You can find all quantum number labels and formats in the tables below
Quantum number labels and corresponding formats for each species in the ExoMolHR Database
| Molecule | Isotopologue | J Format | Quantum Number Labels & Formats |
|---|---|---|---|
| AlCl | 27Al35Cl |
J
%7d
|
|
| AlCl | 27Al37Cl |
J
%7d
|
|
| AlH | 27Al1H |
J
%7d
|
|
| AlO | 26Al16O |
J
%7.1f
|
|
| AlO | 27Al16O |
J
%7.1f
|
|
| AlO | 27Al17O |
J
%7.1f
|
|
| AlO | 27Al18O |
J
%7.1f
|
|
| BeH | 9Be1H |
J
%7.1f
|
|
| BeH | 9Be2H |
J
%7.1f
|
|
| C2 | 12C2 |
J
%7d
|
|
| C2H2 | 12C21H2 |
J
%7d
|
|
| C3 | 12C12C13C |
J
%7d
|
|
| C3 | 12C13C12C |
J
%7d
|
|
| C3 | 12C3 |
J
%7d
|
|
| CH4 | 12C1H4 |
J
%7d
|
|
| CH+ | 12C1H+ |
J
%7d
|
|
| CH+ | 13C1H+ |
J
%7d
|
|
| CN | 12C14N |
J
%7.1f
|
|
| CN | 12C15N |
J
%7.1f
|
|
| CN | 13C14N |
J
%7.1f
|
|
| CN | 13C15N |
J
%7.1f
|
|
| CO | 12C16O |
J
%7d
|
|
| CO2 | 12C16O2 |
J
%7d
|
|
| CO2 | 12C17O2 |
J
%7d
|
|
| CO2 | 12C18O2 |
J
%7d
|
|
| CO2 | 13C16O2 |
J
%7d
|
|
| CO2 | 13C17O2 |
J
%7d
|
|
| CO2 | 13C18O2 |
J
%7d
|
|
| CO2 | 16O12C17O |
J
%7d
|
|
| CO2 | 16O12C18O |
J
%7d
|
|
| CO2 | 16O13C17O |
J
%7d
|
|
| CO2 | 16O13C18O |
J
%7d
|
|
| CO2 | 17O12C18O |
J
%7d
|
|
| CO2 | 17O13C18O |
J
%7d
|
|
| CaH | 40Ca1H |
J
%7.1f
|
|
| CaO | 40Ca16O |
J
%7d
|
|
| CaOH | 40Ca16O1H |
J
%7.1f
|
|
| H2CO | 1H212C16O |
J
%7d
|
|
| H2CS | 1H212C32S |
J
%7d
|
|
| H2O | 1H216O |
J
%7d
|
|
| H2S | 1H232S |
J
%7d
|
|
| H3O+ | 1H316O+ |
J
%7d
|
|
| H3+ | 1H22H+ |
J
%7d
|
|
| H3+ | 1H3+ |
J
%7d
|
|
| H3+ | 2H21H+ |
J
%7d
|
|
| H3+ | 2H3+ |
J
%7d
|
|
| KH | 39K1H |
J
%7d
|
|
| KH | 40K1H |
J
%7d
|
|
| KH | 41K1H |
J
%7d
|
|
| LiOH | 6Li16O1H |
J
%7d
|
|
| LiOH | 7Li16O1H |
J
%7d
|
|
| MgH | 24Mg1H |
J
%7.1f
|
|
| MgH | 25Mg1H |
J
%7.1f
|
|
| MgH | 26Mg1H |
J
%7.1f
|
|
| MgO | 24Mg16O |
J
%7d
|
|
| MgO | 24Mg17O |
J
%7d
|
|
| MgO | 24Mg18O |
J
%7d
|
|
| MgO | 25Mg16O |
J
%7d
|
|
| MgO | 26Mg16O |
J
%7d
|
|
| N2 | 14N2 |
J
%7d
|
|
| N2O | 14N216O |
J
%7d
|
|
| N2O | 14N217O |
J
%7d
|
|
| N2O | 14N218O |
J
%7d
|
|
| N2O | 15N14N16O |
J
%7d
|
|
| NH | 14N1H |
J
%7d
|
|
| NH | 14N2H |
J
%7d
|
|
| NH | 15N1H |
J
%7d
|
|
| NH | 15N2H |
J
%7d
|
|
| NH3 | 14N1H22H |
J
%7d
|
|
| NH3 | 14N1H3 |
J
%7d
|
|
| NH3 | 14N2H21H |
J
%7d
|
|
| NH3 | 15N1H3 |
J
%7d
|
|
| NO | 14N16O |
J
%7.1f
|
|
| NO+ | 14N16O+ |
J
%7d
|
|
| NiH | 58Ni1H |
J
%7.1f
|
|
| NiH | 58Ni2H |
J
%7.1f
|
|
| NiH | 60Ni1H |
J
%7.1f
|
|
| NiH | 62Ni1H |
J
%7.1f
|
|
| OCS | 16O12C32S |
J
%7d
|
|
| OH | 16O1H |
J
%7.1f
|
|
| PH | 31P1H |
J
%7d
|
|
| PN | 31P14N |
J
%7d
|
|
| PS | 31P32S |
J
%7.1f
|
|
| SO | 32S16O |
J
%7d
|
|
| SO2 | 32S16O2 |
J
%7d
|
|
| SiN | 28Si14N |
J
%7.1f
|
|
| SiN | 28Si15N |
J
%7.1f
|
|
| SiN | 29Si14N |
J
%7.1f
|
|
| SiN | 30Si14N |
J
%7.1f
|
|
| SiO | 28Si16O |
J
%7d
|
|
| TiO | 46Ti16O |
J
%7d
|
|
| TiO | 47Ti16O |
J
%7d
|
|
| TiO | 48Ti16O |
J
%7d
|
|
| TiO | 49Ti16O |
J
%7d
|
|
| TiO | 50Ti16O |
J
%7d
|
|
| VO | 51V16O |
J
%7.1f
|
|
| YO | 89Y16O |
J
%7.1f
|
|
| YO | 89Y17O |
J
%7.1f
|
|
| YO | 89Y18O |
J
%7.1f
|
|
| ZrO | 90Zr16O |
J
%7d
|
|
| ZrO | 91Zr16O |
J
%7d
|
|
| ZrO | 92Zr16O |
J
%7d
|
|
| ZrO | 93Zr16O |
J
%7d
|
|
| ZrO | 94Zr16O |
J
%7d
|
|
| ZrO | 96Zr16O |
J
%7d
|
|
