Abstract: Eu11Zn4Sn2As12 is a p-type semiconductor that has been proposed to undergo 3D-to-2D electronic transport as the carrier concentration increases. This commensurately modulated structure in space group R3̅m has been shown to improve its thermoelectric properties upon Na doping, concurrently decreasing electrical resistivity while maintaining a large Seebeck coefficient. In this study, Eu11Zn4Sn2As12 was doped with Cu with the goal of substituting in the [Zn2As3]5− defect hexagonal layers to improve electrical transport. Thermal conductivity, carrier concentration, mobility, electrical resistivity, and the Seebeck coefficients as a function of temperature from 300 to 600 K were measured as a function of Cu content. A maximum zT600K of 0.24 for Eu11Zn4-xCuxSn2As12, x = 0.6, was reached. Methods: The samples, Eu11Zn4-xCuxSn2As12 (x = 0.0, 0.2, 0.4, 0.6) were synthesized and analyzed by powder X-ray diffraction and pressed into dense pellets by Spark Plasma Sintering. The pellets were ≥ 98 % dense by the Archimedes method. Scanning electron microscopy (SEM) and energy-dispersive spectroscopy were obtained and provided in the publication's supporting information. Thermal conductivity, carrier concentration, mobility, electrical resistivity, and the Seebeck coefficients were collected as a function of temperature from 300 to 600 K. Powder X-Ray Diffraction: The sintered sample pellets were ground in a mortar and pestle for PXRD analysis. Samples were plated onto a zero-background X-ray quartz plate, and diffraction was performed with a Bruker D8 Advance Eco diffractometer with Cu Kα radiation (λ = 1.5405 Å) at 40 kV and 25 mA at room temperature. Data was collected with a 0.01 step size and a 2θ range from 20° - 80°. Thermal Conductivity: A Netzsch Laser Flash Analysis (LFA) 475 Microflash instrument was used to measure the thermal diffusivity of the pellets (polished flat and parallel and sprayed with graphite to ensure laser absorption). Thermal conductivity was calculated using thermal diffusivity using the equation κ = λδCp, where κ is thermal conductivity, λ is thermal diffusivity, δ is the sample density, and Cp is the Dulong-Petit heat capacity. Seebeck, Resistivity, and Hall Measurement: Seebeck coefficient measurements were obtained from a custom-built instrument under nitrogen atmosphere and pressure of 300 Torr from 300 to 600K. Resistivity and Hall measurements were obtained with an in-house-built instrument using the van der Pauw geometry. Hall coefficient measurements used 80 mA current and 1 T magnetic field. TechnicalInfo: # Data from: Role of copper doping in modulating the thermoelectric properties of Eu~11~Zn~4~Sn~2~As~12~ Dataset DOI: [10.5061/dryad.d7wm37qgk](https://doi.org/10.5061/dryad.d7wm37qgk) ## Description of the data and file structure The folder entitled Eu11Zn4Sn2As12_Cu_Doping.zip contains 4 *.csv* files, one for each composition of Eu~11~Zn~4−x~*Cu~x~Sn~2~As~12~ (*x* = 0.0, 0.2, 0.4, 0.6) The data are provided in column with room Temperature powder X-ray diffraction, electrical resistivity as a function of temperature (300-600 K), Seebeck coefficients as a function of temperature (300-600 K), thermal conductivity as a function of temperature (300-600 K), carrier concentration as a function of temperature (300-600 K), and Hall mobility as a function of temperature (300-600 K). #### Folder: Eu11Zn4Sn2As12_Cu_Doping.zip **Description:** Contains 4 *.csv files: * Eu11Zn4-xCuxSn2As12_x=0 * Eu11Zn4-xCuxSn2As12_x=0.2 * Eu11Zn4-xCuxSn2As12_x=0.4 * Eu11Zn4-xCuxSn2As12_x=0.6 ## Files and variables File: Eu11Eu4-xCuxSn2As12_x=0.0\ Room temperature powder X-ray diffraction (PXRD) data are provided in columns A and B, with two-theta/degree (column A) and intensity/arbitrary units (au) (column B). Column C is empty. Resistivity vs Temperature data are provided in columns D and E), with Temperature/K (column D) and resistivity/mOhm cm (column E). Column F is empty. Seebeck coefficient vs Temperature data is provided in Columns G and H, with Temperature/K and Seebeck coefficient/µV/K. Column I is empty. Thermal conductivity vs Temperature data are provided in columns J and K, with Temperature/K (column J) and thermal conductivity/W/m K (column K). Column L is empty. Carrier concentration vs Temperature data are found in columns M and N, with Temperature/K (column M) and carrier concentration/h^+^ cm ^-3^ (column N). Hall mobility vs Temperature is provided in columns O and P, with Temperature/K (column O) and Hall mobility/cm^2^ V ^-1^ s ^-1^ (column P). File: Eu11Eu4-xCuxSn2As12_x=0.2\ Room temperature powder X-ray diffraction (PXRD) data are provided in columns A and B, with two-theta/degree (column A) and intensity/arbitrary units (au) (column B). Column C is empty. Resistivity vs Temperature data are provided in columns D and E), with Temperature/K (column D) and resistivity/mOhm cm (column E). Column F is empty. Seebeck coefficient vs Temperature data (measured twice to show reproducibiity) is provided in Columns G-J, with Temperature/K and Seebeck coefficient/µV/K. Column K is empty. Thermal conductivity vs Temperature data are provided in columns L and M, with Temperature/K (column L) and thermal conductivity/W/m K (column M). Column N is empty. Carrier concentration vs Temperature data are found in columns O and P, with Temperature/K (column O) and carrier concentration/h^+^ cm ^-3^ (column P). Hall mobility vs Temperature is provided in columns Q and R, with Temperature/K (column Q) and Hall mobility/cm^2^ V ^-1^ s ^-1^ (column R). File: Eu11Zn4-xCuxSn2As12_x=0.4\ Room temperature powder X-ray diffraction (PXRD) data are provided in columns A and B, with two-theta/degree (column A) and intensity/arbitrary units (au) (column B). Column C is empty. Resistivity vs Temperature data are provided in columns D and E), with Temperature/K (column D) and resistivity/mOhm cm (column E). Column F is empty. Seebeck coefficient vs Temperature data (measured twice to show reproducibiity) is provided in Columns G-J, with Temperature/K and Seebeck coefficient/µV/K. Column K is empty. Thermal conductivity vs Temperature data are provided in columns L and M, with Temperature/K (column L) and thermal conductivity/W/m K (column M). Column N is empty. Carrier concentration vs Temperature data are found in columns O and P, with Temperature/K (column O) and carrier concentration/h^+^ cm ^-3^ (column P). Hall mobility vs Temperature is provided in columns Q and R, with Temperature/K (column Q) and Hall mobility/cm^2^ V ^-1^ s ^-1^ (column R). File: Eu11Zn4-xCuxSn2As12_x=0.6\ Room temperature powder X-ray diffraction (PXRD) data are provided in columns A and B, with two-theta/degree (column A) and intensity/arbitrary units (au) (column B). Column C is empty. Resistivity vs Temperature data are provided in columns D and E), with Temperature/K (column D) and resistivity/mOhm cm (column E). Column F is empty. Seebeck coefficient vs Temperature data is provided in Columns G and H, with Temperature/K and Seebeck coefficient/µV/K. Column I is empty. Thermal conductivity vs Temperature data are provided in columns J and K, with Temperature/K (column J) and thermal conductivity/W/m K (column K). Column L is empty. Carrier concentration vs Temperature data are found in columns M and N, with Temperature/K (column M) and carrier concentration/h^+^ cm ^-3^ (column N). Hall mobility vs Temperature is provided in columns O and P, with Temperature/K (column O) and Hall mobility/cm^2^ V ^-1^ s ^-1^ (column P).
