Knowledge Bank

Using both chirped pulse-, and low frequency cavity-based Fourier transform spectroscopy over 700 transitions have been recorded for the title molecule for the first time. The C$1$, C$2$ and C$3$ carbon-13 species have been observed in natural abundance allowing a substitution structure for the CCC backbone to be determined. Nearly all the transitions observed were either $a$-type $R$ branches or $b$-type $Q$ branches. No $c$-type transitions were observed. The $\chi aa$, $\chi bb$, $\chi cc$ and $\chi ab$ components of the iodine nuclear quadrupole coupling tensor have been determined. Of note, several forbidden transitions were also observed, such as $Jk-1,k+1$ $F$ = 14$\mathrm{<mrow\; data-mjx-texclass="ORD">4,10</mrow>}$ 23/2 $\leftarrow$ 12$\mathrm{<mrow\; data-mjx-texclass="ORD">5,7</mrow>}$ 21/2. In this particular case it seems that the upper energy level is nearly degenerate with a level connected to the lower energy level by a $\mu a$ dipole component term, but the lower energy level is also nearly degenerate with a second level connected to the upper energy level, again by a $\mu a$ dipole component term. The two intermediate energy levels are themselves connected by a $\mu b$ dipole component term. Near degeneracies such as these, together with a large $\chi ab$ value ($\approx$ 1 GHz) mean that certain $\Delta J=2$ transitions become allowed. This phenomena has been previously observed for 1-iodopropane by Fujitake and Hayashi (J. Mol. Spect, 127, (1988), 112-124).