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Nanometer-Thick Conjugated Microporous Polymer Films for Selective and Sensitive Vapor-Phase TNT Detection
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Nanometer-Thick Conjugated Microporous Polymer Films for Selective and Sensitive Vapor-Phase TNT Detection
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  • Venkata Suresh Mothika*
    Venkata Suresh Mothika
    Macromolecular Chemistry Group, Bergische Universität Wuppertal, Gaußstraße 20, 42119 Wuppertal, Germany
    *E-mail: [email protected]
  • André Räupke
    André Räupke
    Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
  • Kai Oliver Brinkmann
    Kai Oliver Brinkmann
    Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
  • Thomas Riedl
    Thomas Riedl
    Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
    More by Thomas Riedl
  • Gunther Brunklaus
    Gunther Brunklaus
    Institut für Physikalische Chemie, Westfälische Wilhelms-Universität, Corrensstr. 46, D-48149 Münster, Germany
  • Ullrich Scherf
    Ullrich Scherf
    Macromolecular Chemistry Group, Bergische Universität Wuppertal, Gaußstraße 20, 42119 Wuppertal, Germany
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ACS Applied Nano Materials

Cite this: ACS Appl. Nano Mater. 2018, 1, 11, 6483–6492
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https://doi.org/10.1021/acsanm.8b01779
Published October 16, 2018

Copyright © 2018 American Chemical Society. This publication is licensed under these Terms of Use.

Abstract

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Conjugated microporous polymer (CMP) thin films often show fast and amplified signal response and potential for developing portable sensing devices. Here, we elucidate electrochemical generation of three CMP thin films and their fluorescence response to trinitrotoluene (TNT). A tetra(carbazolylphenyl)ethylene monomer TPETCz-derived CMP thin film (PTPETCz, SBET: 930 m2/g) displayed fluorescence (λmax = 525 nm) quenching to nearly 95% in 3 min, when the CMP film is exposed to 33 ppb TNT vapors. Interestingly, PTPETCz is highly sensitive (30% quenching) to TNT vapors of low concentrations (5–10 ppb) and also remarkably selective toward TNT compared to other analytes. In contrast, an only mere response was observed when a nonporous monomer TPETCz-film was exposed to 0.2 ppm TNT. So, the microporosity and extended π-conjugation of the polymer facilitating suitable host–guest interactions is found to be essential toward highly sensitive detection of TNT. Fluorenone-cored CMP thin films (PFLCz) showed no response, while PTPEFLCz containing both tetraphenylethylene and fluorenone structural units showed nearly 70% of emission quenching in the presence of 0.2 ppm TNT. Therefore, the presence of electron-donating TPE core is a prerequisite for efficient photoinduced electron transfer from polymer to nitroarenes.