more »
« less
Data from: Advancing the Ca14AlSb11 structure type: Synthesis and characterization of Yb14CdSb11 for thermoelectric applications
Abstract: The ternary phase Yb14CdSb11 has been synthesized using both flux and polycrystalline methods. The crystal structure was 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) Å and c = 22.1346(5) Å, 90 K, Z = 8, R1 = 2.65 %: wR2 = 4.58 %. The polycrystalline form of the compound was synthesized from a stoichiometric reaction of Yb4Sb3, CdSb, Yb, and Sb. The elemental composition was confirmed using scanning electron microscopy and energy-dispersive spectroscopy (SEM-EDS), and phase purity was verified by powder X-ray diffraction (PXRD). Thermoelectric measurements, including resistivity, Seebeck coefficient, thermal conductivity, Hall carrier concentration, and Hall mobility, were conducted from 300 to 1273 K. Yb14CdSb11 exhibited a peak zT = 0.80 at 1150 K. Carrier concentration and Hall mobility ranged from to holescm^-3^ and from 1019 cm²V-¹s-^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, it is expected that this phase should also be a promising p-type candidate for high-temperature energy conversion applications. TechnicalInfo: # Data from: Advancing the Ca14AlSb11 structure type: Synthesis and characterization of Yb14CdSb11 for thermoelectric applications ## Description of the data and file structure ### Files and variables #### File: Dryad_PXRD_data.zip **Description:** Heat capacity, powder x-ray diffraction data for CdSb, Yb4Sb3, and Yb14CdSb11, carrier concentration, mobility, electrical resistivity, Seebeck coefficients, thermal conductivity, and zT for Yb14CdSb11. The zip file entitled Yb14CdSb11_All_Data.zip includes data files with Heat Capacity ("Heat capacity_YbCdSb.dat"), Powder X-ray Diffraction data of the binary precursors ("PXRD CdSb.txt", "PXRD Yb4Sb3.txt", and "PXRD_Yb14CdSb11.txt", and Thermoelectric transport data. **Heat Capacity** Heat capacity measurements of a single crystal were done in a Quantum Design PPMS from 2 K to 300 K. **Powder X-ray Diffraction (PXRD)** PXRD data were collected on each sample using a Bruker zero background holder on a Bruker D8 Eco Advanced employing Cu K∝ radiation (λ = 1.54 Å) with a Ni filter to remove Cu Kβ. **Seebeck Coefficient and Electrical Resistivity** Seebeck, resistivity, and Hall data were collected as a function of temperature under high vacuum at the Jet Propulsion Laboratory (JPL). Resistivity and Hall Van der Pauw measurements were performed with a current of 100 mA and a 0.8 T magnet. Seebeck coefficient was measured using a custom two-probe instrument under a high vacuum. Temperature-dependent Seebeck coefficients, electrical resistivity, and thermal conductivity were fit to six-order polynomials to calculate* zT* values. T (K):** **Temperature in Kelvin; r-fit (mΩ·cm): electrical resistivity; S-fit (µV/K): Seebeck coefficient; L- Lorenz number; K-fit: total thermal conductivity; K_e: electronic thermal conductivity; K_L: lattice (phonon) thermal conductivity; PF: power factor; ZT (dimensionless): thermoelectric figure of merit. **Thermal Conductivity** Thermal diffusivity was measured on densified pellets using laser flash analysis on a Netzsch LFA 475 Microflash under Ar(g) flow. The fully densified pellet was sliced into a thin disk (<1.5 mm) and polished until flat with parallel sides. The density of this disk was measured using Archimedes' method with toluene as the liquid. The heat capacity of Yb14CdSb11 was estimated using an adjusted heat capacity, Cp, based on the experimental heat capacity for Yb14MnSb11 and adjusting for the molecular weight of the Yb14CdSb11 analog: Where MM is the molar mass of the respective compounds. This adjusted heat capacity was employed to give the total thermal conductivity according to the equation: κ = D × Cp × *d* (D = measured diffusivity; Cp = heat capacity adjusted; *d* = the temperature-adjusted density). The coefficient of thermal expansion (CTE) measured for Yb14MnSb11 was also employed. This procedure is consistent with past practice for compounds with the Yb14MSb11, compared to previously published work.
