基礎物理学選書5B.量子力学(Ⅱ)

著作者：小出昭一郎
発行所：裳華房

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p.13　(19)式　“\(\varphi_{1'}(\boldsymbol{r}_1)\)”→“\(\varphi_{l'}(\boldsymbol{r}_1)\)”
p.29　“\(\int\cdots\int\varPhi^*Q(\tau_1,\tau_2,\cdots,\tau_N)\varPhi'd\tau_1\cdots d\tau_N\)”→“\(\int\cdots\int\varPhi^*Q(\tau_1,\tau_2,\cdots,\tau_N)\varPhi d\tau_1\cdots d\tau_N\)”
p.38　l.8　“（17～18ページ）”→“（18ページ）”
p.50　“§9.2 [例題 2]（17ページ）”→“§9.2 [例題 2]（16～17ページ）”
p.63　l.22　“わかるが（読者みずから検証せよ）．”→“わかる（読者みずから検証せよ）．”
p.66　l.10　“\(\mid{}^3\varPhi\rangle\)”→“\(\mid{}^3\varPhi_0\rangle\)”
p.74　l.7　“\(\|\begin{matrix}\varphi_l&\varphi_{-l}&\cdots&\varphi_{-l}\end{matrix}\|\)”→“\(\|\begin{matrix}\varphi_l&\varphi_{l-1}&\cdots&\varphi_{-l}\end{matrix}\|\)”
p.76　10-5表　“\(\frac{1}{\sqrt{2}}\left(\left|\begin{array}{cc}\varphi_1&\bar{\varphi}_)\end{array}\right|+\left|\begin{array}{cc}\bar{\varphi}_1&\varphi_0\end{array}\right|\right)\)”→“\(\frac{1}{\sqrt{2}}\left(\left|\begin{array}{cc}\varphi_1&\bar{\varphi}_0\end{array}\right|+\left|\begin{array}{cc}\bar{\varphi}_1&\varphi_0\end{array}\right|\right)\)”
“\(|\begin{array}{cc}\bar{\varphi}_0&\bar{\varphi}_{-1}\end{array}|)\)”→“\(|\begin{array}{cc}\bar{\varphi}_0&\bar{\varphi}_{-1}\end{array}|\)”
p.84　l.4　“\(\delta_{J,M}\)”→“\(\varPhi_{J,M}\)”
p.90　(6 c)　“\(\begin{eqnarray}\left\{\begin{array}{1}k_y=\frac{2\pi}{L}n_y\\k_x=\frac{2\pi}{L}n_x\\k_z=\frac{2\pi}{L}n_z\end{array}\right.\end{eqnarray}\)”→“\(\begin{eqnarray}\left\{\begin{array}{1}k_x=\frac{2\pi}{L}n_x\\k_y=\frac{2\pi}{L}n_y\\k_z=\frac{2\pi}{L}n_z\end{array}\right.\end{eqnarray}\)”
p.98　“規格化されて完全直交関数系”→“規格化された完全直交関数系”
p.110　l.1　“\(b_{\boldsymbol{k}\ \uparrow}=u_{\boldsymbol{k}}a_{\boldsymbol{k}\ \uparrow}-v_{\boldsymbol{k}}{a_{-\boldsymbol{k}\ \downarrow}}^*\)”→“\(b_{\boldsymbol{k}\ \uparrow}=u_ka_{\boldsymbol{k}\ \uparrow}-v_k{a_{-\boldsymbol{k}\ \downarrow}}^*\)”
l.15　(10 a)　“\(b_{k\ \downarrow}\)”→“\(b_{\boldsymbol{k}\ \downarrow}\)”
p.111　l.3　“\(u_kv_k({a_{\boldsymbol{k}\ \uparrow}}^*{a_{-\boldsymbol{k}\ \downarrow}}^*+{a_{\boldsymbol{k}'\ \uparrow}}^*{a_{\boldsymbol{k}'\ \downarrow}}^*)\mid0\rangle\)”→“\(u_kv_k({a_{\boldsymbol{k}\ \uparrow}}^*{a_{-\boldsymbol{k}\ \downarrow}}^*+{a_{\boldsymbol{k}'\ \uparrow}}^*{a_{-\boldsymbol{k}'\ \downarrow}}^*)\mid0\rangle\)”
p.117　“一方を地方で展開した式”→“一方を他方で展開した式”
p.120 (10)式　“\(\rho(\boldsymbol r')\)”→“\(\rho(\boldsymbol r',\ t)\)”
p.126　l.1　“\(\displaystyle\mathrm{i}\hbar\frac{d}{dt}\psi(\boldsymbol{r},\ t)=\psi(\boldsymbol{r},\ t)\mathscr{H}-\mathscr{H}\psi(\boldsymbol{r},\ t)\)”→“\(\displaystyle\mathrm{i}\hbar\frac{d}{dt}\boldsymbol{\psi}(\boldsymbol{r},\ t)=\boldsymbol{\psi}(\boldsymbol{r},\ t)\mathscr{H}-\mathscr{H}\boldsymbol{\psi}(\boldsymbol{r},\ t)\)”
l.5“\(\displaystyle \mathrm{i}\hbar\frac{\partial}{\partial t}\psi(\boldsymbol{r},\ t)=\sum_{\mu}\sum_{\nu}\varepsilon_{\nu}\varphi_{\mu}(\boldsymbol{r})\mathrm{e}^{-\mathrm{i}\varepsilon_{\mu}t/\hbar}(a_{\mu}{a_{\nu}}^*a_{\nu}-{a_{\nu}}^*a_{\nu}a_{\mu})\)”→“\(\displaystyle \mathrm{i}\hbar\frac{\partial}{\partial t}\boldsymbol{\psi}(\boldsymbol{r},\ t)=\sum_{\mu}\sum_{\nu}\varepsilon_{\nu}\varphi_{\mu}(\boldsymbol{r})\mathrm{e}^{-\mathrm{i}\varepsilon_{\mu}t/\hbar}(a_{\mu}{a_{\nu}}^*a_{\nu}-{a_{\nu}}^*a_{\nu}a_{\mu})\)”
l.13　“\(\displaystyle \mathrm{i}\hbar\frac{\partial}{\partial t}\psi(\boldsymbol{r},\ t)=\sum_{\mu}\varepsilon_{\mu}\varphi_{\mu}(\boldsymbol{r})\mathrm{e}^{-\mathrm{i}\varepsilon_{\mu}t/\hbar}a_{\mu}\)”→“\(\displaystyle \mathrm{i}\hbar\frac{\partial}{\partial t}\boldsymbol{\psi}(\boldsymbol{r},\ t)=\sum_{\mu}\varepsilon_{\mu}\varphi_{\mu}(\boldsymbol{r})\mathrm{e}^{-\mathrm{i}\varepsilon_{\mu}t/\hbar}a_{\mu}\)”