Continuous spin field in the AdS$_6$ space (Part II)

Part II. Derivation of Operator Constraints Defining the Representation Building on the geometric formulation from Part I, this part of our talk is devoted to a system of operator constraints generalizing the flat space case. We will shown that these constraints form a closed algebra and fix the Casimir operators, whose eigenvalues are determined by the parameters $\mu$ and $s$.