Molecule Types <Prev Next>

Linear Molecules

See Making a linear molecule data file and the worked example: The Schumann-Runge Bands of O2 for an introduction to working with linear molecules.

PGOPHER will calculate Hund's cases (a) and (b) exactly, and will work with the other possible cases, though these typically require more work to set up.

Quantum Numbers

The following standard quantum numbers are used for linear molecules:
J
 Total angular momentum excluding nuclear spin
F
 Total angular momentum
S
 Total electron spin angular momentum. This must be set for each State
N
 J-S = Total angular momentum excluding nuclear and electron spin.
Λ The projection of the electronic orbital angular momentum onto the z axis of the molecule. This must be set for each State
Ω The projection of J onto the axis of the molecule; Ω = Λ + Σ where Σ is the projection of S onto the axis of the molecule.
Fn
 The notation F1, F2, F3 ... is an alternative notation for the components of a multiplet, ordered by energy with with F1 being the lowest.

Symmetry

For molecules with a centre of symmetry, Symmetric must be set at the Molecule level, and gerade set true or false for each State. If Symmetric is false, then gerade is ignored. Note that it is not possible to have gerade and ungerade states in the same manifold.

The overall parity of a particular state is displayed or read as + or -. In addition the J adjusted parity, e or f, is also displayed in most circumstances if JAdjustSym is set True at the Mixture level. Either form can be used on input, and in addition 0 for + and 1 for - parity. Note that JAdjustSym should be set to False if simulating hyperfine structure as otherwise confusing results can be obtained.

Basis States

The basis states used by  PGOPHER are Hund's case (a) though, as discussed under State, it will correctly calculate any Hund's case. The basis states are displayed as:
|Name J +- Omega>
where Name is the manifold and state name. If hyperfine structure is included in the calculation then F (and intermediate quantum numbers if there is more than one nucleus) is added to the end.

State Labels

The possible contents of state labels are:
Name
 The manifold and state name
J
 The J quantum number; not shown if ShowJ is false at the Molecule level
N
 The N quantum number; not shown if ShowN is false at the Molecule level or all states are singlet states
Ω The Ω quantum number; not shown if ShowOmega is false at the Molecule level (the default) or all states are singlet states
Fn
 The component of the multiplet numbered from 1 in order of increasing energy; not shown if ShowFNumber is false at the Molecule level or all states are singlet states. This contains the same information as the Ω quantum number, so it does not usually make sense to show both.
e/f
 The parity; not shown if Showef is false at the Molecule level.

Hyperfine quantum numbers are added at the end as required.
For example, a regular 2Π state may give the following label:
X v=0 7.5  7 F1e
where the name is X v=0, J = 7.5, N = 7 the parity is e and it is the F1 component (Ω = 1/2).

Note that the only guaranteed quantum numbers are the total angular momentum and symmetry; while PGOPHER tries to work out sensible assignments of the other quantum numbers there are cases where this is not possible, or the choice the program makes is not the same as other programs. This most commonly arises in the case of perturbations, or where S > J. The algorithm used can be adjusted by the EigenSearch and LimitSearch settings at the Manifold level; you may want to use LimitSearch = True as this can give more consistent results for the F1/F2... and N labels. Variations in the quantum number assignment does not affect other parts of the calculation, so the simulated positions and intensities are not affected by these considerations.

Branch Labels

The general format is ΔNΔJFn'Fn"p"(J) though, as for the state labels above some elements may be omitted:

ΔN The change in the N quantum number expressed as a P, Q or R; not shown if ShowN is false at the Molecule level or all states are singlet states
ΔJ The change J quantum number, expressed as P, Q or R.
Fn'Fn" The upper and lower (spin-orbit) component number. If the two numbers are the same, only one number is shown.
p" The lower state parity, expressed as e or f.
F',F
 If nuclear spin is included, the upper and lower state hyperfine (F) quantum numbers are added.

For example, a 2Π - 2Π band may give the following transition:

rR1e(6.5)    A v=0 7.5  7 F1e - X v=0 6.5  6 F1e

implying ΔN = +1 ( r ), ΔJ = +1 ( R ), F1 - F1 (1), e-e, J" = 6.5.

Further Details