A boron-doped helicene as a highly soluble, benchtop-stable green emitter

Polycyclic aromatic hydrocarbons (PAHs) are important constituents of many organic optoelectronic materials. In order to optimise a given PAH for a specific application, one has to be able to adjust its frontier orbital energy levels and, in turn, its light absorption/ emission characteristics and electron-accepting capacity. A very efficient approach relies on substitutional doping, i.e. the replacement of selected carbon atoms within the p-conjugated framework by other p-block elements. Among the possible dopants, N, P and S atoms lead to p-type materials, whereas B atoms give n-type PAHs, due to the inherently electron deficient and Lewis acidic nature of triarylboranes. For the fabrication of organic semiconductor devices, both p-type and n-type materials are required. Compared to the established p-type organic semiconductors, their B-doped congeners are far less well developed. Nevertheless, promising perspectives for the future already become evident: boron incorporation can lead to deeply coloured and/or highly luminescent compounds, capable of accepting electrons in a reversible manner and at comparatively low applied voltages. On the downside, many organoboranes are sensitive to air and moisture, such that sterically demanding substituents have to be attached for kinetic protection. Only in special cases, when three-coordinate B atoms constitute integral parts of a rigidly fixed cyclic skeleton, steric shielding is no longer necessary, because structural constraint disfavours adduct formation with Lewis bases, such as O2 and H2O. 6,7 Unfortunately, extended rigid PAHs usually require solubilising sidechains to make them solution processable. Solubilising sidechains, similar to the kinetically shielding substituents mentioned above, tend to perturb intermolecular interactions in organic layers, which is detrimental to efficient charge-carrier transport. Compared to planar PAHs, the solubility of related helicenes is typically much higher. In addition, p-donor helicenes have been found to form charge-transfer complexes with numerous p-acceptors, thereby indicating that their twisted scaffold still permits significant interactions with neighbouring p-electron clouds. We therefore decided to prepare the B-doped [4]helicene 1 (Fig. 1) as a member of an attractive new class of target compounds for further materials development. The actual design of 1 takes into account that its phosphorus analogue 2 already exists, such that 1 and 2 would give a unique pair of isostructural nand p-type compounds. Hatakeyama et al. synthesised 2 from Ar–PCl2 through a tandem phospha-Friedel–Crafts reaction under carefully optimised conditions (Ar = 2,6-(naphth-1-yl)2phenyl). 10 Related electrophilic borylation reactions have also been published. Yet, after some exploratory experiments we decided against a tandem bora-Friedel–Crafts strategy and rather opted for a twofold C–C-coupling approach using the tetrahalogenated triarylboranes 5 and 6 as starting materials (Scheme 1). In the case of 5, we aimed at the intramolecular nucleophilic substitution of both fluorine atoms by naphthyl anions generated through iodine–lithium exchange.

Polycyclic aromatic hydrocarbons (PAHs) are important constituents of many organic optoelectronic materials. In order to optimise a given PAH for a specific application, one has to be able to adjust its frontier orbital energy levels and, in turn, its light absorption/ emission characteristics and electron-accepting capacity. A very efficient approach relies on substitutional doping, i.e. the replacement of selected carbon atoms within the p-conjugated framework by other p-block elements. 1 Among the possible dopants, N, P and S atoms lead to p-type materials, whereas B atoms give n-type PAHs, due to the inherently electron deficient and Lewis acidic nature of triarylboranes. For the fabrication of organic semiconductor devices, both p-type and n-type materials are required. 2 Compared to the established p-type organic semiconductors, their B-doped congeners are far less well developed. 3,4 Nevertheless, promising perspectives for the future already become evident: boron incorporation can lead to deeply coloured and/or highly luminescent compounds, capable of accepting electrons in a reversible manner and at comparatively low applied voltages. 5 On the downside, many organoboranes are sensitive to air and moisture, such that sterically demanding substituents have to be attached for kinetic protection. Only in special cases, when three-coordinate B atoms constitute integral parts of a rigidly fixed cyclic skeleton, steric shielding is no longer necessary, because structural constraint disfavours adduct formation with Lewis bases, such as O 2 and H 2 O. 6,7 Unfortunately, extended rigid PAHs usually require solubilising sidechains to make them solution processable. Solubilising sidechains, similar to the kinetically shielding substituents mentioned above, tend to perturb intermolecular interactions in organic layers, which is detrimental to efficient charge-carrier transport. 4 Compared to planar PAHs, the solubility of related helicenes is typically much higher. 8 In addition, p-donor helicenes have been found to form charge-transfer complexes with numerous p-acceptors, thereby indicating that their twisted scaffold still permits significant interactions with neighbouring p-electron clouds. 8,9 We therefore decided to prepare the B-doped [4]helicene 1 (Fig. 1) as a member of an attractive new class of target compounds for further materials development. The actual design of 1 takes into account that its phosphorus analogue 2 already exists, 10 such that 1 and 2 would give a unique pair of isostructural n-and p-type compounds.
