&	343.54	\\
57 (13, 45	) - 56	 (12, 44)	&	999597.559	&	0.09	&	19.3721	&	B 	&	565.96	\\
57 (13, 44	) - 56	 (12, 45)	&	999597.576	&	0.09	&	19.3721	&	B 	&	565.96	\\
26 (26, 1) - 26 (25, 2	)	&	999902.893	&	5.38	&	0.99380	&	B 	&	516.84	\\
26 (26, 0) - 26 (25, 1	)	&	999902.893	&	5.38	&	0.99380	&	B 	&	516.84	\\
27 (26, 2) - 27 (25, 3	)	&	999988.702	&	5.38	&	1.95270	&	B 	&	524.81	\\
27 (26, 1) - 27 (25, 2	)	&	999988.702	&	5.38	&	1.95270	&	B 	&	524.81	\\
\hline
\hline
\multicolumn{6}{r}{{\it{The entire table is available in electronic form on the CDS website http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/}}}  
\end{tabular}
\end{table*}
}


\onllongtab{9}{\begin{table}
\caption{\label{pldinplane}Sample table of the predicted transitions of the ground  vibrational state of CH$_2$DCH$_2$CN in-plane}
\centering
\begin{tabular}{ c c c c c c }
\hline 
\hline
Transition    						    & Calc. Frequency & Calc. Error & S & Dipole & E$\mathrm{_l}$  \\
J' (K'$\mathrm{_a}$, K'$\mathrm{_c}$) - J" (K"$\mathrm{_a}$, K"$\mathrm{_c}$) & (MHz)               & (MHz)        &    &           & (cm$^{-1}$) \\
\hline
3 (0,	3) - 2	 (0, 2	) &	25254.521	&	0.03	&	2.9995	&	A 	&	0.84	\\
3 (2,	2) - 2	 (2, 1	) &	25278.632	&	0.03	&	1.6667	&	A 	&	3.97	\\
3 (2,	1) - 2	 (2, 0	) &	25301.661	&	0.03	&	1.6667	&	A 	&	3.97	\\
4 (1,	3) - 4	 (0, 4	) &	25630.983	&	0.03	&	4.3159	&	B 	&	2.81	\\
3 (1,	2) - 2	 (1, 1	) &	25910.592	&	0.03	&	2.6666	&	A 	&	1.65	\\
5 (1,	4) - 5	 (0, 5	) &	26781.045	&	0.03	&	5.1502	&	B 	&	4.21	\\
6 (1,	5) - 6	 (0, 6	) &	28206.908	&	0.03	&	5.9108	&	B 	&	5.89	\\
7 (1,	6) - 7	 (0, 7	) &	29932.070	&	0.03	&	6.5861	&	B 	&	7.85	\\
6 (0,	6) - 5	 (1, 5	) &	29934.274	&	0.03	&	2.8151	&	B 	&	4.89	\\
8 (1,	7) - 8	 (0, 8	) &	31982.230	&	0.03	&	7.1666	&	B 	&	10.08	\\
4 (1,	4) - 3	 (1, 3	) &	32843.643	&	0.03	&	3.7498	&	A 	&	2.43	\\
4 (0,	4) - 3	 (0, 3	) &	33645.594	&	0.03	&	3.9988	&	A 	&	1.69	\\
4 (2,	3) - 3	 (2, 2	) &	33700.082	&	0.03	&	3	&	A 	&	4.81	\\
4 (3, 2) - 3	 (3, 1	) &	33717.726	&	0.03	&	1.75	&	A 	&	8.72	\\
...	&	&	&	&	&	\\
52 (2	, 50	) - 51	(1, 51)  &	996822.420	&	0.19	&	0.1924	&	B 	&	358.79	\\
81 (22, 59	) - 81	(21, 60) &	996989.852	&	0.59	&	39.3263	&	B 	&	1276.12	\\
81 (22, 60	) - 81	(21, 61) &	996989.852	&	0.59	&	39.3263	&	B 	&	1276.12	\\
77 (8	, 69	) - 76	(7, 70)  &	997182.226	&	0.09	&	14.1792	&	B 	&	863.19	\\
82 (22, 61	) - 82	(21, 62) &	997192.282	&	0.6	&	39.908	&	B 	&	1299.13	\\
82 (22, 60	) - 82	(21, 61) &	997192.282	&	0.6	&	39.908	&	B 	&	1299.13	\\
83 (22, 61	) - 83	(21, 62) &	997394.781	&	0.62	&	40.4899	&	B 	&	1322.41	\\
83 (22, 62	) - 83	(21, 63) &	997394.781	&	0.62	&	40.4899	&	B 	&	1322.41	\\
84 (22, 62	) - 84	(21, 63) &	997597.271	&	0.63	&	41.072	&	B 	&	1345.98	\\
84 (22, 63	) - 84	(21, 64) &	997597.271	&	0.63	&	41.072	&	B 	&	1345.98	\\
58 (9	, 49	) - 58	(6, 52)  &	997690.309	&	0.07	&	0.1427	&	B 	&	511.44	\\
75 (7	, 68	) - 74	(6, 69)  &	998163.363	&	0.13	&	8.4514	&	B 	&	810.36	\\
33 (16, 17	) - 32	(15, 18) &	998409.251	&	0.04	&	17.5865	&	B 	&	323.7	\\
33 (16, 18	) - 32	(15, 17) &	998409.251	&	0.04	&	17.5865	&	B 	&	323.7	\\
52 (3	, 50	) - 51	(0, 51)  &	999456.472	&	0.19	&	0.1921	&	B 	&	358.79	\\
55 (12, 44	) - 54	(11, 43) &	999572.240	&	0.03	&	18.7605	&	B 	&	512.11	\\
55 (12, 43	) - 54	(11, 44) &	99