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Supplementary material: A variationally computed IR line list for the methyl radical CH3

<p>Supplementary material to the manuscript:&nbsp;A.&nbsp;Y. Adam,&nbsp;A. Yachmenev, S.&nbsp;N. Yurchenko, P. Jensen, A variationally computed IR line list for the methyl radical CH<sub>3</sub>, submitted</p> <p>Contains following files</p> <ol> <li><em><strong>ch3_pes_f90.txt</strong></em> -&nbsp;Fortran 90 routine for calculating potential energy values for CH<sub>3</sub>.&nbsp;Please rename to ch3_pes.f90 before compiling.</li> <li><em><strong>ch3_dms_f90.txt</strong></em> - Fortran 90 routine for calculating electric dipole moment values for CH<sub>3</sub>.&nbsp;Please rename to ch3_dms.f90 before compiling.</li> <li><em><strong>ch3_pes_inp.txt</strong></em> - an input file for ch3_pes.f90 containing the ab initio potential energy parameters of CH<sub>3</sub>.&nbsp;</li> <li><em><strong>ch3_dms_inp.txt</strong></em> - an input file for ch3_dms.f90 containing the ab initio dipole moment parameters of CH<sub>3</sub>.</li> <li><em><strong>12C-1H3__AYYJ.pf</strong></em> - Partition function of CH<sub>3</sub></li> <li><em><strong>12C-1H3__AYYJ.states.bz2</strong></em> - Labelled ro-vibrational states for CH<sub>3</sub></li> <li><em><strong>12C-1H3__AYYJ__00000-01000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>,&nbsp;0-1000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__01000-02000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 1000-2000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__02000-03000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 2000-3000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__03000-04000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 3000-4000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__04000-05000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 4000-5000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__05000-06000.trans.bz2 </strong></em>- Transition file for CH<sub>3</sub>, 5000-6000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__06000-07000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 6000-7000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__07000-08000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 7000-8000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__08000-09000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 8000-9000 cm<sup>-1</sup></li> <li><em><strong>12C-1H3__AYYJ__09000-10000.trans.bz2</strong></em> - Transition file for CH<sub>3</sub>, 9000-10000 cm<sup>-1</sup></li> </ol> <p><br> <strong>Byte-by-byte description of .trans</strong>&nbsp;<br> -------------------------------------------------------------------------------<br> &nbsp; Bytes Format Units &nbsp; Label &nbsp;Explanations<br> -------------------------------------------------------------------------------<br> &nbsp; 1- 12 i12 &nbsp; &nbsp; --- &nbsp; &nbsp; N&#39; &nbsp; &nbsp;Upper state ID<br> &nbsp;14- 24 i12 &nbsp; &nbsp; --- &nbsp; &nbsp; N&quot; &nbsp; &nbsp;Lower state ID<br> &nbsp;27- 36 e10.4 &nbsp; s-1 &nbsp; &nbsp; A &nbsp; &nbsp; Einstein A-coefficient of the transition<br> -------------------------------------------------------------------------------</p> <p><br> <strong>Column-by-column description of states files: 12C-1H3__AYYJ.states.bz2</strong></p> <p>(QN=Quantum number)<br> ----------------------------------------------------------------------<br> &nbsp; Bytes Format Units &nbsp;Label &nbsp;Explanations<br> ----------------------------------------------------------------------<br> &nbsp; &nbsp;1- 12 &nbsp;i12 &nbsp; --- &nbsp; i &nbsp; &nbsp; &nbsp;State ID, non-negative integer index,&nbsp;starting at 1<br> &nbsp; 