Lattice thermal conductivity reduction in Ca 3 AlSb 3 and Ca 5 Al 2 Sb 6 by manipulating the covalent tetrahedral chain

Understanding the structural and physical origins of low thermal conductivity is critical to improving and designing efficient thermoelectric materials. For two distinct Zintl Ca-Al-Sb compounds with different stoichiometric ratios (Ca AlSb and Ca Al Sb ), experimental measurements suggest the low l...

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Veröffentlicht in:Physical chemistry chemical physics : PCCP 2024-11, Vol.26 (45), p.28595-28605
Hauptverfasser: Zhang, Chi, Zhai, Wenya, Li, Jingyu, Zhu, Jianbo, Ou, Zengfu, Li, Lanwei, Liu, Peng-Fei, Liu, Xiaobing, Yan, Yuli, Zhang, Yongsheng
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container_issue 45
container_start_page 28595
container_title Physical chemistry chemical physics : PCCP
container_volume 26
creator Zhang, Chi
Zhai, Wenya
Li, Jingyu
Zhu, Jianbo
Ou, Zengfu
Li, Lanwei
Liu, Peng-Fei
Liu, Xiaobing
Yan, Yuli
Zhang, Yongsheng
description Understanding the structural and physical origins of low thermal conductivity is critical to improving and designing efficient thermoelectric materials. For two distinct Zintl Ca-Al-Sb compounds with different stoichiometric ratios (Ca AlSb and Ca Al Sb ), experimental measurements suggest the low lattice thermal conductivities (∼1.43 W mK for Ca AlSb and 1.52 W mK for Ca Al Sb at 300 K). In order to understand the physical origin of the low thermal conductivity, we present the first-principles studies on the lattice dynamics and phonon-transport properties. The theoretically calculated lattice thermal conductivity of Ca AlSb and Ca Al Sb is ∼1.61 W mK for Ca AlSb and 1.85 W mK for Ca Al Sb at 300 K, which is in reasonable agreement with the experimental measurements. The low lattice thermal conductivity is attributed to the low acoustic Debye temperature and strong optical-acoustic phonon couplings in the two Ca-Al-Sb compounds. It is worth noting that the thermal conductivity of Ca AlSb and Ca Al Sb along the direction (along the Al-Sb chain) is obviously higher than that along the / direction (perpendicular to the chain). The high lattice thermal conductivity along the Al-Sb chain is due to the strong Al-Sb covalent bond. From the phonon density of states (PDOS), the obviously frequency regions dominated by different atoms suggest that forming defects with one atom would only shift its related PDOS and might not affect the PDOS of others. Based on the understandings of the crystal structure, PDOS and atomic displacement parameter, we represent a methodology to further lower their lattice thermal conductivity: substituting heavier atoms along the Al-Sb chain to strongly scatter phonons. When using Tl to substitute Al, the vibration frequency of the Tl dopant is only 1/3 of that of the substituted Al atom. The significantly decreased vibration frequency will introduce a low phonon band within the PDOS, which will suppress the lattice thermal conductivity. Our work not only elucidates the physical mechanism of low lattice thermal conductivity in Ca AlSb and Ca Al Sb Zintl compounds, but also offers an efficient approach (breaking the covalent tetrahedral chains) to further block the heat transport.
doi_str_mv 10.1039/D4CP03574G
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For two distinct Zintl Ca-Al-Sb compounds with different stoichiometric ratios (Ca AlSb and Ca Al Sb ), experimental measurements suggest the low lattice thermal conductivities (∼1.43 W mK for Ca AlSb and 1.52 W mK for Ca Al Sb at 300 K). In order to understand the physical origin of the low thermal conductivity, we present the first-principles studies on the lattice dynamics and phonon-transport properties. The theoretically calculated lattice thermal conductivity of Ca AlSb and Ca Al Sb is ∼1.61 W mK for Ca AlSb and 1.85 W mK for Ca Al Sb at 300 K, which is in reasonable agreement with the experimental measurements. The low lattice thermal conductivity is attributed to the low acoustic Debye temperature and strong optical-acoustic phonon couplings in the two Ca-Al-Sb compounds. It is worth noting that the thermal conductivity of Ca AlSb and Ca Al Sb along the direction (along the Al-Sb chain) is obviously higher than that along the / direction (perpendicular to the chain). The high lattice thermal conductivity along the Al-Sb chain is due to the strong Al-Sb covalent bond. From the phonon density of states (PDOS), the obviously frequency regions dominated by different atoms suggest that forming defects with one atom would only shift its related PDOS and might not affect the PDOS of others. Based on the understandings of the crystal structure, PDOS and atomic displacement parameter, we represent a methodology to further lower their lattice thermal conductivity: substituting heavier atoms along the Al-Sb chain to strongly scatter phonons. When using Tl to substitute Al, the vibration frequency of the Tl dopant is only 1/3 of that of the substituted Al atom. The significantly decreased vibration frequency will introduce a low phonon band within the PDOS, which will suppress the lattice thermal conductivity. Our work not only elucidates the physical mechanism of low lattice thermal conductivity in Ca AlSb and Ca Al Sb Zintl compounds, but also offers an efficient approach (breaking the covalent tetrahedral chains) to further block the heat transport.