261 research outputs found

    Semiconducting Organosilicon-based Hybrids for the Next Generation of Stretchable Electronics

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    During past years, organic-based electronic devices revealed high promise to supplement the ubiquitous silicon-based electronic devices and enable new fields of applications. At the center of this development is the considerable progress regarding ฯ€-conjugated polymer semiconductors (PSCs): Due to their processability from solution, light-weight, as well as low-cost, PSCs are now evolving towards production-scale of new technologies, e.g., in organic solar cells (OSCs), organic field-effect transistors (OFETs), and organic light emitting diodes (OLEDs). Especially OFETs are of fundamental importance, as they constitute the switching units in all logic circuits and display technologies. However, the future world is expected to be full with smart electronics and communication devices integrated in clothes, tools and even interacting with the human body, e.g., as on-skin wearable sensors. For this the electrically-active material, just as a human tissue, requires to combine several properties in addition to being charge conducting: They need to show (i) mechanical softness, (ii) capacity to repair, (iii) multimodal sensitivity, as well as (iv) biodegradability. Here, PSCs still face challenges as they are brittle and break upon applying a mechanical stress. When trying to address this issue, the existing knowledge on mechanical properties of well-established polymeric plastics, e.g., polystyrene, cannot be directly applied for several reasons, e.g., (i) the bulkiness of monomers (including long side-chains), (ii) the rigid ฯ€-conjugated backbone, (iii) the low degree of polymerization, (iv) the small quantities in which PSCs are available, etc. Moreover, these kinds of materials should not only be mechanically compliant and stretchable, but furthermore retain their charge mobility upon stretching, and withstand numerous of mechanical stretching cycles. Considering this complex problem, researchers have been developing and investigating several approaches to combine good electrical properties and mechanical compliance within one material. These approaches include (i) stress-accommodating engineering, (ii) blending of PSCs into elastic matrix, as well as (iii) molecular engineering approach. The latter seeks to interlink mechanical and electrical properties on the molecular level, i.e., synthesize polymers that are charge conducting and stretchable. Different strategies were tested, from the modification of side chains, to the introduction of conjugation breakings spacers into the backbone. Selected works sought to incorporate stretchability and conductivity by utilizing block copolymers, i.e., covalently linking a conjugated and a non-conjugated polymer chain, resulting in a phase separation of both constituents and preserving their respective properties. The ultimate goal of this work is to achieve an intrinsically stretchable and electrically high-performing PSC via the block copolymer approach. This is done by connecting organosilicone, namely the polydimethylsiloxane (PDMS) elastomer โ€“ possessing outstanding mechanical properties, as well as good environmental and air stability โ€“ with a conjugated diketopyrrolopyrrole (DPP)-based donor-acceptor copolymer. The final obtained structure of this polymer is a tri-block copolymer (TBC) consisting of an inner DPP-based polymer block and two outer soft PDMS polymer blocks. The content of PDMS block can be controlled and be very high (up to 67 wt%), and easy processing, e.g., via shear coating, is possible. Relatively high charge carrier mobilities โ€“ in the same range as the reference DPP-based copolymer (i.e., without outer PDMS blocks) โ€“ are retained, and the block copolymers withstands numerous stretching cycles (up to 1500 cycles) without losing electrical functionality. Finally, one of the block copolymers was successfully incorporated into a biosensor for COVID-19 antibodies and antigens detection. Overall, the findings of this work show that the block copolymer is a highly versatile approach to obtain functional and stretchable semiconductors with high charge carrier mobilities. Block copolymers consisting of a high-performing donor-acceptor PSC and a biocompatible elastomer could contribute towards one of the long-term goals of organic electronics โ€“ the realization of mechanically compliant materials for applications in stretchable electronics (e.g., wearable sensors, electronic skin, etc.)