more »
« less
- Award ID(s):
- 2307231
- PAR ID:
- 10694776
- Publisher / Repository:
- Dryad
- Date Published:
- Edition / Version:
- 7
- Subject(s) / Keyword(s):
- FOS: Chemical sciences FOS: Chemical sciences Heat Capacity Yb13CdSb11 PXRD CdSb PXRD Yb4Sb3 PXRD Yb14CdSb11 Resistivity Yb14CdSb11 Mobility Yb14CdSb11 carrier concentration Yb14CdSb11 Seebeck Yb14CdSb11 Thermal Conductivity Yb14CdSb11 zT Yb14CdSb11
- Format(s):
- Medium: X Size: 123915 bytes
- Size(s):
- 123915 bytes
- Right(s):
- Creative Commons Zero v1.0 Universal
- Sponsoring Org:
- National Science Foundation
More Like this
-
-
Abstract: Zintl compounds with the Ca14AlSb11 structure type (14-1-11) have attracted interest for their excellent thermoelectric properties at high temperatures. However, few bismuth-containing 14-1-11 compounds have been reported and investigated for their thermoelectric properties. A new member of this family, Yb14ZnBi11, has been synthesized as single crystals using the lead-flux method. Single-crystal diffraction confirms that it belongs to the Ca14AlSb11 structure type and that it crystallizes in the tetragonal space group I41/acd (No. 142; Z = 8). Thermoelectric properties were measured on dense pellets of polycrystalline Yb14ZnBi11. It shows a low thermal conductivity of 0.77 W/m K at room temperature and a low electrical resistivity of 0.91 mOhm cm at 367 K. However, a low Seebeck coefficient results in overall low thermoelectric performance. The potential of Yb14ZnBi11 for thermoelectric applications highlights the vast array of unexplored compounds available in this structure type for future research. Methods: Powder X-ray Diffraction Powder X-ray Diffraction (PXRD) data collected at room temperature using a Bruker D8 ECO ADVANCE powder X-ray diffraction (PXRD) diffractometer on zero-background off-axis quartz plates. Cu Kα radiation was used with a step size of 0.02° over the 2θ angles of 20° to 80°. Spark Plasma Sintering After sieving the powder sample through a 100-mesh screen, it was loaded into a 12.7 mm graphite die. Initially, the powder was cold-pressed at 5 kN using a Dr. Sinter Junior Spark Plasma Sintering system (Fuji Electronic Industrial Co., LTD) under Ar gas. The applied force was increased to 9 kN, and the powder was sintered at 900 °C for 30 minutes. The resulting pellets exhibited a density greater than 98 %, measured by the Archimedes' principle. Thermal Transport Properties Thermal diffusivity was measured on the pressed pellets using a Netzsch LFA 475 Microflash under Ar flow. A graphite coating was applied to the pellets’ surface to ensure maximum absorption of the laser. The total thermal conductivity was then calculated using the equation, к = D × Cp × 𝜌. In this equation, D represents the measured thermal diffusivity, Cp denotes the heat capacity, and 𝜌 denotes the material's density. The heat capacity was approximated using the Dulong–Petit law. Seebeck Coefficient and Electrical Resistivity The Linseis LSR-3 instrument was utilized to measure the Seebeck coefficient and electrical resistivity of a bar that was cut from the pellet. For the measurements, Pt/Rh thermocouples were arranged in a four-probe configuration under a static helium atmosphere. Additionally, a polished zirconium ribbon was placed inside the susceptor to serve as an oxygen sponge, thereby protecting the sample’s integrity. TechnicalInfo: # Crystal structure, synthesis, and thermoelectric properties of Yb~14~ZnBi~11~ Dataset DOI: [10.5061/dryad.18931zdc9](https://doi.org/10.5061/dryad.18931zdc9) # Description of the data and file structure The folder entitled Yb14ZnBi11_Data.zip contains 4 *.