Biljana Bozic-Weber, Sven Y. Brauchli, Edwin C. Constable*, Sebastian O. Fürer, Catherine E. Housecroft*, Frederik J. Malzner, Iain A. Wright and Jennifer A. Zampese
Department of Chemistry, University of Basel, Spitalstrasse 51, CH4056 Basel, Switzerland. E-mail: edwin.constable@unibas.ch; catherine.housecroft@unibas.ch; Fax: +41 61 267 1018; Tel: +41 61 267 1008
First published on 12th July 2013
The syntheses of five homoleptic copper(I) complexes [CuL2][PF6] are described in which L is a 4,4′-di(4-bromophenyl)-6,6′-dialkyl-2,2′-bipyridine ligand (compounds 1–4 with methyl, nbutyl, isobutyl and hexyl substituents, respectively) or 4,4′-di(4-bromophenyl)-6,6′-diphenyl-2,2′-bipyridine (5). The new ligands 2–5 and copper(I) complexes [CuL2][PF6] (L = 1–5) have been fully characterized. The single crystal structures of 2{[Cu(1)2][PF6]}·3Me2CO, [Cu(2)2][PF6], 2{[Cu(3)2][PF6]}·Et2O and [Cu(5)2][PF6]·CH2Cl2 have been determined. The first three structures show similar distorted tetrahedral environments for the Cu+ ions with angles between the least squares planes of the bpy domains of 85.6, 86.4 and 82.9°, respectively; in contrast, the Cu+ ion in [Cu(5)2][PF6]·CH2Cl2 is in a flattened coordinate environment due to intra-cation face-to-face π-interactions. The solution absorption spectra of the complexes with ligands 1–4 are virtually identical with an MLCT band with values of λmax = 481–488 nm. In contrast, the absorption spectrum of [Cu(5)2][PF6] shows two broad bands in the visible region. Cyclic voltammetric data show that oxidation of the copper(I) centre occurs at a more positive potential in [Cu(2)2][PF6], [Cu(3)2][PF6] and [Cu(4)2][PF6] than in [Cu(1)2][PF6] or [Cu(5)2][PF6] with the latter being oxidized at the lowest potential. The complexes have been used to prepare dye-sensitized solar cells (DSCs) incorporating heteroleptic dyes of type [Cu(L)(Lanchor)]+ where L is 1–5 and Lanchor is a 6,6′-dimethyl-2,2′-bipyridine functionalized in the 4- and 4′-positions with phosphonic acid groups with (Lanchor = 7) and without (Lanchor = 6) a spacer between the metal-binding and anchoring domains. The presence of the spacer results in enhanced performances of the dyes, and the highest energy conversion efficiencies are observed for the dyes [Cu(3)(7)]+ (η = 2.43% compared to 5.96% for standard dye N719) and [Cu(5)(7)]+ (η = 2.89% compared to 5.96% for N719). Measurements taken periodically over the course of a week indicate that the cells undergo a ripening process (most clearly seen for [Cu(5)(6)]+ and [Cu(5)(7)]+) before their optimum performances are achieved. IPCE (EQE) data are presented and confirm that, although the photo-to-current conversions are promising (37–49% for λmax ≈ 480 nm), the copper(I) dyes do not realize the broad spectral response exhibited by N719.
Our recent investigations of copper(I)-based dyes have capitalized on the lability of copper(I) bis(diimine) complexes in solution which allows heteroleptic complexes containing {CuI(bpy)2} cores (bpy = 2,2′-bipyridine) to be assembled in situ by facile ligand exchange.9,12–14 One of the two ligands in the complex is selected for its ability to anchor the complex to a mesoporous TiO2 surface. Typical choices of anchoring units are carboxylic acid, phosphonic acid or phenol groups, but we have recently shown that DSCs incorporating dyes with phosphonic acid anchoring groups typically exhibit the best performances,9,13,14 consistent with the observations of Grätzel.15 The ancillary ligand in the dye is designed to provide efficient light-harvesting properties. It is well established that a 6,6′-dimethyl substitution pattern is required in bpy ligands for stabilization of copper(I).16 On the other hand, the photophysical and electrochemical properties of copper(I) bis(diimine) complexes are strongly influenced by the electronic and steric effects of the substituents, viz. 6,6′-substituents in bpy and 2,9-substituents in 1,10-phenanthroline (phen).8,17–22 Here we investigate the effects of varying the steric demands of the 6,6′-substituents in the bpy derived ancillary ligands 1–4 (Scheme 1) and the effects of going from alkyl to phenyl substituents (5, Scheme 1), in conjunction with the effects of introducing an aromatic spacer in the phosphonic acid anchoring ligands 6 and 7 (Scheme 1). The inclusion of the bromo-substituent in ancillary ligands 1–5 provides a built-in handle for further derivatization and tuning of electronic properties of the ligand as we have illustrated with the decoration of 1 with first and second generation hole-transport dendrons.14 The choice of 6,6′-substituents in 1–4 was made to explore the effects of alkyl chain length and steric demands on the performance of the surface-anchored dye. In anticipation that longer chains might inhibit assembly of dye complexes on the surface, we decided to trial a new anchoring ligand, 7, in which a phenyl spacer extends the spatial separation of the metal centre from the anchoring units compared to dyes incorporating anchoring ligand 6 (Scheme 2).
