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Kumar et al. Energy Mater. 2025, 5, 500109  https://dx.doi.org/10.20517/energymater.2025.22  Page 3 of 17

               Recent advances in TE performance using the HEA concept have been introduced, including the n-type
                                                                                       [21]
               PbSe-based high-entropy material (Pb Sb 0.012 Sn Se Te S , ZT = 1.8 at 900 K) , p-type PbSe-based
                                                                 0.25 0.25
                                                             0.5
                                                 0.89
                                                         0.1
               high-entropy material (Pb Na 0.025 Cd Se S Te , ZT = 2.0 at 900 K) , and p-type GeTe based
                                                                                 [22]
                                                      0.5 0.25
                                       0.935
                                                  0.04
                                                             0.25
               high-entropy material (Ge Ag Sb Pb Bi Te, ZT = 2.7 at 750 K)  On the other hand, the HEA
                                                                             [23]
                                               0.13
                                          0.11
                                                       0.01
                                                   0.12
                                      0.61
               concept has not yet been successful in improving the TE performance of bismuth tellurides for
                                         [17]
               room-temperature applications .
               Here we investigated the anisotropic thermoelectric properties of the composites consisting of p-type
               bismuth antimony telluride (BST: Te-excess Bi Sb Te ) and heavy metallic HEA nanoparticles (HEA:
                                                         0.4
                                                                3
                                                            1.6
               TaNb HfZrTi). Since the Te-excess effectively enhances the TE performance of the p-type bismuth
                    2
               antimony telluride [9,11] , the composition of the Bi Sb Te  with additional Te was used for the BST matrix.
                                                                3
                                                            1.6
                                                         0.4
               The TaNb HfZrTi is one of the representative HEAs with a body-centered cubic (BCC) phase and high
                        2
               mechanical strength . To minimize a chemical doping effect, which can decrease the ZT value by deviating
                                [24]
               from the optimized carrier concentration, a mixed powder with the BST and HEA was used in the hot-press
               sintering process. The carrier concentrations, Seebeck coefficients (S), and Fermi energies (E ) of
                                                                                                      F
               theBST+HEA  (x = 0, 0.1, 0.5, 1.0 vol%) samples are not significantly affected by the addition of HEA. On
                           x
               the other hand, the significantly enhanced electrical conductivity σ and reduced κ  are observed in the x =
                                                                                     L
               0.1 vol% sample for the parallel (Pa) direction to the hot-press direction. The enhanced Pa-direction σ and
               the decrease of κ  of theBST+HEA  samples are mainly affected by the enlarged carrier mean free paths λ e
                                            x
                              L
               and decrease of phonon mean free path λ , which is a realization of PGEC . The increased λ  can be
                                                                                  [15]
                                                    ph
                                                                                                   e
               explained by the improved grain connectivity due to the HEA nanoparticles for the Pa-direction of the BST
               grains. Grain connectivity, which refers to the interconnection between grains, has a significant impact on
               transport characteristics [25-29] . The increased λ  in theBST+HEA  samples further supports that the HEA
                                                                      x
                                                      ph
               nanoparticles can improve the grain connectivity of the BST grains. As a result, the ZT values of
               theBST+HEA  samples are enhanced from 1.09 (x = 0) to 1.33 (x = 0.1 vol%) at 350 K in the Pa-direction
                           x
               due to the improved σ and reduced κ  These results clearly show that incorporating HEA nanoparticles is a
                                               L.
               promising strategy for improving the performance of the anisotropic thermoelectric materials. Additionally,
               controlling of the grain connectivity could be a good concept to improve the transport characteristics in
                                                   [30]
               various materials such as superconductors , batteries [31,32] , solar cells [33,34] , and semiconductors [35,36] .
               EXPERIMENTAL
               Materials
               The polycrystalline Te-excess BST samples were synthesized using the conventional melting method. The
               stoichiometric amounts of Bi (99.999%), Sb (99.999%), and Te (99.999%) were sealed in evacuated quartz
                                                                    [9]
               tubes under high vacuum with the excess tellurium (~7 W%) . The elements in the quartz ampule were
               melted at 923 K for 24 h and then water-quenched. The obtained ingots were pulverized into the powder
               using an agate mortar and pestle under an argon atmosphere. The TaNb HfZrTi HEA powders were
                                                                                 2
               synthesized by the planetary ball milling method using powder elements. The stoichiometric ratios of Ta
               (99.98%), Nb (99.8%), Hf (99.6%), Zr (99.5%), and Ti (99.5%) powders were loaded into a stainless-steel jar
               with stainless-steel balls under an argon atmosphere. The ball milling process was carried out at a rotation
                                     [24]
               speed of 400 rpm for 12 h .
               The obtained BST and HEA (0, 0.1, 0.5 and 1.0 vol%) powders were mixed using a physical multimixer in
               vibration mode for 24 h. The mixed powders were loaded into a graphite die with an inner diameter of
               15 mm and sintered using the hot-press method at 763 K under uniaxial pressure of 50 MPa for 60 min. The
               relative densities of the sintered samples were above 95% compared to the calculated densities.
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