    Room-temperature bandlike transport and Hall effect in a high-mobility ambipolar polymer

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    The advent of new-class of high-mobility semiconducting polymers opens up a window to address fundamental issues in electrical transport mechanism such as hopping between localized states versus extended state conduction. Here, we investigate the origin of ultra-low degree of disorder (~ 16 meV) and band-like negative temperature (T) coefficient of the field effect electron mobility in a high performance diketopyrrolopyrrole (DPP)-based semiconducting polymer. Models based on the framework of mobility edge (ME) with exponential density of states are invoked to explain the trends in transport. The temperature window over which the system demonstrates de-localized transport was tuned by a systematic introduction of disorder at the transport interface. Additionally, the Hall mobility extracted from Hall-voltage measurements in these devices was found to be comparable to field effect mobility in the high T band-like regime. Comprehensive studies with different combinations of dielectrics and semiconductors demonstrate the effectiveness of rationale molecular design which emphasizes uniform-energetic landscape and low re-organization energy

    Very large ฯ€-conjugation despite strong nonplanarity : a path for designing new semiconducting polymers

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    When two ฯ€-conjugated fragments are connected by a bond between two sp2 carbon atoms, a torsion around this bond is expected to break the overall ฯ€-conjugation. We show that for specially selected monomers, the ฯ€-conjugation is insensitive to torsions around a Cโ€“C bond up to about 60ยฐ. We provide a number of examples for this very unexpected phenomenon and a simple explanation. We propose that this feature can be incorporated into conjugated polymers to generate semiconducting materials that are extremely insensitive to structural disorder

    Structural engineering on specific organic-solar cells and transistors:from materials synthesis to device fabrication

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    Development of Organic Semiconductors for Soft Electronics