The formats and descriptions corresponding to quantum number labels
| Label | Fortran Format | C Format | Description |
|---|---|---|---|
| $J$ | I7/F7.1 | %7d/%7.1f | Rotational angular momentum excluding nuclear spin |
| F | I7 | %7d | Final angular momentum including nuclear spin (Only used in hyperfine-resolved datasets) |
| +/- | A1 | %1s | Total parity: + or - |
| e/f | A1 | %1s | Kronig rotationless parity: e or f |
| g/u | A1 | %1s | Gerade/ungerade: g or u |
| s/a | A1 | %1s | Inversional parity: s or a |
| Jpar | A1 | %1s | Parity excluding hyperfine effects: e or f |
| invpar, $\tau_\rm{inv}$ | I1 | %1d | Inversion parity (inversion-tunnelling molecules): 0 or 1 |
| rotpar, $\tau_\rm{rot}$ | I3 | %3d | Rotational parity |
| ivib | I2 | %2d | Index in vibrational symmetry block |
| irot | I2 | %2d | Index in rotational symmetry block |
| ElecState | A12 | %12s | Electronic state following the PyValem notation |
| $|\Lambda|$ | I5 | %5d | Projection of electronic angular momentum |
| $|\Sigma|$ | I5 | %5d | Projection of the electronic spin |
| $|\Omega|$ | I5 | %5d | Projection of the total angular momentum $\Omega = |\Lambda \pm \Sigma|$ |
| G$_{\rm{tot}}$ | A3 | %3s | Total symmetry |
| G$_{\rm{rot}}$ | A3 | %3s | Rotational symmetry |
| G$_{\rm{rve}}$ | A3 | %3s | Rovibrational (total) symmetry |
| G$_{\rm{vib}}$ | A3 | %3s | Vibrational symmetry |
| G$_{\rm{tor}}$ | A3 | %3s | Torsional symmetry |
| N | I3/I5 | %3d/%5d | Rotational quantum number excluding electron spin |
| L | I3 | %3d | Vibronic angular momentum quantum number |
| P | I2 | %2d | Polyad number |
| Pnum | I3 | %3d | Polyad counting number |
| Fi | I2/A4 | %2d/%4s | Spin component |
| U | A1 | %1s | U-notation of H$_3^+$ |
| G | I2 | %2d | Absolute value of $k-l_2$ |
| K | I3 | %3d | Projection of $J$ onto axis of molecular symmetry |
| $v$ | I3 | %3d | Vibrational quantum number |
| $n$ | I2 | %2d | Polyad or rotational counting number |
| $l$ | I2 | %2d | Normal mode vibrational angular momentum quantum number |
| $K_a$ | I2 | %2d | $K_a$ rotational quantum number |
| $K_b$ | I2 | %2d | $K_b$ rotational quantum number |
| $K_c$ | I2 | %2d | $K_c$ rotational quantum number |
| $v_i$ | I2 | %2d | Vibrational quantum number associated with the normal mode $v_i$ |
| $v_ia$,$v_ib$ | I2 | %2d | Vibrational quantum number |
| $n_i$ | I2/I4 | %2d/%4d | Normal mode vibrational quantum number |
| $l_i$ | I2 | %2d | Vibrational angular momentum quantum number associated with degenerate vibrational mode $v_i$ |
| $L_i$ | I4 | %4d | Vibrational angular momentum quantum number associated with degenerate vibrational mode $v_i$ |
| $M_i$, $m_i$ | I4 | %4d | Vibrational multiplicity quantum number associated with triply degenerate modes |
| $v_2lin$ | I2 | %2d | Linear molecule bending $v_2$ mode vibrational quantum number |
| $n_2lin$ | I2 | %2d | Normal mode linear molecule bending quantum number |
| Coef | F5.2 | %5.2f | Coefficient with the largest contribution to the ($J=0$) contracted set |
| nblock | I5 | %5d | Counting number in symmetry block denoted by ($J$, $\Gamma_\rm{tot}$, P) |
| nsisomer | A1 | %1s | Nuclear spin isomer |
ExoMolHR uses ExoMol data supported by ERC Advanced Investigator Projects 267219 and 883830