reference to the results presented in Table \[FTandlasertransition\] while accounting for the different [A$^1\Pi$]{} $\Lambda$-doubling components accessed by one- and two-photon transitions, leading to an absolute calibration uncertainty of VUV-FT of 0.01[cm$^{-1}$]{}. The frequencies of strongly absorbed, unsaturated, and unblended [A$^1\Pi-$X$^1\Sigma^+$]{} transitions were determined with a $1\sigma$ random uncertainty of 0.01 [cm$^{-1}$]{}and with somewhat greater uncertainties for weak and blended lines and those measured at 900K temperature, leading to total frequency uncertainties that vary between 0.01 and 0.03 [cm$^{-1}$]{}.

Transition vacuum wave numbers resulting from the combined analysis of all three [A$^1\Pi-$X$^1\Sigma^+$]{}$(0,0)$ spectra are presented in Table \[FTandlasertransition\] and vacuum wave numbers of the perturber lines are listed in Table \[FT-pert\].

[c@l@l@l@l@l@l]{}\
& &\
\
$J'' $ & R$_e(J'')  $ & Q$_f(J'')  $ & P $_e(J'')   $ & R $_e(J'')   $ & Q $_f(J'')   $ & P$_e(J'')$\
\
0 & 64754.15$^{ }$ & & & & &\
1 & 64756.51$^{ }$ & 64750.49$^{ }$ & & 22173.83$^{ wb }$ & 22166.35$^{ wb }$ & 22162.65$^{ wb }$\
2 & 64758.16$^{ b }$ & 64749.21$^{ }$ & 64743.12$^{ }$ & 22178.97$^{ w }$ & 22167.744$^{ }$ & 22160.34$^{ wb }$\
3 & 64759.15$^{ b }$ & 64747.26$^{ }$ & 64738.13$^{ }$ 