\begin{table}%T1
%\centering
\par
\caption{New magnetic dipole constants in
Mn I (A, in 10$^{-3}$ cm$^{-1}$) and comparison with previous
results.\label{tab1}}
\begin{tabular}{@{}llclll}
\hline\hline
Configuration & Level$^*$ & $E$ (cm$^{-1}$)$^*$& \multicolumn{2}{c}{$A$ (10$^{-3}$ cm$^{-1}$)} &  Ref. \\
 & & & This work & Previous &  \\ 
\hline
\par
3d$^5$4s$^2$ & a $^6$S$_{5/2}$ & 0 &  & --2.4157 & Davis et al.
(\cite{1971DAV})$^a$
\\
\\
3d$^6$($^5$D)4s & a $^6$D$_{9/2}$ & 17052.29 &  & 17.022 &
Dembczy\'nski et al.
(\cite{1979DEM})$^b$\\
& a $^6$D$_{7/2}$ & 17282.00 &  & 15.308 & Dembczy\'nski et al.
(\cite{1979DEM})$^b$\\
& a $^6$D$_{5/2}$ & 17451.52 &  & 14.567 & Dembczy\'nski et al.
(\cite{1979DEM})$^b$\\
& a $^6$D$_{3/2}$ & 17568.48 &  & 15.657 & Dembczy\'nski et al.
(\cite{1979DEM})$^b$\\
& a $^6$D$_{1/2}$ & 17637.15 &  & 29.422 & Dembczy\'nski et al.
(\cite{1979DEM})$^b$
\\
3d$^5$($^6$S)4s4p & z $^8$P$^\circ_{5/2}$ & 18402.46 &  &
19.08 & Handrich et al. (\cite{1969HAN})$^c$\\
& z $^8$P$^\circ_{7/2}$ & 18531.64 &  &18.23 & Handrich et al. (\cite{1969HAN})$^c$\\
& z $^8$P$^\circ_{9/2}$ & 18705.37 &  & 14.01 & Handrich et al.
(\cite{1969HAN})$^c$
\\
3d$^6$($^5$D)4s & a $^4$D$_{7/2}$ & 23296.67 & --5.5(3) & --5.7&
 Melendez (\cite{1999MEL})$^d$\\
& a $^4$D$_{5/2}$ & 23549.20 & --4.7(2) & --4.6& Melendez (\cite{1999MEL})$^d$\\
& a $^4$D$_{3/2}$ & 23719.52 & 0.9(4) & 0& Beynon (\cite{1977BEY})$^e$\\
& a $^4$D$_{1/2}$ & 23818.87 & 50.4(9) & 37 & Beynon
(\cite{1977BEY})$^e$
\\
3d$^5$ ($^6$S) 4s4p ($^3$P$^\circ$) & z $^6$P$^\circ_{3/2}$ &
24779.32 &  & 19.07 & Handrich et al. (\cite{1969HAN})$^c$\\
& z $^6$P$^\circ_{5/2}$ & 24788.05 &  & 15.591 & Handrich et al. (\cite{1969HAN})$^c$\\
& z $^6$P$^\circ_{7/2}$ & 24802.25 &  & 14.312 & Handrich et al.
