Abby Caseya,
Yang Hana,
Mark F. Wyattb,
Thomas D. Anthopoulosc and
Martin Heeney*a
aDept. Chemistry and Centre for Plastic Electronics, Imperial College London, London SW7 2AZ, UK. E-mail: m.heeney@imperial.ac.uk
bEPSRC UK National Mass Spectrometry Facility (NMSF), Swansea University Medical School, Singleton Park, Swansea, SA2 8PP UK
cDepartment of Physics and Centre for Plastic Electronics Imperial College London SW7 2AZ, UK
First published on 14th October 2015
The synthesis of the first soluble thieno[3,2-b]thiophene based porphyrazine (ZnTTPz) is reported from the cyclisation of 2,3-dicyano-5-octylthieno[3,2-b]thiophene. ZnTTPz can be considered the all thiophene analogue of naphthalocyanine. ZnTTPz exhibits a red-shifted absorption in solution and thin film, as well as a reduced band gap in comparison to the thiophene analogue due to an increased conjugation length. Films of ZnTTPz processed from solution exhibit p-type semiconducting behaviour in field-effect transistors with low hysteresis and reasonable charge carrier mobility.
Phthalocyanine consists of four benzenoid units fused to a central porphyrazine (Pz) core. Changing the type of aromatic group fused to the Pz core greatly influences the optoelectronic properties and solid state packing of the material. For instance, replacing the benzene groups (phthalocyanine – Pc) for naphthalene (naphthalocyanine – Nc) results in a significant red shift of the Q-band absorption (HOMO–LUMO transition) into the near-IR region. There are two regioisomers of naphthalocyanine: 2,3-Nc made from 2,3-dicyanonaphthalene in which the rings are linearly annulated, and 1,2-Nc made from 1,2-dicyanonapthalene in which the rings are angularly annulated. The magnitude of the Q-band shift is strongly dependent on the nature on this annulation. In addition, whilst 2,3-Ncs exist as a single isomer, 1,2-Ncs have four possible isomeric structures of C4h, CS, C2v and D2h symmetry.6,7 The replacement of the benzenoid units with heterocyclic groups is another route to tune the properties of the ring.8–12 For instance the incorporation of electron rich heterocycles such as thiophene (TPz)13 or selenophene (SePz)14 results in materials showing promising p-type charge carrier mobility in transistor devices.
Inspired by the promising transistor performance of TPz we have looked at extending the conjugation length by replacing thiophene with fused thieno[3,2-b]thiophene to form TTPz. TPz and TTPz can be considered the thiophene analogues of Pc and NPc respectively. More accurately TTPz can be considered as the thiophene analogue of 1,2-Nc as it also exists as four isomers with C4h, CS, C2v and D2h symmetry. Replacing the sulfur heteroatom in TTPz with vinyl groups directly leads to 1,2-Nc (see Fig. 1).
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| Fig. 1 Structures of zinc phthalocyanine (ZnPc), zinc-1,2-naphthalocyanine (Zn-1,2-Nc), tetrahydrobenzothiophene-fused porphyrazine (ZnTPz)18 and zinc 5-octylthienothiophene-fused porphyrazine (ZnTTPz). | ||
Herein, we report the first synthesis of ZnTTPz, and compare its optoelectronic properties to the reported properties of ZnPc,15 Zn-1,2-Nc,16 Zn-2,3-Nc17 and an alkylated derivative of ZnTPz.18 We also report the preliminary transistor performance in bottom gate transistor devices.
Fusing the thieno[3,2-b]thiophene unit to the porphyrazine core via the 2, 3 positions gives rise to four possible structural isomers, (see Fig. 2). The final cyclisation step forming the porphyrazine ring is expected to give a mixture of all four isomers due to a lack of selectivity. When synthesising CuTPz Takimiya and co-workers also made a mixture of isomers that could not be separated.13 Unlike CuTPz each isomer of ZnTTPz is structurally very different, resulting in the alkyl chains of each isomer pointing in different directions to the alkyl chains of the other isomers (see Fig. 2). However, despite the structural dissimilarity of the isomers we were still unable to separate them by column chromatography or size-exclusion chromatography. 1H NMR spectroscopy of ZnTTPz gave broad signals presumably due to the presence of the different isomers, the aromatic protons on the thienothiophene unit gave broad signals between 6.44 and 5.94 ppm (see Fig. S7†).