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    Organic semiconductors, Soft electronics, Colloid, Mini-emulsion synthesis, Breath-figure moldingOrganic semiconductor based soft electronic devices are demonstrated: (1) effects of conjugation length on charge transport in polymer semiconductors, (2) water-borne colloids of organic semiconductors, and (3) breath-figure molding of polymer semiconductors for sensors. To improve the charge carrier mobility of diketopyrrolopyrrole donor-acceptor copolymer semiconductors, the length of the donor building block is controlled using vinylene moieties, and its effects on crystalline structure and charge transport are systematically studied. We synthesize P29-DPP-TBT with two vinylene linkages between thiophene units and compare it with P29-DPP-TVT with single vinylene linkage. Density functional theory calculations predict enhanced backbone planarity of P29-DPP-TBT compared to P29-DPP-TVT, which can be related with the increased conjugation length of P29-DPP-TBT as proved by the increased free exciton bandwidth extracted from UV-vis absorption spectra and the wavenumber shift of the Cโ€“C peaks to higher values in Raman spectra. From two-dimensional grazing incident X-ray diffraction studies, it is turned out that the paracrystalline disorder is lower in P29-DPP-TBT than in P29-DPP-TVT. Near-edge X-ray absorption fine structure spectroscopy reveal that more edge-on structure of polymer backbone is formed in the case of P29-DPP-TBT. By measuring the temperature-dependence of the charge carrier mobilities, it is turned out that the activation energy for charge hopping is lower for P29-DPP-TBT than for P29-DPP-TVT. Collectively, these results imply that the substitution of extended ฯ€-conjugated donor moiety of polymeric semiconductors can yield a more planar backbone structure and thus enhanced intermolecular interaction which enables more perfect crystalline structure as well as enhanced charge transport behavior. A synthetic approach has demonstrated to enhance coalescence phenomenon during solidification of water-borne colloids so that thin, even, and continuous film morphology of polymer semiconductors can be realized. From theoretical study of complex colloids, it is shown that small-sized and uniform colloid particles are essential to minimize depletion contact energy between colloid particles and thus to enhance coalescence. Therefore, the newly synthesized polymer semiconductor is designed for better molecular affinity with surfactants, so that phase transfer of polymer semiconductors from organic phase to water phase can proceed more efficiently during mini-emulsion synthesis. This is achieved by substituting a Si atom to the branching C atom of the alkyl solubilizing group of a conventional donor-acceptor polymer semiconductor. Such