Abstract
The cluster theory which is developed to describe the glassy phase of Rb1−x(NH4)xH2PO4 is extended to explain the anomalous behaviour in the dielectric susceptibility χ of this phase. It is shown that χ begins to deviate from the normal value of the paraelectric phase at and below the glass transition temperature Tg, and the deficient part of the susceptibility below Tg is precisely proportional to the glass order parameter properly redefined.