Table 1 compares both the experimental and theoretically calculated excitation energies of ZnTPz, ZnTTPz, ZnPc, Zn-1,2-Nc and Zn-2,3-Nc. DFT calculations, performed with a B3LYP level of theory and basis set of 631G(d), were used to approximate the excitation energies. DFT calculations for both ZnTPz and ZnTTPz were carried out on the C4h isomer. The UV/Vis spectra of ZnTTPz in both chloroform solution and as a thin film are shown in Fig. 3a. As is typical with porphyrazine derivatives ZnTTPz shows two main absorptions, the B-band in the blue region at 370 nm and the Q-band in the red region at 693 nm which corresponds to the HOMO–LUMO transition. The Q-band of ZnTTPz peaked at 689 nm in THF, a significant red-shift of 24 nm in comparison to a derivative of ZnTPz with cyclic tetrahydrobenzo solubilising groups, which had an absorption maximum at 665 nm in THF according to literature.18 For further comparison, the Q band of alkylated CuTPz absorbs at 657 nm in toluene.13 The red-shift can be attributed to the extension of the conjugation length caused by substituting the thiophene in ZnTPz for thieno[3,2-b]thiophene in ZnTTPz.
| Molecule | Experimental λmax (nm) | Excitation energy (nm) B3LYP/631G(d) |
|---|---|---|
| a Experimental λmax is for tetrahydrobenzo substituted ZnTPz.18b λmax of absorption spectra in THF.c λmax of absorption spectra in DMSO. | ||
| ZnTPza,18 | 665b | 581 |
| ZnTTPz | 689b, 696c | 631 |
| ZnPc15 | 668b, 672c | 593 |
| Zn-1,2-Nc16 | 684c | 614 |
| Zn-2,3-Nc17 | 766c | 694 |
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| Fig. 3 (a) Absorbance spectroscopy of ZnTTPz in chloroform solution and in thin film (b) absorbance and photoluminescence spectroscopy of ZnTTPz in chloroform solution. | ||
Upon film formation the Q-band of ZnTTPz broadens to both the blue and red regions either side of the solution Q-band. This suggests the formation of both cofacial H-aggregates and J-aggregates in the film, accounting for the blue and red shifts respectively. The absorption maximum of ZnTTPz in thin film was 710 nm, a red shift of 17 nm from chloroform solution. The optical band gap, measured from the absorption onset in thin film, had a value of 1.42 eV. ZnTTPz had a high molar extinction coefficient (ε) of 131
000 M−1 cm−1 (693 nm) in chloroform solution. The absorbance and photoluminescence spectra of ZnTTPz in chloroform solution are compared in Fig. 3b. The narrow absorption band of ZnTTPz is mirrored with a narrow emission band red shifted by 11 nm. Small Stokes shifts are characteristic of phthalocyanine and its derivatives; the rigidity of these molecules means there is little structural rearrangement between the ground state and excited state geometries.
It is interesting to note that whilst the experimental λmax of ZnTPz18 is slightly blue shifted in comparison to ZnPc15 (both in THF according to literature), the peak absorption of ZnTTPz is red-shifted by 12 nm in comparison to the λmax of Zn-1,2-Nc reported in the literature (both in DMSO see Table 1). These observations are supported by DFT calculations (see Table 1). Although DFT calculations approximated the excitation energies of the molecules to be much higher than those measured experimentally, accurate trends in band gaps shifts between molecules were predicted. For-instance DFT calculations predict the ZnTPz λmax to be blue shifted by 12 nm in comparison to ZnPc and the ZnTTPz λmax to be red shifted by 17 nm in comparison to Zn-1,2-Nc which compares fairly well with the experimentally observed data. Linear annulation of the benzene rings in Nc (2,3-Nc) is known to lead to strongly red-shifted Q-bands in comparison to angularly annulated Nc (1,2-Nc).19 We also observe that the Q-band of ZnTTPz is significantly blue shifted (70 nm) in comparison to the λmax of Zn-2,3-Nc reported in the literature.17 DFT calculations once again accurately predict this large red shift, estimating it to be 63 nm (see Table 1).
The electrochemical properties of ZnTTPz were investigated using cyclic voltammetry. The cyclic voltammograms for ZnTTPz are shown in Fig. S1.† The oxidation peak of ZnTTPz appeared to be partially reversible and the HOMO level was therefore estimated from the half wave oxidation potential (E1/2) giving a value of −5.02 eV. The reduction peak however was irreversible and the LUMO level was therefore estimated from the onset of first reduction, giving a value of −3.44 eV. The electrical band gap of ZnTTPz was therefore 1.58 eV, having a slightly larger value than the optical band gap of 1.42 eV which does not take into account exciton binding energy. The ionisation potential of ZnTTPz in thin film was measured using photoelectron spectroscopy in air (PESA) and had a value of −5.08 eV. Due to the longer conjugation length of ZnTTPz, the ionisation potential is raised in energy by ∼0.1 eV in comparison to copper 5-hexylthiophene-fused porphyrazine (CuTPz), which according to PESA measurements in the literature had an ionisation potential of −5.20 eV.13 Changing the central metal atom from Cu to Zn in phthalocyanines has little reported effect on the energy of the HOMO level.20
