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growth polymerization, PPYP 1b was of modest molecular
weight (trial 1: Mw = 10000 Da; trial 2: Mw = 12000 Da vs.
polystyrene standards) with an expectedly moderate polydis-
persity index (trial 1: PDI = 2.0; trial 2: PDI = 1.8).[13] Strik-
ingly, the GPC chromatogram shows several partially
resolved peaks at the low MW end (i.e. long retention time).
These peaks were significantly more prominent in the GPC
trace of the methanol-soluble material separated during the
precipitation of 1b (Figure 2). Speculating that these signals
were attributable to oligomers with formulation 1b bearing
alkyne end-groups [MALDI-TOF analysis shows ions for 1b
(n = 1 and 2; X = H-C ꢀ C-C6H2R2-; Y=-C ꢀ C-H)], the peak
maximum for each GPC signal was used to estimate the
molecular weight (vs. polystyrene) of each oligomer (neces-
sarily, each oligomer would be monodisperse). On that basis,
each peak in the chromatogram could be tentatively assigned
to a specific oligomer 1b (n = 1–5). Although the GPC
molecular weights (vs. polystyrene) were significantly over-
estimated [for example, n = 5: 3290 (GPC); 2297 (FW)],
a plot of formula weight vs. GPC molecular weight was linear
with a near-zero intercept (see the Supporting Information).
Importantly, such an observation not only suggests that the
assignments are correct but is consistent with the expected
overestimation of MW by GPC (vs. polystyrene) for a rigid
linear polymer such as PPYP.[14]
Figure 3. Molecular structures of 2·O (a) and 3·O (b) (50% probability
ellipsoids). Hydrogen atoms are omitted for clarity. Selected distances
() and angles (8): 2·O (a): P1-O1 1.481(2), P1-C1 1.793(3), P1-C7
1.751(3), P1-C15 1.750(3), C7-C8 1.201(4), C8-C9 1.443(4), C15-C16
1.204(4), C16-C17 1.439(4); C1-P1-C7 105.57(13), C1-P1-C15 105.30-
(13), C1-P1-O1 113.22(13), C7-P1-O1 115.08(12), C15-P1-O1 112.64-
(12), P1-C7-C8 173.6(3), C7-C8-C9 178.0(3), P1-C15-C16 173.4(3), C15-
C16-C17 178.1(3); 3·O (b): P1-O1 1.480(2), P1-C1 1.802(3), P1-C7
1.797(3), P1-C13 1.746(3), C13-C14 1.196(4), C14-C15 1.441(4); C1-P1-
C7 107.3(1), C1-P1-C13 104.6(1), C1-P1-O1 112.5(1), C7-P1-O1 111.1-
(1), C13-P1-O1 116.0(1), C7-P1-C13 104.6(1), P1-C13-C14 176.5(3),
C13-C14-C15 178.7(3). Angles between planes (8): 2·O (a): C9-C14 and
C17-C22 9.1, C1-C6 and C9-C14 79.9, C1-C6 and C17-C22 88.5; 3·O
(b): C15-C17’ and C7-C12 23.6, C15-C17’ and C1-C6 82.3.
To gain insight into any possible conjugative effects within
PPYPs, the X-ray crystal structures for model compounds 2·O
and 3·O were determined. Molecular structures are shown in
Figure 3.[15] Particularly interesting is that the C ꢀ C bond
lengths [2·O: 1.203(6) ; 3·O: 1.196(4) ] are at the long end
of the normal range for alkynes (ca. 1.18 ).[16] The P-Csp
bonds (2·O: 1.750(4) ; 3·O: 1.746(3) ] are shorter than the
P-CAr bonds [2·O: 1.793(3) ; 3·O: 1.800(4) ] but both are
significantly shorter than
a typical P-C single bond
(1.84 ).[16] Similar trends have been observed for related
alkynylphosphanes [for example, Ph2P(O)(C ꢀ CPh),[17]
Mes2P(C ꢀ CPh),[9f] and P(CCPh)3].[18] In addition, the aryl
rings bearing alkyne moieties are fairly close to coplanar
(angle between planes: 9.18). Similarly, in 3·O the angle
between the central arylene ring and one of the P-Ph rings is
23.68. The slight shortening of P-C and slight lengthening of
C ꢀ C bonds combined with the tendency for towards co-
planarity of the aryl groups in 2·O and 3·O may be reflective
of conjugative effects through the phosphorus moieties.
Although crystal packing effects could also contribute to the
relative orientations of the aryl rings, intermolecular pi-
stacking does not appear to be significant since there are no
close contacts between the aryl or arylene moieties of
adjacent molecules. The closest intermolecular contacts are
between the oxygen and the P-phenyl hydrogens in 2·O
(O1···H3 = 2.39 ) and between the oxygen and the C16-CH2
hydrogen of the hexyl substituent in 3·O (O1···H = 2.49 ).
Further insight into the electronic properties of PPYPs
may be gained by examining their photophysical properties.
The UV/Vis absorption spectra of polymers 1b and 1b·O
were recorded along with models 2, 2·O and 3·O. Each species
shows four characteristic bands in the UV region as does 1,4-
diethynyl-2,5-di-n-hexylbenzene. The absorption spectra for
the polymers are shown in Figure 4 (top). Importantly, the
two highest energy bands are significantly bathochromically
shifted for polymer 1b (lmax = 289 and 305 nm; e ꢁ 2
104 mÀ1 cmÀ1) relative to model 2 (lmax = 257 and 267 nm; e
ꢁ 4 104 mÀ1 cmÀ1) and 1,4-diethynyl-2,5-di-n-hexylbenzene
(lmax = 265 and 274 nm; e
ꢁ
3 104 mÀ1 cmÀ1). The two
lower energy bands of 1b (lmax = 317, 330 nm; e ꢁ 2
104 mÀ1 cmÀ1) are significantly more intense but less red-
shifted than in 2 (lmax = 306, 328 nm; e ꢁ 4 103 mÀ1 cmÀ1) and
1,4-diethynyl-2,5-di-n-hexylbenzene (lmax = 297, 308 nm; e
ꢁ 6 103 mÀ1 cmÀ1). A significant red shift in the absorbance
maxima is also observed for the oxidized PPYP (1b·O) when
compared to models (2·O and 3·O). Consistently, a low energy
tail that extends into the visible region is observed for the
PPYPs. In addition, each displays an additional weak
absorption (1b: 384 nm, 1b·O: 382 nm). A similar feature
has also been observed for poly(p-phenylene phosphane)s.[4g]
We have also investigated the emission properties for
these new PPYPs. Perhaps most striking is that a THF
solution of 1b·O shows a strong blue emission under a black
(UV) light whilst no such emission is observed for 1b.[19] For
1b·O, irradiation at 318 nm gives a broad emission spectrum
(lem = 339 nm) that extends well into the visible region
(Figure 4, bottom). Interestingly, model 2·O is not fluorescent
ꢀ 2015 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2015, 54, 11438 –11442