Recent Progress in Piezo‐Phototronic Effect Enhanced Solar Cells

Zhu, Laipan; Wang, Zhong Lin

doi:10.1002/adfm.201808214

Cited by 66 publications

(35 citation statements)

References 136 publications

(209 reference statements)

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“…Along with the theoretical studies, a number of experimental studies demonstrate the piezo‐phototronic effect on charge carrier characteristics and performances of a solar cell . The experimental results are consistent with the theoretical analysis in the previous section.…”

Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Sosupporting

confidence: 83%

“…by using a typical n‐type piezoelectric ZnO NWs and p‐type non‐piezoelectric material . Assuming that J SC is free from stress/strain, photocurrent of a solar cell with a piezoelectric effect can be written as the equation (8) below, where ρ piezo is the density of piezoelectric charges, W piezo is the width of the created piezoelectric charge zone

true normalJ = J_{p n 0} \cdot normale normalx normalp ([], {{- q}^{2} ρ_{p i e z o} W^{2} (2 k T ϵ_{s})}^{- 1}) ([] e x p (q V / k T) - 1) - J_{S C}

…”

Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Somentioning

confidence: 99%

“…V oc of a solar cell can be re‐written as the equation (10) by assuming that J SC

≫

J pn , which holds for a typical solar cell

true V_{O C} \approx \frac{k T}{q} \cdot \ln ((), \frac{J_{s o l a r}}{J_{p n}}) = \frac{k T}{q} \cdot [\ln ((), \frac{J_{s o l a r}}{J_{p n 0}}) + {q^{2} ρ_{p i e z o} W^{2} ((), 2, k, T, ϵ_{s})}^{- 1}]

…”

Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Somentioning

confidence: 99%

“…[97] Assuming that J SC is free from stress/strain, photocurrent of a solar cell with a piezoelectric effect can be written as the equation (8) below, where ρ piezo is the density of piezoelectric charges, W piezo is the width of the created piezoelectric charge zone. [93,99,100]…”

Section: Theoretical Analysis Of Piezo-phototronic Effect On Solar Cellsmentioning

confidence: 99%

“…V oc of a solar cell can be re-written as the equation (10) by assuming that J SC �J pn , which holds for a typical solar cell. [99,100]…”

Section: Theoretical Analysis Of Piezo-phototronic Effect On Solar Cellsmentioning

confidence: 99%

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Quantum Dots for Hybrid Energy Harvesting: From Integration to Piezo‐Phototronics

Cho

Pak

et al. 2019

Israel Journal of Chemistry

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Energy harvesting, which converts wasted environmental energy into electricity by utilizing various physical effects, hasattracted tremendous research interests as is one of the key technologies to realize advanced electronics in the future. In this review, we introduce recent progress in the field of hybrid energy harvesting technology. In particular, we focus on a quantum dots (QD)‐based hybrid energy harvesting device. Attributed to fascinating material properties that QD possess, employment of QDs into hybrid energy harvesting has shown great potential for independent and sustainable energy supply.First, an integration of a QD solar cell into a mechanical energy harvester is discussed to harness different types of environmental energy sources simultaneously. Second, a comprehensive explanation of a piezotronic and piezo‐phototronic effect is provided, which is followed by QD‐based piezo‐phototronic applications. Finally, we summarize recent progress that has been made in energy harvesting technology involving a photovoltaic and piezo/triboelectric effect

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Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Sosupporting

confidence: 83%

true normalJ = J_{p n 0} \cdot normale normalx normalp ([], {{- q}^{2} ρ_{p i e z o} W^{2} (2 k T ϵ_{s})}^{- 1}) ([] e x p (q V / k T) - 1) - J_{S C}

…”

Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Somentioning

confidence: 99%

“…V oc of a solar cell can be re‐written as the equation (10) by assuming that J SC

≫

J pn , which holds for a typical solar cell

true V_{O C} \approx \frac{k T}{q} \cdot \ln ((), \frac{J_{s o l a r}}{J_{p n}}) = \frac{k T}{q} \cdot [\ln ((), \frac{J_{s o l a r}}{J_{p n 0}}) + {q^{2} ρ_{p i e z o} W^{2} ((), 2, k, T, ϵ_{s})}^{- 1}]

