download from tex_latex@bbs.sjtu.edu.cn

Makefile

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+BASE = diss
+PDFREADER = evince
+
+all: pdf
+
+pdf: ${BASE}.pdf
+
+${BASE}.pdf: ${BASE}.tex
+	# xelatex -no-pdf --interaction=nonstopmode ${BASE}
+	# bibtex ${BASE}
+	# xelatex -no-pdf --interaction=nonstopmode ${BASE}
+	# xelatex --interaction=nonstopmode ${BASE}
+
+view: ${BASE}.pdf
+	$PDFREADER ${BASE}.pdf&
+
+tar: ${BASE}.pdf
+
+# TARSOURCE = *.tex *.pdf *.bst *.cfg *.cls Makefile body
+# figures reference
+
+# ${BASE}.tar: ${TARSOURCE}
+#      tar jcf ${BASE}.tar.bz2 ${TARSOURCE}
+
+clean:
+	cp diss.pdf README.pdf
+	find ./ -iname '*.aux' | xargs rm
+	find ./ -iname '*.log' | xargs rm
+	find ./ -iname '*.lot' | xargs rm
+	find ./ -iname '*.out' | xargs rm
+	find ./ -iname '*.toc' | xargs rm
+	find ./ -iname '*.blg' | xargs rm
+	find ./ -iname '*.bbl' | xargs rm
+	find ./ -iname '*.lof' | xargs rm
+	find ./ -iname '*.xdv' | xargs rm
+	mv ${BASE}.pdf mythesis.pdf
+	rm ${BASE}.xdv ${BASE}.pdf
+# cleantex
+# if [ -e ${BASE}.xdv ]; then rm ${BASE}.xdv; fi
+# cd body && cleantex && cd ..
+
+test:
+	xelatex --no-pdf diss
+
+distclean: clean
+	if [ -e ${BASE}.pdf ]; then rm ${BASE}.pdf; fi
+

body/abstract.aux

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body/abstract.tex

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+%%==================================================
+%% abstract.tex for SJTU Master Thesis
+%% based on CASthesis
+%% modified by wei.jianwen@gmail.com
+%% version: 0.3a
+%% Encoding: UTF-8
+%% last update: Dec 5th, 2010
+%%==================================================
+
+\begin{abstract}
+
+  上海交通大学是我国历史最悠久的高等学府之一，是教育部直属、教育部与上海市共建的全国重点大学，是国家 “七五”、“八五”重点建设和“211工程”、“985工程”的首批建设高校。经过113年的不懈努力，上海交通大学已经成为一所“综合性、研究型、国际化”的国内一流、国际知名大学，并正在向世界一流大学稳步迈进。
+  学校现有本科专业67个，涵盖经济学、法学、文学、理学、工学、农学、医学和管理学等8个学科门类；拥有工科物理、工科数学和电工电子等3个国家工科基础课程教学基地，生命科学和集成电路等2个国家人才培养基地和教育部大学生文化素质教育基地，以及国家生物学理科人才培养基地；有国家级实验教学示范中心5个，上海市实验教学示范中心4个；有国家级教学团队5个，上海市级教学团队9各；有国家级教学名师奖获得者6人，上海市教学名师奖获得者32人；有国家级精品课程40门，上海市精品课程100门；有国家级双语示范课程5门；2005年和2009年，作为第一完成单位，共获得国家级教学成果22项、上海市级教学成果105项。
+
+  \keywords{\large 上海交大 \quad 饮水思源 \quad 爱国荣校}
+\end{abstract}
+
+\begin{englishabstract}
+
+  Shanghai Jiao Tong University (SJTU), directly subordinate to the Ministry of Education, is a key university in China, jointly run by the Ministry and Shanghai Municipality.
+  SJTU has beautiful campuses, occupying an area of more than 200 hectare in total, and possesses plenty of advanced teaching and research equipment and facilities. Now, it has six campuses, the Xuhui, the Minhang, the Qibao, the Shangzhong Road , the Fahuazheng Road and the Chongqing Road(south). Over the past decade, the number of students in SJTU has grown from 5,000 to more than 38,000, the floorage of various buildings from 230,000 square meters to 800,000 square meters, and the area of campuses from 40ha to 200ha. Apart from the major buildings such as the Lecture Buildings, Laboratory Buildings, Dormitories and Gymnasiums, SJTU also has the Bao Zhaolong Library which is well-known throughout the country. Various laboratories, including university central laboratories such as "Computer Center" and "Audio-visual Education Center" are equipped with advanced research and teaching equipment and facilities.
+
+  \englishkeywords{\large SJTU, master thesis, XeTeX/LaTeX template}
+\end{englishabstract}