In line with the good solubility of 1, its solid-state structure reveals a twisted helical scaffold with a dihedral angle of 19.1(3)1 between the phenylene rings establishing the fjord region of the molecule (Fig. 2). In stark contrast, a structurally related, partially fused trinaphthylborane, in which the carbon skeleton is forced into planarity, showed very poor solubility even in C 6 D 5 Cl at 120 1C. 19 Each single crystal of 1 consists of molecules possessing the same absolute configuration (chiral space group P2 1 2 1 2 1 ), which is indicative of a favourable interaction between the homochiral helicenes. 8 The B-C bond lengths of 1 fall into the range of 1.532(13)-1.576(11) Å and are thus slightly shorter than those of the non-fused precursor 6 (1.572(7)-1.598(7) Å; Fig. 2). The boron atoms of 1 and 6 adopt trigonal-planar geometries.
1 gives rise to a broad 11 B NMR signal at 50 ppm, in good agreement with previous measurements on other B-doped PAHs. 6,19,20 The most downfield-shifted proton resonance at d = 8.79 belongs to the hydrogen atoms pointing into the fjord region of 1. The signals of the carbon atoms involved in the C-C-coupling reaction shift from 123.6/130.9 ppm (6) to 133.1/140.8 ppm (1).
The neat solid [4]helicene 1 possesses an orange colour. In cyclohexane solution, its longest-wavelength UV/vis absorption band appears at l max = 462 nm with an onset at 485 nm (optical band gap E opt G = 2.6 eV; Fig. 3). However, only concentrated solutions appear yellow-orange to the naked eye, whereas dilute solutions of 1 look green because of the bright green fluorescence brought about by the absorption of daylight (in concentrated samples, the fluorescence is largely quenched due to self-absorption). Upon excitation at l ex = 440 nm, cyclohexane solutions of 1 emit light with a wavelength of l em = 485 nm. Corresponding to the rigid molecular scaffold of 1, we note an appreciable quantum yield of QY = 81% and a rather small Stokes shift of 1026 cm À1 . The fluorescence band shows only a small positive solvatochromism (e.g., l em = 485 nm (cyclohexane), 500 nm (CHCl 3 )), thereby proving that it has little charge-transfer character.
In the cyclic voltammogram of 1, a reversible redox event is visible at E 1/2 = À 1.91 V (o-dichlorobenzene; vs. FcH/FcH + ). An irreversible transition is observed in the anodic region with a peak potential E pa = 1.14 V and an onset of approximately 1.00 V (electrochemical band gap E CV G E 2.9 eV). Compound 1 is still sufficiently Lewis acidic to form a pale yellow pyridine adduct 1Ápy. It crystallises from a mixture of 1  and excess pyridine in toluene/heptane with two crystallographically independent molecules in the asymmetric unit (Fig. 2). The B-N bonds are rather long 19 (1.693(7) Å, 1.695(7) Å) and the helical distortion of the PAH framework increases significantly upon adduct formation (dihedral angle between the terminal phenylene rings: 38.3(2)1/42.9(2)1 (1Ápy) vs. 19.1 (3)1 (1)). As evidenced by the recurrence of the green fluorescence of 1, microcrystalline 1Ápy readily loses its pyridine ligand when exposed to a dynamic vacuum or even to a stream of nitrogen. In pyridine-d 5 , the 11 B NMR signal of 1Ápy (À2 ppm) appears significantly upfield shifted compared to the resonance of the free Lewis acid 1 (50 ppm). Moreover, tetracoordination of the boron centre results in a significantly better shielding of all ortho-/para-CH carbon atoms.
First evidence for the successful derivatisation of 1 was gathered through its room-temperature bromination with N-bromosuccinimide in CHCl 3 . 19,21 Even though the reaction is not selective, HPLC workup finally provided an identifiable product. According to mass spectrometry, we obtained monobrominated 1 (m/z = 416); NMR spectroscopy indicated an H/Br exchange at the former phenyl ring and meta to the B atom.
To summarise, the benchtop-stable [4]helicene 1, which contains a B atom in the ring junction, shows excellent solubility even in hexane. Solubilising or kinetically protecting substituents are not required. As a general concept, we therefore propose to exploit the moderate helical distortion of PAHs for the development of solution-processable optoelectronic materials.