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-rw-r--r--latex/know/concept/dirac-notation/source.md12
1 files changed, 6 insertions, 6 deletions
diff --git a/latex/know/concept/dirac-notation/source.md b/latex/know/concept/dirac-notation/source.md
index 7b384ab..47aa370 100644
--- a/latex/know/concept/dirac-notation/source.md
+++ b/latex/know/concept/dirac-notation/source.md
@@ -14,13 +14,13 @@ and therefore cannot be added, but every bra has a corresponding ket and
vice versa.
Bras and kets can only be combined in two ways: the *inner product*
-$\braket{V | W}$, which returns a scalar, and the *outer product*
+$\braket{V}{W}$, which returns a scalar, and the *outer product*
$\ket{V} \bra{W}$, which returns a mapping $\hat{L}$ from kets $\ket{V}$
to other kets $\ket{V'}$, i.e. a linear operator. Recall that the
Hilbert inner product must satisfy:
$$\begin{aligned}
- \braket{V | W} = \braket{W | V}^*
+ \braket{V}{W} = \braket{W}{V}^*
\end{aligned}$$
So far, nothing has been said about the actual representation of bras or
@@ -40,10 +40,10 @@ $$\begin{aligned}
\end{bmatrix}
\end{aligned}$$
-The inner product $\braket{V | W}$ is then just the familiar dot product $V \cdot W$:
+The inner product $\braket{V}{W}$ is then just the familiar dot product $V \cdot W$:
$$\begin{gathered}
- \braket{V | W}
+ \braket{V}{W}
=
\begin{bmatrix}
v_1^* & \cdots & v_N^*
@@ -91,7 +91,7 @@ $$\begin{aligned}
Consequently, the inner product is simply the following familiar integral:
$$\begin{gathered}
- \braket{f | g}
+ \braket{f}{g}
= F[g(x)]
= \int_a^b f^*(x) \: g(x) \dd{x}
\end{gathered}$$
@@ -115,5 +115,5 @@ $$\begin{aligned}
\\
&= \Big( \int_a^b u^*(x) \: f(x) \dd{x} \Big) \Big( \int_a^b g^*(\xi) \: w(\xi) \dd{\xi} \Big)
\\
- &= \braket{u | f} \braket{g | w}
+ &= \braket{u}{f} \braket{g}{w}
\end{aligned}$$