(\cite{1969HAN})$^c$
\\ 
3d$^5$4s$^2$ & a $^4$G$_{11/2}$ & 25265.74 & 13.6(5)& & \\
 & a $^4$G$_{9/2}$ & 25285.43  & 13.7(5)&  &\\
 & a $^4$G$_{7/2}$ & 25287.74 & 15.0(5)&  &\\
 & a $^4$G$_{5/2}$ & 25281.04 & 20.2(2)&  &
\\
3d$^5$ ($^6$S) 4s4p ($^3$P$^\circ$) & z $^4$P$^\circ_{5/2}$ &
31001.15 &  & --20.3 & Kronfeldt et al. (\cite{1985KRON})$^f$\\
& z $^4$P$^\circ_{3/2}$ &31076.42 &  & --27.4 & Kronfeldt et al. (\cite{1985KRON})$^f$\\
& z $^4$P$^\circ_{1/2}$ & 31124.95 & --73.2(5) & --56 & Beynon
(\cite{1977BEY})$^e$
\\
%y6P
3d$^5$ ($^6$S) 4s4p ($^1$P$^\circ$) & y $^6$P$^\circ_{3/2}$ &
35689.98 &  & --32.4 & Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& y $^6$P$^\circ_{5/2}$ &35725.85 &  & --18.0 & Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& y $^6$P$^\circ_{7/2}$ & 35769.97 &  & --13.0 & Luc \& Gerstenkorn
(\cite{1972LG})$^g$
\\
%e8S
3d$^5$($^7$S)5s & e $^8$S$_{7/2}$ & 39431.31 &  25.2(5)& 24 &
Beynon (\cite{1977BEY})$^e$
\\
%e6S
3d$^5$($^7$S)5s & e $^6$S$_{5/2}$ & 41403.93 &  & (29) & Beynon
(\cite{1977BEY})$^e$
\\
%z6D
 3d$^6$ ($^5$D) 4p & z $^6$D$^\circ_{9/2}$ & 41789.48 & 3.1(1) & 3.5&
Beynon (\cite{1977BEY})$^e$\\
& z $^6$D$^\circ_{7/2}$ & 41932.64 & 1.4(2) & 2 & Beynon (\cite{1977BEY})$^e$\\
& z $^6$D$^\circ_{5/2}$ & 42053.73 & --8.3(5) & 3& Beynon (\cite{1977BEY})$^e$\\
& z $^6$D$^\circ_{3/2}$ & 42143.57 & --4.7(2) & --3.5 & Beynon (\cite{1977BEY})$^e$\\
& z $^6$D$^\circ_{1/2}$& 42198.56 & --26.3(4) & (--8) & Beynon
(\cite{1977BEY})$^e$
\\
%Z6F°
 3d$^6$($^5$D)4p & z $^6$F$^\circ_{11/2}$ & 43314.23 & 6.0(5) &  \\
  & z $^6$F$^\circ_{9/2}$ & 43428.58 & 5.2(4) &  \\
  & z $^6$F$^\circ_{7/2}$ &  43524.08 & 4.6(3)  &  \\
  & z $^6$F$^\circ_{5/2}$ & 43595.50 &  5.8 (3)  &  \\
  & z $^6$F$^\circ_{3/2}$ & 43644.45 & 9.1 (5)  &  \\
  \hline
   & z $^6$F$^\circ_{1/2}$ & 43672.66 &    &
\\
3d$^6$($^5$D)4p & z $^4$F$^\circ_{9/2}$ & 44288.76 & 4.5(5) & (5)
& Beynon (\cite{1977BEY})$^e$\\
& z $^4$F$^\circ_{7/2}$ & 44523.45 & 6.0(4) & 6 & Beynon (\cite{1977BEY})$^e$\\
& z $^4$F$^\circ_{5/2}$ & 44696.29 & 9.9(4) & 10 & Beynon (\cite{1977BEY})$^e$\\
& z $^4$F$^\circ_{3/2}$ & 44814.23 & 22.4(9) & 18 & Beynon
(\cite{1977BEY})$^e$
\\
 3d$^6$($^5$D)4p & x $^6$P$^\circ_{7/2}$ & 44993.92 & 9.1 (3) &  &  \\
 & x $^6$P$^\circ_{5/2}$ & 45156.11 & 8.7 (9) &  &  \\
 & x $^6$P$^\circ_{3/2}$ & 45259.17 & 12 (2) &  &
\\
3d$^6$($^6$D)4p & z $^4$D$^\circ_{7/2}$ & 45754.27 &  & 5&
