Formal delta
The formal delta over a field
given by the Fourier series expansion of the Dirac delta.
Properties
Let
Let
Note these fail for non-integer powers.
Proof of 1β6
First we prove ^P1. Consider the special case
. Then π£ ( π§ ) = π£ π π§ π π£ ( π§ ) πΏ ( π π§ ) = ( π£ π π§ π ) ( β π β β€ π π π§ π ) = β π β β€ π π π£ π π§ π + π = β π β β€ π π β π π£ π π§ π = ( π β π π£ π ) ( β π β β€ π π π§ π ) = π£ ( π β 1 ) πΏ ( π π§ ) whence follows ^P1 by linearity. The proof of ^PA is similar. Let
. Then π ( π§ 1 , π§ 2 ) = β π , π β β€ π§ π 1 π§ π 2 π ( π§ 1 , π§ 2 ) πΏ ( π π§ 1 / π§ 2 ) = ( β π , π β β€ π₯ ( π , π ) π§ π 1 π§ π 2 ) ( β π β β€ π π π§ π 1 π§ β π 2 ) = β π , π , π β β€ π π π₯ ( π , π ) π§ π + π 1 π§ π β π 2 = β π , π , π β β€ π π β π π₯ ( π , π ) π§ π 1 π§ π + π β π 2 = π ( π β 1 π§ 2 , π§ 2 ) πΏ ( π π§ 1 / π§ 2 ) Then ^P3 and ^PC follow by taking appropriate derivatives, and ^P2 and ^PB are special cases.
Footnotes
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1988. Vertex operator algebras and the Monster, Β§2.1βΒ§2.2, p. 52ff β©