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Quantification of Oxygen and Carbon in Calcium Targets for Reliable Ca$(p,pα)$ Measurements

Junki Tanaka, Riku Matsumura, Taichi Miyagawa

Abstract

Reliable extraction of Ca$(p,pα)$ cross sections requires accurate correction for oxygen and carbon impurities in calcium targets. In this work, the relative amounts of these light elements in $^{40,42,44,48}$Ca targets are determined using 65-MeV proton elastic scattering, where the Ca/Mylar yield ratios provide a direct measure of the corresponding O and C atomic ratios. These experimentally determined ratios are then applied to the 392-MeV $(p,pα)$ spectra to subtract the O and C contributions in a fully data-driven manner. The method does not rely on assumptions about absolute contamination levels or reaction-model calculations, and enables a consistent and reliable determination of Ca$(p,pα)$ yields across the calcium isotopic chain.

Quantification of Oxygen and Carbon in Calcium Targets for Reliable Ca$(p,pα)$ Measurements

Abstract

Reliable extraction of Ca cross sections requires accurate correction for oxygen and carbon impurities in calcium targets. In this work, the relative amounts of these light elements in Ca targets are determined using 65-MeV proton elastic scattering, where the Ca/Mylar yield ratios provide a direct measure of the corresponding O and C atomic ratios. These experimentally determined ratios are then applied to the 392-MeV spectra to subtract the O and C contributions in a fully data-driven manner. The method does not rely on assumptions about absolute contamination levels or reaction-model calculations, and enables a consistent and reliable determination of Ca yields across the calcium isotopic chain.
Paper Structure (6 equations, 4 figures, 2 tables)

This paper contains 6 equations, 4 figures, 2 tables.

Figures (4)

  • Figure 1: The Grand Raiden spectrometer was positioned at a laboratory angle of $\theta_{\rm lab}=28^\circ$ with respect to the beam axis. Elastically scattered protons were transported to the focal plane and measured using drift chambers for position determination and plastic scintillators for energy-loss and timing measurements. Identical spectrometer settings were employed for the Ca and Mylar targets to ensure identical kinematic and acceptance conditions.
  • Figure 2: Grand Raiden focal-plane $X$ position distributions corresponding to the energy spectra of protons from 65-MeV elastic scattering on the Mylar, $^{\rm nat}$Ca, $^{42}$Ca, $^{44}$Ca, and $^{48}$Ca targets.
  • Figure 3: $(p,p\alpha)$$S_\alpha$ spectrum for the ${}^{44}$Ca target. The black curve shows the measured spectrum. The blue and green curves indicate the estimated ${}^{16}$O$(p,p\alpha)$ and ${}^{12}$C$(p,p\alpha)$ contributions, respectively, scaled from the Mylar reference data. The red curve represents their sum.
  • Figure 4: $(p,p\alpha)$$S_\alpha$ spectrum for the ${}^{40}$Ca target. The black curve shows the measured spectrum. The blue and green curves indicate the estimated ${}^{16}$O$(p,p\alpha)$ and ${}^{12}$C$(p,p\alpha)$ contributions, respectively, scaled from the Mylar reference data. The red curve represents their sum.