Aromaticity reversals between the electronic ground (S
0
) and low-lying singlet (S
1
, S
2
) and
triplet
(T
1
, T
2
, T
3
) states of naphthalene
and anthracene are investigated by calculating the respective off-nucleus
isotropic magnetic shielding distributions using complete-active-space
self-consistent field (CASSCF) wavefunctions involving gauge-including
atomic orbitals (GIAOs). The shielding distributions around the aromatic
S
0
, antiaromatic S
1
(
1
L
b
), and aromatic S
2
(
1
L
a
) states
in naphthalene are found to resemble the outcomes of fusing together
the respective S
0
, S
1
, and S
2
shielding
distributions of two benzene rings. In anthracene,
1
L
a
is lower in energy than
1
L
b
, and as
a result, the S
1
state becomes aromatic, and the S
2
state becomes antiaromatic; the corresponding shielding distributions
are found to resemble extensions by one ring of those around the S
2
and S
1
states in naphthalene. The lowest antiaromatic
singlet state of either molecule is found to be significantly more
antiaromatic than the respective T
1
state, which shows
that it would be incorrect to assume that the similarity between the
(anti)aromaticities of the S
1
and T
1
states
in benzene, cyclobutadiene, and cyclooctatetraene would be maintained
in polycyclic aromatic hydrocarbons.