Quantum Mechanics for Mathematicians

(lily) #1

  • Mis identified withM+J 0 by equation 26.1, with basis elementqjgoing
    tozj, andpjtoizj.

  • Mis identified withM−J 0 by equation 26.2, with basis elementqjgoing
    tozj, andpjto−izj.

  • Mis identified with elements ofM+J 0 ⊕ M−J 0 that are invariant under
    conjugation, with basis elementqjgoing to√^12 (zj+zj) andpjto√i 2 (zj−
    zj).


26.2 Compatible complex structures and posi-


tivity


Our interest is in vector spacesMthat come with a symplectic structure Ω,
a non-degenerate antisymmetric bilinear form. To successfully use a complex
structureJfor quantization, it will turn out that it must be compatible with Ω
in the following sense:


Definition(Compatible complex structure).A complex structure onMis said
to be compatible withΩif


Ω(Jv 1 ,Jv 2 ) = Ω(v 1 ,v 2 ) (26.5)

Equivalently,J∈Sp(2d,R), the group of linear transformations ofMpreserv-
ingΩ.


The standard complex structureJ=J 0 is compatible with Ω, since (treating
thed= 1 case, which generalizes easily, and using equations 16.2 and 26.3)


Ω(J 0 (cqq+cpp),J 0 (c′qq+c′pp))

=

((

0 − 1

1 0

)(

cq
cp

))T(

0 1

−1 0

)((

0 − 1

1 0

)(

c′q
c′p

))

=

(

cq cp

)

(

0 1

−1 0

)(

0 1

−1 0

)(

0 − 1

1 0

)(

c′q
c′p

)

=

(

cq cp

)

(

0 1

−1 0

)(

c′q
c′p

)

=Ω(cqq+cpp,c′qq+c′pp)

More simply, the matrix forJ 0 is obviously inSL(2,R) =Sp(2,R).
Note that elementsgof the groupSp(2d,R) act on the set of compatible
complex structures by
J→gJg−^1 (26.6)


This takes complex structures to complex structures since


(gJg−^1 )(gJg−^1 ) =gJ^2 g−^1 =− 1
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