Sasikumar
Arumugam
a,
Iain A.
Wright
a,
Anto R.
Inigo
*a,
Salvatore
Gambino
bc,
Calvyn T.
Howells
b,
Alexander L.
Kanibolotsky
a,
Peter J.
Skabara
*a and
Ifor D. W.
Samuel
*b
aWestCHEM, Department of Pure and Applied Chemistry, University of Strathclyde, 295, Cathedral Street, Glasgow, G1 1XL, UK. E-mail: anto.inigo@strath.ac.uk; peter.skabara@strath.ac.uk
bOrganic Semiconductor Centre, SUPA, School of Physics & Astronomy, University of St Andrews, St Andrews, KY16 9SS, UK. E-mail: idws@st-andrews.ac.uk
cCentre for Biomolecular Nanotechnologies@UniLe, Istituto Italiano di tecnologia, Via Barsanti, 73010 Arnesano (Le), Italy. E-mail: salvatore.gambino@iit.it
First published on 12th November 2013
Charge transport has been studied in a germanium-centred oligothiophene cruciform featuring 2-D close packing in the bulk. The morphology has been found to play a significant role in charge carrier transport, evidenced by time-of-flight and field effect transistor measurements. Thermal step-annealing leads to the formation of smaller crystalline domains which are favourable for charge transport in device applications.
Fig. 1 Structure (top) and packing diagram (bottom) of Ge-cruciform, obtained from single-crystal XRD studies.7 |
Controlling the morphology of bulk heterojunctions is important for efficient organic photovoltaics.8–11 The propensity for the Ge-cruciform material to crystallise in a 2-D close-packing motif allows us to gain control over the morphology of this material through post-thermal treatment. Here we show for the Ge-cruciform that step-annealing leads to the formation of smaller crystalline domains which favour hole transport compared to those annealed directly to the final temperature, where we see the formation of larger crystalline domains which are not favourable for charge transport. We demonstrate how controlling the morphology of this layer within a planar architecture can alter the performance of a photovoltaic device.
Fig. 2 shows the transfer characteristics of two sets of samples with one sample annealed in successive step temperatures of 50, 75, 100 and 120 °C for 20 minutes (data shown for 120 °C), and another sample was annealed straight to 120 °C for 20 minutes. The effect of contact resistances on the output characteristics (Fig. SI1†) of samples annealed straight to 120 °C is stronger than in the case of samples step-annealed to 120 °C. The temperature dependent mobilities of step-annealed samples are shown in Fig. 3 (crossed circles). It can be clearly seen that mobility increases by an order of magnitude moving from 4 × 10−6 cm2 V−1 s−1 (unannealed, Fig. SI2†) up to 4 × 10−5 cm2 V−1 s−1 after being step-annealed to 120 °C. Meanwhile, the samples annealed straight to 120 °C exhibited much lower mobility, 4 ± 2 × 10−6 cm2 V−1 s−1, compared to that of samples with step-annealing.