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/D4CP03574G</identifier><identifier>PMID: 39523952</identifier><language>eng</language><publisher>England</publisher><ispartof>Physical chemistry chemical physics : PCCP, 2024-11, Vol.26 (45), p.28595-28605</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c582-5a229753c2eac7a655975b5f6383fa56e555eb58f43956ffd58b602eb33dbce63</cites><orcidid>0000-0003-0839-4182 ; 0000-0002-9170-5238</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/39523952$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Zhang, Chi</creatorcontrib><creatorcontrib>Zhai, Wenya</creatorcontrib><creatorcontrib>Li, Jingyu</creatorcontrib><creatorcontrib>Zhu, Jianbo</creatorcontrib><creatorcontrib>Ou, Zengfu</creatorcontrib><creatorcontrib>Li, Lanwei</creatorcontrib><creatorcontrib>Liu, Peng-Fei</creatorcontrib><creatorcontrib>Liu, Xiaobing</creatorcontrib><creatorcontrib>Yan, Yuli</creatorcontrib><creatorcontrib>Zhang, Yongsheng</creatorcontrib><title>Lattice thermal conductivity reduction in Ca 3 AlSb 3 and Ca 5 Al 2 Sb 6 by manipulating the covalent tetrahedral chain</title><title>Physical chemistry chemical physics : PCCP</title><addtitle>Phys Chem Chem Phys</addtitle><description>Understanding the structural and physical origins of low thermal conductivity is critical to improving and designing efficient thermoelectric materials. For two distinct Zintl Ca-Al-Sb compounds with different stoichiometric ratios (Ca AlSb and Ca Al Sb ), experimental measurements suggest the low lattice thermal conductivities (∼1.43 W mK for Ca AlSb and 1.52 W mK for Ca Al Sb at 300 K). In order to understand the physical origin of the low thermal conductivity, we present the first-principles studies on the lattice dynamics and phonon-transport properties. The theoretically calculated lattice thermal conductivity of Ca AlSb and Ca Al Sb is ∼1.61 W mK for Ca AlSb and 1.85 W mK for Ca Al Sb at 300 K, which is in reasonable agreement with the experimental measurements. The low lattice thermal conductivity is attributed to the low acoustic Debye temperature and strong optical-acoustic phonon couplings in the two Ca-Al-Sb compounds. It is worth noting that the thermal conductivity of Ca AlSb and Ca Al Sb along the direction (along the Al-Sb chain) is obviously higher than that along the / direction (perpendicular to the chain). The high lattice thermal conductivity along the Al-Sb chain is due to the strong Al-Sb covalent bond. From the phonon density of states (PDOS), the obviously frequency regions dominated by different atoms suggest that forming defects with one atom would only shift its related PDOS and might not affect the PDOS of others. Based on the understandings of the crystal structure, PDOS and atomic displacement parameter, we represent a methodology to further lower their lattice thermal conductivity: substituting heavier atoms along the Al-Sb chain to strongly scatter phonons. When using Tl to substitute Al, the vibration frequency of the Tl dopant is only 1/3 of that of the substituted Al atom. The significantly decreased vibration frequency will introduce a low phonon band within the PDOS, which will suppress the lattice thermal conductivity. 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For two distinct Zintl Ca-Al-Sb compounds with different stoichiometric ratios (Ca AlSb and Ca Al Sb ), experimental measurements suggest the low lattice thermal conductivities (∼1.43 W mK for Ca AlSb and 1.52 W mK for Ca Al Sb at 300 K). In order to understand the physical origin of the low thermal conductivity, we present the first-principles studies on the lattice dynamics and phonon-transport properties. The theoretically calculated lattice thermal conductivity of Ca AlSb and Ca Al Sb is ∼1.61 W mK for Ca AlSb and 1.85 W mK for Ca Al Sb at 300 K, which is in reasonable agreement with the experimental measurements. The low lattice thermal conductivity is attributed to the low acoustic Debye temperature and strong optical-acoustic phonon couplings in the two Ca-Al-Sb compounds. It is worth noting that the thermal conductivity of Ca AlSb and Ca Al Sb along the direction (along the Al-Sb chain) is obviously higher than that along the / direction (perpendicular to the chain). The high lattice thermal conductivity along the Al-Sb chain is due to the strong Al-Sb covalent bond. From the phonon density of states (PDOS), the obviously frequency regions dominated by different atoms suggest that forming defects with one atom would only shift its related PDOS and might not affect the PDOS of others. Based on the understandings of the crystal structure, PDOS and atomic displacement parameter, we represent a methodology to further lower their lattice thermal conductivity: substituting heavier atoms along the Al-Sb chain to strongly scatter phonons. When using Tl to substitute Al, the vibration frequency of the Tl dopant is only 1/3 of that of the substituted Al atom. The significantly decreased vibration frequency will introduce a low phonon band within the PDOS, which will suppress the lattice thermal conductivity. Our work not only elucidates the physical mechanism of low lattice thermal conductivity in Ca AlSb and Ca Al Sb Zintl compounds, but also offers an efficient approach (breaking the covalent tetrahedral chains) to further block the heat transport.</abstract><cop>England</cop><pmid>39523952</pmid><doi>10.1039/D4CP03574G</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0003-0839-4182</orcidid><orcidid>https://orcid.org/0000-0002-9170-5238</orcidid></addata></record>
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title Lattice thermal conductivity reduction in Ca 3 AlSb 3 and Ca 5 Al 2 Sb 6 by manipulating the covalent tetrahedral chain
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