Copyright © 2018 American Chemical Society

1. Introduction

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Research efforts on trace-level detection of explosive chemical vapors are rapidly increasing owing to its importance in environment and defense/security applications. (1,2) Several explosive sensors based on small molecules, conjugated polymers, self-assembled organic nanomaterials, and metal–organic frameworks have been studied for both solution and vapor-phase explosives detection up to detection limits of part per trillion (ppt). (3−14) The microporous environment of metal/organic frameworks enabling fast diffusion of analytes and effective host–guest interactions was key for the enhanced sensitivity, while extended π-conjugation in conjugated polymers was shown to be a very promising feature for amplified signal transduction. (11−14) In this context, conjugated microporous polymers (CMPs) (15−21) featuring both microporosity and extended π-conjugation with large surface area are unique for fluorescence-based sensing of explosive vapors. Efficient exciton migration along the polymer network and an excellent analyte diffusion opportunity can be useful for fast and amplified fluorescence response. (22−24) Moreover, CMPs are thermally and chemically stable due to strong C–C linkages between connecting building blocks. (25−29) Several chemically synthesized CMP powders have been studied for fluorescence-based sensing of chemical analytes; (30−36) however, their limited processability often restricts device fabrication. For an example, silsesquioxane-based porous polymers or porphyrin networks were solution-processed onto lightweight paper or thin-layer chromatography (TLC) plate substrates and used as portable sensors for chemical sensing. Nevertheless, they use expensive Pd(0) catalysts, and additional efforts were needed to remove trace catalyst impurities and to control film thickness. (37−39)
Recently, the electro-oxidative polymerization technique for synthesizing CMP thin films gained significant attention. (40−44) This catalyst-free technique is cost-effective and can provide highly pure CMPs in short times with excellent control over film thickness. These films can be grown on a large variety of electrodes including flexible substrates thus enabling device fabrication. (45−47) Electropolymerization approaches of carbazolyl and thienyl building blocks into CMP thin films for various applications were studied recently. (48) The electrochemical sensing of nitroaromatic compounds (NACs) using various CMP thin films with detection levels of several micrograms per milliliter was also reported. (49) Tetraphenylethylene (TPE)-based materials show aggregation-induced emission (AIE) and have been widely studied for sensing of various small molecules including explosives. (50−55) Recently, fluorescence quenching of CMP thin films (PTPETPOcCz, SBET = 2170 m2/g) by TNT in aqueous solution (50 ppm) was studied by us, (56) while Jiang et al. reported polyTPECz-based thin films showing fluorescence quenching response to 50 ppm 2,4,6-trinitriphenol (TNP) solutions with good selectivity, low detection limits, and proper fluorescence retention after the analyte was washed out. (57) Solution-phase sensing methods are, in principle, applicable to environmental safety devices, but with certain limitations due to the use of liquid systems, although good performance can be achieved. Having encouraging results of solution-phase optical sensing based on thin films of TPE-cored networks from our previous studies, we now propose to use PTPETCz (SBET = 930 m2/g) thin films with their strongly greenish-cyan emission (λmax: 525 nm) also for vapor-phase explosive sensing. Vapor-phase sensing can be distinctly different from solution-phase processes, since the nitroaromatic compounds possess quite different vapor pressures. Generally, vapor-phase sensing may be more relevant to real-time sensing. (58)PTPETCz used in the presented study is higher fluorescent if compared to the previously studied PTPTCz (49) and, believably, it may act as superior-performing optical sensor. There are relatively few reports on electrogenerated CMP thin films for vapor-phase sensing of explosives. (59) TPBCz-CMP films were already studied for vapor-phase sensing with good performance, (60) and the further development of such materials may be important for homeland security applications. CMP thin films prepared by other techniques were also shown to be promising vapor-phase sensors. (58,59,62) The present work on electrogenerated PTPETCz films also documents a very encouraging sensing performance with high sensitivity and short response time. The electropolymerization approach represents a favorable approach for creating high-quality CMP thin films that are suitable for device fabrication (as reported, e.g., by Jiang et al. and by Ma et al.). (45−47) However, reports on electropolymerized CMP thin films showing high sensitivity for trace-level trinitrotoluene (TNT) vapors are scarce. We recently reported CMP thin films for vapor-phase sensing of NACs including sensing of 5 ppb TNT based on efficient fluorescence quenching. (59) In our new experiments, the PTPETCz emission is strongly quenched (95%) when exposed to 33 ppb of TNT vapor in 3 min and also showed excellent selectivity if compared to the response to various other nitroaromatic analytes (Scheme 1). PTPETCz showed remarkable selective response to TNT vapors among the nitroaromatic compounds studied. To our surprise, an appreciable fluorescence response (30% quenching) even to lower concentrations (5–10 ppb) of TNT vapors is observed. We further studied the dependence between film thickness and sensitivity to TNT vapors for the CMP films. Intriguing AIE property of TPE cored materials was shown to be responsible for its efficient sensing properties. (50−55,61) The PTPETCz-based sensing response may be similarly explained. CMP thin films grown from the fluorenone-cored carbazolyl derivative FLCz exhibited no remarkable response to TNT. In contrast, a CMP thin film prepared from a mixture of monomers 1,1,2,2-tetra[4-(carbazol-9-yl)phenyl]ethene (TPETCz) and 2,7-di(carbazol-9-yl)-fluoren-9-one (FLCz) displayed appreciable responses to TNT in the vapor phase. Although several CMP-based thin films have been reported for trace-level explosive detection, (58,59,62) we believe that the present work represents a promising new example among the already reported systems that have been studied for vapor-phase TNT sensing.

Scheme 1

Scheme 1. Schematic Illustration of the Electropolymerization of TPETCz into Fluorescent PTPETCz Thin Film, and the Fluorescence Quenching in the Presence of Trace TNT Vapors

2. Experimental Section

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Materials and Methods

All reagents and chemicals required have been purchased from commercial chemical suppliers, unless stated. TPETCz is synthesized according to a literature procedure. (56)1H NMR spectra are measured using Bruker Avance III 400 MHz machine. APCI mass spectra are measured on a Bruker Daltronik microTOF system (KrF*-Laser ATLEX-SI, ATL). Bulk polymers synthesized by the chemical oxidation method are purified by washing with supercritical CO2 in a Tousimis Samdri-795 system. Bulk polymer samples and thin films are activated on a Belprep-vac II at 140 °C and ∼2 Pa over 10 h for adsorption measurements. Kr adsorption measurements are performed using a BEL Japan Inc. Belsorp-max system at 77 K in the relative pressure range of 0–0.6, P0 = 1 atm. Ionization potential measurements are performed with atmospheric pressure ultraviolet photoelectron spectroscopy System (Riken Keiki AC-2). Thermogravimetric analyses (TGA) are recorded at a Mettler Toledo TGA/DSC1 STAR machine under Ar atmosphere with a heating rate of 5 °C per min. UV/Vis absorption and Fourier transform infrared (FTIR) measurements are performed using JASCO V-670 and FTIR-4200 machines, respectively. Photoluminescence (PL) is measured using a HORIBA Scientific FluoroMax-4 spectrofluorometer connected to a QuantaPhi integrating sphere for determination of PL quantum yields. Photoluminescence measurements for sensing experiments are recorded using diode-pumped solid-state laser photoexcitation (λ = 355 nm, 11 mW/cm2) coupled into a monochromator and detected with a cooled charge-coupled device camera (Princeton Instruments). Atomic force microscopy (AFM) images of the thin films are obtained on a Bruker diInnova system operated in tapping mode; the surface roughness is extracted from the topography images.