![]() | ||
Scheme 1 Ancillary ligands 1–5 and anchoring ligands 6 and 7, with the labelling scheme for 1H NMR spectroscopic assignments. Alkyl chains are labelled a, b... starting from the ring-attached CH2 unit. |
![]() | ||
Scheme 2 Schematic representation of the ten dyes studied in this work. |
Electrochemical measurements were made on a CH Instruments 900B potentiostat using glassy carbon, platinum wire and silver wire as the working, counter, and reference electrodes, respectively. Samples were dissolved in HPLC grade CH2Cl2 (10−4 to 10−5 mol dm−3) containing 0.1 mol dm−3 [nBu4N][PF6] as the supporting electrolyte; all solutions were degassed with argon. Cp2Fe was used as the internal reference.
(1E,5E)-1,6-Bis(4-bromophenyl)hexa-1,5-diene-3,4-dione and compound 1 were prepared as previously reported.14 Compound 623 was prepared by a modified literature method.24
The electrodes were cooled to ca. 80 °C and immersed in a 1 mM DMSO solution of the anchoring ligand 6 or 7 for 20 h. The colourless electrode was removed from the solution, washed with DMSO and EtOH and dried under a stream of N2. The electrode with the adsorbed anchoring ligand was immersed in a 1 mM MeCN solution of [Cu(L)2][PF6] (L = 1–4) and in a 1 mM CH2Cl2 solution of [Cu(5)2][PF6] for 4 days to produce red-orange coloured electrodes. The electrodes were removed from the solution and were washed with CH2Cl2 and dried under a stream of N2.
Each counter electrode was prepared from an FTO glass plate (Solaronix TCO22-7, 2.2 mm thickness, sheet resistance ≈7 Ω square−1) with a previously drilled hole. Residual organic impurities were removed by heating for 15 min at 500 °C on a heating plate and the perforated plate was washed with water, then 0.1 M HCl solution in EtOH and finally ultrasonicated in an acetone bath for 15 min. It was dried on a heating plate at 500 °C for 15 min. The Pt catalyst was deposited on the FTO glass plate by coating with Platisol T (2 × 25.0 μL), Solaronix, and dried on a heating plate at 500 °C for 15 min.
The dye-covered TiO2 electrode and Pt counter-electrode were assembled using a thermoplast hot-melt sealing foil (Solaronix, Meltonix 1170-25 Series, 25 microns thick) by heating while pressing them together. The electrolyte comprised LiI (0.1 mol dm−3), I2 (0.05 mol dm−3), 1-methylbenzimidazole (0.5 mol dm−3) and 1-butyl-3-methylimidazolinium iodide (0.6 mol dm−3) in methoxypropionitrile, and was introduced into the cell by vacuum backfilling. The hole on the counter electrode was finally sealed using the hot-melt sealing foil and a cover glass.
The solar cell measurements and testing protocol were performed using fully masked cells. A black coloured copper sheet was used for masking with a single aperture of an average area of 0.06012 cm2 (with a standard deviation of 1%) placed over the screen printed dye-sensitized TiO2 circle. The area of the aperture in the mask was smaller than the active area of the dye-sensitized TiO2 dot (0.288 cm2). For complete masking, tape was also applied over the edges and rear of the cell. Current density–voltage (I–V) measurements were made by irradiating from behind using a light source SolarSim 150 (100 mW cm−2 = 1 sun). The power of the simulated light was calibrated by using a reference Si photodiode. The standard dye N719 was purchased from Solaronix.
The quantum efficiency measurements were performed on an Spe-Quest quantum efficiency setup from Rera Systems (Netherlands) equipped with a 100 W halogen lamp (QTH) and a lambda 300 grating monochromator from Lot Oriel. The monochromatic light was modulated to 3 Hz using a chopper wheel from ThorLabs. The cell response was amplified with a large dynamic range IV converter from CVI Melles Griot and then measured with an SR830 DSP Lock-In amplifier from Stanford Research.
![]() | ||
Scheme 3 Synthetic route to compounds 2–5. |
The electrospray mass spectrum of each of compounds 2–5 exhibited a peak envelope as the base peak which corresponded to [M + H]+ and with an isotope pattern characteristic of the presence of two bromine atoms. The 1H and 13C NMR spectra were in accord with a 4,4′,6,6′-substituted 2,2′-bipyridine, and the spectra were assigned using COSY, NOESY, DEPT, HMQC and HMBC methods. The 1H NMR resonances for protons HA5 and HA3 were distinguished by the appearance of a cross peak in the HMBC spectrum of each of compounds 2–4 between signals for Ca and HA5. In the 500 MHz 1H NMR spectra of 2, 3 and 4, the signals for HB2 and HB3 overlap, and unambiguous assignments of the CB2 and CB3 resonances were not made from the HMQC or HMBC spectra.