a chemical modification increases the volumetric portion of hydrophobic alkyl chains and thus enables higher solu-bility as well as higher hydrophobicity, all of which are closely related with enhancing molecular affinity be-tween polymer semiconductor and surfactants. As a result, the performance of organic field-effect transistors fabricated from water-borne colloids can be improved to a level similar to the case of organic solvents. More importantly, the reproducibility of transistor performance is also greatly improved due to the small and uni-form water-borne colloidal particles. Strategically designed polymer semiconductor thin film morphology with both high responsivity to the specific gas analyte and high signal transport efficiency is reported to realize high-performance flexible NOx gas sensors. Breath-Figure (BF) molding of polymer semiconductors enables a finely defined degree of nano-porosity in polymer films with high reproducibility while maintaining a high charge carrier mobility characteristics of organic field effect transistors (OFETs). The optimized BF-OFET with a donor-acceptor copolymer exhibits a maximum responsivity of over 104%, sensitivity of 774%/ppm, and limit of detection (LOD) of 110 ppb against NO. When tested across at NO concentrations of 0.2โ€“10 ppm, the BF-OFET gas sensor ex-hibits a response time of 100โ€“300 s, which is suitable for safety purposes in practical applications. Further-more, BF-OFETs show a high reproducibility as confirmed by statistical analysis on 64 independently fabri-cated devices. Selectivity to NOx analytes is tested by comparing the sensing ability of BF-OFET to other re-ducing gases and volatile organic compounds. Finally, flexible BF-OFETs conjugated with plastic substrates are demonstrated and they exhibit a sensitivity of 500%/ppm and LOD of 215 ppb, with a responsivity degradation of only 14.2% after 10,000 bending cycle at 1% strain.YPart โ… . Effects of conjugation length on crystalline perfectness and charge transport in diketopyrrolopyrrole-based polymer semiconductors 1 โ… . Introduction 2 โ…ก. Experimental Section 3 2.1 Materials 3 2.2 Device fabrication 3 2.3 Characterization 4 2.4 Measurements 4 โ…ข. Results and Discussions 5 โ…ฃ. Conclusion 13 โ…ค. References 14 Part โ…ก. Facilitating Phase Transfer of Polymer Semiconductor in Mini-Emulsion Synthesis via Molecular Affinity Engineering 18 โ… . Introduction 19 โ…ก. Experimental Section 21 2.1 Materials 21 2.2 Colloid synthesis 21 2.3 Device fabrication 21 2.4 Characterization 21 2.5 Measurements 22 โ…ข. Results and Discussions 22 3.1 Efficiency of Mini-emulsion 22 3.2 Film Morphology 26 3.3 Crystallinity and Molecular Orientation 28 3.3 Electrical Properties of Organic Field-effect Transistors (OFETs) 30 โ…ฃ. Conclusion 32 โ…ค. References 33 Part โ…ข. Breath-Figure