From eb3b977374409dac1ffc3d4636d6f244f540f6cd Mon Sep 17 00:00:00 2001 From: chn Date: Mon, 28 Apr 2025 21:06:08 +0800 Subject: [PATCH] =?UTF-8?q?=E4=BD=BF=E7=94=A8tabularray?= MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit --- paper/main.tex | 401 ++++++++++++++++++++++++------------------------- 1 file changed, 198 insertions(+), 203 deletions(-) diff --git a/paper/main.tex b/paper/main.tex index 40f4c35..9cdcbc7 100644 --- a/paper/main.tex +++ b/paper/main.tex @@ -121,77 +121,75 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories: \begin{sidewaystable} \centering { - \newcommand{\twocol}[1]{\multicolumn{2}{C{1cm}|}{#1}} - \newcommand{\threecol}[1]{\multicolumn{3}{C{1.5cm}|}{#1}} - \newcommand{\wthreecol}[1]{\multicolumn{3}{C{2cm}|}{#1}} - \newcommand{\allcol}[1]{\multicolumn{26}{C{16cm}|}{#1}} - \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 \caption{Weak- and None-polarized phonons near $\Gamma$ point} - \begin{tabular}{ - | C{4cm} % header - | C{0.5cm} | C{0.5cm} | C{0.5cm} % E2 - | C{0.5cm} | C{0.5cm} | C{0.5cm} % E2 - | C{0.5cm} | C{0.5cm} % E1 - | C{1cm} | C{1cm} % 2B1 - | C{0.5cm} | C{0.5cm} | C{1cm} % A1 - | C{0.5cm} | C{0.5cm} % E1 - | C{0.5cm} | C{0.5cm} | C{0.5cm} % E2 - | C{0.5cm} | C{0.5cm} | C{0.5cm} % E2 - | C{0.5cm} | C{0.5cm} | C{1cm} % A1 - | C{1cm} | C{1cm} % 2B1 - | } - \hline - \textbf{\makecell{Direction of Incident \\ \& Scattered Light}} - & \allcol{\makecell{Any direction \\ (not depend on direction of incident \& scattered light)}} - \\ \hline + \begin{tblr}{ + hlines,vlines,colsep=2pt,width=\textwidth, + colspec={ + X[10,c,m] + *{3}{X[c,m]} % E2 + *{3}{X[c,m]} % E2 + *{2}{X[c,m]} % E1 + *{2}{X[4,c,m]} % 2B1 + *{2}{X[c,m]} X[2,c,m] % A1 + *{2}{X[c,m]} % E1 + *{3}{X[c,m]} % E2 + *{3}{X[c,m]} % E2 + *{2}{X[c,m]} X[2,c,m] % A1 + *{2}{X[4,c,m]} % 2B1 + } + } + \textbf{Direction of Incident \& Scattered Light} + & \SetCell[c=26]{}{Any direction \\ (not depend on direction of incident \& scattered light)} + & & & & & & & & & & & & & & & & & & & & & & & & & + \\ \textbf{Number of Phonon} - & 1 & \twocol{2} % E2 - & 3 & \twocol{4} % E2 - & 5 & 6 % E1 - & 7 & 8 % 2B1 - & \wthreecol{9} % A1 - & 10 & 11 % E1 - & 12 & \twocol{13} % E2 - & 14 & \twocol{15} % E2 - & \wthreecol{16} % A1 - & 17 & 18 % 2B1 - \\ \hline + & 1 & \SetCell[c=2]{} 2 & % E2 + & 3 & \SetCell[c=2]{} 4 & % E2 + & 5 & 6 % E1 + & 7 & 8 % 2B1 + & \SetCell[c=3]{} 9 & & % A1 + & 10 & 11 % E1 + & 12 & \SetCell[c=2]{} 13 & % E2 + & 14 & \SetCell[c=2]{} 15 & % E2 + & \SetCell[c=3]{} 16 & & % A1 + & 17 & 18 % 2B1 + \\ \textbf{Vibration Direction} - & x & \twocol{y} % E2 - & x & \twocol{y} % E2 - & x & y % E1 - & z & z % 2B1 - & \wthreecol{z} % A1 - & x & y % E1 - & x & \twocol{y} % E2 - & x & \twocol{y} % E2 - & \wthreecol{z} % A1 - & z & z % 2B1 - \\ \hline + & x & \SetCell[c=2]{} y & % E2 + & x & \SetCell[c=2]{} y & % E2 + & x & y % E1 + & z & z % 2B1 + & \SetCell[c=3]{} z & & % A1 + & x & y % E1 + & x & \SetCell[c=2]{} y & % E2 + & x & \SetCell[c=2]{} y & % E2 + & \SetCell[c=3]{} z & & % A1 + & z & z % 2B1 + \\ \textbf{Representation in Group $\mathrm{C_{6v}}$} - & \threecol{$\mathrm{E_2}$} % E2 - & \threecol{$\mathrm{E_2}$} % E2 - & \twocol{$\mathrm{E_1}$} % E1 - & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 - & \wthreecol{$\mathrm{A_1}$} % A1 - & \twocol{$\mathrm{E_1}$} % E1 - & \threecol{$\mathrm{E_2}$} % E2 - & \threecol{$\mathrm{E_2}$} % E2 - & \wthreecol{$\mathrm{A_1}$} % A1 - & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 - \\ \hline + & \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2 + & \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2 + & \SetCell[c=2]{} $\mathrm{E_1}$ & % E1 + & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1 + & \SetCell[c=2]{} $\mathrm{E_1}$ & % E1 + & \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2 + & \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1 + & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 + \\ \textbf{Representation in Group $\mathrm{C_{2v}}$} - & $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2 - & $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2 - & $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1 - & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 - & \wthreecol{$\mathrm{A_1}$} % A1 - & $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1 - & $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2 - & $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2 - & \wthreecol{$\mathrm{A_1}$} % A1 - & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 - \\ \hline + & $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2 + & $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2 + & $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1 + & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1 + & $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1 + & $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2 + & $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1 + & $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1 + \\ \textbf{Scattering in Polarization} & xy & xx & yy % E2 & xy & xx & yy % E2 @@ -203,128 +201,126 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories: & xy & xx & yy % E2 & xx & yy & zz % A1 & - & - % 2B1 - \\ \hline + \\ \textbf{Raman Intensity (a.u.)