Solid-State NMR Measurements

13C{1H} cross-polarization magic-angle spinning (CPMAS) spectra were recorded at 50.33 MHz using a Bruker AVANCE III 200 NMR spectrometer with a contact time of 2.5 ms, averaging 17 408 transients at a relaxation delay of 2 s; the contact pulse was ramped from 70% to 100% of the optimized power level of 55 W. All experiments were performed at room temperature (air-conditioned to 20 °C), employing a standard Bruker 2.5 mm double resonance MAS probe spinning at 20 kHz, typical π/2-pulse lengths of 3.5 μs (reflecting a radiofrequency (RF) field strength of 71.4 kHz) and SPINAL64 proton decoupling (200.15 MHz; 10π/12 pulse set to 5.8 μs) at rather modest power levels of 32 W (13C) and 20 W (1H), respectively. The 13C spectra were referenced with 1-13C and 15N isotope-enriched solid α-glycine as secondary standard (176.0 ppm for 13C_carbonyl). In addition, the line width of the 13C_carbonyl peak served as internal check for proper adjustment of the magic angle.

Electropolymerization

Thin film generation follows similar procedure as reported by our group earlier. (40,43,49) Monomer solutions (0.1 mM) are prepared in dichloromethane/acetonitrile (4:1) with 0.1 M tetrabutylammonium perchlorate (TBAP) as supporting electrolyte. A three-electrode cell connected to electrochemical workstation PAR VersaSTAT 4 is used under Ar atmosphere at 25 °C. Indium tin oxide (ITO) plates are used as working electrode (WE) combined with a platinum counter electrode (CE) and Ag°/AgNO3 (0.1 M AgNO3, 0.6 V vs normal hydrogen electrode (NHE), nonaqueous reference) as reference electrode (RE). Potentiostatic regimes are applied for generating porous polymer films on the ITO electrodes. For sensing experiments the films are grown by applying five cyclic voltammograms (CVs) between −0.2 and 1.1 V with a scan rate of 0.1 V s–1. Thicker films used for gas adsorption measurements are prepared by the chronoamperometry method by applying a constant potential of 1.1 V for 20 min followed by a discharging step at 0 V for 60 s to discharge the deposited films. Free-standing thin films are delaminated from the electrodes, dried after rinsing with CH3CN and CH2Cl2, and used for Kr adsorption measurements. The films are activated at 140 °C prior to the adsorption measurements.

Synthesis of 2,7-Di(carbazol-9-yl)-fluoren-9-one (FLCz)

2,7-Dibromo-9H-fluoren-9-one (1 g, 2.94 mmol), 9H-carbazole (7.34 mmol, 1.22 g), 2,2′-bipyridyl (229.4 mg, 1.47 mmol), CuI (1.297 g, 7.34 mmol), and K2CO3 (2 g, 14.7 mmol) are degassed in a double-neck flask and purged with Ar three times. To this mixture o-dichlorobenzene (30 mL) is added, and the batch is stirred at 180 °C under dark conditions for 48 h. Next the mixture is cooled to room temperature, filtered, and washed with dichloromethane several times. The filtrate is concentrated under reduced pressure, and the crude product is purified by column chromatography using chloroform/tetrahydrofuran (THF)/hexane (9:0.5:0.5) as eluent. Finally the product is recrystallized from a cyclohexane/chloroform (1:1) mixture. Red needlelike crystals are obtained after 3 d. Yield: 0.66 g (44%). 1H NMR (400 MHz, CDCl3): δ = 8.20 (d, 4 H), 8.0 (t, 2 H), 7.89 (d, 2H), 7.82 (d, 2H), 7.50 (m, 8 H), 7.37 (d, 4 H) ppm; 13C NMR (600 MHz, CDCl3) δ: 191.8, 142.28, 140.45, 139.01, 136.29, 133.07, 126.23, 123.75, 123.11, 121.74, 120.39, 109.72. Mass spectrometry (MS) atmospheric pressure chemical ionization (APCI) calcd for C37H23N2O: 511.1805, found m/z = 511.1808 (M+).

Synthesis of PTPETCz Bulk

It was synthesized using similar procedure reported by Scherf et al. (56) and obtained as pale green solid.

Synthesis of PFLCz Bulk

FLCz (0.12 mmol, 61 mg) is dissolved in 15 mL of dry chloroform and added dropwise to a suspension of FeCl3 (0.66 mmol, 108 mg) and stirred for 24 h at room temperature. To this mixture 100 mL of methanol is added and stirred for 1 h to precipitate the polymer. Precipitates are collected by filtration and washed thoroughly with methanol. Further, the powders are treated with concentrated HCl (35%) for 2 h and washed with water and methanol thoroughly. Compounds are purified by Soxhlet extraction with THF and methanol followed by supercritical CO2 washing (as described before) as final purification. (63)PFLCz is obtained as a red solid, yield: 48 mg (78%)

Synthesis of PTPEFLCz Bulk

TPETCz (0.12 mmol, 116 mg) and FLCz (0.12 mmol, 61 mg) are dissolved in 30 mL of dry chloroform and added dropwise to a suspension of FeCl3 (1.32 mmol, 216 mg), and the mixture is stirred for 24 h at room temperature. To this mixture 200 mL of methanol is added and stirred for 1 h to precipitate the polymer. The precipitates are collected by filtration and washed thoroughly with methanol. Further, the powder is treated with concentrated HCl (35%) for 2 h and washed with water and methanol thoroughly. The product is finally purified by Soxhlet extraction with THF and methanol followed by supercritical CO2 washing. PTPEFLCz is obtained as orange-red solid, yield: 87 mg (73%).