Molding of Polymer Transistors to Implement Flexible and High-Performance NOx Sensors 36 โ… . Introduction 37 โ…ก. Experimental Section 39 2.1 Device fabrication 39 2.2 Film characterization 39 2.3 Measurements 40 โ…ข. Results and Discussions 40 โ…ฃ. Conclusion 50 โ…ค. References 51 ๊ตญ๋ฌธ์š”์•ฝ 55๋ณธ ๋…ผ๋ฌธ์€ ์œ ๊ธฐ ๋ฐ˜๋„์ฒด๋ฅผ ์ด์šฉํ•œ ์œ ์—ฐ ์†Œ์ž ๊ฐœ๋ฐœ ๋ฐฉ๋ฒ•๋“ค์„ ์ œ์‹œํ•œ๋‹ค: (1) ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ ๊ณต์•ก ๊ธธ์ด์— ๋”ฐ๋ฅธ ์ „ํ•˜ ์ด๋™ ์˜ํ–ฅ, (2) ์ˆ˜๋ถ„์‚ฐ ์œ ๊ธฐ ๋ฐ˜๋„์ฒด ์ฝœ๋กœ์ด๋“œ ํ•ฉ์„ฑ ๋ฐ ์ด๋ฅผ ์ด์šฉํ•œ ์†Œ์ž ๊ฐœ๋ฐœ, (3) breath-figure ํŒจํ„ด ๋ชฐ๋”ฉ๋ฒ•์„ ์ด์šฉํ•œ ์„ผ์„œ ๊ฐœ๋ฐœ. ๋””์ผ€ํ† ํ”ผ๋กค๋กœํ”ผ๋กค(diketopyrrolopyrrole) ์ „์ž ์ฃผ๊ฐœ-๋ฐ›๊ฐœ ๊ตฌ์กฐ์˜ ๊ณต์ค‘ํ•ฉ์ฒด ๋ฐ˜๋„์ฒด์˜ ์ „ํ•˜ ์šด๋ฐ˜์ฒด ์ด๋™์„ฑ์„ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด, ์ฃผ๊ฐœ ๊ตฌ์กฐ์˜ ๊ธธ์ด๋Š” ๋น„๋‹๋ Œ ๋‹จ์œ„์ฒด๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ์ œ์–ด๋œ ์ฑ„ ๊ฒฐ์ • ๊ตฌ์กฐ ๋ฐ ์ „ํ•˜ ์ˆ˜์†ก์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์ฒด๊ณ„์ ์œผ๋กœ ์—ฐ๊ตฌํ•œ๋‹ค. ํ‹ฐ์˜คํŽœ ๋‹จ์œ„์ฒด ์‚ฌ์ด์— 2 ๊ฐœ์˜ ๋น„๋‹๋ Œ ๊ฒฐํ•ฉ์„ ๊ฐ–๋Š” P29-DPP-TBT๋ฅผ ํ•ฉ์„ฑํ•˜๊ณ  ๋‹จ์ผ ๋น„๋‹๋ Œ ๊ฒฐํ•ฉ์„ ๊ฐ–๋Š” P29-DPP-TVT์™€ ๋น„๊ตํ•œ๋‹ค. ๋ถ„์ž ์ด๋ก  ๊ณ„์‚ฐ์„ ํ†ตํ•˜์—ฌ P29-DPP-TVT์™€ ๋น„๊ตํ•˜์—ฌ P29-DPP-TBT์˜ ํ–ฅ์ƒ๋œ ๋ฐฑ๋ณธ ํ‰๋ฉด์„ฑ์„ ์˜ˆ์ธกํ•˜๊ณ , ์ž์™ธ์„ -๊ฐ€์‹œ๊ด‘์„  ํก๊ด‘ ์ŠคํŽ™ํŠธ๋Ÿผ๊ณผ ๋ผ๋งŒ ์ŠคํŽ™ํŠธ๋Ÿผ์„ ์ด์šฉํ•˜์—ฌ ์ถ”์ถœ๋œ ์ž์œ  ์—‘์‹œํ†ค ๋Œ€์—ญํญ์ด ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ P29-DPP-TBT์˜ ๊ณต์•ก ๊ธธ์ด๊ฐ€ ๊ธธ์–ด์ง์„ ์ฆ๋ช…ํ•œ๋‹ค. 2 ์ฐจ์› X- ์„  ํšŒ์ ˆ ๋ถ„์„๋ฒ•์„ ์ด์šฉํ•˜์—ฌ, P29-DPP-TVT๋ณด๋‹ค P29-DPP-TBT์—์„œ ๊ฒฐ์ •์„ฑ์ด ๋›ฐ์–ด๋‚จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ถ”๊ฐ€์ ์œผ๋กœ, X- ์„  ํก์ˆ˜ ๋ฏธ์„ธ ๊ตฌ์กฐ ๋ถ„๊ด‘๋ฒ•์—์„œ P29-DPP-TBT์˜ ๊ฒฝ์šฐ์— ๊ณ ๋ถ„์ž ๋ฐฑ๋ณธ์ด ๋” ๋งŽ์€ ์—์ง€-์˜จ ๊ตฌ์กฐ๋กœ ํ˜•์„ฑ๋จ์„ ๋ณด์—ฌ์ค€๋‹ค. ์ „ํ•˜์ด๋™๋„์˜ ์˜จ๋„ ์˜์กด์„ฑ์„ ์ธก์ •ํ•จ์œผ๋กœ์จ, ์ „ํ•˜ ํ˜ธํ•‘์„ ์œ„ํ•œ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋Š” P29-DPP-TVT๋ณด๋‹ค P29-DPP-TBT์— ๋Œ€ํ•ด ๋” ๋‚ฎ์€ ๊ฒƒ์œผ๋กœ ๋ฐํ˜€์กŒ๋‹ค. ์ข…ํ•ฉ์ ์œผ๋กœ, ์ด๋“ค ๊ฒฐ๊ณผ๋Š” ๊ณต์ค‘ํ•ฉ์ฒด ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ ์—ฐ์žฅ๋œ ฯ€- ๊ณต์•ก ์ „์ž ์ฃผ๊ฐœ ๋ถ€๋ถ„์˜ ์น˜ํ™˜์ด ๋ณด๋‹ค ํ‰๋ฉด์  ์ธ ๊ณจ๊ฒฉ ๊ตฌ์กฐ๋ฅผ ์ƒ์„ฑํ•  ์ˆ˜ ์žˆ๊ณ , ์ด์— ๋”ฐ๋ผ ๋ณด๋‹ค ์™„์ „ํ•œ ๊ฒฐ์ •์งˆ ๊ตฌ์กฐ ๋ฐ ํ–ฅ์ƒ๋œ ์ „ํ•˜ ์ˆ˜์†ก ๊ฑฐ๋™์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜์—ฌ ๋ถ„์ž๊ฐ„ ์ƒํ˜ธ ์ž‘์šฉ์„ ํ–ฅ์ƒ์‹œํ‚ฌ ์ˆ˜ ์žˆ์Œ์„ ์˜๋ฏธํ•œ๋‹ค. ๊ณ ๋ถ„์ž ํ•ฉ์„ฑ ์ธก๋ฉด์— ์žˆ์–ด ์ˆ˜์„ฑ ์ฝœ๋กœ์ด๋“œ์˜ ๋ฐ•๋ง‰ํ™” ๋™์•ˆ ์‘์ถ• ํ˜„์ƒ์„ ํ–ฅ์ƒ์‹œ์ผœ์„œ, ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ ์–‡๊ณ  ๊ท ์ผํ•˜๋ฉฐ ์—ฐ์†์ ์ธ ๋ฐ•๋ง‰ ํ˜•ํƒœ๊ฐ€ ์‹คํ˜„๋  ์ˆ˜ ์žˆ์Œ์„ ์ž…์ฆํ•˜์˜€๋‹ค. ์ฝœ๋กœ์ด๋“œ์— ๋Œ€ํ•œ ์ด๋ก ์  ์—ฐ๊ตฌ๋กœ, ํฌ๊ธฐ๊ฐ€ ์ž‘๊ณ  ๊ท ์ผํ•œ ์ฝœ๋กœ์ด๋“œ ์ž…์ž๊ฐ€ ์ฝœ๋กœ์ด๋“œ ์ž…์ž ์‚ฌ์ด์˜ ๊ณตํ• ์ ‘์ด‰ ์—๋„ˆ์ง€๋ฅผ ์ตœ์†Œํ™”ํ•˜๊ณ  ๋”ฐ๋ผ์„œ ์‘์ถ•์„ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ๋ฐ ํ•„์ˆ˜์ ์ด๋ผ๋Š” ๊ฒƒ์ด ๋ฐํ˜€์กŒ๋‹ค. ๋”ฐ๋ผ์„œ, ์ƒˆ๋กญ๊ฒŒ ํ•ฉ์„ฑ๋œ ๊ณต์ค‘ํ•ฉ์ฒด ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด๋Š” ๊ณ„๋ฉดํ™œ์„ฑ์ œ์™€์˜ ๋ถ„์ž ์นœํ™”์„ฑ์ด ํ–ฅ์ƒ๋˜๋„๋ก ์„ค๊ณ„๋˜์–ด, ์œ ๊ธฐ์ƒ์œผ๋กœ๋ถ€ํ„ฐ ์ˆ˜์ƒ์œผ๋กœ ๊ณต์ค‘ํ•ฉ์ฒด ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ ์ƒ ์ „์ด๊ฐ€ ๋ฏธ๋‹ˆ-์—๋ฉ€์ ผ ํ•ฉ์„ฑ ๋™์•ˆ ๋ณด๋‹ค ํšจ์œจ์ ์œผ๋กœ ์ง„ํ–‰๋  ์ˆ˜ ์žˆ๋‹ค. ์ด๋Š” ํ†ต์ƒ์ ์ธ ์ „์ž ์ฃผ๊ฐœ-๋ฐ›๊ฐœ ๊ตฌ์กฐ์˜ ๊ณต์ค‘ํ•ฉ์ฒด ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ ์•Œํ‚ฌ ์ฒด์ธ ๊ทธ๋ฃน์˜ ๋ถ„ ์ง€ํ˜• C ์›์ž์— Si ์›์ž๋ฅผ ์น˜ํ™˜ํ•จ์œผ๋กœ์จ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ํ™”ํ•™์  ๋ณ€ํ˜•์€ ์†Œ์ˆ˜์„ฑ ์•Œํ‚ฌ ์ฒด์ธ์˜ ๋ถ€ํ”ผ๋ฅผ ์ฆ๊ฐ€์‹œํ‚ค๊ณ  ๋”ฐ๋ผ์„œ ๋” ๋†’์€ ์šฉํ•ด๋„ ๋ฐ ๋” ๋†’์€ ์†Œ์ˆ˜์„ฑ์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜๋ฉฐ, ์ด๋Š” ๋ชจ๋‘ ๊ณต์ค‘ํ•ฉ์ฒด ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์™€ ๊ณ„๋ฉดํ™œ์„ฑ์ œ ์‚ฌ์ด์˜ ๋ถ„์ž ์นœํ™”๋„๋ฅผ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ๊ฒƒ๊ณผ ๋ฐ€์ ‘ํ•œ ๊ด€๋ จ์ด ์žˆ๋‹ค. ๊ฒฐ๊ณผ์ ์œผ๋กœ, ์ˆ˜๊ณ„ ์ฝœ๋กœ์ด๋“œ๋กœ ์ œ์กฐ๋œ ์œ ๊ธฐ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ์„ฑ๋Šฅ์€ ์œ ๊ธฐ ์šฉ๋งค์˜ ๊ฒฝ์šฐ์™€ ์œ ์‚ฌํ•œ ์ˆ˜์ค€์œผ๋กœ ๊ฐœ์„ ๋  ์ˆ˜ ์žˆ์Œ์„ ์ž…์ฆํ•˜์˜€๋‹ค. ๋”๋ถˆ์–ด ์ž‘๊ณ  ๊ท ์ผํ•œ ์ˆ˜์„ฑ ์ฝœ๋กœ์ด๋“œ ์ž…์ž๋กœ ์ธํ•ด ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ ์„ฑ๋Šฅ์˜ ์žฌํ˜„์„ฑ์ด ํฌ๊ฒŒ ํ–ฅ์ƒ๋œ๋‹ค. ํŠน์ • ๊ฐ€์Šค ๋ถ„์„ ๋ฌผ์งˆ์— ๋Œ€ํ•œ ๋†’์€ ๋ฐ˜์‘์„ฑ๊ณผ ๋†’์€ ์‹ ํ˜ธ ์ „์†ก ํšจ์œจ์„ ๋ชจ๋‘ ๊ฐ–์ถ˜ ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด ๋ฐ•๋ง‰ ๋ชจํด๋กœ์ง€๋ฅผ ๊ตฌํ˜„ํ•จ์œผ๋กœ์จ, ๊ณ ์„ฑ๋Šฅ์˜ ์œ ์—ฐํ•œ NOx ๊ฐ€์Šค ์„ผ์„œ๋ฅผ ์‹คํ˜„ํ•˜์˜€๋‹ค. ๊ณ ๋ถ„์ž ๋ฐ˜๋„์ฒด์˜ Breath-Figure (BF) ๋ชฐ๋”ฉ์€ ์œ ๊ธฐ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ (OFET)์˜ ๋†’์€ ์ „ํ•˜ ์บ๋ฆฌ์–ด ์ด๋™ ํŠน์„ฑ์„ ์œ ์ง€ํ•˜๋ฉด์„œ ๊ณ ๋ถ„์ž ๋ฐ•๋ง‰์—์„œ ๋ฏธ์„ธํ•œ ํฌ๊ธฐ์˜ ๋‚˜๋…ธ ๋‹ค๊ณต์„ฑ ํ‘œ๋ฉด ๊ฐœ์งˆ์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜์˜€๋‹ค. ์ „์ž ์ฃผ๊ฐœ-๋ฐ›๊ฐœ ๊ตฌ์กฐ์˜ ๊ณต์ค‘ํ•ฉ์ฒด ๊ธฐ๋ฐ˜์˜ ์ตœ์ ํ™”๋œ BF-OFET๋Š” ์ตœ๋Œ€ 104 % ์ด์ƒ์˜ ๋ฐ˜์‘์„ฑ๊ณผ, 774% / ppm์˜ ๊ฐ๋„ ๋ฐ NO์— ๋Œ€ํ•œ 110 ppb์˜ ๊ฒ€์ถœ ํ•œ๊ณ„ (LOD)๋ฅผ ๋‚˜ํƒ€๋‚ธ๋‹ค. 0.2 ~ 10ppm์˜ NO ๋†๋„์—์„œ ์ธก์ •์‹œ์— BF-OFET ๊ฐ€์Šค ์„ผ์„œ๋Š” 100 ~ 300 ์ดˆ์˜ ์‘๋‹ต ์‹œ๊ฐ„์„ ๋‚˜ํƒ€๋‚ด๋ฉฐ ์ด๋Š” ์‹ค์ œ ์‘์šฉ ์†Œ์ž๋กœ ์“ฐ์ผ ์ˆ˜ ์žˆ๋Š” ์ˆ˜์ค€์ด๋‹ค. ๋˜ํ•œ, BF-OFET๋Š” 64 ๊ฐœ์˜ ๋…๋ฆฝ์ ์œผ๋กœ ์ œ์กฐ๋œ ์†Œ์ž์— ๋Œ€ํ•œ ํ†ต๊ณ„ ๋ถ„์„์— ์˜ํ•ด ํ™•์ธ ๋œ ๋ฐ”์™€ ๊ฐ™์ด ๋†’์€ ์žฌํ˜„์„ฑ์„ ๋‚˜ํƒ€๋‚ธ๋‹ค. NOx ๊ฐ€์Šค์— ๋Œ€ํ•œ ์„ ํƒ์„ฑ์€ BF-OFET์˜ ๊ฐ์ง€ ๋Šฅ๋ ฅ์„ ๋‹ค๋ฅธ ํ™˜์› ๊ฐ€์Šค ๋ฐ ํœ˜๋ฐœ์„ฑ ์œ ๊ธฐ ํ™”ํ•ฉ๋ฌผ๊ณผ ๋น„๊ตํ•˜์—ฌ ์ธก์ •ํ•˜์˜€๋‹ค. ์ตœ์ข…์ ์œผ๋กœ ํ”Œ๋ผ์Šคํ‹ฑ ๊ธฐํŒ๊ณผ ์ ‘ํ•ฉ๋œ ์œ ์—ฐํ•œ BF-OFET์„ ๊ตฌํ˜„ํ•˜์˜€์œผ๋ฉฐ ์ด ์†Œ์ž๋Š” 1% ๋ณ€ํ˜•๋ฅ ์—์„œ 10,000 ํšŒ ๊ตฝํž˜ ์ฃผ๊ธฐ ํ›„ 14.2%์˜ ์‘๋‹ต์„ฑ ์ €ํ•˜๋ฅผ ๋ณด์˜€์œผ๋ฉฐ, 500 % / ppm์˜ ๊ฐ๋„์™€ 215ppb์˜ LOD๋ฅผ ๋‚˜ํƒ€๋ƒˆ๋‹ค.MasterdCollectio

