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Classical Partition Identities and Basic Hypergeometric Series 13 in which the coefficient of x` qn reads as Y X P P 1 ` n k∈S mk q k∈S kmk [x`qn ] = [x q ] x 1 − xqk k∈S mk ≥0 k∈S = X P o Pk∈S mk = ` k∈S kmk = n 1. mk ≥0: k∈S The last sum enumerates the solutions of the system of Diophantine equations X mk = `    k∈S X   kmk = n  k∈S  which are the number of partitions 1m1 , 2m2 , · · · , nmn of n with exactly `-parts in S.  B1.2. Partitions into distinct parts in S. Next we study the generating functions of partitions into distinct parts in S. If we denote by Q(n|S) and Q` (n|S) the corresponding partition numbers with distinct parts from S, then their generating functions read respectively as ∞ X Y  1 + qk (B1.2a) Q(n|S) qn = n=0 X k∈S ` n Q` (n|S) x q = `,n≥0 Y  1 + xqk . (B1.2b) k∈S Proof. For the first identity, observing that X 1 + qk = qkmk mk =0,1 we can reformulate the product on the right hand side as Y Y X X P  1 + qk = qkmk = q k∈S kmk . k∈S mk =0,1 k∈S mk =0,1 k∈S Extracting the coefficient of qn , we obtain Y X P  [qn] 1 + qk = [qn] q k∈S kmk = k∈S mk =0,1 k∈S P X k∈S kmk =n mk =0,1: k∈S 1.