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calculated rovib spectral data for cis and trans HOCO at 296 K - J Phys Chem A Paper The Rovibrational Spectra of trans- and cis- HOCO, Calculated by MULTIMODE with ab initio Potential Energy and Dipole Moment Surfaces Stuart Carter, Yimin Wang and Joel M. Bowman∗

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https://figshare.com/articles/dataset/calculated_rovib_spectral_data_for_cis_and_trans_HOCO_at_296_K_-_J_Phys_Chem_A_Paper_The_Rovibrational_Spectra_of_trans-_and_cis-_HOCO_Calculated_by_MULTIMODE_with_ab_initio_Potential_Energy_and_Dipole_Moment_Surfaces_Stuart_Carter_Yimin_Wang_and_Joel_M_B/4643797
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The Rovibrational Spectra of trans- and cis- HOCO, Calculated by MULTIMODE with ab initio Potential Energy and Dipole Moment Surfaces Stuart Carter, Yimin Wang and Joel M. Bowman∗
   Supporting Information Description   The two files ‘trans296’ and cis296” are all spectral line intensities, as described in the paper, for trans and cis-HOCO, respectively at 296 K as a function of increasing transition energy, as shown in Figures 1 and 2 of the paper.  Each record in the files has a header with labels J" (N1,N2,N3,N4,N5,N6)" Ka" Kc" S   E" J' (N1,N2,N3,N4,N5,N6)' Ka' Kc' E' E'-E"  R^2(AU)  R^2(DEBYE^2) S(1/ATM/CM2) S(CM/MOLE) (P,Q,R?) followed by the corresponding data.  Each record is separated  by  **************************************************     All quantities denoted with “ are for the initial state and those denoted with ‘ are for the final state.  All energies, E” or E’ are in cm-1.  J Ka Kc are standard rotation quantum numbers, N1, etc. are labels for vibrational states corresponding to the normal modes in order of increasing energy, WITH THE EXCEPTION OF N6. This is a label for the delocalized torsion mode.  Here is the convention.  N6 = 0 is the ground torsion state of trans, N6=1 is the first excited torsion state of trans then for trans the sequence continues at N6=3, 5, 7, 9 etc for the first overtone, second overtone etc of trans.  N6=2 denotes the ground torsion state of cis.  (This is what is shown below).  Then N6=4,6,8, 10… denote excited cis torsions.  At some value of N6 we start to see delocalized states.  (See Wang, Y.; Carter, S.; Bowman, J. M. Variational Calculations Of Vibrational Energies and 
IR Spectra of trans- and cis-HOCO Using New ab initio Potential Energy and Dipole Moment 
Surfaces. J. Phys. Chem. A 2013, 117, 9343–9352. for a discussion of these.)  All data refer to the ground vibrational of cis or trans-HOCO for a range of J from 0 to 9 inclusive.  Note the quantum assignments (N1,N2,N3,N4,N5,N6)' for final states is just a rough guide.  In the example below 0 0 0 0 0 2 represents the ground vibrational state of cis-HOCO S is a symmetry label which here is always 1 and so can be basically ignored.   The third line is the transition energy, E’-E”, R^2 and S in two sets of units.  These are directly from eq. (1) of the paper, E” corresponds to Er and E’-E” to ni of that equation.  Finally a label for the type of rotational branch is given.  *************************************************************** 1   0   0   0     0      0    2    0   1    1  552.4591791570921 1   0   0   0     0   0   2   1  0    556.8613154782342 4.402136321142166  0.3578071515953164 2.311301415783682 0.151578443037134  6.1136425631820724E-021 Q
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2017-02-10
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