*csv* files, one for each data set. The data for Yb14ZnBi11 are provided in columns with room temperature powder X-ray diffraction data as two-theta and Intensity (arbitrary unit), electrical resistivity as a function of temperature (300 - 1000 K), Seebeck coefficients as a function of temperature (300-1000 K), and thermal conductivity as a function of temperature (300-1000 K). ## Folder: Yb14ZnSb11.zip Description: Contains 4 *.csv files: * X-ray Diffraction Data * Resistivity_Data * Seebeck_Data * Thermal Conductivity_Data ## Files and variables **File: X-ray Diffraction Data** Room temperature powder X-ray diffraction (PXRD) data for Yb14ZnBi11 are provided in columns A and B, with two-theta/degree (column A) and intensity/arbitrary units (au) (column B) **File: Resistivity_Data** Temperature dependent electrical resistivity data for Yb14ZnBi11 is provided in columns A and B, with temperature/K (column A) and resistivity/mOhm cm (column B) **File: Seebeck_Data** Temperature dependent Seebeck coefficient data for Yb14ZnBi11 is provided in columns A and B, with temperature/K (column A) and Seebeck coefficient/µV/K (column B) **File: Thermal Conductivity_Data** Temperature dependent Thermal conductivity data for Yb14ZnBi11 is provided in columns A and B, with temperature/K (column A) and thermal conductivity/W/m K (column B)more » « less
-
Abstract: Zintl compounds of the Ca14AlSb11 structure type, especially Yb14MSb11 (M = Mg, Mn, Zn), have emerged as leading contenders for high-temperature thermoelectric applications because of their very low thermal conductivity and excellent electronic properties. In comparison, the lighter arsenic-based compounds have received less attention, as they are generally thought to have poor thermoelectric performance due to higher thermal conductivity. In this study, we synthesized 4 compounds, Eu14MAs11 (M = Mg, Zn, Cd) and Eu14Zn1.2As11, and refined their powder diffraction patterns using Rietveld refinement. We measured the transport properties of these compounds to demonstrate that diffuson conduction is common across these compositions, resulting in a lattice thermal conductivity of about 0.55 W m-1 K-1 at 298 K and challenging the usual relationship between mass and lattice thermal conductivity. The combination of low thermal conductivity and high valley degeneracy enables these materials to reach impressive thermoelectric performance, with Eu14MgAs11 achieving a maximum zT of 1.3 at 1250 K. TechnicalInfo: # Data from: Diffuson-driven lattice thermal conductivity in Zintl arsenides: disrupting mass-thermal conductivity relation for high thermoelectric performance Dataset DOI: [10.5061/dryad.37pvmcvzv](https://doi.org/10.5061/dryad.37pvmcvzv) ## Description of the data and file structure Four compounds were synthesized and characterized: Eu~14~MgAs~11~, Eu~14~CdAs~11~, Eu~14~Zn~1.2~As~11~, Eu~14~ZnAs~11~. **Synthesis:** The compounds were synthesized with binary phases, EuA and *M*~2~As~3~ (*M* = Mg, Cd, Zn). For the Eu~14~MgAs~11~ phase, EuH~2~ was also employed to achieve phase pure product. Stoichiometric mixtures were milled in a 650 cm^3^ steel grinding vial with two 12.7 mm balls employing a SPEX mixer-mill. The resulting powder was transferred to a tantalum tube and sealed using an Ar-fille arc welder. The tantalum tube was further sealed in a fused silica tube under vacuum and annealed in a furnace at 1100 °C for 96 h. **Powder X-ray Diffraction (PXRD):** The powder sample was ground with a mortar and pestle and sieved through a 100-mesh screen for X-ray diffraction measurements. The fine powder was taken on a zero background off-axis SiO~2~ plate by using solvent-smearing techniques with ethanol. PXRD experiments were performed using a Bruker D8 ADVANCE ECO instrument at room temperature. Data were collected from 15° to 80° 2θ with a step size of 0.01638° 2θ using Cu K~α1~ and K~α2~ radiations with Ni