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body/app1.tex

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+%%==================================================
+%% app1.tex for SJTU Master Thesis
+%% based on CASthesis
+%% modified by wei.jianwen@gmail.com
+%% version: 0.3a
+%% Encoding: UTF-8
+%% last update: Dec 5th, 2010
+%%==================================================
+
+\chapter{模板更新记录}
+\label{chap:updatelog}
+
+\textbf{2010年12月5日} v0.3a发布，移植到~\XeTeX/\LaTeX~上。
+
+\textbf{2009年12月25日} v0.2a发布，模板由CASthesis改名为sjtumaster。在diss.tex中可以方便地改变正文字号、切换但双面打印。增加了不编号的一章“全文总结”。
+添加了可伸缩符号(等号、箭头)的例子，增加了长标题换行的例子。
+
+\textbf{2009年11月20日} v0.1c发布，增加了Linux下使用ctex宏包的注意事项、.bib条目的规范要求，
+修正了ctexbook与listings共同使用时的断页错误。
+
+\textbf{2009年11月13日} v0.1b发布，完善了模板使用说明，增加了定理环境、并列子图、三线表格的例子。
+
+\textbf{2009年11月12日} 上海交通大学硕士学位论文~\LaTeX~模板发布，版本0.1a。
+

body/app2.aux

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body/app2.tex

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+%% app2.tex for SJTU Master Thesis
+%% based on CASthesis
+%% modified by wei.jianwen@gmail.com
+%% version: 0.3a
+%% Encoding: UTF-8
+%% last update: Dec 5th, 2010
+%%==================================================
+
+\chapter{Maxwell Equations}
+
+选择二维情况，有如下的偏振矢量
+\begin{subequations}
+  \begin{eqnarray}
+    {\bf E}&=&E_z(r,\theta)\hat{\bf z} \\
+    {\bf H}&=&H_r(r,\theta))\hat{ \bf r}+H_\theta(r,\theta)\hat{\bm
+      \theta}
+  \end{eqnarray}
+\end{subequations}
+对上式求旋度
+\begin{subequations}
+  \begin{eqnarray}
+    \nabla\times{\bf E}&=&\frac{1}{r}\frac{\partial E_z}{\partial\theta}{\hat{\bf r}}-\frac{\partial E_z}{\partial r}{\hat{\bm\theta}}\\
+    \nabla\times{\bf H}&=&\left[\frac{1}{r}\frac{\partial}{\partial
+        r}(rH_\theta)-\frac{1}{r}\frac{\partial
+        H_r}{\partial\theta}\right]{\hat{\bf z}}
+  \end{eqnarray}
+\end{subequations}
+因为在柱坐标系下，$\overline{\overline\mu}$是对角的，所以Maxwell方程组中电场$\bf
+E$的旋度
+\begin{subequations}
+  \begin{eqnarray}
+    &&\nabla\times{\bf E}=\mathbf{i}\omega{\bf B} \\
+    &&\frac{1}{r}\frac{\partial E_z}{\partial\theta}{\hat{\bf
+        r}}-\frac{\partial E_z}{\partial
+      r}{\hat{\bm\theta}}=\mathbf{i}\omega\mu_rH_r{\hat{\bf r}}+\mathbf{i}\omega\mu_\theta
+    H_\theta{\hat{\bm\theta}}
+  \end{eqnarray}
+\end{subequations}
+所以$\bf H$的各个分量可以写为：
+\begin{subequations}
+  \begin{eqnarray}
+    H_r=\frac{1}{\mathbf{i}\omega\mu_r}\frac{1}{r}\frac{\partial
+      E_z}{\partial\theta } \\
+    H_\theta=-\frac{1}{\mathbf{i}\omega\mu_\theta}\frac{\partial E_z}{\partial r}
+  \end{eqnarray}
+\end{subequations}
+同样地，在柱坐标系下，$\overline{\overline\epsilon}$是对角的，所以Maxwell方程组中磁场$\bf
+H$的旋度
+\begin{subequations}
+  \begin{eqnarray}
+    &&\nabla\times{\bf H}=-\mathbf{i}\omega{\bf D}\\
+    &&\left[\frac{1}{r}\frac{\partial}{\partial
+        r}(rH_\theta)-\frac{1}{r}\frac{\partial
+        H_r}{\partial\theta}\right]{\hat{\bf
+        z}}=-\mathbf{i}\omega{\overline{\overline\epsilon}}{\bf
+      E}=-\mathbf{i}\omega\epsilon_zE_z{\hat{\bf z}} \\
+    &&\frac{1}{r}\frac{\partial}{\partial
+      r}(rH_\theta)-\frac{1}{r}\frac{\partial
+      H_r}{\partial\theta}=-\mathbf{i}\omega\epsilon_zE_z
+  \end{eqnarray}
+\end{subequations}
+由此我们可以得到关于$E_z$的波函数方程：
+\begin{eqnarray}
+  \frac{1}{\mu_\theta\epsilon_z}\frac{1}{r}\frac{\partial}{\partial r}
+  \left(r\frac{\partial E_z}{\partial r}\right)+
+  \frac{1}{\mu_r\epsilon_z}\frac{1}{r^2}\frac{\partial^2E_z}{\partial\theta^2}
+  +\omega^2 E_z=0
+\end{eqnarray}

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