Compounds 1–4 each contain alkyl substituents in the 6,6′-positions and their electronic absorption spectra are similar, being dominated by an intense band at 255 nm with a weaker band close to 305 nm (Fig. 1). Introduction of the 6- and 6′-phenyl substituents in compound 5 red-shifts both absorptions (to 265 and 321 nm). The enhancement of intensity of the higher energy band is consistent with the latter arising from π*←π transitions. The lower energy absorption shows no change in intensity along the series of five compounds, and is assigned to π*←n(py) transitions.
![]() | ||
Fig. 1 Absorption spectra of ligands 1–5 (CH2Cl2, 1.0 × 10−5 mol dm−3). |
In terms of ligand design for dyes for DSCs, compound 5 appears superior to 1–4 in terms of red-shifting of the spectral response, and we later confirm that this trend is preserved in the homoleptic copper(I) complexes of these ligands.
![]() | ||
Scheme 4 Synthesis of 7: (i) [Pd(PPh3)4], Cs2CO3, HPO3Et2, THF, microwave, 110 °C, 90 min; (ii) aqueous HCl, reflux, 48 h. |
Scheme 4 summarizes the synthesis of 7 from the corresponding ester, 7a (in turn obtained from ligand 1); preparation of the latter was based upon a literature method.31 After deprotection by treatment with aqueous HCl and workup, 7a was isolated in 65% yield. The base peak in the ESI mass spectrum (m/z 609.3) arose from the [M + H]+ ion and a much less intense peak at m/z 631.2 was assigned to [M + Na]+.
X-ray quality crystals of 7a were grown by diffusion of a mixture of pentane and hexane (1:
1 by volume) into a concentrated acetone solution of the compound. Structural determination confirmed the structure shown in Fig. 2. The bpy unit adopts the expected trans conformation and the two halves of the molecule are related by an inversion centre. Compound 7a is disordered and the OEt group containing O3 has been modelled over two sites with 49 and 51% occupancies; the methyl group of the second OEt unit has been modelled over two sites of occupancies 74 and 26%. The phenyl ring is twisted through 29.3° with respect to the pyridine ring. Although the molecules pack with the aromatic domains over one another, the presence of the methyl substituents prevents efficient face-to-face π-stacking interactions. The dominant packing forces involve CH⋯O and CH⋯N contacts.
![]() | ||
Fig. 2 ORTEP representation of compound 7a (ellipsoids plotted at 40% probability level; only the major occupancy sites are shown). Symmetry code i = 1 − x, 1 − y, 1 − z. Selected bond distances and angles: N1–C2 = 1.3389(14), N1–C6 = 1.3442(13), C10–P1 = 1.7888(9), P1–O1 = 1.4629(9), P1–O3 = 1.5457(16), P1–O2 = 1.5885(8), O2–C13 = 1.4515(14), O3–C15 = 1.461(3) Å; C2–N1–C6 = 117.68(8), O1–P1–O3, 107.04(8), O1–P1–O2 = 115.27(4), O3–P1–O2 = 103.00(7), O1–P1–C10 = 113.61(5), O3–P1–C10 = 110.31(6), O2–P1–C10 = 107.07(5)°. |
Quantitative conversion of the ester 7a into phosphonic acid 7 was achieved using aqueous HCl (6 M) at reflux followed by treatment of the residue obtained with aqueous acetic acid. This latter step appears to be essential for the isolation of pure 7. Compound 7 is poorly soluble in most common solvents and it was not possible to obtain an electrospray mass spectrum. However, satisfactory elemental analysis was obtained for the hydrate 7·H2O. The solubility of 7 in DMSO-d6 was sufficient to permit a 1H NMR spectrum to be recorded, but 13C NMR resonances could only be assigned using HMQC and HMBC methods; no cross peaks associated with CA2 (see Scheme 1 for atom labelling) in the HMBC spectrum were observed. Compound 7 dissolved readily in CF3CO2D. The 1H NMR spectrum was consistent with protonation of 7, although it is difficult to assess from the change in the chemical shift of the signal for HA3 (δ 8.53 ppm for 7 in DMSO-d6 to δ 8.67 ppm for the compound in CF3CO2D) whether the species present is [H27]2+ (trans-conformation of the bpy unit) or [H7]+ (cis-bpy). These conformational changes have been confirmed structurally for salts of [Hdmbpy]+ and [H2dmbpy]2+ (dmbpy = 6,6′-dimethyl-2,2′-bipyridine),32 and we have recently observed that addition of aliquots of trifluoroacetic acid to a CDCl3 solution of a ligand closely related to 7 leads to an initial downfield shift of the signals for HA3 from δ 8.39 to 8.53 ppm, followed by an upfield shift to δ 8.34 ppm corresponding to formation of first the monoprotonated and then the diprotonated ligand.33 Fully assigned NMR spectroscopic data for protonated 7 are given in the Experimental section.
![]() | ||
Fig. 3 The base peak envelope in the ESI mass spectrum of [Cu(3)2][PF6]. |
The 1H and 13C NMR spectra of the complexes were consistent with a single ligand environment in each complex. The spectra have been fully assigned using routine 2D methods.
