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Table 1:

New molecular data for 12COa.
\begin{displaymath}{
{
\begin{tabular}{cc r@{.}l r@{.}l r@{ }l c r@{.}l c r@{.}l...
... 2238&8 & 42&51 & 13, 15, 17, 18 & k \\
\hline
\end{tabular}}}\end{displaymath}
References: (1) $\lambda_0$ and $\nu_0$ from Ubachs et al. (1994); (2) $A_{{\rm tot}}$ from Ubachs et al. (1994); (3) $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from Ubachs et al. (1994); (4) $\lambda_0$ and $\nu_0$ from vDB88; (5) $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from vDB88; (6) $f_{{{\rm v}}'0}$ and $A_{{\rm tot}}$ from Eidelsberg et al. (2006); (7) $\lambda_0$, $\nu_0$, $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from Cacciani et al. (2002); (8) $A_{{\rm tot}}$ from Drabbels et al. (1993); (9) $f_{{{\rm v}}'0}$ from Eidelsberg et al. (2004); (10) $\lambda_0$, $\nu_0$, $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from Ubachs et al. (2000); (11) $f_{{{\rm v}}'0}$ from Eidelsberg et al. (2006); (12) $A_{{\rm tot}}$ from Ubachs et al. (2000); (13) $\omega_{{\rm e}}'$, $\omega_{{\rm e}}x_{{\rm e}}'$ from Kepa (1988); (14) $\lambda_0$, $\nu_0$, $A_{{\rm tot}}$, $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from Cacciani et al. (2001); (15) $f_{{{\rm v}}'0}$ from Federman et al. (2001); (16) $\omega_{{\rm e}}'$, $\omega_{{\rm e}}x_{{\rm e}}'$ from Tilford & Vanderslice (1968); (17) $\lambda_0$, $\nu_0$, $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from Cacciani & Ubachs (2004); (18) $A_{{\rm tot}}$ from Cacciani et al. (1998).
Notes. a $\lambda_0$, $\nu_0$, ID and v' from Eidelsberg et al. (1992), $f_{{{\rm v}}'0}$, $A_{{\rm tot}}$, $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from ER90, unless noted otherwise. All $\eta$ are recomputed from the $f_{{{\rm v}}'0}$ and $A_{{\rm tot}}$. The notation a(b) in this and following tables means  $a~\times~10^{b}$. Many values are rounded off from higher-precision values in the references.
b The numbering follows vDB88. Their bands 1 and 2 are split into four and two components. The corresponding ER90 indices are also given.
c  $\omega_{{\rm e}}'$ and $\omega_{{\rm e}}x_{{\rm e}}'$ from the CO ground state (Guelachvili et al. 1983). $\omega_{{\rm e}}y_{{\rm e}}'$ and $\omega_{{\rm e}}z_{{\rm e}}'$ (not listed) are included in the model.
d  $\omega_{{\rm e}}'$ and $\omega_{{\rm e}}x_{{\rm e}}'$ from the CO+ $X~^2\Sigma^+$ state (Haridass et al. 2000).
e  $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from the CO+ $A~^2\Pi$ state (Haridass et al. 2000).
f  $\omega_{{\rm e}}'$ and $\omega_{{\rm e}}x_{{\rm e}}'$ from the CO+ $A~^2\Pi$ state (Haridass et al. 2000). $\omega_{{\rm e}}y_{{\rm e}}'$ (not listed) is included in the model.
g Vibrational constants derived from the different $\nu_0$ in one of six vibrational series: bands 30-27, 28-21, 25-20-16-8, 24-19, 22-18 or 15-5.
h  $B_{{\rm v}}'$ and $D_{{\rm v}}'$ from the CO+ $X~^2\Sigma^+$ state (Haridass et al. 2000).
i  $A_{{\rm tot}}$ depends on parity and/or rotational level (see Table 3). $A_{{\rm tot}}$ and $\eta$ are listed here for J'=0 and f parity.
j  $B_{{\rm v}}'$ and $D_{{\rm v}}'$ computed from the C18O values of ER90.
k $B_{{\rm v}}'$ and $D_{{\rm v}}'$ depend on parity (see Table 2); values are listed here for f parity.

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