pellman
- 683
- 6
Suppose we have time-dependent operator a(t) with the equal-time commutator
[a(t),a^{\dag}(t)]=1
and in particular
[a(0),a^{\dag}(0)]=1
with Hamiltonian
H=\hbar \omega(a^\dag a+1/2)
The Heisenberg equation of motion
\frac{da}{dt}=\frac{i}{\hbar}[H,a]=-i\omega a
implies that a(t)=a_0e^{-i\omega t} where a_0 is a constant operator. Thus a^\dag a=e^{+i\omega t}a^\dag_0 a_0 e^{-i\omega t}=a^\dag_0 a_0 and so
H(t)=\hbar \omega(a^\dag_0 a_0+1/2)
for all times. Since a_0=a(0),
[a_0,a^{\dag}_0]=1
means that
\frac{i}{\hbar}[H(t),a_0]=-i\omega a_0
for all times. But this it so say that
\frac{da_0}{dt}=-i\omega a_0\neq 0
contradicting that a_0 is a constant. Where did I go wrong?
[a(t),a^{\dag}(t)]=1
and in particular
[a(0),a^{\dag}(0)]=1
with Hamiltonian
H=\hbar \omega(a^\dag a+1/2)
The Heisenberg equation of motion
\frac{da}{dt}=\frac{i}{\hbar}[H,a]=-i\omega a
implies that a(t)=a_0e^{-i\omega t} where a_0 is a constant operator. Thus a^\dag a=e^{+i\omega t}a^\dag_0 a_0 e^{-i\omega t}=a^\dag_0 a_0 and so
H(t)=\hbar \omega(a^\dag_0 a_0+1/2)
for all times. Since a_0=a(0),
[a_0,a^{\dag}_0]=1
means that
\frac{i}{\hbar}[H(t),a_0]=-i\omega a_0
for all times. But this it so say that
\frac{da_0}{dt}=-i\omega a_0\neq 0
contradicting that a_0 is a constant. Where did I go wrong?