3. Results and Discussion

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Electropolymerization and Kr Adsorption

1,1,2,2-Tetra[4-(carbazol-9-yl)phenyl]ethene (TPETCz) is prepared in a procedure previously followed by our group, (56) while the 2,7-di(carbazol-9-yl)-fluoren-9-one (FLCz) monomer is synthesized in a condensation reaction of 2,7-dibromo-fluoren-9-one and carbazole under reflux conditions (see Supporting Information for details). Initially, the electrochemical behavior of the monomers is studied using 0.1 mM solution of the corresponding monomer in CH2Cl2/CH3CN (4:1) mixture with 0.1 M TBAP as supporting electrolyte. Figure 1a shows the first CV cycle of TPETCz, FLCz, and their 1:1 mixture (TPETCz/FLCz). TPETCz displays first reversible oxidation peak at ∼0.9 V, which can be attributed to the formation of stable radial cations at the TPE cores, and this signal was also observed for TPETCz/FLCz. In addition, monomers TPETCz, FLCz, and TPETCz/FLCz (1:1 mixture) exhibited irreversible oxidation peak at 1.1 V, which can be assigned to the oxidation of carbazole moieties of the monomers. Figure 1b–d displays the cyclic voltammograms of electro-oxidation and polymerization of TPETCz, FLCz, and TPETCz/FLCz with an applied oxidation potential of 1.1 V up to 20 cycles to form CMP thin films PTPETCz, PFLCz, and PTPEFLCz, respectively. For PTPETCz, it can be seen that starting from the second electrochemical cycle reversible peaks of charging and discharging are developed in the potential range from 0.5 to 0.8 V with gradual rise in current with increasing cycle number. This gradual rise in the current with increasing sweep cycle number reflects continuous growth of the polymer films at the electrode (ITO). In monomer-free solution the as-grown electrogenerated CMP films showed two reversible peaks for different scan rates from 0.005 to 0.2 V s–1 as evidence for charging/discharging processes in the polymers through reversible radical cation/dication formation (Figure S1). Further, a linear relationship between peak current and scan rate is observed, suggesting deposition of uniform, electroactive polymer deposits on the electrode. Similar polymer film growth characteristics are observed for FLCz and TPECz/FLCz (Figure S1). It can be noted that polymer growth is uniform throughout the ITO electrodes with a continuous coverage of the electrode surface. Formation of CMP thin films is evident from the FTIR spectra: New bands around 744 cm–1 correspond to the C–H bending vibration mode of N-substituted carbazoles that are present in polymer PTPETCz films; similar bands are also observed for PFLCz and PTPEFLCz. Additional bands around 802 cm–1 appeared for all polymers and represent C–H bending vibrations of 3- or 6-substituted carbazoles, thereby demonstrating the formation of “C–C” linkages between the carbazole moieties (Figure S2). Figures 2a & S3 shows the AFM images of three different CMP films grown by applying five cyclovoltammetric cycles. The thicknesses are calculated from the topography images to be 15, 38, and 19 nm for PTPETCz, PFLCz, and PTPEFLCz with an average roughness of 3.7, 7.5, and 4.5 nm, respectively. The low roughness values imply that the thin films are best suited for device fabrication.

Figure 1

Figure 1. (a) CVs of monomers (0.1 mM) TPETCz (black), FLCz (red), and their 1:1 mixture (TPECz/FLCz) (blue) in dichloromethane/acetonitrile (4:1) containing 0.1 M TBAP, ITO electrodes, potential range 0–1.5 V. (b–d) First 20 consecutive CV cycles showing electropolymerization and growth of CMP thin films of (b) PTPETCz, (c) PFLCz, and (d) PTPEFLCz, ITO electrodes, prepared from corresponding monomer (0.1 mM) solutions containing 0.1 M TBAP.

Figure 2

Figure 2. (a) AFM images of CMP thin film of PTPETCz grown over five CV cycles and (b, c) digital images of free-standing PTPETCz or PFLCZ thin films, respectively. Kr gas adsorption isotherms of (d) CMP thin films prepared by electropolymerization and (e) CMP powders synthesized by chemical oxidation with FeCl3; PTPETCz (navy blue), PFLCz (green), and PTPEFLCz (black), all measured at 77 K.