    A Bottom-up Computational Approach to Semiconducting Block Copolymers

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    Conjugated polymers are very attractive materials for the scientists and industry due to low cost of the organic compounds, their lightweight, easy large-area processing from solution at low temperature and mechanical flexibility. Moreover, these materials are multifunctional and advanced technologies require both simultaneous n- and p-type conductance, i.e. ambipolarity. However, there are some hindrances which do not allow the wide spreading of this new generation of semiconductors into the market, first of all, due to their instability to ambient conditions. Moreover, determination of the tunable parameters which are responsible for high efficiency and controlled crystal packing ordering of the devices is rather complicated. A lot of efforts are done in order to improve the performance of the organic electronics as well as to shed light on the relation between the chemical structure and their intrinsic properties. Additionally, the governing factors which define the conductive properties of these materials are still under debate and this remains a great challenge for the researchers. One way to gain insight into the characteristics of polymeric materials is to begin exploring the polymers from their small constitutive units and then step-by-step to construct and characterize every compound up to macromolecular level. In this work, the semiconducting block copolymers, as promising candidates for application in organic transistors, are investigated starting from their small donor and acceptor blocks up to monomers and macromolecules, using computational methods running on different time and length scales. It is found out that the charge transport depends on the symmetry of molecules and the hopping mobilities can be predicted from isolated stacks of dimers, which are defined by minimum energy, without knowledge of the actual crystal structure. Interestingly, the polymers moieties prefer to build up mixed stacks and the flanks form segregated columns if there are no present defects in the samples. At each step of the investigation the results are compared with available experimental data

    Investigation of Low Optical-Gap Donor and Acceptor Materials for Organic Solar Cells

