The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18
Title: The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18
Thermoelectric materials can convert heat into electricity. They are used to generate electricity when other power sources are not available or to increase energy efficiency by recycling waste heat. The Yb 21 Mn 4 Sb 18 phase was previously shown to have good thermoelectric performance due to its large Seebeck coefficient (∼290 μV K −1 ) and low thermal conductivity (0.4 W m −1 K −1 ). These characteristics stem respectively from the unique [Mn 4 Sb 10 ] 22− subunit and the large unit cell/site disorder inherent in this phase. The solid solutions, Yb 21 Mn 4− x Cd x Sb 18 ( x = 0, 0.5, 1.0, 1.5) and Yb 21− y Ca y Mn 4 Sb 18 ( y = 3, 6, 9, 10.5) have been prepared, their structures characterized and thermoelectric properties from room temperature to 800 K measured. A detailed look into the structural disorder for the Cd and Ca solid solutions was performed using synchrotron powder X-ray diffraction and pair distribution function methods and shows that these are highly disordered structures. The substitution of Cd gives rise to more metallic behavior whereas Ca substitution results in high resistivity. As both Cd and Ca are isoelectronic substitutions, the changes in properties are attributed to changes in the electronic structure. Both solid solutions show that the thermal conductivities remain extremely low (∼0.4 W m −1 K −1 ) and that the Seebeck coefficients remain high (>200 μV K −1 ). The temperature dependence of the carrier mobility with increased Ca substitution, changing from approximately T −1 to T −0.5 , suggests that another scattering mechanism is being introduced. As the bonding changes from polar covalent with Yb to ionic for Ca, polar optical phonon scattering becomes the dominant mechanism. Experimental studies of the Cd solid solutions result in a max zT of ∼1 at 800 K and, more importantly for application purposes, a ZT avg ∼ 0.6 from 300 K to 800 K. more »« less
Perez, Christopher J.; Wood, Maxwell; Ricci, Francesco; Yu, Guodong; Vo, Trinh; Bux, Sabah K.; Hautier, Geoffroy; Rignanese, Gian-Marco; Snyder, G. Jeffrey; Kauzlarich, Susan M.
(, Science Advances)
null
(Ed.)
The Zintl phases, Yb 14 M Sb 11 ( M = Mn, Mg, Al, Zn), are now some of the highest thermoelectric efficiency p-type materials with stability above 873 K. Yb 14 MnSb 11 gained prominence as the first p-type thermoelectric material to double the efficiency of SiGe alloy, the heritage material in radioisotope thermoelectric generators used to power NASA’s deep space exploration. This study investigates the solid solution of Yb 14 Mg 1− x Al x Sb 11 (0 ≤ x ≤ 1), which enables a full mapping of the metal-to-semiconductor transition. Using a combined theoretical and experimental approach, we show that a second, high valley degeneracy ( N v = 8) band is responsible for the groundbreaking performance of Yb 14 M Sb 11 . This multiband understanding of the properties provides insight into other thermoelectric systems (La 3− x Te 4 , SnTe, Ag 9 AlSe 6 , and Eu 9 CdSb 9 ), and the model predicts that an increase in carrier concentration can lead to zT > 1.5 in Yb 14 M Sb 11 systems.
Garay, Luis; Borgsmiller, Leah; Zavanelli, Duncan; Snyder, G Jeffrey; Fettinger, James; Kauzlarich, Susan
(, Dryad)
Abstract: Single crystals of Eu5-xYbxAl3Sb6 and Eu5-x-ySrxYbyAl3Sb6 were synthesized by flux methods and their structures determined by single-crystal X-ray diffraction, confirming the monoclinic C2/m symmetry. The Al content in these phases can be increased from 3 to 4 by metallurgical mixing of the elements to form polycrystalline powders. A comparative study of polycrystalline synthesized Eu5Al4Sb6 and its Sr- and Yb-substituted solid solutions, along with the pseudo-quinary phase Eu2.5Sr2Yb0.5Al4Sb6, is presented. Substituting Eu2+ with the more ionic Sr2+ enhances mobility and increases the magnitude of the Seebeck coefficient, while the more covalent Yb2+ drives the system metallic, lowering Seebeck values but improving zT to 0.8 at 873 K. The quinary phase further suppresses bipolar conduction, delaying the high-temperature downturn observed in both ternary solid solutions. Across all compositions, thermal conductivities remain exceptionally low (<1 W m⁻¹ K⁻¹), enabling promising figures of merit. Methods: The datasets (Powder X-ray diffraction and Thermoelectric property measurements) for the phase pure powders are provided. Compositions are provided below. Synthesis: Phase pure powders of composition Eu5.08Al4Sb4, Eu5Al4Sb6, Eu5-xAxAl4Sb6(A = Sr:x= 0.5, 2.5, 5; A = Yb:x= 0.5, 1, 1.5, 2, 5) and Eu2.5Sr2Yb0.5Al4Sb6Powder X-ray Diffraction (PXRD): PXRD data were collected at room temperature in air on ground single crystals and bulk powders of both solid solutions using a Bruker D8 Advance Eco diffractometer with Cu Kα radiation, 1000 W (40 kV, 25 mA), over 2θ = 15–85°, with a step size of 0.02°, and a scan rate of 1 s per step. Polycrystalline samples and ground single crystals were prepared on a zero-background holder using isopropanol. Thermal Conductivity Thermal Diffusivity (D) was measured on thin (1.19 to 1.2 mm thick) slices of Eu5-xAxAl4Sb6 (A = Sr and Yb) pellets using a Netzsch LFA 457 Microflash under a flow of high-purity Ar with a polished piece of Zr ribbon wrapped around the sample holder to act as an oxygen catcher. The thermal conductivity (κ) was determined using the equation: κ = D x ρ x Cp. The Dulong-Petit heat capacity value, Cp, was calculated from 3R/atom (R = gas constant). The pellets’ density (ρ) was measured in replicate using the Archimedes method with toluene as the liquid. All samples were > 95% of their theoretical crystallographic densities, calculated using the Arrhenius method. Electrical Resistivity and Seebeck A Linseis LSR-3 instrument was used to measure resistivity and the Seebeck coefficient employing the four-probe method from 350 K to 800 K under a He atmosphere. The instrument was calibrated with a constantan standard before use. The sample geometries were bar-shaped (10.5 mm x 4 mm x 2 mm) and polished before measurements with 8 mm probes. Multiple samples were measured to ensure reproducibility, and the data were cross-checked with measurements taken at Northwestern University. At Northwestern, electrical resistivity and Hall effect data were measured using a home-built Hall instrument. This set-up uses a four-point van der Pauw resistivity measurement with molybdenum leads and a current of 100 mA. Seebeck coefficient data were collected using a home-built two-probe Seebeck instrument with chromel/Nb thermocouples. TechnicalInfo: # One cation makes a difference: structure-thermoelectric interplay in pseudo-rock salt intermetallic Eu5-*x*A*x*Al3Sb6 (A = Sr and Yb) Dataset DOI: [10.5061/dryad.mkkwh71f1](https://doi.org/10.5061/dryad.mkkwh71f1) ## Description of the data