Free-standing polymer thin films necessary for porosity measurements are prepared using the chronoamperometry method by applying a constant oxidation potential of 1.1 V for 20 min followed by treatment at 0 V for 60 s to discharge the deposited films (Figure 2b,c). These free-standing CMP films were room-temperature-dried and used for Kr adsorption measurements. Prior to this, the thermal stability of the thin films is studied (all films have been dried by heating under vacuum at 140 °C). As shown in Figures S4–S6, initial weight loss (<2%) can be attributed to trapped solvents. All the films showed no further weight loss up to 200 °C, and further heating results in slow loss of nearly 30% mass until 650 °C. All the CMP thin films were activated at 140 °C ensuring to remove guest solvent molecules under vacuum prior to Kr gas adsorption measurements. Commonly, nitrogen gas sorption measurements are used for porous CMP materials to determine the specific surface area. However, electrogenerated CMPN thin films are generally obtained in small amounts and are not suited for nitrogen measurements, mainly due to the higher vapor pressure of N2 at 77 K. In contrast, Kr with its low saturation pressure (1.63 Torr) at 77 K facilitates determination of pressure changes with greater precision even for low amounts materials such as thin films. Therefore Kr is used for the determination of Brunauer–Emmett–Teller (BET) surface area of thin films. (64) Kr adsorption measurements of PTPETCz, PFLCz, and PTPEFLCz at 77 K up to a relative pressure (P/Po) of 0.6 showed type-I uptake profiles with higher uptake in the low-pressure region thus suggesting a microporous nature of the polymer thin films (Figure 2d). No characteristic hysteresis loop was observed in the pressure range of 0.3–0.6 P/Po for all CMP films (Figure S7). However, in the low-pressure region, the desorption process did not follow the adsorption path and showed a slight hysteresis; this may be attributed to a restricted access to the pores in microporous polymers. (65) The maximum gas uptake is observed to be 258, 133, and 142 mL/g, respectively. Application of the BET model on the Kr adsorption isotherms yielded surface areas of 930, 504, and 509 m2/g for PTPETCz, PFLCz, and PTPEFLCz, respectively; the corresponding BET constants and fitting parameters are shown in Figure S8. For comparison with the thin-film results, PTPETCz, PFLCz, and PTPEFLCz bulk CMPs are also synthesized by chemical oxidation using FeCl3 as oxidizing agent from the corresponding monomers at room temperature (see Experimental Section). To avoid collapse of porosity during conventional activation methods, CMP powders are desolvated using the supercritical CO2 drying method before further characterization. Figures S9 and S10 show the FTIR spectra of all bulk polymers along with those of the corresponding monomers. Stretching vibrations at 1597 (νC═C) and 1720 cm–1C═O) confirm the presence of tetraphenylethylene or fluorenone moieties in PTPETCz, or PFLCz, or PTPEFLCz bulk CMPs. Also, a band around 746 cm–1 corresponding to the C–H bending vibration mode of N-substituted carbazoles is present in monomer TPETCz and polymer PTPETCz bulk; a similar band is observed for FLCz and PFLCz bulk. New bands around 800 cm–1 that appeared for all polymers correspond to C–H bending vibrations of 3- or 6-substituted carbazoles (not in TPETCz), thereby demonstrating the formation of C–C linkages between the carbazole moieties. Further on, the bulk polymers were characterized by 13C–CP/MAS solid-state NMR spectroscopy: A peak at 189 ppm can be assigned to the carbonyl carbon of fluorenone moiety present in the polymers PFLCz and PTPEFLCz bulk. The peaks in the range of 110–140 ppm can be ascribed to the aromatic C present in polymers (Figures S11 and S12). Thermogravimetric analysis (TGA) of PTPETCz, PFLCz, and PTPEFLCz bulk showed no apparent weight loss up to 300 °C thus suggesting appreciable thermal stability of all polymers; a steady weight loss until 500 °C and up to 70% (Figures S13–15) total weight loss on further heating is observed. Kr gas adsorption of bulk CMPs also showed type-I uptake profiles with final gas uptake of 475, 226, and 278 mL/g (Figure 2e) for PTPETCz, PFLCz, and PTPEFLCz bulk, respectively, suggesting their microporous nature. Application of the BET model on these Kr isotherms provided surface areas of 1375, 836, and 902 m2/g for PTPETCz, PFLCz, and PTPEFLCz bulk, respectively, and the corresponding BET constants and fitting parameters are shown in Figure S16. The BET surface areas as calculated from Kr gas adsorption measurements of the thin films were lower if compared to the corresponding bulk CMP powders. On the one hand, FeCl3-assisted oxidative coupling may lead to a higher cross-linking density of the building blocks and, as a consequence, to a microporous network with higher BET surface area. On the other hand, electropolymerization probably leads to a reduced cross-linking density, probably due to the preferential formation of dimeric carbazolic linkages.

