Carbazole Electroactive Amorphous Molecular Material: Molecular Design, Synthesis, Characterization and Application in Perovskite Solar Cells

: In perovskite photovoltaics (PSCs), the role of the hole transporting material (HTM) is highly important as it significantly influents to the global device’s performance and stability. Hole transporter ensures the extraction of hole at the perovskite/HTM interface and transport it towards the cathode. Thus, accurate molecular design affording to efficient and cost ‐ effective HTM is of major interest. Small molecules having glass forming property is an attractive class as it can form morphologically stable thin film. Herein, a carbazole molecular glass bearing a polymerizable function was designed and synthetized. Its characteristics are suitable for application as HTM in PSCs. The preliminary photovoltaic application lead to device efficiency of 14%–15% depending on the chemical composition of the perovskite employed. These promising results open the way to design new alternative molecular and polymeric HTMs suitable for solution processed hybrid solar cells. septum ‐ sealed system purged and then argon refilled. This procedure was repeated five times. The mixture was stirred an argon atmosphere for The mixture and with × and brine × over anhydrous MgSO 4 , filtered and concentrated under reduced pressure. This crude product was subjected to a fast column chromatography separation eluting with CH 2 Cl 2. The fractions were combined, and removed to give a viscous which (200 vigorous precipitate then


Introduction
In perovskite photovoltaics (PSCs), the active component generally compose of a perovskite (PVK) layer sandwiched between two charge transport layers of different nature made from a hole (HTM) and an electron (ETM) transporting materials, respectively [1]. The HTM plays an important role as it extracts hole at the hole transporting layer/PVK interface and transport them towards the cathode [2]. HTMs are thus designed to have high charge transport capacity and suitable HOMO and LUMO energy levels (EHOMO & ELUMO) being compatible with that of the perovskite material. This provides suitable driving force for charge transfer at the HTM/PVK interfaces and block the back electron transfer. Other researched characteristics include excellent thermal and photochemical stability, amorphous homogeneous thin film forming capacity and high hydrophobic nature to protect the perovskite from moisture [3]. Huge research effort was done to the development of molecular HTMs for hybrid photovoltaic devices, including PSCs [4,5]. In solid state, small molecules tend to crystallize. So fabrication of their amorphous thin film stable above ambient temperature required meticulously engineered small conjugated molecules [6]. Among the different HTM families (such as thiophene [7], fused thiophene [8,9], furan [10], acridine [11], trizatruxenes [12], etc.) carbazole derivatives occupy an important place thanks to their unique properties [13,14]. We have shown that carbazole is an excellent platform to design not only HTMs for solid-state dye-sensitized solar cells (DSSCs) [15] and PSCs [16][17][18][19] but also as photoinitiators for photopolymerization and 3D printing technique [20][21][22][23]. Herein, we prepare a novel molecular glass denoted as iDM1 (Scheme 1) and test it as HTM in PSCs. Scheme 1. Molecular structure of the novel molecular glass (iDM1).
In iDM1 structure the carbazole core bears two di(4-methoxyphenyl)aminyl moieties, which is commonly used in combination with carbazole to construct HTMs [13]. at its 2,7 positions. The methoxy group plays an important role in designing hole transporters: it effectively tunes the solubility as well as the optical and electrochemical properties of targeted molecules [24]. On the other hand, it provides a good interaction with the perovskite surface [25]. The 4-vinylbenzyl chain at the 9-position of the carbazole offer the possibility of transforming iDM1 into its corresponding polymer for a possibly monomer vs. polymer comparative study [17].