and file structure **PXRD data collection (located in folder PXRD)** PXRD data were collected at room temperature in air on ground single crystals and bulk powders of both solid solutions using a Bruker D8 Advance Eco diffractometer with Cu Kα radiation, 1000 W (40 kV, 25 mA), over 2θ = 15–85°, with a step size of 0.02°, and a scan rate of 1 s per step. Polycrystalline samples were prepared on a zero-background holder using isopropanol. **Thermal Conductivity (located in folder TE properties)** Thermal Diffusivity (*D)* was measured on thin (1.19 to 1.2 mm thick) slices of Eu5-*x*A*x*Al4Sb6 (A = Sr and Yb) pellets using a Netzsch LFA 457 Microflash under a flow of high-purity Ar with a polished piece of Zr ribbon wrapped around the sample holder to act as an oxygen catcher. The thermal conductivity (κ) was determined using the equation: κ = *D* x ρ x C~p~. The Dulong-Petit heat capacity value, C~p~, was calculated from 3*R*/atom (R = gas constant). The pellets’ density (ρ) was measured in replicate using the Archimedes method with toluene as the liquid. All samples were > 95% of their theoretical crystallographic densities, calculated using the Arrhenius method. **Electrical Resistivity, Seebeck, and Hall Data Collection** A Linseis LSR-3 instrument was used to measure resistivity and the Seebeck coefficient employing the four-probe method from 350 K to 800 K under a He atmosphere. The instrument was calibrated with a constantan standard before use. The sample geometries were bar-shaped (10.5 mm x 4 mm x 2 mm) and polished before measurements with 8 mm probes. Multiple samples were measured to ensure reproducibility, and the data were cross-checked with measurements taken at Northwestern University. At Northwestern, electrical resistivity and Hall effect data were measured using a home-built Hall instrument. This set-up uses a four-point van der Pauw resistivity measurement with molybdenum leads and a current of 100 mA. Seebeck coefficient data were collected using a home-built two-probe Seebeck instrument with chromel/Nb thermocouples. ### Files and variables #### File: EuSrYbAlSb6_ChemMater_D.zip **Description:** There are 2 folders for each type of data: Powder X-ray Diffraction (**PXRD**) data for the polycrystalline synthesized samples indicated above; (**TE Properties**) Thermoelectric properties provides the electrical resistivity and Seebeck coefficient as a function of temperature for the polycrystalline samples. #### PXRD folder has 3 sub-folders: EuYbSr, Sr, Yb. The sub-folders contain dataset (.cvs) indicated by the cation composition of the polycrystalline synthesized sample. **Sub-Folder** **EuYbSr**: contains the PXRD data for Eu~2.5~Sr~2~Yb~0.5~Al~4~Sb~6~ **Sub-Folder** **Sr**: contains the PXRD data for Eu~2.5~Sr~2.5~Al~4~Sb~6~; Eu~4.5~Sr~0.5~Al~4~Sb~6~; Sr~5~Al~4~Sb~6~ **Sub-Folder** **Yb**: contains the PXRD data for Yb~5~Al~4~Sb~6;~ Eu~4~Yb~1~Al~4~Sb~6~; Eu~3~Yb~2~Al~4~Sb~6~; Eu~3.5~Yb~1.5~Al~4~Sb~6~; Eu~4.5~Yb~0.5~Al~4~Sb~6~ Each *.cvs dataset is indicated by the sample composition. Each dataset contains a header with the composition; column 1: 2-theta (degree); column 2: intensity (arbitrary units (a.u.)). #### **TE** **Properties** folder has 4 sub-folders: **Eu,** **EuYbSr**, **Sr**, **Yb**. The sub-folders contain dataset (*.cvs) indicated by the cation composition of the polycrystalline synthesized sample. Each *.cvs file has the composition of the element in the A column, and Temperature/K and Resistivity/ mOhm•cm; Seebeck Coefficient/ µV/K; Thermal Conductivity/W •m^-1^ •K^-1^ and ( if collected) carrier concentration/ h/cm^3^ and Hall mobility /cm^2^•V^-1^•s^-1^ **Sub-Folder Eu**: contains TE data for Eu~5~Al~4~Sb~6~; Eu~5.08~Al~4~Sb~6~; **Sub-Folder EuYbSr:** contains TE data for Eu~2.5~Sr~2.0~Yb~0.5~Al~4~Sb~6~ **Sub-Folder Sr:** contains TE data for Sr~5~Al~4~Sb~6~; Eu~2.5~Sr~2.5~Al~4~Sb~6~; Eu~4.5~Sr~0.5~Al~4~Sb~6~; **Sub-Folder Yb:** contains TE data for Yb~5~Al~4~Sb~6;~ Eu~4~Yb~1~Al~4~Sb~6~; Eu~3~Yb~2~Al~4~Sb~6~; Eu~3.5~Yb~1.5~Al~4~Sb~6~; Eu~4.5~Yb~0.5~Al~4~Sb~6~; ####
