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2 changes: 1 addition & 1 deletion Chaps/AppendixC.tex
Original file line number Diff line number Diff line change
Expand Up @@ -16,7 +16,7 @@ \section{引言}
随着构象计算的日益成功,人们甚至可以选择孤立分子的计算结果,而不是在凝聚介质中获得的实验结果,因为前者可能更适合气相。

除了产生关于势能面全局最小点的信息外,量子力学计算还可以产生局域最小点的信息,这些局域最小点可能不会被直接观测到,但是
很可能会被包哦旱灾反应路径中。类似的,关于过渡态和能垒的信息也可以得到,这些信息一般很难甚至不可能通过其他方式获得。
很可能会被包含在反应路径中。类似的,关于过渡态和能垒的信息也可以得到,这些信息一般很难甚至不可能通过其他方式获得。

收集一个势能面上这些所有的信息是很困难的。对于N个原子的体系,它的能量是一个具有$3N-6$(或者$3N-5$)个自由度的函数。
为了进行详细的统计计算,人们可能不得不面对这个“3N”问题,并访问势能面上所有热力学可得的区域。
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2 changes: 1 addition & 1 deletion Chaps/Chap1.tex
Original file line number Diff line number Diff line change
Expand Up @@ -456,7 +456,7 @@ \subsection{行列式}
\begin{equation}
\begin{vmatrix}
A_{11} & A_{12} \\ A_{21} &A_{22}
\end{vmatrix} = \left(-1\right)^0 A_{11}A_{12} + \left(-1\right)^1 A_{12}A_{21} = A_{11}A_{12} - A_{12}A_{21}
\end{vmatrix} = \left(-1\right)^0 A_{11}A_{22} + \left(-1\right)^1 A_{12}A_{21} = A_{11}A_{22} - A_{12}A_{21}
\label{eq:1.39}
\end{equation}
由这些定义,我们可以得出以下关于行列式的重要性质:
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