The Table listed below provides examples of how the quantum numbers were resolved based on the "rules" that have been defined by JPL and CDMS. In general, while many of the examples provided below describe how the quantum numbers were translated, many of the molecular species contained in this database and others do NOT follow any exact rule for interpreting the transition. If there are questions on the translation, the user should refer back to the original reference of the molecule. All the references for each species contained in Splatalogue can be found by clicking on the molecular species of interest in the display list. See figure below:
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In addition, if the user wants to see the quantum number code, they can turn on the "Quantum Number Code" display contained in the "Miscellaneous" options in the left hand pane. | ![]() |
| Code Number |
Molecular Examples |
Electronic State(s) |
Unresolved QN | Description and Notes |
|---|---|---|---|---|
| 101 | CO, HCN, N2O | 1&Sigma | N | N = J, integer values |
| 102 | SO, C2S | 3&Sigma | N J | N, J, integer values |
| 112 | AlF, C17O | 1&Sigma | J F+1⁄2 | one nuclear spin, I=5⁄2 (Al, O) |
| 113 | 33SO | 3&Sigma | N J F+1⁄2 | one nuclear spin, I=3⁄2 (Cl) |
| 114 | HCCN | 3&Sigma | N J F1 F+1⁄2 | two nuclear spins, I=1 (N and H) |
| 123 | AlCl | 1&Sigma | J F+1⁄2 F | two nuclear spins, I=5⁄2(Al) I=3⁄2(Cl) | C15N, C2H | 2&Sigma | N J+1⁄2 F | one nuclear spin, I=1⁄2(15N, H) |
| 133 | SiN, MgNC | 2&Sigma | N J+1⁄2 F+1⁄2 | one nuclear spin, I=1(N) |
| 144 | 13CN | 2&Sigma | N J+1⁄2 F1 F | CDMS: J=N+S, F1=J+I(13C), F=F1+I (N) | N J+1⁄2 F2 F | JPL: J=N ± S; F1=S-I (13C)=0, F2=N
F1=S+I(13C)=1,
F2=N, N ±
1 |
(Q=12+2 = 14, for two I=1/2 spins, one I=1) |
| 154 | 13C2H, 13CCCCH | 2&Sigma | N J+1⁄2 F1 F+1⁄2 | Q=12, 3 spins of 1/2 (I=1/2, I=1/2, S=1/2),
N+1⁄2=J, J+1⁄2=F1,
F1+1⁄2=F |
| 202 | CH3C15N, CH3NC | 1A1 | N K | no hyperfine structure from nitrogen |
| 203 | SiC | 3&Pi | N p J | &Omega=1: N=J; &Omega=2: N=J+1; &Omega=2:N=J-1;
Exception: the J=1-0 & J=2-1 don't correspond to above rules
p is 1 or -1; for even J: 1=e & -1=f; for odd J: 1=f & -1=e |
13CH3CN | 1A1 | N K F | I=1/2 (13C) |
| 213 | SO+ | 2&Pir | N P J+1⁄2 | for &Pi1/2: J=N+1⁄2; for &Pi3/2: J=N-1⁄2
Lower States for odd J: p=1&rarr e ; p=-1 &rarr f
&Delta J=1, parity changes, but e-e or f-f |
CH335Cl | 1A1 | N K F+1⁄2 |
| 224 | CH, l-C7H, C8H | 2&Pir | N P J+1⁄2 F | for &Pi1/2: J=N+1⁄2; for &Pi3/2: J=N-1⁄2
Lower States for odd J: p=1&rarr e ; p=-1 &rarr f
&Delta J=0 (&Lambda -doublet), parity changes, but e-f
Lower States for odd J: p=1&rarr e ; p=-1 &rarr f
&Delta J=1, parity changes, but e-e or f-f |
| 234 | SiNC, SiCN | 2&Pir | N P J+1⁄2 F+1⁄2 | one nuclear spin, I=1 (N) for &Pi1/2: J=N+1⁄2; for &Pi3/2: J=N-1⁄2
Lower States for odd J: p=1&rarr e ; p=-1 &rarr f
&Delta J=1, parity changes, but e-e or f-f |
| 303 | HOCO+ | N Ka Kc | J=N | |
| ND3 | J Ka v | The K column has some strange alpha codes | ||
| 304 | CH2NH, NH2CHO | N Ka Kc | J=N | |
| 314 | CH2CN | 2B1 | N Ka Kc J+1⁄2 | there is a separate hyperfine structure calculation |
| 325 | HCO | 1A' | N Ka Kc J+1⁄2 F | |
| 814 | NO, NS | 2&Pir | J+1⁄2 &Omega+1⁄2 p F+1⁄2 | &Omega=1: &Pi1/2; &Omega=2, &Pi3/2 |
| 999 | CH3OH | N Ka Kc p v | From CDMS. For JPL CH3OH see code 1303
P is + or - for the A state only
The CDMS data is identical to SLAIM with exception of no calc
value where measurements are listed. |
|
| 1202 | CF+, CS | 1&Sigma | N=J v | |
| 1224 | CN | 2&Sigma | N v J+1⁄2 F | |
| 1234 | CN | 2&Sigma | N v J+1⁄2 F+1⁄2 | |
| 1303 | HCN, HNC, HCO+ | 1&Sigma | J l/p v | |
| CH3CCH | J K v | v is always 0 here | NH3, 15NH3 | J K v | v is 0 or 1 for Os and Oa sym and asy states | CH3OH | J K v | v=1-4 for diff. A and E labels (use SLAIM) |
| 1304 | CH3CN | N K v F | v=0 ground; v=1 K*l=0 l-doubling; v=2 K*l=0 1v8 CCN bend | |
| 1314 | N p v F | |||
| 1325 | l-C3H | 2&Pir | N p v J+1⁄2 F | |
| 1345 | i-C3H | 2B2 | N Ka Kc J+1⁄2 F | |
| 1404 | CH3OCH3, glycol, c-C3H2 | N Ka Kc v | ||
| 1405 | H2CCNH, NH2CO2CH3 | N Ka Kc v F | The "F" QN can also denote an A or E state as in the case for NH2CO2CH3 or 0s or 0a states as in NH2D | |
| 1905 | OH | 2&Pir | J+1⁄2 &Omega+1⁄2 p v F | column 2: 1=&Pi1/2 and 2=&Pi3/2; p is 1 or -1 and v is always 0
Only needs columns 1, 2, 3, 5 |
| 2306 | CH2 | 3B1 | N Ka Kc J Itot F | I |
| 3406 | H2NCH2CN | N Ka Kc F1 F | ||
| 6315 | CH2CN | 2B1 | N Ka Kc n F+1⁄2 | n is a combined quantum number (QN) because more than
  6 QNs are needed |
| 7416 | NH2 | N Ka Kc v n F | Column 4 is always 0; Column 5 ranges from 1-23=unknown |