Fig. 2 Transfer characteristics for sample (top) after step-annealing from RT to 120 °C in 20 minutes steps and (bottom) annealed straight to 120 °C for 20 minutes. |
Fig. 3 Temperature dependent mobility of step-annealed Ge-cruciform measured by time-of-flight and organic field effect transistor methods. |
Although organic semiconducting materials have been known to exhibit improved performance after annealing closer to their glass transition temperature,12–14 a large variation in mobility due to step-annealing is very interesting and may play a direct role in the efficiency of, for example, organic photovoltaic (OPV) devices. However, for OPV device applications mobility measurements in the direction perpendicular to the substrate surface are required.7,15–17 To evaluate this, charge carrier mobilities were also measured using the charge generation layer – time-of-flight (CGL-TOF) method.18,19Fig. 4 shows the hole photocurrent transient for an as-cast film on linear and log–log scales (inset), at room temperature and for an applied electric field E = 3.3 × 104 V cm−1. The absence of a clear plateau in the photocurrent transient on a linear scale is indicative of highly dispersive charge transport behaviour. In order to estimate the transit time (ttr), a log–log plot was necessary, which allowed measurement of the transit time from the change of slope of the photocurrent transient, ttr = 43 μs. The transit time corresponds to a mobility of μ = 1 × 10−5 cm2 V−1 s−1. We have studied the hole mobility field dependence, as shown in Fig. SI4† (squared dots). As the electric field is increased from 3.3 × 104 V cm−1 to 3.3 × 105 V cm−1, the hole mobility increases from 1 × 10−5 cm2 V−1 s−1 to 3 × 10−5 cm2 V−1 s−1. This field dependent mobility is typical of organic semiconducting materials governed by the Poole–Frenkel relationship with an initial dip and then linear relationship at higher electric fields.20–23
Fig. 4 Hole photocurrent transient on linear and log–log scale (inset) for a film of Ge-cruciform, at room temperature and for an applied electric field E = 3.3 × 104 V cm−1. |
Room temperature CGL-TOF measurements were also performed on annealed samples in the same way as for FET mobility (see ESI†). Fig. SI4† shows the hole mobility field dependence for the as-cast sample and the annealed ones at temperatures of 50 and 75 °C. The change in slope (decreasing gradient with increasing temperature) of the field dependent mobility with respect to temperature can be related to the positional disorder present in the material.19,22,24
For a direct comparison, Fig. 3 (open circles) shows hole mobility measurements on an as-cast sample and an annealed one at temperatures of 50, 75 and 100 °C. Again, it can be clearly seen that mobility increases by an order of magnitude moving from 1 × 10−5 cm2 V−1 s−1, for the as-cast sample, up to 1 × 10−4 cm2 V−1 s−1 for the sample annealed at 100 °C.
It is worth noting here that the charge transport direction in the TOF method is perpendicular to the plane of the substrate, whereas the charge transport direction in OFETs is parallel to the plane of the substrates. While these two different types of measurements are governed by different physical phenomena, for example low level charge carrier density in TOF as opposed to high charge carrier density in OFETs, the general trend of mobility with respect to increase in annealing temperature remains the same. Though one would expect an order of magnitude higher mobility in OFETs than TOF, such differences in absolute mobility values should be accounted by detailed structural morphology with respect to charge transport parameters in the respective charge transport directions since the morphology parameters have larger effects on charge carrier mobility.25 While these detailed structural and charge transport studies are beyond the scope of this article, the current trend in mobility shown in Fig. 3 with respect to successive annealing temperature indicates that the charge transport pathways in directions parallel and perpendicular to the substrate plane are greatly enhanced by successive annealing and cooling.
Further morphological studies using scanning microscopies support this assumption. Tapping mode AFM height images of as-cast films show that the surface structure is amorphous (Fig. SI5†). In the case of step-annealed samples, crystalline structures start to form around 50 °C. There is no significant difference in the domain or crystalline structures of the samples annealed at temperatures between 50 and 100 °C (Fig. SI5†). However, the rms surface roughness of samples subsequently annealed at 75 and 100 °C is almost double compared to that of samples annealed at 50 °C. This could be due to the reason that crystalline domains start to form above 75 °C, which is further confirmed by independent measurements discussed below. Annealing of the same samples even further at 120 °C for 20 minutes produces broken rod-like crystalline domains of ∼200 nm length and 20 nm width (Fig. 5, top).
Fig. 5 Tapping mode AFM images of Ge-cruciform: (top) annealed at 120 °C for 20 minutes after prior annealing at 50, 75, 100 for 20 minutes; (bottom) annealing straight to 120 °C for 20 minutes. |
In the case of samples annealed straight to 120 °C, the tapping mode AFM height images show a nice branching fibrillar structure (Fig. 5, bottom). The structures were of ∼10 μm length and ∼1 μm width. The horizontal separations between these crystalline rods were as long as 8 μm with random alignment. The random alignment of these bulky rods would be a detrimental factor for observing higher mobilities, since the charge carriers have to overcome rough interfaces in addition to unfavourable alignment of these domains to the direction of the electric field.