Opara, Ivan Chinonso; Fettinger, James C; Star, Kurt E; Bux, Sabah K; Shen, Zihao; Taufour, Valentin; Kauzlarich, Susan M
(, Zeitschrift für anorganische und allgemeine Chemie)
The ternary phase, Yb14CdSb11, has been synthesized by flux and polycrystalline methods. The crystal structure is determined via single-crystal X-ray diffraction, revealing that it crystallizes in the Ca14AlSb11 structure type (I41/acd space group with unit cell parameters of a = 16.5962(2) & Aring; and c = 22.1346(5) & Aring;, 90 K, Z = 8, R1 = 2.65%, and wR2 = 4.58%). The polycrystalline form of the compound is synthesized from a stoichiometric reaction of Yb4Sb3, CdSb, Yb, and Sb. The elemental composition is confirmed using scanning electron microscopy and energy-dispersive spectroscopy, and phase purity is verified by powder X-ray diffraction. Thermoelectric measurements, including resistivity, Seebeck coefficient, thermal conductivity, Hall carrier concentration, and Hall mobility, are conducted from 300 to 1273 K. Yb14CdSb11 exhibits a peak zT = 0.90 at 1200 K. Carrier concentration and Hall mobility range from 6.99 x 1020-1.01 x 1021 cm-3 and 4.45-9.35 x 10-1 cm2 V-1 s-1, respectively. This carrier concentration is lower than that reported for the Zn or Mn analogs leading to a lower thermoelectric figure of merit at high temperatures. However, with appropriate doping, this phase should also be a promising p-type candidate for high-temperature energy conversion applications.
Islam, Md Minhajul; Wróblewska, Maria; Shen, Zihao; Toberer, Eric S; Taufour, Valentin; Kauzlarich, Susan M
(, Chemistry of Materials)
Compositional diversity and intriguing structural features have made Zintl phases excellent candidates as thermoelectric materials. Zintl phase with 21-4-18 composition has shown high thermoelectric performance in the mid- to high-temperature ranges. The complex crystal structure and favorable transport properties of these compounds indicate the potential for high thermoelectric efficiency. Arsenic-based Eu21Zn4As18, belonging to the Ca21Mn4Sb18 structure type, exhibits a semiconductor-like p-type transport behavior and has a calculated band gap of 0.49 eV. The compound is paramagnetic at high temperatures, with an antiferromagnetic transition occurring at T-N = similar to 10 K. The moment obtained from the Curie-Weiss data fit aligns with Eu2+ ions. At the same time, the field-dependent measurement at 2 K indicates complex magnetic ordering with a saturation moment consistent with Eu2+ ions. Pristine Eu21Zn4As18 exhibits an ultralow lattice thermal conductivity of 0.40 W m(-1) K-1 at 873 K. Electronic transport properties measurement shows evidence of bipolar conduction across much of the measured temperature range (450-780 K). However, the Seebeck coefficient remains extremely high (>440 mu V K-1) across this range, indicating the potential for high zT if an appropriate dopant is found. This work represents the first report on the temperature-dependent thermal conductivity, Seebeck coefficient, and thermoelectric efficiency of the arsenic-containing Zintl phase with 21-4-18 composition, showcasing its promise for further optimization of the thermoelectric performance.
Justl, Andrew P.; Winston, Logan D.; Bux, Sabah K.; Kauzlarich, Susan M.
(, ACS Applied Energy Materials)
N/A
(Ed.)