Synthesis and Characterization of the Hole Transporting Material
The general conditions for the chemical synthesis, the structural analysis and the investigation of the iDM1′s thermal, morphologic, photo-physical and electrochemical characteristics were done following our previously well-established procedure [18]. Scheme 2 illustrates different step of the synthesis of the targeted molecule iDM1. Briefly, 2,7-dibromocarbazole was prepared in suitable yield in two steps from 4,4′-dibromobiphenyl following literature procedure [26]. It was then subjected to a N-benzylation reaction in strong basic medium affording the 2,7-dibromo-9-(4vinylbenzyl)-2,7-dibromocarbazole. Subsequently, the later was engaged in a twofold Pd-catalyzed Buchwald-Hartwig amination with di(4-methoxyphenyl)amine affording to iDM1 as a yellowish powder after purification.
Synthesis of iDM1: In a dry 100-mL round-bottom flask, 2,7-dibromocarbazole (195 mg, 0.6 mmol), 4-vinylbenzyl bromide (177 mg, 0.9 mmol), NaOH (190 mg, 4.7 mmol, dissolved in 1 mL of water) and DMSO (6 mL) were charged. The mixture was heated to 50 °C for 4 h and allowed to cool to room temperature. The reaction mixture was quenched with brine (10 mL) and extracted with CH2Cl2 (3 × 15 mL). The organic layers were combined, washed with brine and water, dried over anhydrous MgSO4, filtered and concentrated under reduced pressure. The crude product was purified by column chromatography eluting with CH2Cl2/petroleum ether (4/6 v/v) to yield a white solid (160 mg, 85% yield). The compound was directly engaged in the next step without further characterization. In an oven-dried Schlenk under argon stream, the freshly prepared N-(4vinylbenzyl)-2,7-dibromocarbazole (311 mg, 1.0 mmol), 4,4′-dimethoxydiphenylamine (688 mg, 3.0 mmol), palladium(II) acetate (12 mg, 0.05 mmol), sodium tert-butoxide (384 mg, 4.0 mmol), tri-tertbutyl phosphine (20 mg, 0.1 mmol, dissolved in 1 mL of distilled toluene) and freshly distilled toluene (10 mL) were charged. The septum-sealed Schlenk system was vacuum purged and then argon refilled. This procedure was repeated five times. The mixture was stirred under an argon atmosphere in sealed Schlenk tubes at 105 °C for 80 h and allowed to cool to room temperature. The reaction mixture was diluted with ethyl acetate (75 mL) and washed with water (3 × 100 mL) and brine (1 × 50 mL), dried over anhydrous MgSO4, filtered and concentrated under reduced pressure. This crude product was subjected to a fast column chromatography separation eluting with CH2Cl2. The collected fractions were combined, and solvent was removed under vacuum to give a viscous oil which was added to methanol (200 mL) with vigorous stirring. The precipitate was then filtered, rinsed with methanol several times. The final purification was done by silica gel chromatography eluting with hexane/ethyl acetate (4/1 v/v) affording a yellowish solid (500 mg, 68% yield). 1

Preparation and Characterization of Perovskite Solar Cells
The different steps for preparing perovskite photovoltaic devices (substrate etching, cleaning and preparation of FTO/bl-TiO2/meso-TiO2 layer, preparation and deposition of the hole transporting layer, thermal evaporation of gold back electrode and J-V characterizations) were followed from our previous optimized procedure [17][18][19]27]. In this work, different perovskite layers, named MAPI(2), MAPI(1)-SOF and FAMA were elaborated by two-step sequential and one-step deposition techniques by spin coating. The detailed procedure for each perovskite is detailed below.
Step 2: methylammonium iodide (MAI, 40 mg) was dissolved in 2-propanol (1 mL). 100 μL of this solution was dropped on top of PbI2 layer and wait for 20 s before starting the spinning (4000 rpm/s, 4000 rpm, 30 s). The sample was subsequently annealed at 115 °C for 1 h to form a dark-brown perovskite layer.

MAPI(1)-SOF:
The preparation of this CH3NH3PbI3 perovskite layer was inspired from the work of Park et al. [28], for which the precursors (PbI2 and MAI in 1:1 molar ratio) were dissolved in a mixed DMF and DMSO solvent. PbI2 (461 mg) and MAI (159 mg) were dissolved in a mixture of DMF (723 μL) and of DMSO (81 μL). 45 μL of this solution was then deposited onto the ETM layer by using a two-step spin-coating program: (1) spinning at 1000 rpm for 10 s and (2) then at 4000 rpm for 20 s. At 7 s of the second step spinning program, chlorobenzene (110 μL) was slowly dripped onto the rotating substrate before the surface changed to turbid due to the rapid vaporization of DMF. The obtained film was then heated at 105 °C for 1 h on a hotplate.

Thermal Properties
Thermogravimetric analysis (TGA, Figure 1a) shown that iDM1 has high thermal stability with decomposition temperature (Td) of 425 °C, which ensures the stability of the molecule below 400 °C. The molecule is thus thermally stable enough for optoelectronic and photovoltaic applications [29,30].
The differential scanning calorimetry analysis (DSC, Figure 1b) revealed the glass forming property of iDM1. During the first heating scan iDM1 showed a sharp and intense endothermic transition centered at 166.7 °C, which is attributed to its melting point (Tm). On the second one, only the glass transition was recorded at the glass transition's temperature (Tg) of 62.5 °C. This value is slightly higher than that of its 3,6-isomer reported earlier (Tg = 61 °C) [17] due to its higher steric hindrance of the 2,7-disubstituted molecule.

Optical Properties
In dilute solution, iDM1 mostly absorbs in the UV region and poorly absorbs in the visible spectral domain with the maximum absorption centered at the wavelength λmax = 391 nm (Figure 1c). This characteristic can make iDM1 a promising photoinitiator for light emitting diode induced photopolymerization [31]. Additionally, this avoids competitive absorption with light absorber when applied as HTM in hybrid solar cells. In solution, iDM1 photoluminescence is centered at the wavelength of 419 nm. A Stock shift of 28 nm was recorded, which is somehow smaller than that of its 3,6-isomer reported earlier [17]. In thin film, the absorption slightly redshifts to 397 nm, due to the steric hindrance of iDM1 avoiding molecular aggregation in the solid state. The optical bandgap (Eg = 2.85 eV), calculated from the absorption onset of the thin film (Figure 1c, 435 nm), is somewhat close to that of its 3,6-isomer [17] and Spiro-OMeTAD [15].

