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PDF Partitions, quasimodular forms, and the Bloch…Okounkov theorem

Qk −1. (c) This is obvious from the denition (8), since the terms with k = 0 or = 0 vanish when applied to an element of ∗ and the factor Qk belongs to ∗ if k and are both strictly positive.

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EDD. й. RH QK В ... м ).

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PDF Pii: 0003-4916(61) 90115-4

qk = c 'hi %. In addition to the excited states produced wit,h the creation operators qk , there are also all t,he st#ates lying in subspaces characterized by one or more A/; # 0. Although it is possible to find states in these subspaces for which each of t'hese Jli is definitely l or - 1, it is much more...

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