13- 25 &nbsp;i12 &nbsp; cm-1 &nbsp;E &nbsp; &nbsp; &nbsp;State energy term value in cm<sup>-1</sup><br> &nbsp; 26- 32 &nbsp;i6 &nbsp; &nbsp;--- &nbsp; g &nbsp; &nbsp; &nbsp;Total state degeneracy<br> &nbsp; 33- 40 &nbsp;i7 &nbsp; &nbsp;--- &nbsp; J &nbsp; &nbsp; &nbsp;[0/85] J&nbsp;quantum number, the total&nbsp;angular momentum excluding nuclear and electronic spin<br> &nbsp; 41- 45 &nbsp;i5 &nbsp; &nbsp;--- &nbsp; G &nbsp; &nbsp; &nbsp;[1/6] Total symmetry in D3h(M),&nbsp;(1,2,3,4,5,6)=A1&#39;,A2&#39;,E&#39;,A1&quot;,A2&quot;,E&quot;<br> &nbsp; 46- 51 &nbsp;i6 &nbsp; &nbsp;--- &nbsp; n1 &nbsp; &nbsp; A1&#39;, Normal mode quantum number (QN)<br> &nbsp; 52- 55 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n2 &nbsp; &nbsp; A1&#39;, Normal mode QN<br> &nbsp; 56- 59 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n3 &nbsp; &nbsp; E&#39;, Normal mode QN<br> &nbsp; 60- 63 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; l3 &nbsp; &nbsp; E&#39;, Normal mode QN<br> &nbsp; 64- 67 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n4 &nbsp; &nbsp; E&#39;, Normal mode QN<br> &nbsp; 68- 71 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; l4 &nbsp; &nbsp; E&#39;, Normal mode QN<br> &nbsp; 73- 76 &nbsp;i5 &nbsp; &nbsp;--- &nbsp; Gv &nbsp; &nbsp; Vibrational component symmetry in D3h(M)<br> &nbsp; 81- 83 &nbsp;i3 &nbsp; &nbsp;--- &nbsp; J &nbsp; &nbsp; &nbsp;[0/85] J is the total angular&nbsp;momentum excluding nuclear and electronic spin<br> &nbsp; 85- 87 &nbsp;i3 &nbsp; &nbsp;--- &nbsp; K &nbsp; &nbsp; &nbsp;[0/85] Projection of J on axis of molec.&nbsp;symmetry, in units of hbar<br> &nbsp; 90- 91 &nbsp;i2 &nbsp; &nbsp;--- &nbsp; Pr &nbsp; &nbsp; [0/1] Rotational parity tau, defined as (-1)<sup>tau</sup><br> &nbsp; 94- 95 &nbsp;i2 &nbsp; &nbsp;--- &nbsp; Gr &nbsp; &nbsp; Rotational component symmetry in D3h(M)<br> &nbsp; 98-102 &nbsp;f4.2 &nbsp;--- &nbsp; C^2 &nbsp; &nbsp;[0/1] Largest coefficient<br> &nbsp;106-109 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n1 &nbsp; &nbsp; TROVE QN C-H local model stretch<br> &nbsp;110-113 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n2 &nbsp; &nbsp; TROVE QN C-H local model stretch<br> &nbsp;114-117 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n3 &nbsp; &nbsp; TROVE QN C-H local model stretch<br> &nbsp;118-121 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n4 &nbsp; &nbsp; TROVE QN CHH local mode bend<br> &nbsp;122-125 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n5 &nbsp; &nbsp; TROVE QN CHH local mode bend<br> &nbsp;126-129 &nbsp;i4 &nbsp; &nbsp;--- &nbsp; n6 &nbsp; &nbsp; TROVE inversional QN<br> ----------------------------------------------------------------------</p> <p><strong>Byte-by-byte description of 12C-1H3__AYYJ.pf</strong><br> -------------------------------------------------------------------------------<br> &nbsp; Bytes Format Units &nbsp; Label &nbsp;Explanations<br> -------------------------------------------------------------------------------<br> &nbsp; 1- 9 &nbsp;f9.1 &nbsp; &nbsp;K &nbsp; &nbsp; &nbsp; T &nbsp; &nbsp; &nbsp;Temperature in Kelvin<br> &nbsp;11- 25 f15.4 &nbsp; --- &nbsp; &nbsp; Q &nbsp; &nbsp; &nbsp;Parition funcion<br> -------------------------------------------------------------------------------</p> <p><br> <strong>Contact Information</strong></p> <p>Andrey Yachmenev<br> andrey.yachmenev@desy.de<br> Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY,&nbsp;<br> Notkestrasse 85, D-22607 Hamburg, Germany,</p> <p>Sergei Yurchenko<br> s.yurchenko@ucl.ac.uk<br> Department of Physics and Astronomy, University College London,<br> Gower Street, London WC1E 6BT, United Kingdom</p> <p>&nbsp;</p>

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