A complete series
of experimental and theoretical investigations
on the supramolecular polymerization of chiral (1 and 2) and achiral (3) oligo(phenylene ethynylene)
tricarboxamides (OPE-TAs) is reported. The performance of seargents-and-soldiers
(SaS) and majority rules (MR) experiments has allowed deriving a full
set of thermodynamic parameters, including the helix reversal penalty
(HRP) and the mismatch penalty (MMP). The results described illustrate
the influence exerted by the number of stereogenic centers per monomeric
unit and the temperature on the chiral amplification phenomenon. While
the HRP decreases upon decreasing the number of chiral side chains,
the MMP follows an opposite trend. The experimental trend observed
in MR experiments contrasts with that reported for benzenetricarboxamides
(BTAs), for which the chiral amplification ability increases by lowering
the number of stereogenic centers or increasing the temperature. Theoretical
calculations predict that the rotational angle between adjacent monomeric
units in the stack (ca. 18°) gradually decreases when decreasing
the number of branched chiral side chains and leads to higher MMP
values, in good accord with the experimental trend. The reduction
of the rotational angle gives rise to less efficient H-bonding interactions
between the peripheral amide functional groups and is suggested to
provoke a decrease of the HRP as experimentally observed. In BTAs,
increasing the number of stereogenic centers per monomeric unit results
in a negligible change of the rotation angle between adjacent units
(ca. 65°), and, consequently, the steric bulk increases with
the number of chiral side chains, leading to higher MMP values. The
data presented herein contribute to shed light on the parameters controlling
the transfer and amplification of chirality processes in supramolecular
polymers, highlighting the enormous influence exerted by the size
of the self-assembling unit on the final helical outcome.
A series
of bis-cyclometalated iridium(III) complexes of general formula [Ir(ppy)2(N∧N)][PF6] (ppy– = 2-phenylpyridinate; N∧N = 2-(1H-imidazol-2-yl)pyridine (1), 2-(2-pyridyl)benzimidazole
(2), 1-methyl-2-pyridin-2-yl-1H-benzimidazole
(3), 2-(4′-thiazolyl)benzimidazole (4), 1-methyl-2-(4′-thiazolyl)benzimidazole (5))
is reported, and their use as electroluminescent materials in light-emitting
electrochemical cell (LEC) devices is investigated. [2][PF6] and [3][PF6] are orange
emitters with intense unstructured emission around 590 nm in acetonitrile
solution. [1][PF6], [4][PF6], and [5][PF6] are green weak emitters
with structured emission bands peaking around 500 nm. The different
photophysical properties are due to the effect that the chemical structure
of the ancillary ligand has on the nature of the emitting triplet
state. Whereas the benzimidazole unit stabilizes the LUMO and gives
rise to a 3MLCT/3LLCT emitting triplet in [2][PF6] and [3][PF6], the
presence of the thiazolyl ring produces the opposite effect in [4][PF6] and [5][PF6] and
the emitting state has a predominant 3LC character. Complexes
with 3MLCT/3LLCT emitting triplets give rise
to LEC devices with luminance values 1 order higher than those of
complexes with 3LC emitting states. Protecting the imidazole
N–H bond with a methyl group, as in complexes [3][PF6] and [5][PF6], shows that
the emissive properties become more stable. [3][PF6] leads to outstanding LECs with simultaneously high luminance
(904 cd m–2), efficiency (9.15 cd A–1), and stability (lifetime over 2500 h).
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