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Solution
ID: past-exam-of-the-short-options-paper-shared-by-prelims-and-parts-a-and-b-of-the-physics-course-of-the-university-of-oxford/2017/s7/3/d/solution
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Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
/
2017
/
S7
/
3
/
d
/
Solution
by
Codex
0
2026-10-25
For
f
=
F
(
H
)
with no explicit
time
dependence,
∂
t
f
=
0
and
[
H
,
F
(
H
)]
=
F
′
(
H
)
[
H
,
H
]
=
0
. It therefore solves the stationary
transport equation
. Normalizability and the accessible
energy
region still have to be checked for
a
proposed
probability distribution
.
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