X-ray quality crystals of 2{[Cu(1)2][PF6]}·3Me2CO were grown by Et2O diffusion into an acetone solution of the complex at room temperature, and Fig. 4 shows the structure of the [Cu(1)2]+ cation. The distorted tetrahedral coordination geometry of atom Cu1 is less flattened than in [Cu(dmbpy)2]+ (dmbpy = 6,6′-dimethyl-2,2′-bipyridine); in [Cu(1)2]+, the angle between the least squares planes containing Cu1 and each bpy unit is 85.6°, compared to angles of 74.3° in [Cu(dmbpy)2][PF6],9 80.9° in [Cu(dmbpy)2][BF4]34 and 80.9° in [Cu(dmbpy)2][ClO4].35 The flexibility of the Cu(bpy)2-unit is consistent with the suggestion35 that packing forces are responsible for the detailed geometry at the copper(I) centre. The two bpy units are close to planar (angles between the planes of the rings containing N1/N2 and N3/N4 = 5.5 and 7.9°, respectively), and the angles between the planes of the pairs of bonded phenyl and pyridine rings range from 10.1 to 34.9°. The variation in the latter is a consequence of packing interactions. Pairs of phenylpyridine units containing N1/C13 and N1i/C13i (symmetry code i = 1 − x, −y, 1 − z) sandwich one acetone solvent molecule which is disordered over two sites positioned about an inversion centre. The phenyl ring of the phenylpyridine unit containing N2 is π-stacked over its symmetry related counterpart (symmetry code = 1 − x, 1 − y, 1 − z) at a separation of 3.4 Å (Fig. S1†), and a similar interaction occurs between the phenylpyridine units containing N3 and N3ii (symmetry code ii = 3 − x, 1 − y, 2 − z). The phenylpyridine unit with N4 shows the greatest deviation from planarity and accommodates a hydrogen-bonded pair of acetone molecules over the pyridine ring (C102H10E...O100iii = 1.65 Å; symmetry code iii = 2 − x, −y, 2 − z). The space-filling diagram in Fig. 5a illustrates the shielding of the copper(I) centre by the methyl substituents.
![]() | ||
Fig. 4 ORTEP diagram of the [Cu(1)2]+ cation in 2{[Cu(1)2][PF6]}·3Me2CO (H atoms omitted and ellipsoids plotted at 40% probability level; only the major occupancy sites are shown). Bond parameters in the coordination sphere: Cu1–N4 = 2.010(4), Cu1–N1 = 2.027(4), Cu1–N3 = 2.034(4), Cu1–N2 = 2.038(4) Å; N4–Cu1–N1 = 130.67(18), N4–Cu1–N3 = 80.68(16), N1–Cu1–N3 = 124.04(16), N4–Cu1–N2 = 129.03(16), N1–Cu1–N2 = 81.49(17), N3–Cu1–N2 = 116.14(17)°. |
![]() | ||
Fig. 5 Space-filling representation of the (a) [Cu(1)2]+, (b) [Cu(2)2]+, (c) [Cu(3)2]+ and (d) [Cu(5)2]+ cations. In [Cu(2)2]+, only the major occupancy sites of the two disordered butyl chains are shown. |
Single crystals of [Cu(2)2][PF6] were grown by Et2O diffusion into an acetone solution of the complex; the structure of the [Cu(2)2]+ cation is shown in Fig. 6. The distorted tetrahedral coordination geometry of Cu1 is essentially the same as that in [Cu(1)2]+ with an angle between least squares planes containing Cu1 and each bpy unit of 86.4°. Each bpy unit is slightly twisted (angles between the planes of the rings containing N1/N2 and N3/N4 = 7.1 and 12.3°, respectively), and the angles between the planes of the pairs of bonded phenyl and pyridine rings lie in the range 11.1–29.8°, again a consequence of packing interactions. The butyl substituents of the ligand containing N3 and N4 are disordered; each of the three terminal C and attached H atoms have been modelled over two sites (C31, C32 and C33 with fractional occupancies 0.54 and 0.46, and C46, C47 and C48 with fractional occupancies 0.51 and 0.49). The presence of the disorder makes it meaningless to comment on the relative orientations of the butyl groups. Nonetheless, using the major occupancy sites, Fig. 5b illustrates how the butyl chains wrap around the copper(I) centre.