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    Development of efficient and clean energy sources to meet the ever-increasing de- mand of humankind is one of the greatest challenges of the 21st century. There is a dire need to decarbonise the power sector, and the focus needs to shift to re- newable resources such as wind and solar energy. In this regard, organic solar cells are a promising and novel technology owing to its low carbon footprint, innovative applications, and possible integration into the current infrastructure. Due to its unique advantages, a considerable research effort has been put into its development in the last decades. As a result, the power conversion efficiency (PCE) of the organic photovoltaics has steadily risen from as low as 0.5% to around 17 % at the current stage. This improvement primarily originates from the better understanding of the underlying physical processes and as a result of extensive material development. In the most general case, organic solar cells consist of a binary blend of an electron donating and an electron accepting organic semiconductor forming the so-called โ€˜bulk-heterojunctionโ€™ (BHJ) morphology. Thermodynamics places an upper limit on the power conversion efficiency (PCE) of binary blend BHJ devices and for further enhancement in efficiency novel device concepts like the use of ternary blends and tandem device architectures is being investigated. In relation to these approaches, the development of low optical-gap (Eopt โ‰ค 1.5 eV) organic semiconductors has gained importance as these materials provide for the complementary absorption with respect to the other components and better harvesting of the solar spectrum. This work mainly deals with the investigation of low optical gap donor and acceptor materials for organic solar cells. We investigate the effect of the molecular structure on the device performance and the photophysical processes in the binary and ternary blend configuration. In the first part of the thesis, we study a family of low optical- gap diketopyrrolopyrrole (DPP) based polymers while varying the conjugated core and the branching position and length of the solubilizing alkyl side chains. The branching position of the side chains is found to have a significant influence on the polymers ability to crystallize, which in turn influences the mobility of free charge carriers. The branching position also affects the solubility of the polymer, which in turn influences the morphology of the bulk-heterojunction (BHJ) and ultimately the yield of photogenerated charge carriers. To investigate the electron transfer and charge separation dynamics in the blends consisting of DPP polymers and fullerene, we employed ultrafast pump-probe spec- troscopic techniques. In the spectroscopy data, we observe signatures suggesting an ultrafast electron transfer process and an efficient charge separation process due to the high mobility of the free charge carriers shortly after separation (โˆผ10-100 ps). ๏ฟผLastly, we investigated indacenodithiophene (IDT) based non-fullerene acceptor (NFA) molecules. In particular, we studied the effect of fluorination on the device performance when these acceptors are blended with PTB7-Th and P3HT donor polymers. The kinetics of the photophysical processes in the binary and ternary blends are characterized using ultrafast spectroscopy and related to the morphology of the blend and the molecular structure of the acceptors. Overall, we investigated the structural variations in the DPP polymers and flu- orinated non-fullerene acceptor (NFA) molecules and suggest design rules for the synthesis of optimal DPP polymers and non-fullerene acceptors to achieve supe- rior device performance. Additionally, we also shed light on the phenomenological processes happening on an ultrafast time scale (0.2-1000 ps) in the binary and the ternary blends with the aim of developing a better understanding of the photophys- ical processes in these promising material systems

    Parallel triplet formation pathways in a singlet fission material

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    Harvesting long-lived free triplets in high yields by utilizing organic singlet fission materials can be the cornerstone for increasing photovoltaic efficiencies potentially. However, except for polyacenes, which are the most studied systems in the singlet fission field, spin-entangled correlated triplet pairs and free triplets born through singlet fission are relatively poorly characterized. By utilizing transient absorption and photoluminescence spectroscopy in supramolecular aggregate thin films consisting of Hamilton-receptor-substituted diketopyrrolopyrrole derivatives, we show that photoexcitation gives rise to the formation of spin-0 correlated triplet pair 1(TT) from the lower Frenkel exciton state. The existence of 1(TT) is proved through faint Herzberg-Teller emission that is enabled by vibronic coupling and correlated with an artifact-free triplet-state photoinduced absorption in the near-infrared. Surprisingly, transient electron paramagnetic resonance reveals that long-lived triplets are produced through classical intersystem crossing instead of 1(TT) dissociation, with the two pathways in competition. Moreover, comparison of the triplet-formation dynamics in J-like and H-like thin films with the same energetics reveals that spin-orbit coupling mediated intersystem crossing persists in both. However, 1(TT) only forms in the J-like film, pinpointing the huge impact of intermolecular coupling geometry on singlet fission dynamics
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