…”

Section: Piezotronic and Piezo‐phototronic Effect On A Quantum Dot Somentioning

confidence: 99%

Section: Theoretical Analysis Of Piezo-phototronic Effect On Solar Cellsmentioning

confidence: 99%

“…V oc of a solar cell can be re-written as the equation (10) by assuming that J SC �J pn , which holds for a typical solar cell. [99,100]…”

Section: Theoretical Analysis Of Piezo-phototronic Effect On Solar Cellsmentioning

confidence: 99%

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Quantum Dots for Hybrid Energy Harvesting: From Integration to Piezo‐Phototronics

Cho

Pak

et al. 2019

Israel Journal of Chemistry

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Interface Engineering in 1D ZnO‐Based Heterostructures for Photoelectrical Devices

Zhao

et al. 2021

Adv Funct Materials

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1D semiconductor materials are widely used in the fields of energy conversion, electronics, and photoelectrical devices, due to their unique ability to connect the nanometer and macroscopic worlds. Among them, 1D‐ZnO plays a vital role in the construction of photoelectrical devices due to its easily modulated morphology and band structure. By combining 1D‐ZnO with other materials to form a variety of heterostructures, the functional diversity of 1D‐ZnO is greatly enriched. Through the means of interface engineering, the behavior of carriers in 1D‐ZnO‐based heterostructures can be adjusted to optimize its photoelectrical performance. A comprehensive understanding of the different integration methods and interface engineering of 1D‐ZnO‐based heterostructures can provide new and more effective methods for the design of next‐generation photoelectrical devices. In this paper, starting with the precise growth of 1D‐ZnO, 1D‐ZnO‐based heterostructures constructed by traditional epitaxial growth and emerging van der Waals stacking are emphatically summarized. The modulation mechanisms by interface engineering on the photoelectrical performance of the above two types of heterostructures are systematically reviewed. Finally, the opportunities and challenges of interface engineering in 1D‐ZnO‐based heterostructures for next‐generation photoelectrical devices are prospected.

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Recent Advances of Green Electricity Generation: Potential in Solar Interfacial Evaporation System

Wang,

Cao,

Cui

et al. 2024

Advanced Materials

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Solar‐driven interfacial evaporation (SDIE) has played a pivotal role in optimizing water‐energy utilization, reducing conventional power costs, and mitigating environmental impacts. The increasing emphasis on the synergistic co‐generation of water and green electricity through SDIE is particularly noteworthy. However, there is a gap of existing reviews that have specifically focused on the mechanistic understanding of green power from WEC systems, the structure‐activity relationship between efficiency of green energy utilization in WEC and materials design in SDIE. Particularly it lacks a comprehensive discussion to address the challenges faced in these areas along with potential solutions. Therefore, this review aims to comprehensively assess the progress and future perspective of green electricity from water‐electricity co‐generation (WEC) systems by investigating the potential expansion of SDIE. Firstly, it provides a comprehensive overview about materials rational design, thermal management and water transportation tunnels in SDIE. Then it summarizes diverse energy sources utilized in the SDIE process, including steaming generation, photovoltaics, salinity gradients effect, temperature gradients effect, and piezoelectric effect. Subsequently, it explores factors that affect generated green electricity efficiency in WEC. Lastly, this review proposes challenges and possible solution in the development of WEC. The timely emergence of this review will promote the sustainable use of energy.This article is protected by copyright. All rights reserved

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Recent Progress in Piezo‐Phototronic Effect Enhanced Solar Cells

Cited by 66 publications

References 136 publications

Quantum Dots for Hybrid Energy Harvesting: From Integration to Piezo‐Phototronics

Quantum Dots for Hybrid Energy Harvesting: From Integration to Piezo‐Phototronics

Interface Engineering in 1D ZnO‐Based Heterostructures for Photoelectrical Devices

Recent Advances of Green Electricity Generation: Potential in Solar Interfacial Evaporation System

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