![]() | ||
Fig. 6 ORTEP representation of the [Cu(2)2]+ cation in [Cu(2)2][PF6] (H atoms omitted and ellipsoids plotted at 40% probability level; only the major occupancy sites are shown). Bond parameters in the coordination sphere: Cu1–N1 = 2.0368(14), Cu1–N2 = 2.0391(14), Cu1–N3 = 2.0283(15), Cu1–N4 = 2.0485(13) Å; N3–Cu1–N1 = 130.38(6), N3–Cu1–N2 = 126.86(6), N1–Cu1–N2 = 81.35(6), N3–Cu1–N4 = 81.16(6), N1–Cu1–N4 = 117.95(6), N2–Cu1–N4 125.08(5)°. |
Single crystals of 2{[Cu(3)2][PF6]}·Et2O were obtained by Et2O diffusion into an acetone–chloroform solution of the complex. Fig. 7 shows the structure of the [Cu(3)2]+ cation. The distorted tetrahedral coordination environment is similar to those in 2{[Cu(1)2][PF6]}·3Me2CO and [Cu(2)2][PF6]; the angle between the least squares planes containing Cu1 and each bpy unit is 82.9°. However, one bpy unit in [Cu(3)2]+ is significantly more twisted than in the complexes containing 1 and 2: angles between the planes of the rings with N1/N2 and N3/N4 of 12.3 and 29.0°, and this is probably a consequence of steric crowding originating from the four isobutyl groups which wrap around the metal centre (Fig. 6c). The isobutyl group containing C1 and C2 is disordered and has been modelled over two positions with site occupancies of 0.59 and 0.41; the carbon atom of the CH2 group is common to both positions. The distortion of the ligand containing N3 and N4 extends to the bromophenyl unit with Br4; the phenylpyridine unit is significantly bowed. The origin of the distortion is not clear but may be associated with interactions with the ordered [PF6]− ion which is sandwiched between the phenyl rings containing C52 and C58 with three short CH⋯F contacts in the range 2.59 and 2.71 Å. In addition, atom Br4 exhibits a short contact with Br2i (Br4⋯Br2i = 3.6922(7) Å, symmetry code i = 1 − x, ½ + y, ½ − z, van der Waals radius of Br = 1.95 Å).36 As in the two previous structures, the extent that each phenylpyridine unit deviates from planarity is controlled by packing forces with twist angles lying in the range 20.1–40.3°. The Et2O molecule is disordered and has been modelled over two sites on a special position.
![]() | ||
Fig. 7 ORTEP representation of the [Cu(3)2]+ cation in [Cu(3)2][PF6] (H atoms omitted and ellipsoids plotted at 40% probability level). Bond parameters in the coordination sphere: Cu1–N2 = 2.029(3), Cu1–N4 = 2.039(3), Cu1–N1 = 2.049(3), Cu1–N3 = 2.063(3) Å; N2–Cu1–N4 = 124.31(11), N2–Cu1–N1 = 81.30(11), N4–Cu1–N1 = 125.99(11), N2–Cu1–N3 = 122.66(11), N4–Cu1–N3 = 81.21(11), N1–Cu1–N3 = 127.62(11)°. |
Crystals of [Cu(5)2][PF6]·CH2Cl2 suitable for X-ray diffraction were grown by diffusion of Et2O into a CH2Cl2 solution of the complex. Fig. 8 shows the structure of the [Cu(5)2]+ cation and bond lengths and angles involving atom Cu1 are given in the caption. The complex crystallizes in the orthorhombic space group Pbcn with atom Cu1 lying on a two-fold axis. In contrast to [Cu(1)2]+, [Cu(2)2]+ and [Cu(3)2]+, the [Cu(5)2]+ cation possesses a flattened structure (Fig. 5) with an angle between the least squares planes containing Cu1 and each bpy unit of only 44.1°. This is a consequence of a π-stacking interaction between each 6- (or 6′-) phenyl-substituent and a pyridine ring of the adjacent ligand. To achieve four such interactions, the bpy domains deviate from planarity (19.6 and 30.3°, respectively) and each phenyl ring twists (31.2 and 62.4°) with respect to the pyridine ring to which it is bonded. Despite these conformational changes, optimal π-stacking interactions with parallel rings are not achieved. The structural features of the copper(I) coordination sphere in [Cu(5)2]+ are consistent with the flattening observed in a range of {Cu(6,6′-Ph2bpy)2}+, {Cu(2,9-Ph2phen)2} and related complexes,20,21,37–50 although within these examples, the efficiency of the intra-cation π-interactions is variable. In [Cu(5)2][PF6]·CH2Cl2, face-to-face π-stacking occurs between pendant phenyl rings of neighbouring cations leading to columns of [Cu(5)2]+ cations running parallel to the a-axis. Additional packing interactions involve short Br⋯Br contacts, and close CH⋯F and CH⋯Cl contacts; both the [PF6]− ion and the CH2Cl2 molecule are ordered.
![]() | ||
Fig. 8 ORTEP representation of the [Cu(5)2]+ cation in [Cu(5)2][PF6]·CH2Cl2 (H atoms omitted and ellipsoids plotted at 30% probability level). Bond parameters in the coordination sphere: Cu1–N1 = 2.013(6), Cu1–N2 = 2.017(6) Å; N1–Cu1–N1i = 83.6(4), N1–Cu1–N2i = 138.5(2), N1–Cu1–N2 = 112.1(2), N2i–Cu1–N2 = 82.0(4)°. Symmetry code i = −x, y, 3/2 − z. |
The solution electronic absorption spectra of [CuL2][PF6] with L = 1–5 are shown in Fig. 9. Spectra for the complexes containing the aliphatic side chains are virtually superimposable with high energy bands assigned to ligand-based π*←π transitions and a broad MLCT band in the visible region (λmax = 481–488 nm). The dual bands observed in the visible region of the spectrum [Cu(5)2][PF6] and the red-shift to 573 nm are consistent with features in the absorption spectrum of [Cu(dpp)2]+ (dpp = 2,9-diphenyl-1,10-phenanthroline) which are explained in terms of the flattened, low-symmetry structure of the complex.9,20 The spectrum of [Cu(5)2][PF6] retains the enhanced spectral response in the higher energy bands observed for ligand 5 compared to 1–4 (Fig. 1).
