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@@ -119,22 +119,23 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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\begin{sidewaystable}
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\centering
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{
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\newcommand{\tworow}[1]{\multirow{2}{*}{#1}}
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\newcommand{\twocol}[1]{\multicolumn{2}{C{1cm}|}{#1}}
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\newcommand{\threecol}[1]{\multicolumn{3}{C{1.5cm}|}{#1}}
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\newcommand{\allcol}[1]{\multicolumn{26}{C{15cm}|}{#1}}
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\caption{Title}
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\newcommand{\wthreecol}[1]{\multicolumn{3}{C{2cm}|}{#1}}
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\newcommand{\allcol}[1]{\multicolumn{26}{C{16cm}|}{#1}}
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\setlength\tabcolsep{0pt} % 不加这句话的话，表格的竖线的宽度会被计入，导致合并后的单元格不居中
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\caption{Weak- and None-polarized phonons near $\Gamma$ point}
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\begin{tabular}{
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| C{4cm} % header
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
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| C{0.5cm} | C{0.5cm} % E1
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| C{1cm} | C{1cm} % 2B1
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % A1
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| C{0.5cm} | C{0.5cm} | C{1cm} % A1
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| C{0.5cm} | C{0.5cm} % E1
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
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| C{0.5cm} | C{0.5cm} | C{0.5cm} % A1
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| C{0.5cm} | C{0.5cm} | C{1cm} % A1
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| C{1cm} | C{1cm} % 2B1
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| }
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\hline
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@@ -143,14 +144,14 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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& 3 & \twocol{4} % E2
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& 5 & 6 % E1
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& 7 & 8 % 2B1
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& \threecol{9} % A1
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& \wthreecol{9} % A1
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& 10 & 11 % E1
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& 12 & \twocol{13} % E2
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& 14 & \twocol{15} % E2
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& \threecol{16} % A1
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& \wthreecol{16} % A1
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& 17 & 18 % 2B1
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\\ \hline
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\textbf{Direction of Incident \& Scattered Light}
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\textbf{\makecell{Direction of Incident \\ \& Scattered Light}}
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& \allcol{\makecell{Any direction \\ (not depend on direction of incident \& scattered light)}}
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\\ \hline
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\textbf{Vibration Direction}
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@@ -158,24 +159,36 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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& x & \twocol{y} % E2
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& x & y % E1
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& z & z % 2B1
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& \threecol{z} % A1
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& \wthreecol{z} % A1
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& x & y % E1
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& x & \twocol{y} % E2
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& x & \twocol{y} % E2
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& \threecol{z} % A1
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& \wthreecol{z} % A1
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& z & z % 2B1
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\\ \hline
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\textbf{Representation in Group $\mathrm{C_{6v}}$}
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& \threecol{$\mathrm{E_2}$}
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& \threecol{$\mathrm{E_2}$}
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& \twocol{$\mathrm{E_1}$}
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& $\mathrm{B_1}$ & $\mathrm{B_1}$
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& \threecol{$\mathrm{A_1}$}
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& \twocol{$\mathrm{E_1}$}
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& \threecol{$\mathrm{E_2}$}
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& \threecol{$\mathrm{E_2}$}
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& \threecol{$\mathrm{A_1}$}
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& $\mathrm{B_1}$ & $\mathrm{B_1}$
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& \threecol{$\mathrm{E_2}$} % E2
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& \threecol{$\mathrm{E_2}$} % E2
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& \twocol{$\mathrm{E_1}$} % E1
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& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
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& \wthreecol{$\mathrm{A_1}$} % A1
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& \twocol{$\mathrm{E_1}$} % E1
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& \threecol{$\mathrm{E_2}$} % E2
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& \threecol{$\mathrm{E_2}$} % E2
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& \wthreecol{$\mathrm{A_1}$} % A1
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& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
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\\ \hline
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\textbf{Representation in Group $\mathrm{C_{2v}}$}
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& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
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& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
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& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
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& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
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& \wthreecol{$\mathrm{A_1}$} % A1
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& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
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& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
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& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
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& \wthreecol{$\mathrm{A_1}$} % A1
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& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
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\\ \hline
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\textbf{Scattering in Polarization}
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& xy & xx & yy % E2
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@@ -206,7 +219,7 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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& \threecol{Yes} % E2
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& \twocol{Yes} % E1
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& No & No % 2B1
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& \threecol{Yes} % A1
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& \wthreecol{Yes} % A1
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& \twocol{No} % E1
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& \threecol{Yes} % E2
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& \threecol{No} % E2
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@@ -214,23 +227,23 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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& No & No % 2B1
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\\ \hline
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\textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)}
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& \threecol{$190.51$} % E2
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& \threecol{$190.51$} % E2
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& \twocol{$257.35$} % E1
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& $389.96$ & $389.96$ % 2B1
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& \threecol{$591.90$} % A1
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& \twocol{$746.91$} % E1
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& \threecol{$756.25$} % E2
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& \threecol{$764.33$} % E2
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& \threecol{$812.87$} % A1
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& $885.68$ & $894.13$ % 2B1
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& \threecol{$190.51$} % E2
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& \threecol{$190.51$} % E2
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& \twocol{$257.35$} % E1
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& $389.96$ & $389.96$ % 2B1
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& \wthreecol{$591.90$} % A1
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& \twocol{$746.91$} % E1
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& \threecol{$756.25$} % E2
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& \threecol{$764.33$} % E2
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& \wthreecol{$812.87$} % A1
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& $885.68$ & $894.13$ % 2B1
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\\ \hline
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\textbf{Wavenumber (Experiment) ($\mathrm{cm^{-1}}$)}
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& \threecol{$195.5$} % E2
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& \threecol{$203.3$} % E2
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& \twocol{$269.7$} % E1
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& - & - % 2B1
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& \threecol{$609.5$} % A1
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& \wthreecol{$609.5$} % A1
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& \twocol{-} % E1
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& \threecol{$776$} % E2
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& \threecol{-} % E2
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@@ -238,16 +251,16 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
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& - & - % 2B1
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\\ \hline
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\textbf{Electrical Polarity}
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& \threecol{None} % E2
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& \threecol{None} % E2
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& \twocol{Weak} % E1
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& None & None % 2B1
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& \threecol{Weak} % A1
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& \twocol{Weak} % E1
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& \threecol{None} % E2
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& \threecol{None} % E2
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& \threecol{Weak} % A1
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& None & None % 2B1
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& \threecol{None} % E2
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& \threecol{None} % E2
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& \twocol{Weak} % E1
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& None & None % 2B1
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& \wthreecol{Weak} % A1
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& \twocol{Weak} % E1
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& \threecol{None} % E2
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& \threecol{None} % E2
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& \wthreecol{Weak} % A1
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& None & None % 2B1
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\\ \hline
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\end{tabular}
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}
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