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We provide a series of arguments which support the idea that the peak seen inthe $\gamma p \to K^+ \Lambda$ reaction around 1920 MeV should correspond tothe recently predicted state of $J^P=1/2^+$ as a bound state of $K \bar{K}N$with a mixture of $a_0(980)N$ and $f_0(980)N$ components. At the same time wepropose polarization experiments in that reaction as a further test of theprediction, as well as a study of the total cross section for $\gamma p \to K^+K^- p$ at energies close to threshold and of $d \sigma/d M_{inv}$ for invariantmasses close to the two kaon threshold.

Searching for signatures around 1920 MeV of a $N^*$ state of three hadron nature