The transistor performance of ZnTTPz was investigated in bottom gate, top contact OFET devices. Gold source drain electrodes were used and the Si/SiO2 dielectric was treated with OTS prior to semiconductor deposition. As-spun films of ZnTTPz from chloroform showed p-type charge transport with hole mobilities on the order of 10−5 cm2 V−1 s−1 with a peak performance of 4.3 × 10−5 cm2 V−1 s−1. Annealing films at 100 °C improved the hole mobility by 2 orders of magnitude to ∼10−3 cm2 V−1 s−1 with a peak performance of 7.8 × 10−3 cm2 V−1 s−1. The transfer characteristics for these devices are shown in Fig. 4. The mobility of ZnTTPz is reduced in comparison to other porphyrazines fused with electron rich five membered rings such as thiophene which gave hole mobilities of 0.1–0.2 cm2 V−1 s−1 and selenophene which had mobilities on the order of 10−2 cm2 V−1 s−1. This is likely to be due to disorder imparted by the mixture of structurally dissimilar isomers (see Fig. 2). In the case of thiophene and selenophene fused porphyrazines the alkyl chain in the 5-position remains in a similar position with respect to the other isomers allowing crystalline, ordered films. ZnTTPz however appears to be amorphous with no obvious transitions in differential scanning calorimetry traces (see Fig. S2†) and no crystalline behaviour observed using polarised optical microscopy at different temperatures. Whilst this may hinder OFET devices, it may benefit solar cell applications to have a less crystalline donor to encourage mixing with PC61BM. For example solar cells made using CuTPz gave poor performance (PCE = 0.13%) due to large domains of the crystalline donor limiting the large donor acceptor interface required for high performance BHJ devices.21 We note that although ZnTTPz is a mixture of isomers, some previous studies have shown that phthalocyanine or porphyrin mixtures can outperform single isomers.22,23 The reduced band gap of ZnTTPz in comparison to CuTPz is also likely to improve solar cell performance through increased photocurrent.
MALDI-TOF MS spectra were acquired using an UltrafleXtreme MALDI-TOF mass spectrometer (Bruker Daltonics, Bremen, Germany), which is equipped with a Nd:YAG laser (λ = 355 nm). Data were acquired using flexControl software v3.4, while post-acquisition processing of data was performed by flexAnalysis software v3.4. MALDI matrix trans-2-[3-(4-tert-butylphenyl)-2-methyl-2-propenylidene]malononitrile (DCTB) was purchased from Insight Biotechnology Ltd. (Wembley, U.K.). Poly(propylene glycol) standard (average molecular weight ∼1000, PPG1000), tetrahydrofuran (THF; BHT stabilised) and sodium acetate (NaOAc) additive were purchased from Sigma-Aldrich (Poole, U.K.). Dichloromethane (DCM) and methanol (MeOH) solvents were purchased from Fisher Scientific (Loughborough, U.K.). DCTB matrix was dissolved in DCM at 20 mg mL−1, while the sample ZnTTPz was prepared in DCM at 1 mg mL−1. PPG1000 was prepared in THF at 10 mg mL−1 and NaOAc was solvated in MeOH at 10 mg mL−1; the PPG solution was mixed in a 20
:
1 ratio with NaOAc to form calibration standard solutions. For initial eternally calibrated MALDI characterisation analysis, the ZnTTPz sample was prepared by mixing with DCTB in a 1
:
49 ratio; 0.5 μL of this mixture solution was spotted onto the MALDI plate and dried in air. MALDI data was acquired in positive-reflection mode. MALDI accurate mass measurement was performed via mixing (ZnTTPz)–DCTB solution with PPG1000 calibration solution, such that the ion intensity of both sample and standard were approximately equivalent when analysed. Acquired data was internally calibrated using the cubic enhanced function from six PPG species bracketing the sample species.
:
9, v/v) to afford 7 as a pale green oil which solidified upon standing (522 mg, 48%). 1H NMR (400 MHz, CDCl3) δ 7.05 (s, 1H), 2.96 (t, J = 7.5 Hz, 2H), 1.79–1.69 (m, 2H), 1.44–1.20 (m, 10H), 0.86 (t, J = 7.1 Hz, 3H). 13C NMR (101 MHz, CDCl3) δ 158.08, 142.88, 137.13, 116.64, 115.98, 111.98, 111.81, 111.34, 31.86, 31.64, 31.25, 29.27, 29.20, 29.05, 22.70, 14.16. MS (EI) m/z = 302.09 (M+˙).
:
9, v/v) to afford ZnTTPz as a dark green solid (20 mg, 7.6%). 1H NMR (400 MHz, CDCl3) δ 6.44–5.94 (br, 4H), 2.66–2.33 (br, 4H), 2.28–2.20 (br, 4H), 1.68–1.40 (br, 8H), 1.39–1.15 (br, 40H), 0.98–0.85 (br, 12H). UV-Vis λmax (CHCl3): 693 (131
000 M−1 cm−1) nm. Accurate mass measurement (C64H72N8S8Zn, MALDI-TOF): calculated for M+˙ isotopic cluster at m/z = 1272.2932, found 1272.2914 (see Fig. S9†).Footnote |
| † Electronic supplementary information (ESI) available: CV's, DSC, NMRs and mass spectra. See DOI: 10.1039/c5ra17859b. Additional data related to this publication can be found at DOI: 10.6084/m9.figshare.1579415 |
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