Thermoelectric materials with crystal-amorphicity duality induced by large atomic size mismatch
نویسندگان
چکیده
•Discovering a material series with crystal structure not previously reported•Large S/Te size mismatch in (Cu,Ag)2(Te,S) inducing crystal-amorphicity duality•Ultralow thermal conductivity and high thermoelectric figure of merit zT Exploration discovering novel high-performance materials are the “fountain youth” for science, engineering, technology. Here, we report series, (Cu1?xAgx)2(Te1?ySy), structurally featured by mismatch-induced duality. The entanglement highly disordered yet crystalline anionic sublattice an amorphous cationic gives rise to extremely low conductivities state-of-the-art 2.0 x = y 0.22 sample. These results attest duality as paradigm-shifting approach beyond classic “phonon-glass electron-crystal” “phonon-liquid paradigm development thermoelectrics. Discovering attaining higher performance eternal pursuit research. (Cu1?xAgx)2(Te1?ySy) (0.16 ? 0.24, 0.16 0.24), which adopts complex orthorhombic differing from any known (Cu/Ag)2(S/Te). This is induced large mismatch: size-mismatched anions Te/S coexists amorphous-like cations Cu/Ag. In context structure-property correlation, gave only interesting electrical properties but also exceptionally lattice 300 1,000 K. A obtained sample at give insights into design develop materials. Nowadays, concerns about environmental issues fossil fuel usage have made sustainable energy technologies urgent front-burner task. To this end, (TE) technology, enables direct green conversion between electricity heat, holds promise waste heat harvesting, distributive spot-size cooling, etc.1Shi X.L. Zou J. Chen Z.G. Advanced design: structures devices.Chem. Rev. 2020; 120: 7399-7515Crossref PubMed Scopus (476) Google Scholar, 2He Tritt T.M. Advances research: looking back moving forward.Science. 2017; 357: 6358Crossref (962) 3Zhang Z. Zhao Wei T.-R. Qiu P. L. Shi X. Cu2Se-Based liquid-like materials: stepping forward.Energy Environ. Sci. 13: 3307-3329Crossref 4Tan G. L.D. Kanatzidis M.G. 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On theory super-lattice alloys.Zeitschrift für Kristallographie - Crystalline Materials. 1935; 91: 23-47Crossref separation expected when atomic difference solute atom solvent larger than 15%. our supplementary study revealed single-phased crystalline-amorphous formed coefficient helps release strain escape separation. duality, natural interpolation PLEC, (short-range ordered) coexisting (long-range material. There was early crystal-glass organic-inorganic perovskites concept explored field research.24Zhu Ertekin E. Mixed phononic non-phononic lead halide perovskites: glass-crystal dynamical disorder, anharmonicity.Energy 216-229Crossref following, display stemming mismatch. average solved single-crystal X-ray diffraction (XRD) data, revealing both ordered components particular, form periodic Cu/Ag short-range ordered, properties, value ?2.0 K (Cu0.78Ag0.22)2(Te0.78S0.22) Doping and/or alloying semiconductors semimetals main route, major restriction solubility limit doping element, governed dopant host substituted. (> 15%) tends facilitate separation.23Hume-Rothery Cu2S, Cu2Te, Ag2S, Ag2Te their potentials TEs. Given (1.35 Å), Ag (1.60 S (1.00 Te (1.40 Å),25Slater J.C. Atomic radii crystals.J. 1964; 41: 3199-3204Crossref (1563) especially Te, what would happen, solid solutions separation, if melt cool admixture Cu, Ag, Te? efforts answer question, observed intriguing phenomena formation nominal compositions 0.13 0.26; 0.16, 0.24; 0.16. characterize purity, microstructures, conducted scanning microscopy (SEM), dispersive (EDS) analysis, powder XRD measurements. As shown Figures 1A S1, elemental segregations impurity phases samples 0.26, consistent previous nearly immiscible Cu2X Te).26Zhao Yue Guan Zhu al.Are Cu2Te-based materials?.Adv. 31e1903480Crossref (42) Scholar,27Guan Enhanced quaternary Cu2-2xAg2xSe1-xSx chalcogenides.ACS Appl. Interfaces. 