Two diacetylide-triphenylamine hole-transport materials (HTM) with varying redox potential have been applied in planar junction The recent development of lead halide perovskite based solar cells has led to a step change in the efficiencies of solution-processable solar cells culminating recently in certified power-conversion efficiencies reaching the range 16-18%. 1 The exceptional performance of these devices has been attributed to key properties of the perovskite layer including excellent electron and exciton mobility and direct band gap of appropriate energy for visible light harvesting.
2To date, Spiro-OMeTAD has been most commonly used as the HTM in the highest efficiency cells, however this material requires an expensive multi-step synthesis and shows holetransport too low to carry all generated current. 3,4 In response, there has been increased recent interest in developing new HTMs aimed at addressing these limitations. [3][4][5][6][7][8][9][10][11][12] This work has explored alternative HTM structures, in particular based on the triarylamine and carbazole motifs, 6-11 leading to impressive power-conversion efficiencies (PCE) reaching around 14%. (Fig. 1a) was synthesised by a similar route to that we already reported for MeO-DATPA.
13This involved Ullmann coupling to form the triarylamine fragment, followed by Sonogashira coupling to add a trimethylsilyl acetylide fragment and, after deprotection to remove the trimethylsilyl unit, a final oxidative homocoupling to form the central diacetylide unit (see ESI â for full details).Single crystals suitable for X-ray diffraction (XRD) were obtained by layer addition in EtOAc/DMSO. Me 2 N-DATPA crystallised in the space group P2 1 /n and showed one molecule in the asymmetric unit (ESI â ). The structure is arranged with the central diacetylide moieties approximately parallel between molecules. As expected the geometry around each triphenylamine is approximately planar and viewed along the long molecular axis, the molecules form herringbone arrangements that run in alternating directions. No intermolecular interactions are within van der Waal radii, however the positioning of Me 2 N-groups on the periphery of the molecule enables