filter to remove Cu K~b~. **Spark Plasma Sintering:** The finely ground powder was loaded into a 12.7 mm internal diameter graphite die (Cal Nano) with graphite plungers and graphite foils on each side inside an argon atmosphere within the glove box. The die was then inserted into a spark plasma sintering device (Dr. Lab Sinter Jr., Fuji Corp.) for pressing under a 50% Air/Ar environment. The powder was heated to 850 °C over 10 minutes, with the applied force increasing from 6 to 10.5 kN during this period. It was then sintered to 900 °C in 1 minute and held at this temperature for 30 minutes to consolidate the sample. The resulting pellets achieved densities greater than 98% of the theoretical density, as measured by the Archimedes method. **Resistivity Measurements:** Resistivity measurements were conducted on densified pellets with a diameter of 12.7 mm at the Jet Propulsion Laboratory (JPL) using a Van der Pauw method. Resistivity was converting into conductivity for the data analysis. **Seebeck Coefficient Measurements:** The Seebeck coefficient was measured at the Jet Propulsion Laboratory (JPL) using a custom-built apparatus generating light pulses via the light-pipe methods with tungsten-niobium thermocouples under high vacuum. **Thermal Conductivity Measurements:** The thermal diffusivity of the pressed pellet was measured from 298 K to 1272 K using a Netzsch LFA-457 unit. The dense pellet was polished to achieve a uniform, consistent thickness. It was coated with graphite to ensure high emissivity of the laser flash. The total thermal conductivity, k, was calculated from the equation k = DC~p~*d*, where D is the measured diffusivity; C~p~ is the heat capacity; *d* is the room temperature density obtained from the Archimedes method. Heat capacity was estimated using the Dulong−Petit law. **Carrier Concentration and Hall Mobility:** Hall coefficient measurements were conducted on densified pellets with a diameter of 12.7 mm at the Jet Propulsion Laboratory (JPL) using a Van der Pauw method with a applied magnetic field of 1.0 T and a current of 100 mA. ### Files and variables #### File: Data.zip **File Description:** The file contains 4 data sets corresponding to the 4 compositions measured, saved as both *.xlsx and *.csv files. The files are named according to the composition: Eu~14~MgAs~11~, Eu~14~CdAs~11~, Eu~14~ZnAs~11~, and Eu~14~Zn~1.2~As~11~ **Data Description:** Each file contains PXRD (2-theta (°), intensity (arbitrary units)); Conductivity vs T (Temperature (K), Conductivity (S cm ^-1^); Seebeck vs T (Temperature (K), Seebeck Coefficient (µV/K)); Carrier Concentration vs T (Temperature (K), Carrier Concentration (h+ , cm ^-3^)), and Hall Mobility vs T (Temperature (K), Hall Mobility (cm^2^ V ^-1^ s ^-1^).more » « less
-
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.more » « less
-
Abstract: Eu5.08Al3Sb6 can be described as a pseudo rock salt-like “(Eu/Al4)Sb” structure. The polycrystalline synthesis of Eu5+xAl3+ySb6 was optimized. The compositions exhibit n-type transport behavior, ultra-low thermal conductivity, and a high Seebeck coefficient. The Eu5.08Al4Sb6 shows a promising zT of 0.8 at a temperature of 873 K. TechnicalInfo: # Optimization of the composition Eu5+xAl3+ySb6 and thermoelectric figure of merit [https://doi.org/10.5061/dryad.1zcrjdg3q](https://doi.org/10.5061/dryad.1zcrjdg3q) ## Description of the data and file structure The data sets are: (1) powder x-ray diffraction (PXRD): PXRD_ChemComm.zip, thermal gravimetric (TG)- Differential scanning calorimetry (DSC): TGDSC_ChemComm.zip and transport data: TransportData_ChemComm.zip **Powder X-ray Diffraction (PXRD):** PXRD_ChemComm.zip PXRD data were collected with a Bruker D8 Advance Eco Diffractometer using Cu Kα radiation from 2θ = 