CH2OH
Hydroxymethyl radical
Species tag 031515
Version2*
Date of EntryDec. 2020
ContributorH. S. P. Müller

The hydroxymethyl radical has a fairly high barrier to inversion of the hydroxyl group. This causes a small splitting of order of 140 MHz. The b-dipole moment component connects the two tuneling states; a-type selection rules hold for pure rotational transitions, but the magnitude of the dipole moment component appears to be very small. With respect to the first entry from Mar. 2017, a large body of transition frequencies was added to the fit. These were published by
(1) O. Chitarra, M.-A. Martin-Drumel, B. Gans, J.-C. Loison, S. Spezzano, V. Lattanzi, H. S. P. Müller, and O. Pirali, 2020, Astron. Astrophys. 644, Art. No. A123.
Many new data were determined, data from the initial paper remeasured, and more data from the initial paper retained than in that initial paper, published by
(2) C. Bermudez, S. Bailleux, and J. Cernicharo, 2017, Astron. Astrophys. 598, Art. No. A9.
The data set still contains only transitions with Ka = 1 ↔ 0. Therefore, calculations for Ka = 2 ↔ 1 should be viewed with great caution, even more so for transitions with higher Ka. Caution is also advised for transitions with calculated uncertainties exceeding 0.2 MHz.
The quantum number format of the standard entry is N, Ka, Kc, vt, TSP, F, where vt is the tunneling state. vt = 0 is also designated as v = 0+, vt = 1 is also designated as v = 0. TSP is an aggregate spin number, which can be translated into (N), J, F1, I, and F through a aggregate_spin_number.txt. While I is given absolute, the other quantum numbers are given relative to F = 0. Alternatively the file with 8 quantum numbers may be consulted.
The eight quantum numbers are N, Ka, Kc, v, J + 0.5, F1, Itot, and F; J, F1, and F include the spin-angular momenta of the electron spin, the spin of the OH-H, and those of the two CH2-H.
At low temperatures, it may be useful to view ortho and para states separately; they are described by Ka + vi being even and odd, respectively. The 11,1, J + 0.5 = F1 = F = 2 level is the lowest para level and is 7.352 cm–1 above ground.
The dipole moment components are from a quantum chemical calculation by
(3) H. S. P. Müller, 2017, unpublished.

Lines Listed6241
Frequency / GHz< 1000
Max. J34
log STR0-7.5
log STR1-5.5
Isotope Corr.-0.0
Egy / (cm–1)0.0
 µa / Dsmall
 µb / D1.47
 µc / D 
 A / MHz194535.
 B / MHz29843.4
 C / MHz25947.5
 Q(300.0)36239.1835
 Q(225.0)23536.0048
 Q(150.0)12816.1289
 Q(75.00)4541.1670
 Q(50.00)2478.2511
 Q(37.50)1613.9624
 Q(25.00)883.3138
 Q(18.75)576.8918
 Q(12.50)317.5271
 Q(9.375)208.5837
 Q(5.000)85.4136
 Q(2.725)40.8305
detected in ISM/CSMno


Database maintained by Holger S. P. Müller and Sven Thorwirth, programming by D. Roth and F. Schlöder