The bonding in the highly homoatomic
np
-
np
(
n 3)-bonded S
2I
42+ (three
+ two
bonds), the Se-I
-bondedSe
2I
42+ (four
+ one
bonds), and their higher-energy isomers have been studied using modern DFT and abinitio calculations and theoretical analysis methods: atoms in molecules (AIM), molecular orbital (MO), naturalbond orbital (NBO), and valence bond (VB) analyses, giving their relative energies, theoretical bond orders, andatomic charges. The aim of this work was to seek theory-based answers to four main questions: (1) Are thepreviously proposed simple
*-
* bonding models valid for S
2I
42+ and Se
2I
42+? (2) What accounts for the differencein the structures of S
2I
42+ and Se
2I
42+? (3) Why are the classically bonded isolobal P
2I
4 and As
2I
4 structures notadopted? (4) Is the high experimentally observed S-S bond order supported by theoretical bond orders, and howdoes it relate to high bond orders between other heavier main group elements? The AIM analysis confirmed thehigh bond orders and established that the weak bonds observed in S
2I
42+ and Se
2I
42+ are real and the bonding inthese cations is covalent in nature. The full MO analysis confirmed that S
2I
42+ contains three
and two
bonds,that the positive charge is essentially equally distributed over all atoms, that the bonding between S
2 and two I
2+units in S
2I
42+ is best described by two mutually perpendicular 4c2e
*-
* bonds, and that in Se
2I
42+, two SeI
2+moieties are
joined by a 6c2e
*-
* bond, both in agreement with previously suggested models. The VB treatmentprovided a complementary approach to MO analysis and provided insight how the formation of the weak bondsaffects the other bonds. The NBO analysis and the calculated AIM charges showed that the minimization of theelectrostatic repulsion between EI
2+ units (E = S, Se) and the delocalization of the positive charge are the mainfactors that explain why the nonclassical structures are favored for S
2I
42+ and Se
2I
42+. The difference in the structuresof S
2I
42+ and Se
2I
42+ is related to the high strength of the S-S
bond compared to the weak S-I
bond and theadditional stabilization from increased delocalization of positive charge in the structure of S
2I
42+ compared to thestructure of Se
2I
42+. The investigation of the E
2X
42+ series (E = S, Se, Te; X = Cl, Br, I) revealed that only S
2I
42+adopts the highly
np
-
np
(
n 3)-bonded structure, while all other dications favor the
-bonded Se
2I
42+ structure.Theoretical bond order calculations for S
2I
42+ confirm the previously presented experimentally based bond ordersfor S-S (2.1-2.3) and I-I (1.3-1.5) bonds. The S-S bond is determined to have the highest reported S-S bondorder in an isolated compound and has a bond order that is either similar to or slightly less than the Si-Si bondorder in the proposed triply bonded [(Me
3Si)
2CH]
2(
iPr)SiSi
SiSi(
iPr)[CH(SiMe
3)
2]
2 depending on the definition ofbond orders used.