Annealing the samples at 120 °C might have given all the molecules relatively similar molecular mobility so that they can form a thermodynamically stable structure, resulting in the long, branching fibrillar structures shown in Fig. 5 (bottom). In contrast, successive step-annealing and cooling up to 120 °C might have reduced the molecular mobility due to the formation of smaller crystals at temperatures lower than 100 °C. These observations show that faster annealing promotes growth over the nucleation of crystalline domains; although molecular mobility is important, the rate of nucleation is presumably the dominating factor for the difference in morphologies under these annealing conditions. Once the temperatures are further raised to 120 °C, the crystalline structures already formed at 100 °C may block movements of mobile molecules to form a dense, short-range ordered (DSRO) medium. This type of DSRO medium would be favourable for any type of electronic devices based on charge transport, such as solar cells or OFETs. To demonstrate the effect of post-processing thermal treatment on device performance we fabricated solar cells with a planar heterojunction structure (Fig. 6 top; for energy levels of components, see Fig. SI6†). For this, a low boiling point solvent was required to enable crystals to form at room temperature whilst also drying rapidly to reduce intermixing and allow for crystal growth when annealed straight to 120 °C. For this, carbon disulphide was selected as it previously demonstrated its ability to control cruciform aggregation in bulk heterojunction OPVs.7 As a comparison, films were also made from the more conventional solvent, chlorobenzene. The films deposited from carbon disulphide or chlorobenzene at room temperature exhibit a similar morphology (Fig. SI7a and SI7c,† respectively). Due to the lower boiling point of carbon disulphide (46 °C), on annealing straight to 120 °C we see the formation of crystalline structures which are rod-shaped (Fig. SI7d†). We observe similar absorption spectra (Fig. SI8†) for films from carbon disulphide or chlorobenzene annealed straight to 120 °C. However, below 450 nm we see some variation due to the size of the structures for films spun from carbon disulphide. Interestingly, we see less structure in absorption for the step-annealed films. Fig. SI9 and SI10† were obtained from a profiler and show the change in morphology between step-annealed and samples annealed straight to 120 °C, respectively. A film of similar thickness was used in the planar devices. Several samples were annealed straight to a given temperature. After acceptor and back electrode deposition they were characterised. A single device that was not annealed was measured at room temperature, then annealed at 50 °C for 20 minutes and measured. The device was subsequently annealed at 75, 100, and 120 °C. Between each temperature ramp of 20 minutes an incident photon to converted electron efficiency (IPCE) measurement was taken. We calculated the short-circuit current density (Jsc) under AM1.5G illumination by integrating each IPCE measurement. We see for a single device that step-annealing increases the IPCE (Fig. 7, top), and we observe a sharp fall in IPCE for devices annealed straight to 100 °C or 120 °C (Fig. 7, bottom). When we compare our results by calculating the short-circuit current (Fig. 6), we see similarities with the mobility measurements (Fig. 3). In our studies we see that the morphology of the semiconductor material is greatly influenced by the thermal annealing process and that this change in morphology affects the mobility. Controlling this process through step-annealing allows us to achieve favourable charge transport for improved device performance. For devices annealed directly to 100 or 120 °C we see larger crystalline structures. We show that these structures are unfavourable for charge transport and lead to poor device performance.
These charge transport measurements on OPV devices, combined with the OFET and TOF results, suggest that the mobilities observed perpendicular to the plane of the substrates by OPV and TOF measurements, and parallel to the plane of substrates by OFET measurements, are influenced by different annealing methods as a function of the material's unique 2-dimensional π–π stacking.
Jsc = q∫Φ × IPCEdλ |
For scanning electron microscopy (SEM) and photophysical studies, films were prepared on fused silica substrates from carbon disulphide or chlorobenzene. Samples for OFET, TOF and OPV were produced using the same procedure. SEM images were recorded with a HITACHI S-4800 scanning electron microscope and UV-visible absorption spectra were recorded with a Varian Cary 300 spectrophotometer.
Footnote |
† Electronic supplementary information (ESI) available: Fig. SI1–SI11 as mentioned above. See DOI: 10.1039/c3tc31670j |
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