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Table 2

Parts of LSD entries 66801 and 66802 respectively with a pure rotational and hyperfine resolved spectrum of malononitrile.

Frequency (MHz) Uncertainty (MHz) Intensity a D2 σmn b (nm2 MHz) gup El (cm−1) J Ka$\[K_a^{\prime \prime}\]$ Kc$\[K_c^{\prime \prime}\]$ I c F c J Ka$\[K_a^{\prime}\]$ Kc$\[K_c^{\prime}\]$ I F
LSD entry 66802, Q = 11210484.6
23498.5408 0.0065 3.77 1.849 × 10−8 45 0.0 1 1 1 2 1 0 0 0 0 0
23498.5408 0.0065 8.09 3.970 × 10−8 45 0.0 1 1 1 2 1 0 0 0 2 2
23498.6914 0.0026 21.33 1.047 × 10−7 45 0.0 1 1 1 1 1 0 0 0 1 1
23498.7473 0.0012 27.65 1.358 × 10−7 105 0.0 1 1 1 2 3 0 0 0 2 2
23498.8031 0.0008 35.56 1.746 × 10−7 75 0.0 1 1 1 1 2 0 0 0 1 1
23498.8979 0.0031 0.75 3.698 × 10−9 45 0.0 1 1 1 0 1 0 0 0 2 2
23498.8980 0.0031 1.62 7.940 × 10−9 45 0.0 1 1 1 0 1 0 0 0 0 0
23498.9147 0.0035 19.75 9.696 × 10−8 75 0.0 1 1 1 2 2 0 0 0 2 2
23498.9706 0.0050 7.11 3.491 × 10−8 15 0.0 1 1 1 1 0 0 0 0 1 1
LSD Entry 66801, Q = 415203.0
23498.7845 0.0006 13.96 6.169 × 10−7 15 0.0 1 1 1 0 0 0

Notes. (a)Intensity corresponds to gJ |⟨m|μx|n⟩|2 for 66801 and to r × 9gF |⟨m|μx|n⟩|2 for 66802 and excludes gs, as explained in the text. The total upper level degeneracy factor gup was calculated including gs. (b)The absorption cross sections, σmn, were calculated for T = 300 K. (c)The following coupling scheme was used: I = I1 + I2, F = J + I.

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