21.3. HILBERTSPACE 325
asamatrixequationintheX-representation:
<x|[X,P]|y> = <x|XP|y>−<x|PX|y>
= <x|XIP|y>−<x|PIX|y>
= <x|X
{∫
dx|z><z|
}
P|y>−<x|P
{∫
dx|z><z|
}
X|y>
=
∫
dz [<x|X|z><z|P|y>−<x|P|z><z|X|y>]
=
∫
dz
[
xδ(x−z)
(
−i ̄h
∂
∂z
δ(z−y)
)
−
(
−i ̄h
∂
∂x
δ(x−z)
)
zδ(z−y)
]
= −i ̄h
[
x
∂
∂x
δ(x−y)−y
∂
∂x
δ(x−y)
]
= −i ̄hδ(x−y)
[
−
∂
∂x
x+y
∂
∂x
]
= i ̄hδ(x−y) (21.137)
(In thenext tolast line, the derivative isunderstoodto beacting onsome func-
tionofxstandingtototheright). Thisexampleisanillustrationofthefactthat
thematrixrepresentationofaproductofoperatorsisequaltotheproductofmatrix
representationsofeachoperator,i.e.
<φm|AB|φn> =
∑
k
<φm|A|φk><φk|B|φn>
[AB]mn =
∑
k
AmkBkn (21.138)
- TheP-representation
TakingtheinnerproductoftheeigenvalueequationP|p 0 >=p 0 |p 0 >withthe
bra<p|,wehavethemomentumeignfunctionsinthemomentum-representation
ψp 0 (p)=<p|p 0 >=δ(p−p 0 ) (21.139)
Theeigenstatesofpositionaregivenby
ψx 0 (p) = <p|x 0 >
= <x 0 |p>∗
= ψp(x)∗
=
1
√
2 π ̄h
e−ip^0 x/ ̄h (21.140)