![]() | ||
Fig. 9 Absorption spectra of CH2Cl2 solutions (1.0 × 10−5 mol dm−3) of [CuL2][PF6] for L = 1–5. |
All the complexes are electrochemically active and cyclic voltammetric data are presented in Table 1. It is well established that in copper(I) diimine complexes, the presence of substituents adjacent to the N,N-donor sites (e.g. 6,6′-positions in 2,2′-bpy or 2,9-sites in 1,10-phenanthroline) stabilizes copper(I) with respect to oxidation by sterically hindering the flattening of the coordination sphere that accompanies the d10 (Cu+) to d9 (Cu2+) electronic configurational change.19,22 Cyclic voltammograms were recorded in CH2Cl2 to avoid problems associated with coordinating solvents such as MeCN.19 The potentials for the metal-centred oxidation process in [CuL2][PF6] with L = 1–4 follow the expected trend, with the complex containing the least sterically demanding (methyl) substituents being the easiest to oxidize: [Cu(1)2]+ < [Cu(2)2]+ ≈ [Cu(3)2]+ ≈ [Cu(4)2]+. The oxidation potential for [Cu(1)2][PF6] (+0.42 V) compares to +0.50 V (vs. Fc/Fc+ in CH2Cl2) for [Cu(dmp)2][PF6] (dmp = 2,9-dimethyl-1,10-phenanthroline). Oxidation of the copper(I) ion in [Cu(5)2]+ occurs at lower potential than in [Cu(1)2]+, and the value of +0.36 V is similar to that reported for [CuL2]+ where L = 4,4′,6,6′-tetraphenyl-2,2′-bipyridine (+0.39 V vs. Fc/Fc+ in CH2Cl2, corrected51 from the published value40 of +0.77 V vs. SCE). The structural reorganization that accompanies metal oxidation is less pronounced in [Cu(5)2]+ than in [Cu(1)2]+. This assumption is based upon the flattened geometry in the former brought about by π-stacking interactions that occur between the phenyl groups of one ligand and the bpy domain of the other. This has been observed in a number of related structures.37–41 Each of the complexes containing aliphatic substituents exhibits an irreversible oxidation process at higher potential (Table 1) most likely associated with the oxidation of the 4-bromophenyl substituent to the corresponding radical cation.52
[CuL2]+ | Anchor | On the day of sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 6 | 3.21 | 477 | 0.72 | 1.10 | 16.6 |
[Cu(2)2]+ | 6 | 3.64 | 478 | 0.71 | 1.24 | 18.8 |
[Cu(3)2]+ | 6 | 4.32 | 515 | 0.69 | 1.54 | 23.2 |
[Cu(4)2]+ | 6 | 3.57 | 475 | 0.71 | 1.21 | 18.3 |
[Cu(5)2]+ | 6 | 0.35 | 473 | 0.56 | 0.09 | 1.38 |
[Cu(1)2]+ | 7 | 5.09 | 497 | 0.72 | 1.82 | 27.5 |
[Cu(2)2]+ | 7 | 5.50 | 497 | 0.71 | 1.95 | 29.5 |
[Cu(3)2]+ | 7 | 6.73 | 541 | 0.70 | 2.55 | 38.5 |
[Cu(4)2]+ | 7 | 5.07 | 507 | 0.71 | 1.83 | 27.7 |
[Cu(5)2]+ | 7 | 2.74 | 605 | 0.66 | 1.10 | 16.6 |
N719 | 15.06 | 634 | 0.69 | 6.62 | 100.0 |
[CuL2]+ | Anchor | 3 days after sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 6 | 4.44 | 500 | 0.72 | 1.60 | 26.3 |
[Cu(2)2]+ | 6 | 3.51 | 506 | 0.67 | 1.19 | 19.5 |
[Cu(3)2]+ | 6 | 4.35 | 543 | 0.65 | 1.54 | 25.3 |
[Cu(4)2]+ | 6 | 3.97 | 505 | 0.70 | 1.40 | 23.0 |
[Cu(5)2]+ | 6 | 2.22 | 534 | 0.68 | 0.81 | 13.3 |
[Cu(1)2]+ | 7 | 5.85 | 519 | 0.72 | 2.19 | 36.0 |
[Cu(2)2]+ | 7 | 5.17 | 524 | 0.67 | 1.82 | 29.9 |
[Cu(3)2]+ | 7 | 7.02 | 566 | 0.63 | 2.49 | 40.8 |
[Cu(4)2]+ | 7 | 5.54 | 496 | 0.68 | 1.87 | 30.6 |
[Cu(5)2]+ | 7 | 6.41 | 600 | 0.73 | 2.80 | 45.9 |
N719 | 14.80 | 673 | 0.61 | 6.09 | 100.0 |
[CuL2]+ | Anchor | 4 days after sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 6 | 4.53 | 507 | 0.72 | 1.65 | 27.7 |