Yb14ZnSb11 is one of the newest additions to the high-performance Yb14MSb11 (M = Mn, Mg, and Zn) family of p type high-temperature thermoelectric materials and shows promise for forming passivating oxide coatings. Work on the oxidation of rare earth (RE)-substituted Yb14−xRExMnSb11 single crystals suggested that substituting late RE elements may form more stable passivation oxide coatings. Yb14−xLuxZnSb11 (x = 0.1, 0.2, 0.3, 0.4, 0.5, and 0.7) samples were synthesized, and Lu-substitution’s effects on thermoelectric and oxidation properties are investigated. The solubility of Lu within the system was found to be quite low with xmax ∼ 0.3; samples with x > 0.3 contained impurities of LuSb. Goldsmid−Sharp band gap estimations show that introducing Lu reduces the apparent band gap. Because of this, the Lu-substituted samples show a reduction in the maximum Seebeck coefficient, decreasing the high-temperature zT. This contrasts with the impact of Lu3+ substitution in Yb14MnSb11, where the addition of Lu3+ for Yb2+ increases resistivity and the Seebeck coefficient. Oxidation of the x = 0.3 solid solution was studied by thermogravimetric-differential scanning calorimetry, powder X-ray diffraction, scanning electron microscopy−energy-dispersive spectroscopy, and optical images. The samples show no mass gain before 785 K, and ensuing oxidation reactions are proposed. At the highest temperatures, significant amounts of Yb14−xLuxZnSb11 remained beneath an oxide coating, suggesting that passivation may be achievable in oxygen environments.
He, Allan, Cerretti, Giacomo, and Kauzlarich, Susan M. The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18. Retrieved from https://par.nsf.gov/biblio/10324460. Materials Advances 2.17 Web. doi:10.1039/d1ma00497b.
He, Allan, Cerretti, Giacomo, & Kauzlarich, Susan M. The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18. Materials Advances, 2 (17). Retrieved from https://par.nsf.gov/biblio/10324460. https://doi.org/10.1039/d1ma00497b
He, Allan, Cerretti, Giacomo, and Kauzlarich, Susan M.
"The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18". Materials Advances 2 (17). Country unknown/Code not available. https://doi.org/10.1039/d1ma00497b.https://par.nsf.gov/biblio/10324460.
@article{osti_10324460,
place = {Country unknown/Code not available},
title = {The impact of site selectivity and disorder on the thermoelectric properties of Yb 21 Mn 4 Sb 18 solid solutions: Yb 21 Mn 4−x Cd x Sb 18 and Yb 21−y Ca y Mn 4 Sb 18},
url = {https://par.nsf.gov/biblio/10324460},
DOI = {10.1039/d1ma00497b},
abstractNote = {Thermoelectric materials can convert heat into electricity. They are used to generate electricity when other power sources are not available or to increase energy efficiency by recycling waste heat. The Yb 21 Mn 4 Sb 18 phase was previously shown to have good thermoelectric performance due to its large Seebeck coefficient (∼290 μV K −1 ) and low thermal conductivity (0.4 W m −1 K −1 ). These characteristics stem respectively from the unique [Mn 4 Sb 10 ] 22− subunit and the large unit cell/site disorder inherent in this phase. The solid solutions, Yb 21 Mn 4− x Cd x Sb 18 ( x = 0, 0.5, 1.0, 1.5) and Yb 21− y Ca y Mn 4 Sb 18 ( y = 3, 6, 9, 10.5) have been prepared, their structures characterized and thermoelectric properties from room temperature to 800 K measured. A detailed look into the structural disorder for the Cd and Ca solid solutions was performed using synchrotron powder X-ray diffraction and pair distribution function methods and shows that these are highly disordered structures. The substitution of Cd gives rise to more metallic behavior whereas Ca substitution results in high resistivity. As both Cd and Ca are isoelectronic substitutions, the changes in properties are attributed to changes in the electronic structure. Both solid solutions show that the thermal conductivities remain extremely low (∼0.4 W m −1 K −1 ) and that the Seebeck coefficients remain high (>200 μV K −1 ). The temperature dependence of the carrier mobility with increased Ca substitution, changing from approximately T −1 to T −0.5 , suggests that another scattering mechanism is being introduced. As the bonding changes from polar covalent with Yb to ionic for Ca, polar optical phonon scattering becomes the dominant mechanism. Experimental studies of the Cd solid solutions result in a max zT of ∼1 at 800 K and, more importantly for application purposes, a ZT avg ∼ 0.6 from 300 K to 800 K.},
journal = {Materials Advances},
volume = {2},
number = {17},
author = {He, Allan and Cerretti, Giacomo and Kauzlarich, Susan M.},
}
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