To begin, we find certain formulas $Q(k,\alpha)= G_1^k(\alpha) G_2^k(\alpha)k = -1, 0, 1,…,9$. These yield that part of the total separability probability, , for generalized (real, complex, quaternionic,\ldots) two-qubit states endowed with random induced measure, for which the determinantal inequality holds. Here denotes a density matrix, obtained by tracing over the pure states in -dimensions, and , its partial transpose. Further, is a Dyson-index-like parameter with for the standard (15-dimensional) convex set of (complex) two-qubit states. For , we obtain the previously reported Hilbert-Schmidt formulas, with (the real case) , (the standard complex case) , and (the quaternionic case) $Q(0,2)= \frac{13}{323} P(0,\alpha)/2G_2^k(\alpha)$ are sums of polynomial-weighted generalized hypergeometric functions , , all with argument $z=\frac{27}{64} =(\frac{3}{4})^3$. We find number-theoretic-based formulas for the upper () and lower () parameter sets of these functions and, then, equivalently express in terms of first-order difference equations. Applications of Zeilberger’s algorithm yield “concise” forms, parallel to the one obtained previously for . For nonnegative half-integer and integer values of , has descending roots starting at . Then, we (C. Dunkl and I) construct a remarkably compact (hypergeometric) form for itself. The possibility of an analogous “master” formula for is, then, investigated, and a number of interesting results found.

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