} - & \threecol{$0.17$} % E2 - & \threecol{$1.13$} % E2 - & \twocol{$2.43$} % E1 - & $0$ & $0$ % 2B1 - & \twocol{$2.83$} & $1.79$ % A1 - & \twocol{$0.09$} % E1 - & \threecol{$88.54$} % E2 - & \threecol{$0.50$} % E2 - & \twocol{$0.01$} & $1.78$ % A1 - & $0$ & $0$ % 2B1 - \\ \hline + & \SetCell[c=3]{} $0.17$ & & % E2 + & \SetCell[c=3]{} $1.13$ & & % E2 + & \SetCell[c=2]{} $2.43$ & % E1 + & $0$ & $0$ % 2B1 + & \SetCell[c=2]{} $2.83$ & & $1.79$ % A1 + & \SetCell[c=2]{} $0.09$ & % E1 + & \SetCell[c=3]{} $88.54$ & & % E2 + & \SetCell[c=3]{} $0.50$ & & % E2 + & \SetCell[c=2]{} $0.01$ & & $1.78$ % A1 + & $0$ & $0$ % 2B1 + \\ \textbf{Visible in Common Raman Experiment} - & \threecol{Yes} % E2 - & \threecol{Yes} % E2 - & \twocol{Yes} % E1 - & No & No % 2B1 - & \wthreecol{Yes} % A1 - & \twocol{No} % E1 - & \threecol{Yes} % E2 - & \threecol{No} % E2 - & \twocol{No} & Yes % A1 - & No & No % 2B1 - \\ \hline + & \SetCell[c=3]{} Yes & & % E2 + & \SetCell[c=3]{} Yes & & % E2 + & \SetCell[c=2]{} Yes & % E1 + & No & No % 2B1 + & \SetCell[c=3]{} Yes & & % A1 + & \SetCell[c=2]{} No & % E1 + & \SetCell[c=3]{} Yes & & % E2 + & \SetCell[c=3]{} No & & % E2 + & \SetCell[c=2]{} No & & Yes % A1 + & No & No % 2B1 + \\ \textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)} - & \threecol{$190.51$} % E2 - & \threecol{$190.51$} % E2 - & \twocol{$257.35$} % E1 - & $389.96$ & $389.96$ % 2B1 - & \wthreecol{$591.90$} % A1 - & \twocol{$746.91$} % E1 - & \threecol{$756.25$} % E2 - & \threecol{$764.33$} % E2 - & \wthreecol{$812.87$} % A1 - & $885.68$ & $894.13$ % 2B1 - \\ \hline + & \SetCell[c=3]{} $190.51$ & & % E2 + & \SetCell[c=3]{} $190.51$ & & % E2 + & \SetCell[c=2]{} $257.35$ & % E1 + & $389.96$ & $389.96$ % 2B1 + & \SetCell[c=3]{} $591.90$ & & % A1 + & \SetCell[c=2]{} $746.91$ & % E1 + & \SetCell[c=3]{} $756.25$ & & % E2 + & \SetCell[c=3]{} $764.33$ & & % E2 + & \SetCell[c=3]{} $812.87$ & & % A1 + & $885.68$ & $894.13$ % 2B1 + \\ \textbf{Wavenumber (Experiment) ($\mathrm{cm^{-1}}$)} - & \threecol{$195.5$} % E2 - & \threecol{$203.3$} % E2 - & \twocol{$269.7$} % E1 - & - & - % 2B1 - & \wthreecol{$609.5$} % A1 - & \twocol{-} % E1 - & \threecol{$776$} % E2 - & \threecol{-} % E2 - & \twocol{-} & $839$ % A1 - & - & - % 2B1 - \\ \hline + & \SetCell[c=3]{} $195.5$ & & % E2 + & \SetCell[c=3]{} $203.3$ & & % E2 + & \SetCell[c=2]{} $269.7$ & % E1 + & - & - % 2B1 + & \SetCell[c=3]{} $609.5$ & & % A1 + & \SetCell[c=2]{} - & % E1 + & \SetCell[c=3]{} $776$ & & % E2 + & \SetCell[c=3]{} - & & % E2 + & \SetCell[c=2]{} - & $839$ % A1 + & - & - % 2B1 + \\ \textbf{Electrical Polarity} - & \threecol{None} % E2 - & \threecol{None} % E2 - & \twocol{Weak} % E1 - & None & None % 2B1 - & \wthreecol{Weak} % A1 - & \twocol{Weak} % E1 - & \threecol{None} % E2 - & \threecol{None} % E2 - & \wthreecol{Weak} % A1 - & None & None % 2B1 - \\ \hline - \end{tabular} + & \SetCell[c=3]{} None & & % E2 + & \SetCell[c=3]{} None & & % E2 + & \SetCell[c=2]{} Weak & % E1 + & None & None % 2B1 + & \SetCell[c=3]{} Weak & & % A1 + & \SetCell[c=2]{} Weak & % E1 + & \SetCell[c=3]{} None & & % E2 + & \SetCell[c=3]{} None & & % E2 + & \SetCell[c=3]{} Weak & & % A1 + & None & None % 2B1 + \\ + \end{tblr} } { - \newcommand{\tworow}[1]{\multirow{2}{*}{#1}} - \newcommand{\twocol}[2]{\multicolumn{2}{C{#1}|}{#2}} - \newcommand{\threecol}[2]{\multicolumn{3}{C{#1}|}{#2}} - \newcommand{\fourcol}[1]{\multicolumn{4}{C{2cm}|}{#1}} - \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 \caption{Strong-polarized phonons near $\Gamma$ point} - \begin{tabular}{ - | C{4cm} % header - | C{1cm} | C{1cm} % z E1 - | C{0.7cm} | C{0.7cm} | C{1cm} % z A1 - | C{0.5cm} | C{0.5cm} | C{0.5cm} % y z - | C{1cm} % y x - | C{1cm} % y y - | C{0.5cm} | C{0.5cm} | C{0.5cm} | C{0.5cm} % 45 y&z mainly z - | C{1cm} % 45 x - | C{0.5cm} | C{0.5cm} | C{0.5cm} | C{0.5cm} % 45 y&z mainly y - | } - \hline + \begin{tblr}{ + hlines,vlines,colsep=2pt,width=\textwidth,hspan=even, + colspec={ + X[5,c,m] + X[c,m] % z x + X[c,m] % z y + *{2}{X[c,m]}X[c,m,1.5] % z z + X[c,m,2]X[c,m]X[c,m,2] % y z + X[c,m,1.5] % y x + X[c,m,2] % y y + *{3}{X[c,m]}X[c,m,1.5] % 45 y&z mainly z + X[c,m,1.5] % 45 x + *{4}{X[c,m]} % 45 y&z mainly y + } + } \textbf{Direction of Incident \& Scattered Light} - & \multicolumn{5}{C{4cm}|}{z} - & \multicolumn{5}{C{3.9cm}|}{y} - & \multicolumn{9}{C{5cm}|}{between z and y, 10\textdegree{} to z} - \\ \hline + & \SetCell[c=5]{} z & & & & + & \SetCell[c=5]{} y & & & & + & \SetCell[c=9]{} between z and y, 10\textdegree{} to z & & & & & & & & + \\ \textbf{Number of Phonon} - & 1 & 2 % z E1 - & \threecol{2.4cm}{3} % z A1 - & \threecol{1.5cm}{1} % y z - & 2 % y x - & 3 % y y - & \fourcol{1} % 45 y&z mainly z - & 2 % 45 x - & \fourcol{3} % 45 y&z mainly y - \\ \hline + & 1 & 2 % z E1 + & \SetCell[c=3]{} 3 & & % z A1 + & \SetCell[c=3]{} 1 & & % y z + & 2 % y x + & 3 % y y + & \SetCell[c=4]{} 1 & & & % 45 y&z mainly z + & 2 % 45 x + & \SetCell[c=4]{} 3 & & & % 45 y&z mainly y + \\ \textbf{Vibration Direction} - & x (TO) & y (TO) % z E1 - & \threecol{2.4cm}{z (LO)} % z A1 - & \threecol{1.5cm}{z (TO)} % y z - & x (TO) % y x - & y (LO) % y y - & \fourcol{y-z mixed (LO-TO mixed)} % 45 y&z mainly z - & x (TO) % 45 x - & \fourcol{y-z mixed (LO-TO mixed)} % 45 y&z mainly y - \\ \hline + & {x \\ (TO)} & {y \\ (TO)} % z E1 + & \SetCell[c=3]{} z (LO) & & % z A1 + & \SetCell[c=3]{} z (TO) & & % y z + & {x \\ (TO)} % y x + & {y \\ (LO)} % y y + & \SetCell[c=4]{} {y-z mixed \\ (LO-TO mixed)} & & & % 45 y&z mainly z + & x (TO) % 45 x + & \SetCell[c=4]{} {y-z mixed \\ (LO-TO mixed)} & & & % 45 y&z mainly y + \\ \textbf{Representation in Group $\mathrm{C_{6v}}$} - & \twocol{2cm}{$\mathrm{E_1}$} - & \threecol{2.4cm}{$\mathrm{A_1}$} - & \multicolumn{14}{C{8.5cm}|}{Not applicable} - \\ \hline + & \SetCell[c=2]{} $\mathrm{E_1}$ & + & \SetCell[c=3]{} $\mathrm{A_1}$ & & + & \SetCell[c=14]{} Not applicable & & & & & & & & & & & & & + \\ \textbf{Representation in Group $\mathrm{C_{2v}}$} - & $\mathrm{B_2}$ & $\mathrm{B_1}$ % z E1 - & \threecol{2.4cm}{$\mathrm{A_1}$} % z A1 - & \threecol{1.5cm}{$\mathrm{A_1}$} % y z - & $\mathrm{B_2}$ % y x - & $\mathrm{B_1}$ % y y - & \fourcol{Not Applicable} % 45 y&z mainly z - & $\mathrm{B_2}$ % 45 x - & \fourcol{Not Applicable} % 45 y&z mainly y - \\ \hline + & $\mathrm{B_2}$ & $\mathrm{B_1}$ % z E1 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % z A1 + & \SetCell[c=3]{} $\mathrm{A_1}$ & & % y z + & $\mathrm{B_2}$ % y x + & $\mathrm{B_1}$ % y y + & \SetCell[c=4]{} Not Applicable & & & % 45 y&z mainly z + & $\mathrm{B_2}$ % 45 x + & \SetCell[c=4]{} Not Applicable & & & % 45 y&z mainly y + \\ \textbf{Scattering in Polarization} & xz & yz % z E1 & xx & yy & zz % z A1 @@ -334,40 +330,39 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories: & xx & yy & yz & zz % 45 y&z mainly z & xz % 45 x & xx & yy & yz & zz % 45 y&z mainly y - \\ \hline + \\ \textbf{Raman Intensity (a.u.)} - & \twocol{2cm}{$53.52$} % z E1 - & \twocol{1.4cm}{$53.52$} & $464.69$ % z A1 - & \twocol{1cm}{$56.86$} & $454.09$ % y z - & $53.52$ % y x - & $53.55$ % y y - & \twocol{1cm}{$53.71$} & $3.20$ & $425.98$ % 45 y&z mainly z - & $53.56$ % 45 x - & \twocol{1cm}{$3.60$} & $50.36$ & $27.99$ % 45 y&z mainly y - \\ \hline + & \SetCell[c=2]{} $53.52$ & % z E1 + & \SetCell[c=2]{} $53.52$ & & $464.69$ % z A1 + & \SetCell[c=2]{} $56.86$ & & $454.09$ % y z + & $53.52$ % y x + & $53.55$ % y y + & \SetCell[c=2]{} $53.71$ & & $3.20$ & $425.98$ % 45 y&z mainly z + & $53.56$ % 45 x + & \SetCell[c=2]{} $3.60$ & & $50.36$ & $27.99$ % 45 y&z mainly y + \\ \textbf{Visible in Common Raman Experiment} - & \twocol{2cm}{Yes} % z E1 - & \twocol{1.4cm}{Yes (LOPC)} & No % z A1 + & \SetCell[c=2]{} Yes & % z E1 + & \SetCell[c=2]{} {Yes \\ (LOPC)} & & No % z A1 & Yes (overfocused) & No & Yes (overfocused) % y z & Yes % y x - & Yes (LOPC) % y y - & \fourcol{???} % 45 y&z mainly z + & {Yes \\ (LOPC)} % y y + & \SetCell[c=4]{} ??? & & & % 45 y&z mainly z & ??? % 45 x - & \fourcol{???} % 45 y&z mainly y - \\ \hline + & \SetCell[c=4]{} ??? & & & % 45 y&z mainly y + \\ \textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)} - & \twocol{2cm}{$776.57$} % z E1 - & \threecol{2.4cm}{$933.80$} % z A1 - & \threecol{1.5cm}{$761.80$} % y z - & $776.57$ % y x - & $941.33$ % y y - & \fourcol{$762.76$} % 45 y&z mainly z - & $776.57$ % 45 x - & \fourcol{$940.86$} % 45 y&z mainly y - \\ \hline - \textbf{Electrical Polarity} & \multicolumn{19}{C{12.9cm}|}{Strong} - \\ \hline - \end{tabular} + & \SetCell[c=2]{} $776.57$ & % z E1 + & \SetCell[c=3]{} $933.80$ & & % z A1 + & \SetCell[c=3]{} $761.80$ & & % y z + & $776.57$ % y x + & $941.33$ % y y + & \SetCell[c=4]{} $762.76$ & & & % 45 y&z mainly z + & $776.57$ % 45 x + & \SetCell[c=4]{} $940.86$ & & & % 45 y&z mainly y + \\ + \textbf{Electrical Polarity} & \SetCell[c=19]{} Strong & & & & & & & & & & & & & & & & & & + \end{tblr} } \label{tab:phonon} \end{sidewaystable}