentz transformed to an electric field in the beam rest frame [5]

  • The first stripping was observed in March, 2006, and 50% efficiency was attained before operations were halted because of a leak in the vacuum chamber near the laser beam absorber

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Summary

Introduction

Hÿ ion laser stripping was initially proposed by Zelensky et al in a paper [1] describing a 3-step stripping method: Hÿ conversion to H0, H0 excitation from ground to upper state, and H0to p conversion using photoionization. Following this initial proposal of the method, modification of the first and third steps using Lorentz stripping was suggested [2]. Two of these proposals have become foundations for proofof-principle (POP) experiments: (i) the frequency sweep excitation [4]; (ii) the broadening of the upper levels by a magnetic field, which is Lorentz transformed to an electric field in the beam rest frame [5]

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