13433-13440Crossref (21) Notably, homogeneous element distributions ranging quantitative analysis accordance compositions. patterns depicted 1B S2. When content all peaks can well indexed suggesting over wide composition range. Note neither Cu2X, Ag2X, CuAgX (X= Te) compunds28Evans H.T. chalcocite djurleite.Zeitschrift Kristallographie. 1979; 150: 299-320Crossref (157) 29Asadov Y.G. Rustamova L.V. Gasimov G.B. Jafarov K.M. Babajev A.G. Structural 2– crystals ( 0.00, 0.10, 0.15, 0.20, 0.25).Phase Transit. 1992; 38: 247-259Crossref (37) 30Sadanaga R. Sueno ?-? transition Ag2S.Mineral. 1967; 124-143Crossref 31Jiang Niu Achieving room-temperature cubic AgCuTe.J. A. 8: 4790-4799Crossref adopt temperature. Thus, convention solutions. Beyond 0.16–0.24 range, observed, agreeing SEM-EDS rules.23Hume-Rothery following discussions, will focus same y, aka (Cu1?xAgx)2(Te1?xSx), otherwise noted. Single-crystal data measured (Cu0.82Ag0.18)2(Te0.82S0.18) 100, 295, 400 point (Imma) unit cell (a 16.3803(8) Å, b 7.3157(4) c 11.1689(6) Å 295 K). detailed crystallographic summarized Table 1 positions listed 2. Figure 1D, complicated, consisting thirteen sites four sites. preferably occupied atoms, other three atoms. For simplicity, assume solely site structural model follow-up discussion calculations. At stage, unable differentiate preferred occupation because disorder. partially ions. Each anion surrounded multiple different polyhedrons, S3. S-Cu/Ag bond distance 2.2697–2.4996 shorter Te-Cu/Ag 2.3956–2.7944 expected. That being said, take appropriate relax sublattice. fully occupied, forming largely (cf. 1E), occupancy factors (SOFs) 0.138 0.561. total, there 48 spread 140 each cell, resulting 1F). We infer drives state; latter former separation.Table 1Crystallographic information KSample(Cu2Te)0.82(Ag2S)0.18a / Å16.3803(8)b Å7.3157(4)c Å11.1689(6)Volume Å31,338.4(1)Space groupImmaCrystal systemorthorhombic?calc g cm?36.965 Open table new tab 2Refined coordinates, occupancies, isotropic displacement parameters KSitesWyckoffXyZOccupancyU (Å2)Te18i0.7194(1)0.250.4153(2)10.0293(9)Te28i0.3756(2)0.250.8011(2)10.046(1)Te34e0.50.750.8523(4)10.0652(14)S4a0.500.510.027(3)Cu/Ag116j0.7295(4)0.3885(11)0.6347(5)0.522(16)0.048(3)Cu/Ag216j0.6488(5)0.5983(12)0.7938(9)0.561(18)0.083(4)Cu/Ag38i0.5873(9)0.250.5775(12)0.52(2)0.077(5)Cu/Ag48i0.5541(10)0.750.6303(11)0.45(3)0.077(8)Cu/Ag516j0.5870(8)0.581(2)0.6687(18)0.374(19)0.102(8)Cu/Ag68h0.50.410(3)0.945(2)0.31(3)0.098(15)Cu/Ag78h0.50.427(3)0.817(3)0.21(2)0.064(14)Cu/Ag88g0.750.479(4)0.750.25(2)0.080(12)Cu/Ag916j0.6303(12)0.415(3)0.5858(15)0.264(18)0.087(10)Cu/Ag1016j0.6295(14)0.575(5)0.968(4)0.19(3)0.064(14)Cu/Ag118f0.580(7)0.510.26(7)0.12(4)Cu/Ag124e0.50.250.628(5)0.18(2)0.077(7)Cu/Ag138h0.50.445(7)0.700(5)0.138(16)0.077(7) super-structure along axis corresponding super triple length. Similar cases Cu2Se Cu2Se1?xTex,32Eikeland Blichfeld A.B. Borup K.A. Overgaard Iversen Crystal across beta alpha Cu2-xSe.IUCrJ. 