Abstract
The angular distribution of proton-${}^{9}$C elastic scattering at 277--300 MeV/nucleon was measured with a newly designed recoil proton spectrometer. The angular distribution was analyzed using the relativistic impulse approximation. The root-mean-square matter radius of ${}^{9}$C was deduced to be $2.{43}_{\ensuremath{-}0.28}^{+0.55}$ fm with different two-parameter Fermi density distributions for protons and neutrons.
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