Abstract:The development of novel bilayer photoanodes plays an essential role in dyesensitized solar cell (DSSC) applications to fabricate efficient devices. Herein, a novel homojunction photoanode consisting of undoped and Ni-doped TiO 2 layers with trace amounts of Ni dopant (0.5% at.) was prepared. After a systematic study on photoconversion efficiency that changes with tuning the location of the doped layer, an in-depth understanding was obtained regarding the physical mechanism of the coupling of structural, optic… Show more
“…The series contact resistance indicated by R s , the charge‐transfer resistance between the counter electrode and the TiO 2 indicated by R 1 , and the resistance value of the TiO 2 /dye/electrolyte indicated by R 2 in the equivalent model are all shown at the initial point of the intercepts with the real axis. [ 70,71 ] The R s values almost remain the same. As shown in Table 6 , the R 1 value for the BODIPY‐loaded device of 85.9 Ω is greater compared to N719 of 6.1 Ω.…”
Section: Resultsmentioning
confidence: 73%
“…[ 72 ] A relatively higher value of HOMO level of the present dye guarantees a larger value of driving force for dye generation. [ 68–71 ] Even though the difference between LUMO level and E c of TiO 2 is appreciable for the dye, J sc value stays behind that of other dyes. [ 68–71 ] This might be attributed to weak light absorption ability of the dye.…”
Section: Resultsmentioning
confidence: 99%
“…[ 68–71 ] Even though the difference between LUMO level and E c of TiO 2 is appreciable for the dye, J sc value stays behind that of other dyes. [ 68–71 ] This might be attributed to weak light absorption ability of the dye. V oc is also associated with energy level of electrolyte.…”
The performance of the created BODIPY based dye compound in dye‐sensitized solar cells (DSSCs) is evaluated. The electrical and charge transport characteristics of the dye are examined using the density functional theory (DFT) and time dependent density functional theory (TD‐DFT). By calculating EHOMO, ELUMO, λmax, Eex, LHE (the light‐harvesting efficiency), reorganization energy, and ΔGinj (the free injection energy), attributes of the dye are identified. In comparison to the performance of N719 dye (5.16%), the device performance of synthesized BODIPY dye is reported to have an efficiency of 0.34%. Electrochemical outcomes are consistent with the efficiency outcomes and have a larger charge transport resistance for BODIPY (85.9 Ω) than for N719 (6.1 Ω).This article is protected by copyright. All rights reserved.
“…The series contact resistance indicated by R s , the charge‐transfer resistance between the counter electrode and the TiO 2 indicated by R 1 , and the resistance value of the TiO 2 /dye/electrolyte indicated by R 2 in the equivalent model are all shown at the initial point of the intercepts with the real axis. [ 70,71 ] The R s values almost remain the same. As shown in Table 6 , the R 1 value for the BODIPY‐loaded device of 85.9 Ω is greater compared to N719 of 6.1 Ω.…”
Section: Resultsmentioning
confidence: 73%
“…[ 72 ] A relatively higher value of HOMO level of the present dye guarantees a larger value of driving force for dye generation. [ 68–71 ] Even though the difference between LUMO level and E c of TiO 2 is appreciable for the dye, J sc value stays behind that of other dyes. [ 68–71 ] This might be attributed to weak light absorption ability of the dye.…”
Section: Resultsmentioning
confidence: 99%
“…[ 68–71 ] Even though the difference between LUMO level and E c of TiO 2 is appreciable for the dye, J sc value stays behind that of other dyes. [ 68–71 ] This might be attributed to weak light absorption ability of the dye. V oc is also associated with energy level of electrolyte.…”
The performance of the created BODIPY based dye compound in dye‐sensitized solar cells (DSSCs) is evaluated. The electrical and charge transport characteristics of the dye are examined using the density functional theory (DFT) and time dependent density functional theory (TD‐DFT). By calculating EHOMO, ELUMO, λmax, Eex, LHE (the light‐harvesting efficiency), reorganization energy, and ΔGinj (the free injection energy), attributes of the dye are identified. In comparison to the performance of N719 dye (5.16%), the device performance of synthesized BODIPY dye is reported to have an efficiency of 0.34%. Electrochemical outcomes are consistent with the efficiency outcomes and have a larger charge transport resistance for BODIPY (85.9 Ω) than for N719 (6.1 Ω).This article is protected by copyright. All rights reserved.
