Here we investigate the decay patterns of the low-lying hidden strangeness nucleon resonances (≡ N ss ) to the strangeness channels by employing the chiral Lagrangian approach, where the N ss states are treated as compact pentaquark states. The S-wave decays of these states to the P B (pseudoscalar meson and baryon) and V B (vector meson and baryon) channels are studied.According to the obtained masses and decay properties, we find four states, namely, N ss (1874) with quantum numbers I(J P ) = 1/2(1/2 − ), N ss (1885) with I(J P ) = 1/2(3/2 − ), N ss (2327) with I(J P ) = 1/2(1/2 − ), and N ss (2252) with I(J P ) = 1/2(3/2 − ), may be associated to the well established nucleon resonances N * (1895), N * (1875), and the newly predicted N * (2355) and N * (2250) by CLAS collaboration, respectively. In addition, several other obtained hidden strangeness nucleon resonances may be expected to be dominant components of the predicted missing resonances in the literatures. * Electronic address: gli@mail.qfnu.edu.cnRecently, triggered by the observation of the P + c pentaquark states, the hidden strange pentaquark states as η ′ N and φN bound states [26], KΣ * and K * Σ bound states [27,28], and compact five-quark states [29] were investigated. In Ref. [30], a possible φp resonance was investigated in the Λ + c → π 0 φp decay by considering a triangle singularity mechanism, where the obtained φp invariant mass distribution agrees with the existing data. It is very