Electrochemical Properties
iDM1's cyclic voltammogram (Figure 1d) shows multiple oxidation processes due to the presence of multiple electron-rich tertiary amine moieties in its structures. The first quasi-reversible oxidation at low potential is attributed to oxidation of the carbazole moiety to form the corresponding radical cation. The onset potential of this oxidation is −0.27 V/Fc/Fc + , which is lower than that of Spiro-OMeTAD (−0.11 V/Fc/Fc + ) [15]. The corresponding energy level of its HOMO orbital (EHOMO) was estimated from this potential by taking the ionization energy of ferrocene (4.8 eV vs. vacuum) as the standard. Its ELUMO was then estimated from the EHOMO and Eg. The EHOMO values of iDM1 and Spiro-OMeTAD are −4.53 eV and −4.69 eV, respectively. Actually, EHOMO of iDM1 is slightly higher than that of Spiro-OMeTAD. The corresponding ELUMO are very close and are −1.68 and −1.69 eV, respectively. This suggests that, energetically, iDM1 could be suitable as an alternative HTM to Spiro-OMeTAD.

Photovoltaic Application
The photovoltaic property of iDM1 was studied in classic PSC architecture (FTO/bl-TiO2/meso-TiO2/Perovskite/HTM/Au) [32], using different perovskite composition and deposition methods. Figure 2 illustrates the different solar cell's layer and their energy alignment. The composition of the hole transporting layer is also shown. In this work, the photovoltaic device was made on FTO/glass substrate and composed of a thin compact blocking-TiO2 layer, a mesoporous TiO2 layer filled and capped with the perovskite absorber of different compositions, a hole transporting layer. Finally, a thin gold metal layer was thermally deposited to serve as device back contact. MAPI(2) denotes the CH3NH3PbI3 perovskite made by 2step sequential spin coating deposition while MAPI(1)-SOF was made by 1-step spin-coating technique from a mixture of DMF/DMSO solvent. FAMA denotes the mixed cation mixed anion perovskite FA0.87MA0.13Pb(I0.87Br0.17)3 [33]. The thickness of the carbazole-based hole transport layer is ca. 200 nm while that made from Spiro-OMeTAD is ca. 150 nm of [19]. The photocurrent/voltage graphs of the best cells are displayed in Figure 3 and the photovoltaic characteristics are summarized in Table 1. All devices delivered photovoltaic performances higher than 14%. In general, MAPI based cells led to more satisfying PCE. However, CH3NH3PbI3 perovskites (MAPI(2) and MAPI(1)-SOF) gave high hysteresis behavior (Figure 3a,b). Finally, PSC constructed with FAMA gave suitable hysteresisfree J-V behavior (Figure 3c). The best cell delivered VOC = 1.01 V, JSC = 22.33 mA.cm −2 , FF = 62.06% and global PCE = 14.04% (the average PCE = 13.95%). In comparison with Spiro-OMeTAD based devices, that of iDM1 gave significantly lower photon to electricity conversion outputs. All photovoltaic characteristics of iDM1 are lower accompanied by more important hysteresis behavior. While iDM1 in combination with FAMA perovskite gave hysteresis-free device with VOC and JSC values approach that of Spiro-OMeTAD, its lower photovoltaic efficiency is due to its lower FF. In comparison to its 3,6-bis(di(4methoxyphenyl)aminyl) substituted isomer bearing the identical polymerizable side chain (DM1), iDM1 gave significantly improvement in term of photovoltaic performance (PCE of DM1 = 12.26%) [17]. We assume that the different in device performance of iDM1 compared to the Spiro-OMeTAD and its 3,6-disubstituted isomer (DM1) is related to the hole transport properties of these materials. This show that 2,7-disubstituted carbazole molecule can be more promising HTM than its more popular 3,6-disubstituted counterpart. However, additional characterizations such as hole mobility measurements, HTM/perovskite thin film fluorescence, optimization of HTM deposition conditions (concentration, additive engineering, etc.) will have to be done in order to explore the full potentiality of this series of hole transporter in perovskite photovoltaics. The chemical conversion of iDM1 into its corresponding polymer will give a complementary comparative study of molecular versus the polymeric materials in term of photovoltaic performance and device stability.

Conclusions
We have successfully synthetized and characterized a polymerizable carbazole molecular glass. When employed as HTM in PSCs, we obtained photovoltaic performance in the range of 14%-15%. Current studies are being focused on the charge transport characterization, synthetizing the full series of compounds and perform their polymerization to prepare the corresponding polymers for comparative studies. This will be subjected to future comparative study of monomer versus its polymeric HTMs in term of the thermal, opto-electro-chemical properties and their influence on the photovoltaic devices performance and stability which is out of the scope of the current study.