20° —80° with a step size of 0.02 ˚ and scan rate of 1 s/step at room temperature in air. The polycrystalline samples were ground inside an Ar-filled glove box and plated on a zero-background holder with isopropanol. **Thermogravimetric (TG)/Differential Scanning Calorimetry (DSC):** TGDSC_ChemComm.zip Melting point studies of aluminum excess were done on polished pellet pieces of Eu5+*x*Al3+*y*Sb6 using TG/DSC (STA 449 F3 Jupiter, Netzsch) from room temperature up to 800°C with a heating rate of 10K/min under a 50 mL/min flow of Ar. A piece of Aluminum metal (Aluminum shot, approx. 4-8mm (0.2-0.3in), Puratronic™, 99.999% (metals basis)) was used as a reference. **Thermal Conductivity:** TransportData_ChemComm.zip Thermal Diffusivity (*D) was measured on thin (1.19 to 1.2 mm thick) slices of Eu5+*x*Al3+*y*Sb6 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 from the equation: κ = *D* x ρ X Cp. All the pellets’ density (ρ) was measured multiple times using the Archimedes method using toluene as the liquid. All samples were > 95% of their theoretical crystallographic densities, calculated using the Arrhenius method. **Transport Measurements:** TransportData_ChemComm.zip A Linseis LSR-3 instrument was used to measure resistivity and Seebeck coefficient employing the four-probe method from 350K to 800K under He atmosphere. The sample geometries were bar-shaped ( 10.5mm x 4mm x 2mm) using 8 mm probes and polished before measurements. Multiple samples were measured to ensure reproducibility, and the data was cross-checked using measurements at JPL and Northwestern. The Seebeck coefficient was measured using a light pulse technique as described above using W/Nb thermocouples. Electrical resistivity (ρ) was measured using the van der Pauw (VDP) technique with a current of 10 mA. Electrical resistivity and Hall effect data were measured using a home-built Hall effect instrument for the samples measured at Northwestern.1 This set-up utilizes a four-point Van der Pauw resistivity measurement with molybdenum leads and a current of 100 mA. Seebeck coefficient data was collected using a home-built two-probe Seebeck instrument with chromel/Nb thermocouples. ### Files and variables #### File: PXRD_ChemComm.zip **Description:** Powder X-ray diffraction data files, collected according to the description provided above. **Variables:** x, y where x = two-theta (˚) and y = X-ray diffraction Intensity (arbitrary units) **Files:** Eu5_08Al3_3Sb6.xy = sample composition Eu5.08Al3.3Sb6 Eu5_08Al4Sb6.xy = sample composition Eu4.08Al4Sb6 Eu5Al3_3Sb6.xy = sample composiiton Eu5Al3.3Sb6 Eu5Al3Sb6.xy = sample composition, Eu5Al3Sb6 Eu5Al4Sb6.xy = sample composition Eu5Al4Sb6 #### File: TGDSC_ChemComm.zip **Description:** Thermogravimetric and differential scanning calorimetry data collected according to the description provided above. **Variables:** Temperature/˚C; Time/min; DSC/(mW/mg); Mass/%; Gas Flow (purge2)/(ml/min); Gas Flow(protective)/(ml/min); Sensit./(uV/mW) **Files:** ExpDat_Aluminum_shot_800C_1.csv = (segment 1) experimental data for aluminum shot taken from 20 ˚C to 800 ˚C. ExpDat_Aluminum_shot_800C_2.csv = (segment 2) experimental data for aluminum shot taken from 800 ˚C to 20˚C. ExpDat_Eu5_08Al3_3Sb6_800C_1.csv = (segment 1) experimental data for sample composition Eu5.08Al3.3Sb6 taken from 20 ˚C to 800 ˚C. ExpDat_Eu5_08Al3_3Sb6_800C_2.csv = (segment 2) experimental data for sample composition Eu5.08Al3.3Sb6 taken from 800 ˚C to 20˚C. ExpDat_Eu5_08Al4Sb6_800C_1.csv = (segment 1) experimental data for sample composition Eu5.08Al4Sb6 taken from 20 ˚C to 800 ˚C. ExpDat_Eu5_08Al4Sb6_800C-2.csv = (segment 2) experimental data for sample composition Eu5.08Al4Sb6 taken from 800 ˚C to 20˚C. ExpDat_Eu5Al3_3Sb6_800C_1.csv = (segment 1) experimental