[Cu(2)2]+ | 6 | 3.56 | 502 | 0.66 | 1.18 | 19.8 |
[Cu(3)2]+ | 6 | 4.44 | 549 | 0.66 | 1.61 | 27.0 |
[Cu(4)2]+ | 6 | 4.21 | 514 | 0.69 | 1.50 | 25.2 |
[Cu(5)2]+ | 6 | 3.53 | 536 | 0.68 | 1.29 | 21.6 |
[Cu(1)2]+ | 7 | 6.01 | 527 | 0.73 | 2.30 | 38.6 |
[Cu(2)2]+ | 7 | 5.30 | 525 | 0.65 | 1.80 | 30.2 |
[Cu(3)2]+ | 7 | 7.06 | 571 | 0.60 | 2.43 | 40.8 |
[Cu(4)2]+ | 7 | 6.07 | 520 | 0.60 | 1.90 | 31.9 |
[Cu(5)2]+ | 7 | 6.70 | 592 | 0.73 | 2.89 | 48.5 |
N719 | 14.66 | 679 | 0.60 | 5.96 | 100.0 |
The surface-bound heteroleptic dyes [Cu(1)(6)]+, [Cu(2)(6)]+, [Cu(3)(6)]+ and [Cu(4)(6)]+ show a gain in values of JSC and VOC over the 4 day period, but overall there is little change to the fill factor for each cell. Of the four alkyl-substituted ligands, 3 (with isobutyl substituents) produces the most efficient dye with a relative energy efficiency, η, reaching 25.2% with respect to N719 measured under the same conditions. The efficiency of the dye is significantly improved by incorporating the aryl spacer into the anchoring ligand (i.e. going from [Cu(3)(6)]+ to [Cu(3)(7)]+), and after 4 days, the cell performs with a relative η of 40.8% (Table 2). A comparison of the values of JSC, VOC and η in Table 2 for a given dye containing 1, 2, 3 or 4 over the 7 day period reveals a small enhancement as the cell initially matures. Unexpectedly, the DSCs containing ligand 5 performed poorly on the first day, but as Table 2 shows, energy conversion efficiency improved considerably as the cell aged. This is mainly due to an increase in the short-circuit current density, for both [Cu(5)(6)]+ and [Cu(5)(7)]+. Once again, the presence of the aryl spacer in the phosphonic acid anchoring ligand is beneficial and a relative efficiency of 48.4% was achieved, compared to 21.6% without the spacer. The highly promising performances of dyes with the diphenyl-substituted ancillary ligand 5 are of interest in the context of recent findings of Chen and coworkers.8 Their key conclusions are that the photoinduced structural changes that occur to [Cu(dpp)2]+ (dpp = 2,9-diphenyl-1,10-phenanthroline) are small, and that changes in the orientations of the phenyl rings upon excitation result in a copper centre protected from solvent attack, thereby prolonging the MLCT lifetime in coordinating solvents. Chen and coworkers also conclude that electronic charge transferred from copper to dpp ligands does not reside on the phenyl rings since conjugation between phen and Ph domains is lost when the ligand changes its conformation. In our case, there is an additional degree of freedom associated with the rotation about the interannular C–C bond of the bpy ligand.
In order to check the reproducibility of our results, a new set of masked solar cells was prepared using anchoring ligand 7, and cell performances were measured over a 7 day period (Table 3). A comparison of the data in Tables 2 and 3 reveals analogous trends, although absolute efficiencies are lower for the second batch of cells than for the first. Fig. 10a shows plots of current density against open-circuit voltage for [Cu(3)(7)]+, illustrating the initial maturing of the cell, followed by consistent behaviour for a week. The ripening process of the cell containing [Cu(5)(7)]+ is illustrated in the I–V curve in Fig. 10b and replicates that observed for the first set of cells. Good fill factors were obtained for all cells in both sets (Tables 2 and 3).
