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\begin{center}
\begin{tabular}{|p{4cm}|p{7.3cm}|p{7.3cm}|}
\hline
Положение & Вместо & Должно быть \\
\hline

&&\\[-1ex]
IV-1989(3), 113, Н:15
& $-i\chi(-\mbox{\textbf r})$
& $-i \textcolor{red}{(-1)^{-l^\prime}} \chi(-\mbox{\textbf r})$
\\

&&\\[-1ex]
IV-1989(3), 114, Н:7
& значения $\textcolor{red}{i} \pm 1/2$ : \dots
& значения $\textcolor{red}{j} \pm 1/2$ : \dots
\\

&&\\[-1ex]
IV-1989(3), 152, В:2
& \dots в виде $\varepsilon \, {\bf \textcolor{red}{p}}_{\mbox{\small шр}} = \hat H
  \varphi_{\mbox{\small шр}}$ \dots
&  \dots в виде $\varepsilon \, \textcolor{red}{\varphi}_{\mbox{\small шр}} = \hat H
  \varphi_{\mbox{\small шр}}$ \dots
\\

&&\\[-1ex]
IV-1989(3), 165, (36,15)
& $\left.\begin{array}{l}f\\g\end{array}\right\}
=\textcolor{red}{2^{3/2} \sqrt{\frac{m\pm\varepsilon}{\varepsilon}}} \; e^\frac{\pi\nu}{2}\dots $
& $\left.\begin{array}{l}f\\g\end{array}\right\}
=\textcolor{red}{2^{1/2} \sqrt{\frac{\varepsilon\pm m}{\varepsilon}}} \; e^\frac{\pi\nu}{2}\dots $
\\

&&\\[-1ex]
IV-1989(3), 225, (52,3)
&  $\langle n', l-1 || r || n l \rangle = i \sqrt{l}
  \frac{(-1)^{n'-\textcolor{red}{1}}}{4(2l-1)!} \dots$
& $\langle n', l-1 || r || n l \rangle = i \sqrt{l}
  \frac{(-1)^{n'-\textcolor{red}{l}}}{4(2l-1)!} \dots$
\\

&&\\[-1ex]
IV-1989(3), 225, (52,4)
& $|\langle 2 p || r || n d \rangle |^2 = \frac{2^{\textcolor{red}{19}} n^9
  (n^2-1)(n-2)^{2n-7}}{(n+2)^{2n+7}}$
& $|\langle 2 p || r || n d \rangle |^2 = \frac{2^{\textcolor{red}{20}} n^9
  (n^2-1)(n-2)^{2n-7}}{(n+2)^{2n+7}}$
\\

&&\\[-1ex]
IV-1989(3), 226, (52,6)
& $\langle n, l-1 || r || n l \rangle = i
\sqrt{l} \cdot \frac{3}{2} \; n \; \sqrt{n^2-l^2}$
& $\langle n, l-1
|| r || n l \rangle = \textcolor{red}{-}i \sqrt{l} \cdot
\frac{3}{2} \; n \; \sqrt{n^2-l^2}$
\\

&&\\[-1ex]
IV-1989(3), 227, (52,9)
& $|\langle n' l' || r || n l \rangle |^2 \sim
\frac{\textcolor{red}{3}}{n'^3}$
& $|\langle n' l' || r || n l \rangle |^2 \sim
\frac{\textcolor{red}{1}}{n'^3}$
\\

&&\\[-1ex]
IV-1989(3), 612, В:3-4
& \dots размер атома пропорционален $Z e^2$ \dots
& \dots размер атома \textcolor{red}{обратно} пропорционален $Z e^2$ \dots
\\

&&\\[-1ex]
IV-1989(3), 612, ф-ла без номера после В:9
& $\langle n l m | \Delta \Phi | n l m \rangle = \dots$
& $\textcolor{red}{e} \, \langle  n l m | \Delta \Phi | n l m \rangle =
\dots$
\\

&&\\[-1ex]
IV-1989(3), 614, (124,2)
& $\delta E_{nl} = -\frac{2}{3\pi} \, \alpha^3 m_\mu Z Q_{nl} \left(
  \frac{m_e}{Z\alpha m_\mu} \right)$
& $\delta E_{nl} = -\frac{2}{3\pi} \, \alpha^3 m_\mu Z^{\textcolor{red}{2}} Q_{nl} \left(
  \frac{m_e}{Z\alpha m_\mu} \right)$
\\

&&\\[-1ex]
IV-1989(3), 615, ф-лы без номера после В:2
& $\frac{\delta E_{10}}{|E_{10}|}
  =
  \textcolor{red}{-6,4 \cdot 10^{-3}} \;,
  \quad
  \frac{\delta E_{20}}{|E_{20}|}
  =
  \textcolor{red}{-2,8 \cdot 10^{-4}} \;,
  \dots$
& $\frac{\delta E_{10}}{|E_{10}|}
  =
  \textcolor{red}{-8,4 \cdot 10^{-4}} \;,
  \quad
  \frac{\delta E_{20}}{|E_{20}|}
  =
  \textcolor{red}{-4,0 \cdot 10^{-4}} \;,
  \dots$
\\

\hline

\end{tabular}
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