data for sample composition Eu5Al3.3Sb6 taken from 20 ˚C to 800 ˚C. ExpDat_Eu5Al3_3Sb6_800C_2.csv = (segment 2) experimental data for sample composition Eu5Al3.3Sb6 taken from 800 ˚C to 20 ˚C. ExpDat_Eu5Al4Sb6_800C_1.csv = (segment 1) experimental data for sample composition Eu5Al4Sb6 taken from 20 ˚C to 800 ˚C. ExpDat_Eu5Al4Sb6_800C_2.csv = (segment 2) experimental data for sample composition Eu5Al4Sb6 taken from 800 ˚C to 20 ˚C. #### File: TransportData_ChemComm.zip **Description:** Hall data and Seebeck data files containing Temperature dependent Hall resistivity, mobility, resistivity, Seebeck. *Variables for Hall Data:* Sample thickness in mm; Temperature/(˚C) ; Temperature/(K); Resistivity/(mohm.cm); Conductivity/(S/cm); Carrier Concentration/(/cm3); Hall Mobility/ (cm2/Vs); Hall Resistivity = R_H/(cm3/C); temperature for resistance = T_Res/(˚C); temperature for Hall data collection = T_Hall/(˚C); Resistance Standard deviation = Res*_*Std/(%); Hall resistance standard deviation = RH*_*Std/(%); Hall mobility standard deviation = muH Std/(%); Applied magnetic field = B field/(Gauss); applied current for resistivity = I_Res/(mA); van der Pauw ration = vdP ratio; resistivity time = Res. Time= time and date for the measurement; Hall time = Hall. Time = time and date for the Hall measurement; lead resistance for the 4 leads = Lead Res. 1, Lead Res. 2, Lead Res. 3, and Lead Res. 4 in Ohm; Probe to ground resistance = Probe-GND REsistance/(Ohm); thermocouple 1 = TC1/(˚C) was not used; thermocouple 2 = TC2/(˚C) was not used. **Variables for Seebeck Data**: Temperature = T/(˚C); Seebeck coefficient = seebfit/(uV/K) **Files:** Eu5_08Al3_3Sb6_HallData.csv = Hall data for sample composition Eu5.08Al3.3Sb6 taken from 20 ˚C to 550 ˚C. Eu5_08Al4Sb6_HallData.csv = Hall data for sample composition Eu5.08Al4Sb6 taken from 20˚C to 550 ˚C. Eu5Al3_3Sb6_HallData.csv = Hall data for sample composition Eu5Al3.3Sb6 taken from 20˚C to 550 ˚C. Eu5Al4Sb6_HallData.csv= Hall data for sample composition Eu5Al4Sb6 taken from 20˚C to 550˚C. Eu5_08Al3_3Sb6_Seebeck.csv = Seebeck data for sample composition Eu5.08Al3.3Sb6 taken from 50 ˚C to 600 ˚C. Eu5_08Al4Sb6_Seebeck.csv = Seebeck data for sample composition Eu5.08Al5Sb6 taken from 50 ˚C to 600 ˚C. Eu5Al3_3Sb6_Seebeck.csv = Seebeck data for sample composition Eu5Al3.3Sb6 taken from 50˚C to 600 ˚C. Eu5Al4Sb6_Seebeck.csv = Seebeck data for sample composition Eu5Al4Sb6 taken from 50˚C to 600 ˚C. **ThermalConductivity Folder:** thermal diffusivity data of all samples; conversion to thermal conductivity data provided in LJGEu5Al3Sb6*_*TD_TC.xlsx file. **Variables:** Sample thickness = #Thickness_RT/(mm); sample diameter = #Diameter/(mm); argon gas flow = #Gas flow/(ml/min); shot number; data collection time = #Time/(min); temperature = #Temperature/(˚C); diffusivity data = #Diffusivity/(mm^2/s); standard deviation based on 3 shots = #Std_Dev/(mm^2/s) Files: Eu5_08Al3_3Sb6TD.csv = thermal diffusivity data for sample composition Eu5.08Al3.3Sb6 taken from 10 ˚C to 550 ˚C. Eu5_08Al4Sb6_TD.csv = thermal diffusivity data for sample composition Eu5.08Al4Sb6 taken from 10 ˚C to 550 ˚C. Eu5Al3_3Sb6_TD.csv = thermal diffusivity data for sample composition Eu5.08Al3.3Sb6 taken from 10 ˚C to 550 ˚C. Eu5Al4Sb6_TD.csv = thermal diffusivity data for sample composition Eu5Al4Sb6 taken from 10 ˚C to 550 ˚C. LJGEu5Al3Sb6_TD_TC.xlsx = Data file providing the conversion of all compositions from thermal diffusivity data to thermal conductivity values. All compositions indicated with headers with temperature = T/(˚C); temperature = T/(K); diffusivity (mm2/s); density /(gm/cm3); Heat Capacity/ ; Thermal Conductivity/(W/mK); Thermal Conductivity/(mW/cmK);more » « less
An official website of the United States government