 Beynon (\cite{1977BEY})$^e$\\
& z $^4$D$^\circ_{5/2}$ & 45940.93 & 1.9(3) & 6& Beynon (\cite{1977BEY})$^e$\\
& z $^4$D$^\circ_{3/2}$ & 46083.89 & 6.1(3) & 8& Beynon (\cite{1977BEY})$^e$\\
& z $^4$D$^\circ_{1/2}$ & 46169.93 &35.0(5)  & 19& Beynon
(\cite{1977BEY})$^e$
\\
 3d$^5$ 4s ($^7$S) 5p & y $^8$P$^\circ_{5/2}$ &45981.44 &  & 27.5 &
Melendez (\cite{1999MEL})$^d$\\
& y $^8$P$^\circ_{7/2}$ & 46000.77 &  & 20.0&Melendez (\cite{1999MEL})$^d$\\
& y $^8$P$^\circ_{9/2}$ & 46026.75 &  & 16.5 & Melendez (\cite{1999MEL})$^d$
\\
3d$^5$4s($^7$S)4d & e $^8$D$_{3/2}$ & 46706.09 & 39 (4) & & \\
& e $^8$D$_{5/2}$ & 46707.03 & 22 (2)  &  & \\
& e $^8$D$_{7/2}$ & 46708.33 & 19 (2) &  & \\
& e $^8$D$_{9/2}$ & 46710.15 & 15 (1) & & \\
& e $^8$D$_{11/2}$ & 46712.58 & 14.0 (8) & &
\\
3d$^6$($^5$D)4p & y $^4$P$^\circ_{5/2}$ & 46901.13 & --1.8(4) & (3)
& Beynon (\cite{1977BEY})$^e$\\
& y $^4$P$^\circ_{3/2}$ & 47154.51 &  & 1 & Beynon (\cite{1977BEY})$^e$\\
& y $^4$P$^\circ_{1/2}$ & 47299.29 & --34(2) & --8 & Beynon
(\cite{1977BEY})$^e$
\\
3d$^5$ 4s ($^7$S) 4d & e $^6$D$_{9/2}$ & 47207.28 &  & 15.5 &
Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& e $^6$D$_{7/2}$ & 47212.06 &  & 15.8 & Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& e $^6$D$_{5/2}$ & 47215.61 &  & 17.6 & Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& e $^6$D$_{3/2}$ & 47218.15 &  & 22.8 & Luc \& Gerstenkorn (\cite{1972LG})$^g$\\
& e $^6$D$_{1/2}$ & 47219.64 &  &  61.6 & Luc \& Gerstenkorn
(\cite{1972LG})$^g$
\\
3d$^5$ 4s ($^5$S) 5s & f $^6$S$_{5/2}$ & 49415.35 & --20.6(3) & --22
& Beynon (\cite{1977BEY})$^e$
\\ 
3d$^5$ 4s ($^5$S) 5s & e $^4$S$_{3/2}$ & 49591.51 & --50.5(4) & --49
& Fisher \& Peck (\cite{1939FP})$^h$\\
\\
3d$^5$ 4s($^7$S)6s & g $^6$S$_{5/2}$& 50904.68 & 23.2(5) &  & \\
\hline
\end{tabular}
\smallskip
$^a$ Spin-exchange optical pumping experiment.\\
$^b$ Laser-rf double resonance.\\
$^c$ Level crossing.\\
$^d$ Fitting of solar profiles.\\
$^e$ Reanalysis of old data. These results are
 quoted only when more accurate data are not available.\\
~Calculated values are given between parentheses.\\
$^f$ Laser-atomic beam spectroscopy.\\
$^g$ Fabry-Perot measurements and Fourier transform spectroscopy.\\
$^h$ Hollow cathode discharge and Fabry-Perot
interferometer.\\
$^*$ The notation and energy level values are
taken from Sugar \& Corliss (\cite{1985SC}).
\end{table}