最終更新日:2022/12/23
例文
In
Chaps.
3,
4,
and
5,
we
saw
that
for
each
spin
type,
the
Schrödinger
picture
wave
equation
for
a
state
and
the
Heisenberg
picture
wave
equation
for
the
associated
quantum
field
had
the
same
form.
In
the
former
case,
the
wave
equation
solution
was
a
state,
i.e.,
a
particle
wave
function.
In
the
latter,
the
wave
equation
solution
was
a
quantum
field,
i.e.,
an
operator
that
created
and
destroyed
states.
For
free
scalars,
this
equation
was
the
Klein-Gordon
equation;
for
spinors,
it
was
the
(no
interactions)
Dirac
equation;
and
for
massless
vectors
(photons),
it
was
Maxwell’s
equation
(sourceless,
in
terms
of
A^𝜇).
復習用の問題
In Chaps. 3, 4, and 5, we saw that for each spin type, the Schrödinger picture wave equation for a state and the Heisenberg picture wave equation for the associated quantum field had the same form. In the former case, the wave equation solution was a state, i.e., a particle wave function. In the latter, the wave equation solution was a quantum field, i.e., an operator that created and destroyed states. For free scalars, this equation was the Klein-Gordon equation; for spinors, it was the (no interactions) Dirac equation; and for massless vectors (photons), it was Maxwell’s equation (sourceless, in terms of A𝜇).
項目の編集設定
- 項目の編集権限を持つユーザー - すべてのユーザー
- 項目の新規作成を審査する
- 項目の編集を審査する
- 項目の削除を審査する
- 重複の恐れのある項目名の追加を審査する
- 項目名の変更を審査する
- 審査に対する投票権限を持つユーザー - 編集者
- 決定に必要な投票数 - 1
例文の編集設定
- 例文の編集権限を持つユーザー - すべてのユーザー
- 例文の削除を審査する
- 審査に対する投票権限を持つユーザー - 編集者
- 決定に必要な投票数 - 1
問題の編集設定
- 問題の編集権限を持つユーザー - すべてのユーザー
- 審査に対する投票権限を持つユーザー - 編集者
- 決定に必要な投票数 - 1