“…One way to further boost the photoelectrochemical performance of doped TiO 2 is to produce heterojunction between doped and undoped TiO 2 , which was demonstrated to suppress charge recombination rate and provide fast charge transport for Ni-doped TiO 2 . 206 A composite catalyst of Cu 3 Pg-C 3 N 4 nano-heterojunctions 207 with TiO 2 can produce synergistic effects in photocatalytic H 2 generation. Multilayer p-n and n-n heterojunctions are effective methods to enhance photocatalysis, as they have built-in electric and/or magnetic fields.…”
Titanium
dioxide (TiO2) is a wide bandgap semiconductor
that has a wide range of applications including wastewater treatment,
photocatalysis, solar cells, and sensors owing to its excellent electronic
and optical properties. However, the wide bandgap of TiO2 (∼3.2 eV) along with the recombination processes of the photoexcited
charge carriers reduce its interfacial charge transport properties
and respective activities. Energetics, optical response, and corresponding
photophysics of excited charge carriers can be altered through doping
and codoping of TiO2 and composite formulation. Therefore, it is very crucial to understand the structure–property
and property-application relationships of doped, co-doped, and composite
TiO2 to maximize the efficiency and extend the fundamental
understanding for their applications in different fields. In this
Perspective, we summarize the ongoing research on the advancement
of undoped, doped, co-doped, and composite TiO2 including
their structure and morphology, energetics, and corresponding photophysics
relative to their applications in photocatalysis, wastewater treatment,
and water-splitting reactions. We then propose our perspectives on
the future potential of energetic manipulation of photocatalytic TiO2 to develop advanced and highly efficacious catalytic materials.
“…These structures are given as photoanode (PA) coated with a mesoporous TiO 2 nanoparticles, a molecular dye that absorbs the sunlight, electrolyte solution that creates a conducive atmosphere for the movement of electrons and a counter electrode (CE) which is platinum coated catalyst. Given that, a great deal of investigation has been done on each component/layer independently to enhance the DSSCs' performance metrics [4]. The component of a DSSC that really determines how effectively light is harvested is called a dye sensitizer.…”
The optimization of the TiO2 mesoporous structure plays significant role in dye-sensitized solar cell (DSSC) to produce efficient devices. In this study, the TiO2 mesoporous layer was coated by using a spin coating equipment with different spin accelerations. As a consequence of this investigation, the impacts of the spin coating acceleration on the optoelectronic and electrical performance characteristics of the DSSC were investigated. It has been shown that altering the spin coating acceleration has a direct impact on the mesoporous layer, which in turn influences the absorption ability of dye. The light absorbance of the sample A5 (coated at 2000 rpm/s) ascended drastically in accordance to other samples. Thanks to this augmentation in absorbance, the current density (JSC) and power conversion efficiency (PCE) values also improved. According to electrochemical impedance spectroscopy analysis, it was attained that recombination resistance values increases with the rising spin coating acceleration rates after 500 rpm/s and reaches up to highest value at 2000 rpm/s. A relatively longer electron lifetime of 40.36 ms and recombination resistance of 12.22 were obtained for the device coated at the rate of 2000 rpm/s. The device coated at a rate of 2000 rpm/s had a PCE (5.51%) that was superior than other devices because of its improved light collecting ability, quick electron transport, suppressed electron recombination, and having longer electron life time. As a starting point for future investigations and applications, results of present study provide an insight into the optimal spin coating parameters for DSSC applications.
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