\begin{table}%t2
%%\centering
\par
\caption{E2 and M1 oscillator strengths
 for the $\rm 3p_{1/2}-3p_{3/2}$ spectral line.\label{tab2}} 
\begin{tabular}{llllll} 
\hline\hline
\ ION \ \ &  $Z$ & $f(E2)^a$ & $f(E2)^b$ & $f(M1)^a$ & $f(M1)^b$ \\
\cline{1-6}                                      
Sc~IX&21&1.072($-$11)&1.412($-$11)&1.548($-$07)&1.576($-$07)\\
Ti~X&22&1.751($-$11)&2.283($-$11)&2.027($-$07)&2.050($-$07)\\
V~XI&23&2.748($-$11)&3.599($-$11)&2.605($-$07)&2.624($-$07)\\
Cr~XII&24&4.225($-$11)&5.542($-$11)&3.249($-$07)&3.310($-$07)\\
Mn~XIII&25&6.311($-$11)&8.353($-$11)&4.109($-$07)&4.121($-$07)\\
Fe~XIV&26&9.370($-$11)&1.235($-$10)&5.065($-$07)&5.073($-$07)\\
Co~XV&27&1.356($-$10)&1.792($-$10)&6.176($-$07)&6.179($-$07)\\
Ni~XVI&28&1.937($-$10)&2.560($-$10)&7.459($-$07)&7.457($-$07)\\
Cu~XVII&29&2.706($-$10)&3.601($-$10)&8.945($-$07)&8.922($-$07)\\
Zn~XVIII&30&3.727($-$10)&4.998($-$10)&1.061($-$06)&1.059($-$06)\\
Ga~XIX&31&5.268($-$10)&6.849($-$10)&1.251($-$06)&1.249($-$06)\\
Ge~XX&32&7.115($-$10)&9.278($-$10)&1.466($-$06)&1.463($-$06)\\
As~XXI&33&9.568($-$10)&1.243($-$09)&1.708($-$06)&1.704($-$06)\\
Se~XXII&34&1.267($-$09)&1.650($-$09)&1.979($-$06)&1.973($-$06)\\
Br~XXIII&35&1.670($-$09)&2.168($-$09)&2.279($-$06)&2.273($-$06)\\
Kr~XXIV&36&2.185($-$09)&2.826($-$09)&2.616($-$06)&2.607($-$06)\\
Rb~XXV&37&2.847($-$09)&3.653($-$09)&2.987($-$06)&2.976($-$06)\\
Sr~XXVI&38&3.672($-$09)&4.686($-$09)&3.397($-$06)&3.384($-$06)\\
Y~XXVII&39&4.705($-$09)&5.968($-$09)&3.847($-$06)&3.832($-$06)\\
Zr~XXVIII&40&5.988($-$09)&7.552($-$09)&4.341($-$06)&4.325($-$06)\\
Nb~XXIX&41&7.575($-$09)&9.495($-$09)&4.882($-$06)&4.864($-$06)\\
Mo~XXX&42&9.527($-$09)&1.187($-$08)&5.472($-$06)&5.453($-$06)\\
Tc~XXXI&43&1.192($-$08)&1.475($-$08)&6.115($-$06)&6.095($-$06)\\
Ru~XXXII&44&1.483($-$08)&1.823($-$08)&6.812($-$06)&6.793($-$06)\\
Rh~XXXIII&45&1.836($-$08)&2.243($-$08)&7.569($-$06)&7.551($-$06)\\
Pd~XXXIV&46&2.262($-$08)&2.745($-$08)&8.387($-$06)&8.372($-$06)\\
Ag~XXXV&47&2.775($-$08)&3.345($-$08)&9.270($-$06)&9.260($-$06)\\
Cd~XXXVI&48&3.389($-$08)&4.058($-$08)&1.022($-$05)&1.022($-$05)\\
In~XXXVII&49&4.123($-$08)&4.903($-$08)&1.124($-$05)&1.125($-$05)\\
Sn~XXXVIII&50&4.995($-$08)&5.901($-$08)&1.234($-$05)&1.236($-$05)\\
Sb~XXXIX&51&6.029($-$08)&7.075($-$08)&1.352($-$05)&1.356($-$05)\\
\hline                               
TeXL&52&7.250($-$08)&8.452($-$08)&1.478($-$05)&1.484($-$05)\\
I~XLI&53&8.689($-$08)&1.006($-$07)&1.613($-$05)&1.621($-$05)\\
Xe~XLII&54&1.038($-$07)&1.194($-$07)&1.757($-$05)&1.768($-$05)\\
Cs~XLIII&55&1.236($-$07)&1.412($-$07)&1.910($-$05)&1.925($-$05)\\
Ba~XLIV&56&1.467($-$07)&1.665($-$07)&2.073($-$05)&2.093($-$05)\\
La~XLV&57&1.736($-$07)&1.958($-$07)&2.247($-$05)&2.271($-$05)\\