Photophysical Studies

On the one hand, monomer TPETCz shows aggregation-induced emission (AIE) in the solid state at λmax = 470 nm due to restricted rotation of the phenyl rotors of the TPE core (Figure S17), while it is practically nonfluorescent in solution, a widely known phenomena in literature. (55) On the other hand, FLCz shows red emission (λmax = 637 nm) in the solid state (Figure S17) due to the presence of the fluorenone chromophore (n-π* transition). We studied the absorption and emission spectra of monomer FLCz in solvents of varying polarity to understand if the emission is dominated by intramolecular charge transfer (ICT). FLCz did not show appreciable changes in the absorption spectra with the variation of the solvent polarity (Figure S18). The emission spectra showed maxima at ca. 585 nm (in toluene, THF) which are red-shifted to 630 nm in dichloromethane, chloroform, and acetonitrile (Figure S18). This indicates some ICT character for the derivatives where the fluorenone unit is in conjugation with other aromatic substituents. The emission behavior indicates an excited-state stabilization with increasing solvent polarity. (66) However, the emission shifts are moderate, pointing for a less distinct ICT character for the FLCz emission. CMP films grown over five oxidative potential cycles for PTPETCz, PFLCz, or PTPEFLCz generation showed a main absorption band peaking at ∼310 nm with a shoulder at 370 nm that is assigned to the π–π* transition of bicarbazole moieties (Figure S19). In case of the fluorenone-containing CMP thin films (PFlCz and PTPEFlCz), a weak absorption band at longer wavelengths in the range of 450–550 nm should represent n−π* transitions. However, in case of PTPETCz thin films (fluorenone-free), an observed weak absorption tailing into the longer wavelength region may be due to light scattering. Therefore, we selected an excitation wavelength of 355 nm for the fluorescence quenching studies. PTPETCz, PFLCz, and PTPEFLCz films showed greenish-cyan (strong), red (weak), and orange-red (moderate) emission peaking at 525, 621, and 608 nm (λex= 355 nm), respectively (Figure S19), with photoluminescence quantum yields (PLQYs) of 4.0%, 0.5%, 1.9%, respectively. A similar emission trend is observed for the PFLCz bulk material when dispersed in solvents of various polarities as seen for the FLCz monomer (Figure S20). The network structure of the π-extended, electron-rich CMPs allows for an efficient exciton migration along polymer strands, the microporosity for an effective diffusion of guest molecules into the porous network; these features make CMPs promising for optical sensing of suited analytes, particularly electron-deficient species such as nitroaromatic compounds.