![]() | ||
Fig. 10 Current density (JSC) against open-circuit voltage (VOC) curves for the dyes (a) [Cu(3)(7)]+ and (b) [Cu(5)(7)]+ over a period of 7 days. |
[CuL2]+ | Anchor | On the day of sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 7 | 4.77 | 503 | 0.73 | 1.76 | 24.9 |
[Cu(2)2]+ | 7 | 4.22 | 482 | 0.74 | 1.49 | 21.1 |
[Cu(3)2]+ | 7 | 6.42 | 555 | 0.73 | 2.60 | 36.7 |
[Cu(4)2]+ | 7 | 4.80 | 502 | 0.72 | 1.74 | 24.6 |
[Cu(5)2]+ | 7 | 3.97 | 605 | 0.69 | 1.67 | 23.6 |
N719 | 15.37 | 648 | 0.71 | 7.08 | 100.0 |
[CuL2]+ | Anchor | 1 day after sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 7 | 6.09 | 520 | 0.74 | 2.33 | 28.4 |
[Cu(2)2]+ | 7 | 5.61 | 499 | 0.74 | 2.06 | 25.1 |
[Cu(3)2]+ | 7 | 6.74 | 571 | 0.73 | 2.81 | 34.2 |
[Cu(4)2]+ | 7 | 5.92 | 510 | 0.73 | 2.19 | 26.6 |
[Cu(5)2]+ | 7 | 6.81 | 611 | 0.72 | 3.01 | 36.6 |
N719 | 17.10 | 677 | 0.71 | 8.22 | 100.0 |
[CuL2]+ | Anchor | 2 days after sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 7 | 5.93 | 525 | 0.74 | 2.31 | 27.8 |
[Cu(2)2]+ | 7 | 5.42 | 501 | 0.73 | 1.99 | 24.0 |
[Cu(3)2]+ | 7 | 6.91 | 576 | 0.72 | 2.87 | 34.6 |
[Cu(4)2]+ | 7 | 5.51 | 521 | 0.73 | 2.09 | 25.2 |
[Cu(5)2]+ | 7 | 6.96 | 606 | 0.74 | 3.10 | 37.4 |
N719 | 17.2 | 684 | 0.71 | 8.30 | 100.0 |
[CuL2]+ | Anchor | 7 days after sealing the cell | ||||
---|---|---|---|---|---|---|
JSC/mA cm−2 | VOC/mV | ff | η/% | Relative η/% | ||
[Cu(1)2]+ | 7 | 5.73 | 530 | 0.74 | 2.26 | 26.8 |
[Cu(2)2]+ | 7 | 5.51 | 513 | 0.74 | 2.09 | 24.7 |
[Cu(3)2]+ | 7 | 6.69 | 584 | 0.73 | 2.85 | 33.7 |
[Cu(4)2]+ | 7 | 5.44 | 531 | 0.71 | 2.05 | 24.3 |
[Cu(5)2]+ | 7 | 7.03 | 590 | 0.73 | 3.01 | 35.6 |
N719 | 17.23 | 696 | 0.71 | 8.45 | 100.0 |
The incident photon-to-current conversion efficiency (IPCE) or external quantum efficiency (EQE) spectra were measured for each of the solar cells detailed in Table 3. The spectra shown in Fig. 11a for [Cu(3)(7)]+ are representative of those of cells containing the dyes [Cu(1)(7)]+, [Cu(2)(7)]+, [Cu(3)(7)]+ and [Cu(4)(7)]+. The peak maxima in the IPCE spectra at ≈470 nm correlate with the observed maxima (λmax = 481–488 nm) in the solution absorption spectra of the homoleptic complexes [Cu(1)2]+, [Cu(2)2]+, [Cu(3)2]+ and [Cu(4)2]+ (Fig. 9). IPCE peak maxima of between 39 and 42% are achieved for [Cu(1)(7)]+, 38–40% for [Cu(2)(7)]+, 47–50% for [Cu(3)(7)]+ and 38–39% for [Cu(4)(7)]+, corresponding to the trends in efficiencies given in Table 3. Fig. 11b shows the IPCE spectra for [Cu(5)(7)]+ from the day of sealing to a week after sealing the cell. Initially an IPCE maximum of 28% is observed but, consistent with the ripening of the cell described above, this increases to 46% after a week. It is noticeable that the shape of the IPCE curve for [Cu(5)(7)]+ is close to those of the other complexes, i.e. the differences observed in the solution absorption spectra between the homoleptic complexes containing alkyl and phenyl substituents are not replicated in the IPCE curves of the heteroleptic complexes. To gain more insight into this, the absorption spectra of the surface-anchored heteroleptic dyes [Cu(3)(7)]+ and [Cu(5)(7)]+ were recorded. The anodes were prepared as described in the Experimental section (solar cell fabrication), and their absorption spectra are shown in Fig. 12. The absorption spectrum of the photoanode with adsorbed [Cu(5)(7)]+ also exhibits an enhanced spectral response at ca. 600 nm as also seen in the homoleptic complex [Cu(5)2]+ in solution (Fig. 9).
![]() | ||
Fig. 11 IPCE spectra for DSCs containing the anchored dyes (a) [Cu(3)(7)]+ and (b) [Cu(5)(7)]+ over a period of a week after sealing the solar cells. |
![]() | ||
Fig. 12 Normalized absorption spectra of photoanodes with surface-anchored heteroleptic dyes [Cu(3)(7)][PF6] and [Cu(5)(7)][PF6]. |
Fig. 13 compares the IPCE spectra of cells containing the five copper(I)-containing dyes with that of N719. The IPCE curves indicate improved response in the red region of the spectrum consistent with the red-shifting of the absorption spectra of the dyes containing ancillary ligand 5. While good photon-to-current quantum efficiency is achieved with the copper(I) dyes over the range 450–550 nm, the dyes do not achieve the broad spectra response exhibited by the state-of-the-art ruthenium(II) dye N719. Specifically, aspects of molecular design that need to be addressed include the further red-shifting of the absorption and also an increase in the absorptivity.
![]() | ||
Fig. 13 IPCE spectra of cells containing the copper(I)-containing dyes compared to a cell with standard dye N719. |
Footnote |
† Electronic supplementary information (ESI) available: Fig. S1. Packing interaction in 2{[Cu(1)2][PF6]}·3Me2CO. CCDC 942069–942073. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c3dt51416a |
This journal is © The Royal Society of Chemistry 2013 |