
\left(
這是我的程式碼,但當我更改為\right)
和\Big)
時它不起作用\Big)
\begin{align*}
\bar{h}_{m}^{jk}&=\omega_{k}h_{m}^{jk}(a)\\
&=\left( \omega_{k}\left\{
\zeta_{h}\mid\zeta_{h}\in p_{1}\circ h_{m}^{jk}(a)\right\} ,\omega
_{k}\left\{ \zeta_{h}\mid\zeta_{h}\in p_{2}\circ h_{m}^{jk}(a)\right\}
,\dots, \right.\\
&\qquad \left.\omega_{k}\left\{ \zeta_{h}\mid\zeta_{h}\in p_{m}\circ h_{m}%
^{jk}(a)\right\} \right) \\
&=\left( \left\{ \bar{\zeta}_{h}\mid\bar{\ze
}_{h}\in p_{1}\circ h_{m}^{jk}(a)\right\} ,\left\{ \bar{\zeta}_{h}\mid
\bar{\zeta}_{h}\in p_{2}\circ h_{m}^{jk}(a)\right\} ,\dots,\left\{ \bar{\zeta
}_{h}\mid\bar{\zeta}_{h}\in p_{m}\circ h_{m}^{jk}(a)\right\} \right) .
\end{align*}
答案1
每個\left
總是與 a 配對\right
,且該配對不能與&
or交叉\\
。無論誰編寫了您的程式碼,實際上(正確地)\left(
與\right.
和\left.
配對\right)
;這.
意味著 TeX 不會排版柵欄,但現在知道要測量多少尺寸。
更改\left(
為\Big(
和\right)
to\Big)
意味著您要離開\left.
並\right.
進入那裡,TeX 會對您要配對的內容感到困惑。解決方案是,當您更改\left(
為\Big(
和\right)
時\Big)
,您還需要刪除現在多餘的\left.
和\right.
。
順便說一句,出於間距目的,您可能需要使用\Bigl(
和\Bigr)
。這告訴 TeX 它正在處理左柵欄或右柵欄。
答案2
像這樣?
\documentclass{article}
\usepackage{mathtools}
\begin{document}
\begin{align*}
\bar{h}_{m}^{jk}
& = \omega_{k}h_{m}^{jk}(a)\\
& = \begin{multlined}[t]
\biggl(\omega_{k}\Bigl\{
\zeta_{h}\mid\zeta_{h}\in p_{1}\circ h_{m}^{jk}(a)\Bigr\},\omega_{k}
\Bigl\{\zeta_{h}\mid\zeta_{h}\in p_{2}\circ h_{m}^{jk}(a)
\Bigr\}, \dots \\
\dots,
\omega_{k}\Bigl\{\zeta_{h}\mid\zeta_{h}\in p_{m}\circ h_{m}^{jk}(a)
\Bigr\}
\biggr)
\end{multlined} \\
& = \begin{multlined}[t]
\biggl(\Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{1}\circ h_{m}^{jk}(a)\Bigr\},
\Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{2}\circ h_{m}^{jk}(a)
\Bigr\},\dots \\
\dots,
\Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{m}\circ h_{m}^{jk}(a)\Bigr\}
\biggr).
\end{multlined}
\end{align*}
\end{document}
附錄:
使用 usealigned
而不是multilined
可以定義錨點,其中是多線方程式的對齊線:
\documentclass{article}
\usepackage{amsmath}
\begin{document}
\begin{align*}
\bar{h}_{m}^{jk}
& = \omega_{k}h_{m}^{jk}(a)\\
& = \begin{aligned}[t]
\biggl(\omega_{k}\Bigl\{
\zeta_{h}\mid\zeta_{h}\in p_{1}\circ h_{m}^{jk}(a)\Bigr\},
& \;\omega_{k}\Bigl\{\zeta_{h}\mid\zeta_{h}\in p_{2}\circ h_{m}^{jk}(a)\Bigr\}, \dots \\
\dots,
& \;\omega_{k}\Bigl\{\zeta_{h}\mid\zeta_{h}\in p_{m}\circ h_{m}^{jk}(a)\Bigr\}\biggr)
\end{aligned} \\
& = \begin{aligned}[t]
\biggl(\Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{1}\circ h_{m}^{jk}(a)\Bigr\},
&\; \Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{2}\circ h_{m}^{jk}(a)\Bigr\},\dots \\
\dots,
&\; \Bigl\{\bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{m}\circ h_{m}^{jk}(a)\Bigr\}\biggr).
\end{aligned}
\end{align*}
\end{document}
答案3
我建議這個變體使用稍微簡單的程式碼,基於 fleqn
from nccmath
、\DeclarePairedDelimiter
命令 frommathtools
和multlined
環境(相同的套件)。
\documentclass[svgnames]{article}
\usepackage{showframe}
\renewcommand{\ShowFrameLinethickness}{0.4pt}
\renewcommand{\ShowFrameColor}{\color{Coral}}
\usepackage{nccmath, mathtools}
\DeclarePairedDelimiter\set\{\}
\begin{document}
\leavevmode\vskip 1cm
\begin{fleqn}
\begin{align*}
\bar{h}_{m}^{jk} &=\omega_{k}h_{m}^{jk}(a) \\
&=\begin{multlined}[t][0.9\linewidth]\Bigl( \omega_{k}\set*{\zeta_{h}\mid\zeta_{h}\in p_{1}\circ h_{m}^{jk}(a)} ,\omega
_{k}\set{ \zeta_{h}\mid\zeta_{h}\in p_{2}\circ h_{m}^{jk}(a)},\dots \\[-1.5ex]
\dots, \omega_{k}\set*{ \zeta_{h}\mid\zeta_{h}\in p_{m}\circ h_{m}^{jk}(a)}\Bigr) \end{multlined} \\
&= \begin{multlined}[t][0.9\linewidth]\Bigl( \set*{ \bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{1}\circ h_{m}^{jk}(a)} ,%
\set*{ \bar{\zeta}_{h}\mid \bar{\zeta}_{h}\in p_{2}\circ h_{m}^{jk}(a)} ,\dots \phantom{.} \\[-1.5ex]
\dots, \set*{ \bar{\zeta}_{h}\mid\bar{\zeta}_{h}\in p_{m}\circ h_{m}^{jk}(a)} \Bigr).
\end{multlined}
\end{align*}
\end{fleqn}
\end{document}