Natural Heisenberg algebras
Normal ordered product
Let π be a space carrying a representation of a natural Heisenberg algebra Λ π₯ π for π = β€ or π = β€ + 1 2 ,
and let π Β± denote the strictly positive and negative parts of π respectively.
The normal ordered product is a procedure for obtaining well-defined operators from infinite expressions.1 2
Definition
In general, if for πΌ β π₯ we have the formal sum of operators
πΌ ( π§ ) = β π β β€ πΌ ( π ) π§ β π
where πΌ ( π ) is a ^homogenous operator of degree π , we define lie
πΌ ( π§ ) Β± = 1 2 πΌ ( 0 ) [ 0 β π ] + β π β π Β± πΌ ( π ) π§ β π βΉ πΌ ( π§ ) = πΌ ( π§ ) + + πΌ ( π§ ) β
where we have used an Iverson bracket .
Then the normal ordered product is defined recursively for { πΌ π } π π = 1 β π₯ by
: πΌ 1 ( π§ ) : = πΌ 1 ( π§ ) : πΌ 1 ( π§ ) β― πΌ π ( π§ ) : = πΌ π ( π§ ) β : πΌ 1 ( π§ ) β― πΌ π β 1 ( π§ ) : + : πΌ 1 ( π§ ) β― πΌ π β 1 ( π§ ) : πΌ π ( π§ ) +
which induces a map π β π₯ β ( E n d β‘ π ) { π§ } .
In particular
: πΌ 1 ( π 1 ) πΌ 2 ( π 2 ) : = { πΌ 1 ( π 1 ) πΌ 2 ( π 2 ) π 1 β€ π 2 πΌ 2 ( π 2 ) πΌ 1 ( π 1 ) π 2 β€ π 1
and
: πΌ ( π§ ) π : = π β β = 0 ( π β ) ( π ( π§ ) β ) β ( π ( π§ ) + ) π β β
For π· β 1
Let π· β 1 be the inverse degree operator on π· ( ( E n d β‘ π ) { π§ } ) , so
π· β 1 πΌ ( π§ ) = π· β 1 πΌ ( π§ ) + + π· β 1 πΌ ( π§ ) β : π· β 1 πΌ 1 ( π§ ) : = π· β 1 πΌ 1 ( π§ ) : π· β 1 πΌ 1 ( π§ ) β― π· β 1 πΌ π ( π§ ) : = π· β 1 πΌ π ( π§ ) β : π· β 1 πΌ 1 ( π§ ) β― π· β 1 πΌ π β 1 ( π§ ) : = + : π· β 1 πΌ 1 ( π§ ) β― π· β 1 πΌ π β 1 ( π§ ) : π· β 1 πΌ π ( π§ ) +
and
: e x p β‘ π· β 1 πΌ ( π§ ) : = β π β β 0 : ( π· β 1 πΌ ( π§ ) ) π : π !
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