Htime independent is the quantum mechanical equivalent of the
rotating frame transformation in the Bloch picture.
Asimilarity transformationapplied to the laboratory frame density
operatorgenerates a transformed density operatorr, such that
r¼UU^1 , ½ 2 : 59
in which U is an operator. A unitary operator is defined by the
relationshipU–1¼Uy.IfUis a unitary operator, then [2.59] is called a
unitary transformation. The equation of motion forris described by
drðtÞ
dt
¼i½He,rðtÞ, ½ 2 : 60
in whichHeis a transformed Hamiltonian. The form of He can be
established as follows:
dr
dt
¼
dUU^1
dt
¼U
d
dt
U^1 þ
dU
dt
U^1 þU
dU^1
dt
¼iU½,HU^1 þ
dU
dt
U^1 UU^1 þUU^1 U
dU^1
dt
¼iU½,HU^1 þ
dU
dt
U^1 rþrU
dU^1
dt
: ½ 2 : 61
The common technique of insertingE¼U–1Uhas been utilized. To
proceed, the following identities are established:
dE
dt
¼
dUU^1
dt
¼
dU
dt
U^1 þU
dU^1
dt
¼0, ½ 2 : 62
which yields
dU
dt
U^1 ¼U
dU^1
dt
, ½ 2 : 63
and
U½,HU^1 ¼UðÞHHU^1 ¼UU^1 UHU^1 UHU^1 UU^1
¼ r,UHU^1
:
½ 2 : 64
44 CHAPTER 2 THEORETICALDESCRIPTION OFNMR SPECTROSCOPY