Quantum Mechanics for Mathematicians

(lily) #1

wherek∈Sp(2d,R), then the automorphism Φkthat defines the Jacobi group
is given by the one studied in section 16.2


Φk

(((

cq
cp

)

,c

))

=

(

k

(

cq
cp

)

,c

)

(18.1)

Note that the Euclidean groupE(d) is a subgroup of the Jacobi groupGJ(d),
the subgroup of elements of the form
(((
0
cp


)

, 0

)

,

(

R 0

0 R

))

whereR∈SO(d). The ((
0
cp


)

, 0

)

⊂H 2 d+1

make up the groupRdof translations in theqjcoordinates, and the


k=

(

R 0

0 R

)

⊂Sp(2d,R)

are symplectic transformations since



(

k

(

cq
cp

)

,k

(

c′q
c′p

))

=Rcq·Rc′p−Rcp·Rc′q

=cq·c′p−cp·c′q

=Ω

((

cq
cp

)

,

(

c′q
c′p

))

(Ris orthogonal so preserves dot products).


18.3 Semi-direct product Lie algebras


We have seen that semi-direct product Lie groups can be constructed by taking
a productN×Kof Lie groups as a set, and imposing a group multiplication
law that uses an action ofK onNby automorphisms. In a similar manner,
semi-direct product Lie algebrasnokcan be constructed by taking the direct
sum ofnandkas vector spaces, and defining a Lie bracket that uses an action of
konnby derivations (the infinitesimal version of automorphisms, see equation
16.17).
Considering first the exampleE(d) =RdoSO(d), recall that elementsE(d)
can be written in the form (
R a
0 1


)

forR∈SO(d) anda∈Rd. The tangent space to this group at the identity will
be given by matrices of the form
(
X a
0 0


)
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