Optical Sensing of TNT

With this in mind, we tested the sensing ability of fluorescent PTPETCz (thickness: 15 nm) against TNT as analyte, an electron-deficient compound used as explosive. Prior to this, the work functions of all CMP films grown over 50 cycles were determined using atmospheric pressure ultraviolet photoelectron spectroscopy (UPS). The work functions are found to be 5.54, 5.4 and 5.55 eV (Figures S21, S22, and S23), respectively. The lowest unoccupied molecular orbital (LUMO) levels are calculated from the reduction potentials of the CMP thin films grown by electropolymerization in cyclic voltammetry measurements (see Supporting Information for details). From these data, the LUMO levels are estimated as −3.55, −3.61, and −3.60 eV for PTPETCz, PFLCz, and PTPEFLCz, respectively. These positions of the HOMO/LUMO energy levels for all CMP films in relation to the energy levels of the studied nitroarene analytes are depicted in Figure S24. For the sensing experiments a dual-chamber system connected with a laser diode for excitation is used to study the optical response of the CMP films toward TNT. All the sensing experiments are performed with films grown over five oxidative cycles. Different concentrations of TNT are exposed to the films on ITO, and simultaneous changes in emission spectra are recorded periodically over time. PTPETCz initially shows constant emission at 525 nm (λex = 355 nm); however, on exposure to TNT (33 ppb) gradual decrease in the emission intensity is observed with time, and an emission quenching of 73% is observed within 60 s. Remarkably, 95% emission quenching of PTPETCz is detected after 3 min (Figure 3a). Emission quenching is also evident for the human eye; please see the photographs of a PTPETCz film before and after TNT exposure (inset of Figure 3a and Figure S25). It is important to emphasize that the microporosity of PTPETCz plays a critical role along with extended π-conjugation for optical sensing with fast response time. Hereby, the microporosity (<1 nm) supports the vapor-phase diffusion of TNT molecules into the CMP network. Mesoporosity of hierarchical porous materials such as mesoporous silica is discussed as preferred scenario for mass transport and diffusion, especially in solution. (67) In the gas/vapor phase, the dominant microporosity of the CMPs should properly facilitate the diffusion of TNT molecules and provides a confined environment, where possible one-to-one host–guest interactions between polymer and analytes are possible. Therefore, even trace-level analytes can be detected in shorter times with high accuracy. In case of mesoporous sensor materials (pore size > 2 nm), the uptake capacity of small analytes can be higher, and multilayer adsorption is possible. (67) This may reduce the average strength of sensor chromophore-analyte interactions resulting in lower sensitivity or longer response times if compared to dominantly microporous materials. The supporting role of the PTPETCz microporosity is evident from comparative sensing experiments performed using monomer TPETCz-films drop-casted on quartz. These films are strongly emissive but nonporous in nature. As depicted in Figure 3b, a drop-casted TPETCz-film exhibited merely 10% decrease of emission when exposed to 0.2 ppm of TNT (ca. 6 times higher concentration as used for the CMP film) over 2 min, thus corresponding to a (ca. 1 order of magnitude) lower sensitivity compared to PTPETCz. The observed moderate emission quenching in the drop-casted film of monomer TPETCz is expected to be a result of interactions at surface-near centers. Interestingly, PTPETCz films also showed appreciable response to very low TNT concentrations of 10 ppb, as shown in Figure 4a: nearly 30% emission quenching is observed after 2 min of exposure. These results are promising if compared to our previously reported vapor-phase TNT thin-film sensors. (59,60) Excitingly, PTPETCz showed only 20% and 1.4% emission quenching when exposed to high vapor-pressure nitroarenes such as 2,4-dinitrotoluene (DNT, 350 ppb) and 4-nitrotoluene (NT, 64 ppm) for 5 min, respectively. We also performed vapor-phase sensing experiments of PTPETCz with 1,3,5-trinitrobenzene (TNB; 10 ppb) and 1,3-dinitrobenzene (DNB; 47 ppb) at room temperature. On the one hand, no fluorescence quenching of PTPETCz was observed for DNB, while in the presence of TNB fluorescence quenching of only 14% is noticed after 5 min. On the other hand, TNT at room temperature showed a fluorescence quenching of nearly 30% in 2 min. Sensing experiments of TNT in the presence of TNB and DNB were not performed due to the unavailability of safety measures for mixtures of explosives. However, no significant changes in emission are observed when exposed to electron-rich arenes such as chlorobenzene and toluene (Figure 4b). The fluorescence quenching of thin-film sensor when exposed to nitroarene vapors should be affected (1) by molecular interactions between sensor and analyte, (2) by the LUMO/LUMO energy offset, and (3) by the diffusion ability of the analytes into the thin films. The quenching believably occurs due to a photoinduced electron transfer from photoexcited PTPETCz to analyte when the LUMO level of analyte is lower than the LUMO of the polymer. As depicted in Figure S24, the LUMO level of PTPETCz (−3.55 eV) is higher than that of LUMO levels of TNT (−3.93 eV) and TNB (−3.97 eV), comparable to that of 2,4-DNT (−3.41 eV) and 1,3-DNB (−3.59 eV), and lower than that of 4-NT (−3.01 eV). (68) So, an efficient electron transfer from polymer to TNT is possible thus leading to strong fluorescence quenching. The reason for the weak response to other analytes may be related to their different LUMO energy levels that are not sufficiently low for electron transfer. This also implies that a high vapor pressure of the analyte is not significantly enough for quenching. Strikingly, TNB with a similar LUMO level as that of TNT showed only 14% quenching at 25 °C after 5 min, and no further increase in response was observed even after increasing the concentration of TNB (by heating analyte chamber to 50 °C). Unfortunately, we were not able to calculate binding constants for our solid-state measurements. Such selective response to vapor-phase nitroarenes was already reported for small molecule-based carbazole derivatives and linear conjugated polymers. (69−72) To check the effect of film thickness on the sensing performance, experiments were performed with PTPTTCz grown over 20 CV cycles (thickness ca. 61 nm). As seen in Figure 4c, an appreciable fluorescence quenching (46%) was observed when exposed to TNT vapors of 33 ppb for 3 min. This value is relatively lower compared to the 15 nm thick films (95% quenching in 3 min). Possible reasons for this lower response of thicker films may be the higher number of fluorescent receptors and longer analyte diffusion times to reach the fluorescent receptors. So, the thickness of CMP film also significantly affects the sensitivity of the porous polymer toward vapor-phase analytes. The decrease in quenching rate with increasing film thickness was also observed in other reports. (41) When the TNT-exposed films of PTPETCz are washed with a toluene/acetonitrile mixture followed by annealing at 140 °C for 1 h under vacuum, nearly 80% of the emission intensity is recovered, and the films are reusable for further sensing cycles (Figure S26). The sensing response of other two CMP films was also studied. The weakly red emissive PFLCz showed no significant response to TNT vapors when exposed more than 10 min even to higher TNT concentrations (0.2 ppm). This is also evident from photographs of films that are illuminated before and after TNT exposure (Figures S25 & S27). This contrasting behavior can be ascribed to the increased electron-accepting character of the PFLCz-film due to the fluorenone units present in the polymer. Interestingly, polymer PTPEFLCz with both TPE and fluorenone units showed appreciable optical response when exposed to TNT (0.2 ppm). As shown in Figures 4d & S28 the PTPEFLCz emission at 608 nm gradually decreased with time when exposed to TNT vapors (0.2 ppm): nearly 70% emission quenching is observed after 2 min. Photographs of the illuminated films showed a clear decrease in the emission intensity when exposed to TNT vapors.

Figure 3

Figure 3. (a) Gradual decrease of PTPETCz emission when exposed to 33 ppb of TNT vapor over time. (inset) Photographs of illuminated PTPETCz thin films on ITO (i) under UV lamp and (ii), (iii) under laser source before and after exposure to TNT, respectively. (b) Fluorescence quenching of PTPETCz films (blue) with time in the presence of TNT vapor (33 ppb), compared to the fluorescence quenching of a drop-casted monomer film (TPETCz) during exposure to TNT vapor (0.2 ppm). (inset) Photographs of illuminated TPETCz film (iv) before and (v) after TNT exposure.

Figure 4

Figure 4. (a) Fluorescence quenching of a PTPETCz film with time in the presence of TNT vapor (10 ppb) and (b) degree of emission quenching of PTPETCz films when exposed to various analyte vapors; TNT (33 ppb, 3 min) and TNB (10 ppb), 1,3-DNB (47 ppb), saturated vapors of 2,4-dinitrotoluene (DNT), nitrotoluene (NT), chlorobenzene (ClBen), and toluene (Tol), exposure time 5 min. (c) Change in fluorescence intensity with time in the presence of TNT vapor (33 ppb) for PTPETCz films of ca. 61 nm thickness and (d) change in fluorescence intensity with time in the presence of TNT vapor (0.2 ppm) for PTPEFLCz films.

