Abstract
The angular variation of the ghost anomaly is found to be identical to that of the $^{8}\mathrm{Be}$ ground state for the reaction $^{9}\mathrm{Be}(d,t)^{8}\mathrm{Be}$ at ${E}_{d}=2.5$ MeV. The anomaly is absent from deuteron spectra of the reaction $^{6}\mathrm{Li}(\ensuremath{\alpha},d)^{8}\mathrm{Be}$, but present in spectra from the reactions $^{7}\mathrm{Li}(\ensuremath{\alpha},t)^{8}\mathrm{Be}$ and $^{9}\mathrm{Be}(p,d)^{8}\mathrm{Be}$. End points of possible three-particle reactions lie close to the observed anomaly so the interpretation is doubtful.
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