In General > s.a. annihilation [modified
versions]; fock
space [number
operator, generalizations]; Normal Order.
* Idea: An operator that
adds a quantum to a (free) field in quantum field theory, or raises the energy
of an oscillator by one level in quantum mechanics.
* In quantum mechanics:
The raising operator for the i-th degree of freedom of a system; Depends
on the choice of a parameter
,
and can
be expressed as
ai = (
i /2
)1/2 qi – i
(1/2![]()
i)1/2 pi ;
A choice of
is equivalent to a choice of complex structure on phase
space.
* Properties: Bosonic
ones satisfy the commutation relations [ak
, ak
'
]
=
0, [ak, ak
'
]
=
kk' and,
for general powers (with n
m)
a
nan
= N (N–1) ··· (N–n+1)
, [an, a
m]
=
k=1n k!
{m \choose k}{n \choose k} a
(m–k) a(n–k)
;
Fermionic ones satisfy the commutation relations {bk, bk'
}
=
kk'.
@ References: Szafraniec RPMP(07)
[characterizations]; Kim et al PRL(08)-a0901 [commutation
relations, for photons, proposed
experiment].
For Different Theories > s.a. Ladder
Operators; quantum
dirac fields.
* Harmonic oscillator:
One normally chooses
= m
,
so H = ![]()
(a
a +
1/2); In the holomorphic representation,
a:= (1/
)
(
+ d/d
)
, a
:=
(1/
)
(
– d/d
)
, where
:=
(m
/
)1/2 x ;
Other relationships are that q = (
/2m
)1/2 (a + a
); L3 =
i
(a2
a1 – a1
a2).
* In quantum field theory:
The operator ak
corresponding
to the coefficient of a negative-frequency mode in a field expansion
(x)
=
k (ak uk(x)
+ a*k u*k(x))
;
In a Fock space
(
):=
{
= (
0,
1,
2,
3,...)},
the creation operator a
(
)
associated with any
is
the adjoint of the corresponding annihilation operator a(
),
a
(
)
:=
(0,
0
,
1
,
2
,...)
; basically, a
|n
=
(n+1)1/2 |n+1
.
@ References: Odake & Sasaki JMP(06)qp [solvable systems].
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send feedback and suggestions to bombelli at olemiss.edu – modified 9
jun 2009