4. Conclusions

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In summary, we have generated different CMP thin films containing two types of fluorescent segments using the electrochemical oxidative polymerization method, including a copolymer made from two monomers of different structure. All CMP films are microporous with appreciable BET surface areas of 930–509 m2/g. Two of the CMPs show an intense fluorescence. This unique combination of properties produces a sensitive and selective optical response to trinitrotoluene in the vapor phase by florescence quenching, for TNT concentrations down to 10 ppb. Our study suggests that combination of electron-donating TPE units combined with an intrinsic microporosity in TPE-containing CMPs is a promising approach for the sensing of electron-poor analytes. Vapor-phase sensing using CMP thin films is, therefore, an interesting platform for developing reliable vapor-phase sensors, also toward other relevant explosives as royal demolition explosive (RDX), trinitrophenol, etc. Hereby, the strategy of synthesizing copolymer-based thin films from electronically different monomers can be useful for a fine-tuning of the electronic properties of the resulting CMPs, possibly also for the development of thin-film materials for visible-light photocatalysis or organic optoelectronics.

Supporting Information

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The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acsanm.8b01779.

  • Synthetic procedure of monomer and bulk polymers, CV of polymers in monomer-free solution, FTIR spectra, solid-state NMR spectra, TGA, absorption and emission spectra of polymer films, ultraviolet photoemission spectra of polymer films, polymer energy-level diagram (PDF)

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Author Information

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  • Corresponding Author
  • Authors
    • André Räupke - Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
    • Kai Oliver Brinkmann - Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
    • Thomas Riedl - Institute of Electronic Devices, University of Wuppertal, Rainer-Gruenter-Str. 21, 42119 Wuppertal, Germany
    • Gunther Brunklaus - Institut für Physikalische Chemie, Westfälische Wilhelms-Universität, Corrensstr. 46, D-48149 Münster, GermanyOrcidhttp://orcid.org/0000-0003-0030-1383
    • Ullrich Scherf - Macromolecular Chemistry Group, Bergische Universität Wuppertal, Gaußstraße 20, 42119 Wuppertal, Germany
  • Notes
    The authors declare no competing financial interest.

Acknowledgments

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V.M.S. thanks Alexander von Humboldt foundation for postdoctoral fellowship.

References

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ACS Applied Nano Materials

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  • Abstract

    Scheme 1

    Scheme 1. Schematic Illustration of the Electropolymerization of TPETCz into Fluorescent PTPETCz Thin Film, and the Fluorescence Quenching in the Presence of Trace TNT Vapors

    Figure 1

    Figure 1. (a) CVs of monomers (0.1 mM) TPETCz (black), FLCz (red), and their 1:1 mixture (TPECz/FLCz) (blue) in dichloromethane/acetonitrile (4:1) containing 0.1 M TBAP, ITO electrodes, potential range 0–1.5 V. (b–d) First 20 consecutive CV cycles showing electropolymerization and growth of CMP thin films of (b) PTPETCz, (c) PFLCz, and (d) PTPEFLCz, ITO electrodes, prepared from corresponding monomer (0.1 mM) solutions containing 0.1 M TBAP.

    Figure 2

    Figure 2. (a) AFM images of CMP thin film of PTPETCz grown over five CV cycles and (b, c) digital images of free-standing PTPETCz or PFLCZ thin films, respectively. Kr gas adsorption isotherms of (d) CMP thin films prepared by electropolymerization and (e) CMP powders synthesized by chemical oxidation with FeCl3; PTPETCz (navy blue), PFLCz (green), and PTPEFLCz (black), all measured at 77 K.

    Figure 3

    Figure 3. (a) Gradual decrease of PTPETCz emission when exposed to 33 ppb of TNT vapor over time. (inset) Photographs of illuminated PTPETCz thin films on ITO (i) under UV lamp and (ii), (iii) under laser source before and after exposure to TNT, respectively. (b) Fluorescence quenching of PTPETCz films (blue) with time in the presence of TNT vapor (33 ppb), compared to the fluorescence quenching of a drop-casted monomer film (TPETCz) during exposure to TNT vapor (0.2 ppm). (inset) Photographs of illuminated TPETCz film (iv) before and (v) after TNT exposure.

    Figure 4

    Figure 4. (a) Fluorescence quenching of a PTPETCz film with time in the presence of TNT vapor (10 ppb) and (b) degree of emission quenching of PTPETCz films when exposed to various analyte vapors; TNT (33 ppb, 3 min) and TNB (10 ppb), 1,3-DNB (47 ppb), saturated vapors of 2,4-dinitrotoluene (DNT), nitrotoluene (NT), chlorobenzene (ClBen), and toluene (Tol), exposure time 5 min. (c) Change in fluorescence intensity with time in the presence of TNT vapor (33 ppb) for PTPETCz films of ca. 61 nm thickness and (d) change in fluorescence intensity with time in the presence of TNT vapor (0.2 ppm) for PTPEFLCz films.

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    • Synthetic procedure of monomer and bulk polymers, CV of polymers in monomer-free solution, FTIR spectra, solid-state NMR spectra, TGA, absorption and emission spectra of polymer films, ultraviolet photoemission spectra of polymer films, polymer energy-level diagram (PDF)


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