Abstract

Electron cyclotron resonance ion sources based charge breeders (ECR-CB) are fundamental devices for Isotope Separation On Line (ISOL) facilities aiming at postaccelerating radioactive ion beams (RIBs). Presently, low intensity RIBs do not allow a conventional tuning of the ECR-CB: as a consequence, it has to be set with a stable 1+ pilot beam first, switching then to the radioactive one without changing any parameter; this procedure is usually called ``blind tuning.'' Besides having different masses, pilot and radioactive beams can also differ in terms of the rms transverse emittance ${\ensuremath{\epsilon}}_{\mathrm{rms}}$ and/or longitudinal energy spread $\mathrm{\ensuremath{\Delta}}E$, so the choice of a given pilot beam can determine the overall performances of the final breeding stage. This paper shows a numerical study of how the capture efficiency of the PHOENIX charge breeder is affected by the aforementioned beam paramaters: the analysis reveals the two-step nature of the process, highlighting the role of the injection optics and the plasma capture capability in the overall performances of this device. The simulations predict highest efficiency for ${\ensuremath{\epsilon}}_{\mathrm{rms}}l5\ensuremath{\pi}\text{ }\text{ }\mathrm{mm}\text{ }\mathrm{mrad}$ and $\mathrm{\ensuremath{\Delta}}El5\text{ }\text{ }\mathrm{eV}$ in a optimum energy range between 2 and 6 eV, thus giving important information on the possibility of blindly tuning an ECR-CB. No isotopical effects were observed, while it clearly came out the necessity to improve the $1+$ beam characteristics with a rf beam cooler prior to the injection into an ECR-CB.

Highlights

  • The European road map of nuclear physics is going through the development of second generation facilities pointing to EURopean Isotope Separation On Line (ISOL) radioactive ion beam facility (EURISOL) [1]: presently, three main projects are ongoing in different Laboratories, High Intensity and Energy-Isotope Separator On Line DEvice (ISOLDE) at CERN [2], Système de Production d’Ions Radioactifs Accélérés en Ligne 2 (SPIRAL2) at Grand accélérateur national d’ions lourds [3], and Selective Production of Exotic Species (SPES) at Istituto Nazionale di Fisica Nucleare-Legnaro National Laboratories (INFN-LNL) [4]

  • An important question arises: what happens to the charge breeder capture efficiency if the stable and radioactive beams have not the same properties? Or, equivalently, to what extent can an ECR-CB be blindly tuned? This paper tries to answer this question: a numerical code describing the charge breeding process is available at INFN, and has been used to analyze the effect of different beam parameters on the charge breeding efficiency: in particular, the transverse beam emittance, the longitudinal energy spread and the mass of the injected ions

  • The first part of the analysis concerned the influence of the beam rms transverse emittance εrms on the capture efficiency: to this purpose, further simulations were carried out giving to this parameter the values εrms 1⁄4 1, 2, 5 and 10π mm mrad, keeping the same Twiss parameters mentioned in the previous section

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Summary

Introduction

The European road map of nuclear physics is going through the development of second generation facilities pointing to EURopean ISOL radioactive ion beam facility (EURISOL) [1]: presently, three main projects are ongoing in different Laboratories, High Intensity and Energy-Isotope Separator On Line DEvice (ISOLDE) at CERN [2], Système de Production d’Ions Radioactifs Accélérés en Ligne 2 (SPIRAL2) at Grand accélérateur national d’ions lourds [3], and Selective Production of Exotic Species (SPES) at Istituto Nazionale di Fisica Nucleare-Legnaro National Laboratories (INFN-LNL) [4]. The low intensity RIBs, presently injected in an ECR-CB, do not allow a real tuning of this device: as a consequence, it has to be set with a stable beam first, switching to the radioactive one, having usually a different mass, without changing any parameter (injection optics included); this technique is known as “blind tuning” [9]. By applying this procedure, an important question arises: what happens to the charge breeder capture efficiency if the stable and radioactive beams have not the same properties? The results and the following data analysis will be shown throughout the paper

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Discussion
Conclusion
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