4: 476-485Crossref (48) regarded structure. details correlated disorder require analyses diffuse scattering.33Roth N. Solving beta-Cu2-xSe using three-dimensional pair distribution function.Acta Crystallogr. Found. Adv. 75: 465-473Crossref (16) plays crucial role stabilizing Ag-free Cu12Te5S actually distinct Cu10Ag2Te5S (i.e., (Cu5/6Ag1/6)2(Te5/6S1/6)) S4. performed extended absorption fine (EXAFS) analyses. Although whole EXAFS spectra too extract information, K-edge spectrum found close Ag2S standard (Figure S5), local around (Cu1?xAgx)2(Te1?xSx) points corroborated data. addition sharp peaks, broad humps clearly patterns, signature 1B). parameters, Rietveld refinement analyses, function Ag/S 1C S1. It note gradually increase inversely decreases increasing contents. Nevertheless, rough linear trend implies substitutionally dope Other hump capacity anomaly near room temperature S6) small change SOF Tables S2–S4), unchanged 100 stable 800 K, undergoes orthorhombic-to-cubic transition, demonstrated high-temperature measurements S6). feature pattern less salient still discernible compared counterpart low-temperature phase. cross-check supplement derived means aberration-corrected transmission (STEM) high-angle annular dark-field (HAADF) detector loss spectroscopy (EELS). 2A 2B atomically resolved HAADF-STEM images [111] zone axis. discern. Nonetheless, composed captured 2B, agreement 2C). dimmer spots, marked pink arrows indicate more these Concomitantly, brighter red squares, better features, turn [010] axis, columns separated. 2D 2E, ring-like arrangement center locate Te. aforementioned 2F). 2D, substitutions defects effectively short-wavelength elevated Besides, sign (red circles) direction, although clear EELS S7 further confirm elements, determined model. All above-mentioned evidences corroborate as-formed dual defects. How does coexistence impact behavior? dependence total plotted 3A. discontinuous jumps approximately attributed exhibit very values significantly lower Cu2Te. reduction caused decreased (?e) S8). (?L), calculated subtracting 3B. show extraordinarily ?L 0.2–0.3 W m?1 K?1 those well-known Bi2Te3 PbTe,34Hao Tang Xing Chu H.-S. Lu al.High efficiency Bi2Te3-based devices generation 300°C.Energy 9: 3120-3127Crossref Scholar,35Pei LaLonde Convergence bands thermoelectrics.Nature. 473: 66-69Crossref (2628) smaller some ?-SiO2,36Cahill D.G. Pohl R.O. Heat flow vibrations glasses.Solid 1989; 70: 927-930Crossref (270) ?-Si,37Pompe Hegenbarth Thermal Si temperatures.phys. stat. sol. 1988; 147: 103-108Crossref (27) ?-Se38White G.K. Woods S.B. Elford M.T. selenium temperatures.Phys. 1958; 112: 111-113Crossref (15) 3B 3). Moreover, independent contrast strong (e.g., ? T?1 Umklapp process) conventional normal compounds. 3C SiO2. conduction behavior plateau 10 30 Such ?-SiO2) rarely SiO2), usually well-defined peak (aka dielectric peak) indicating onset process. has crystalline, disordered, clathrates.39Bentien Christensen Bryan J.D. Sanchez Paschen Steglich clathrates.Phys. 2004; 69045107Crossref (155) Scholar,40Bentien Johnsen Strong phonon coupling 2006; 73094301Crossref (59) origin inspired intense activities.41Christensen Schmøkel M.S. Madsen G.K.H. McIntyre Capelli S.C. “Glass-like” Sr8Ga16Ge30 clathrate off-centered atoms.J. 119: 185102Crossref (22) ScholarTable 3Comparison physical (Cu1?xAgx)2(Te1?xSx); Cu2Te; Ag2S; ?-SiO2 ?-Si, ?-Se temperatureCrystal-amorphicity dualityCrystallineAmorphousMaterials(Cu1?xAgx)2(Te1?xSx)Cu2TeAg2S?-SiO2?-Si?-Se?L (W/mK)0.2–0.30.40.541.4210.15lphonon (Å)2.4–3.03.54.69.33.52.4? (cm2/Vs)12–14134050.1–30.14The ?L, lphonon, ? refer mean free path, mobility, path lphonon estimated equation 1/3Cv v lphonon,43Toberer E.S. Zevalkink Phonon engineering chemistry.J. 21: 15843-15852Crossref (552) Cv ? isochoric sound velocity, 3D, drastically declines below then scarcely changes above resemble 2.4–3.0 interatomic (2.67 Å). consequence character, jointly cover wavelength range phon
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ژورنال
عنوان ژورنال: Joule
سال: 2021
ISSN: ['2542-4351', '2542-4785']
DOI: https://doi.org/10.1016/j.joule.2021.03.012