Ce~XLVI&58&2.049($-$07)&2.296($-$07)&2.431($-$05)&2.462($-$05)\\
Pr~XLVII&59&2.411($-$07)&2.685($-$07)&2.626($-$05)&2.664($-$05)\\
Nd~XLVIII&60&2.830($-$07)&3.132($-$07)&2.833($-$05)&2.880($-$05)\\
Pm~XLIX&61&3.313($-$07)&3.644($-$07)&3.052($-$05)&3.109($-$05)\\
Sm~L&62&3.870($-$07)&4.229($-$07)&3.284($-$05)&3.351($-$05)\\
Eu~LI&63&4.508($-$07)&4.898($-$07)&3.528($-$05)&3.609($-$05)\\  
Gd~LII&64&5.241($-$07)&5.660($-$07)&3.786($-$05)&3.881($-$05)\\                                                            
Tb~LIII&65&6.079($-$07)&6.526($-$07)&4.058($-$05)&4.170($-$05)\\                                                            
Dy~LIV&66&7.035($-$07)&7.509($-$07)&4.345($-$05)&4.475($-$05)\\                                                            
Ho~LV&67&8.123($-$07)&8.623($-$07)&4.646($-$05)&4.797($-$05)\\                                                            
Er~LVI&68&9.366($-$07)&9.884($-$07)&4.963($-$05)&5.138($-$05)\\                                                            
Tm~LVII&69&1.077($-$06)&1.131($-$06)&5.296($-$05)&5.497($-$05)\\                                                            
Yb~LVIII&70&1.237($-$06)&1.292($-$06)&5.645($-$05)&5.876($-$05)\\                                                            
Lu~LIX&71&1.418($-$06)&1.473($-$06)&6.012($-$05)&6.275($-$05)\\                                                            
Hf~LX&72&1.622($-$06)&1.676($-$06)&6.396($-$05)&6.696($-$05)\\                                                            
Ta~LXI&73&1.853($-$06)&1.905($-$06)&6.798($-$05)&7.138($-$05)\\                                                            
W~LXII&74&2.113($-$06)&2.161($-$06)&7.219($-$05)&7.603($-$05)\\ 
Re~LXIII&75&2.403($-$06)&2.449($-$06)&7.658($-$05)&8.092($-$05)\\                                                                                                                      
Os~LXIV&76&2.734($-$06)&2.760($-$06)&8.120($-$05)&8.606($-$05)\\                                                                                                                      
Ir~LXV&77&3.102($-$06)&3.130($-$06)&8.601($-$05)&9.146($-$05)\\                                                                                                                      
Pt~LXVI&78&3.515($-$06)&3.532($-$06)&9.103($-$05)&9.712($-$05)\\                                                                                                                      
Au~LXVII&79&4.190($-$06)&3.979($-$06)&9.790($-$05)&1.031($-$04)\\   
Hg~LXVIII&80&4.494($-$06)&4.479($-$06)&1.017($-$04)&1.043($-$04)\\   
\hline
\end{tabular}
In this table, $A$E($B$) denotes~$A\times 10^B$.\\
${}^a$ This work. \\
${}^{b}$ Huang (1986).
\end{table}