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Hamadani BH. 2.11 - Accurate characterization of indoor photovoltaic performance. JPHYS MATERIALS 2023; 6:10.1088/2515-7639/acc550. [PMID: 37965623 PMCID: PMC10644663 DOI: 10.1088/2515-7639/acc550] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2023]
Abstract
Abstract
Ambient energy harvesting has great potential to contribute to sustainable development and address growing environmental challenges. Converting waste energy from energy-intensive processes and systems (e.g. combustion engines and furnaces) is crucial to reducing their environmental impact and achieving net-zero emissions. Compact energy harvesters will also be key to powering the exponentially growing smart devices ecosystem that is part of the Internet of Things, thus enabling futuristic applications that can improve our quality of life (e.g. smart homes, smart cities, smart manufacturing, and smart healthcare). To achieve these goals, innovative materials are needed to efficiently convert ambient energy into electricity through various physical mechanisms, such as the photovoltaic effect, thermoelectricity, piezoelectricity, triboelectricity, and radiofrequency wireless power transfer. By bringing together the perspectives of experts in various types of energy harvesting materials, this Roadmap provides extensive insights into recent advances and present challenges in the field. Additionally, the Roadmap analyses the key performance metrics of these technologies in relation to their ultimate energy conversion limits. Building on these insights, the Roadmap outlines promising directions for future research to fully harness the potential of energy harvesting materials for green energy anytime, anywhere.
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Gougeon P, Gall P, Huguenot A, Al Rahal Al Orabi R, Gautier R. Synthesis, Crystal and Electronic Structures, and Electrical Properties of the Fifth Member of the Rb 2(Mo 9S 11)(Mo 6nS 6n+2) Series: Rb 10Mo 39S 43, an Atypical Reduced Molybdenum Sulfide Containing Mo 9 and Mo 30 Clusters. Inorg Chem 2019; 58:15236-15245. [DOI: 10.1021/acs.inorgchem.9b02221] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/30/2022]
Affiliation(s)
- Patrick Gougeon
- Univ Rennes, INSA Rennes, ENSC Rennes, CNRS, ISCR-UMR 6226, Rennes F-35000, France
| | - Philippe Gall
- Univ Rennes, INSA Rennes, ENSC Rennes, CNRS, ISCR-UMR 6226, Rennes F-35000, France
| | - Arthur Huguenot
- Univ Rennes, INSA Rennes, ENSC Rennes, CNRS, ISCR-UMR 6226, Rennes F-35000, France
| | | | - Régis Gautier
- Univ Rennes, INSA Rennes, ENSC Rennes, CNRS, ISCR-UMR 6226, Rennes F-35000, France
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Gougeon P, Gall P, Al Rahal Al Orabi R, Boucher B, Fontaine B, Gautier R, Dauscher A, Candolfi C, Lenoir B. Electronic Band Structure and Transport Properties of the Cluster Compound Ag 3Tl 2Mo 15Se 19. Inorg Chem 2019; 58:5533-5542. [PMID: 30973719 DOI: 10.1021/acs.inorgchem.8b03452] [Citation(s) in RCA: 7] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/29/2022]
Abstract
Mo-based cluster compounds are a large class of materials with complex crystal structures that give rise to very low lattice thermal conductivity. Here, we report on the crystal structure and transport property measurements (5-800 K) of the novel Tl-filled compound Ag3Tl2Mo15Se19. This compound adopts a crystal structure described in the rhombohedral R3 c space group [ a = 9.9601(1) Å, c = 57.3025(8) Å, and Z = 6] built by the covalent arrangement of octahedral Mo6 and bioctahedral Mo9 clusters in a 1:1 ratio, with the Ag and Tl atoms filling the large cavities between them. Transport property measurements performed on polycrystalline samples indicate that this compound behaves as a heavily doped semiconductor with mixed electrical conduction. Electronic band structure calculations combined with a semiclassical approach using the Boltzmann transport equation are in good agreement with these measurements. This compound exhibits a lattice thermal conductivity as low as 0.4 W m-1 K-1 because of highly disordered Ag and Tl atoms. Because of the low thermopower values induced by the mixed electrical conduction, the dimensionless thermoelectric figure of merit ZT remains moderate with a peak value of 0.18 at 750 K.
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Affiliation(s)
- Patrick Gougeon
- Univ Rennes, CNRS, ISCR UMR 6226, INSA Rennes, ENSC Rennes , F-35000 Rennes , France
| | - Philippe Gall
- Univ Rennes, CNRS, ISCR UMR 6226, INSA Rennes, ENSC Rennes , F-35000 Rennes , France
| | | | - Benoit Boucher
- Univ Rennes, CNRS, ISCR UMR 6226, INSA Rennes, ENSC Rennes , F-35000 Rennes , France
| | - Bruno Fontaine
- Univ Rennes, CNRS, ISCR UMR 6226, INSA Rennes, ENSC Rennes , F-35000 Rennes , France
| | - Régis Gautier
- Univ Rennes, CNRS, ISCR UMR 6226, INSA Rennes, ENSC Rennes , F-35000 Rennes , France
| | - Anne Dauscher
- Institut Jean Lamour , UMR 7198, CNRS, Université de Lorraine , 2 allée André Guinier-Campus ARTEM, BP 50840 , 54011 Nancy Cedex , France
| | - Christophe Candolfi
- Institut Jean Lamour , UMR 7198, CNRS, Université de Lorraine , 2 allée André Guinier-Campus ARTEM, BP 50840 , 54011 Nancy Cedex , France
| | - Bertrand Lenoir
- Institut Jean Lamour , UMR 7198, CNRS, Université de Lorraine , 2 allée André Guinier-Campus ARTEM, BP 50840 , 54011 Nancy Cedex , France
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