coefficient, σ represents electrical conductivity, T represents working temperature in Kelvin, κ ele denotes electronic thermal conductivity, and κ lat denotes lattice thermal conductivity. [4,5] Extensive efforts are devoted to decoupling these correlative parameters. [6] Electrically, the strategies of band convergence, [2] band alignment, [4,7] densityof-states (DOS) distortion, [8,9] modulation doping, [10] enhancing the symmetry of crystal [11] and quantum confinement [12] are successfully established to equilibrate the Seebeck coefficient (S) and the electrical conductivity (σ) in favor of a superior power factor (PF). [13] It is well known that the enhanced band degeneracy due to band convergence could increase the effective mass a bit without degrading the carrier mobility. And DOS distortion, which improves the band effective mass, is a feasible strategy with risks for deteriorating the carrier mobility. [14] It is clear that the optimal balance between the effective mass and the carrier mobility is beneficial for the electrical performance of TE materials. This relationship primarily depends on the weighted mobility, µW = μ H (m * /m e ) 3/2 , where μ H represents the carrier mobility, m * represents the DOS effective mass, and m e represents the unit electron mass.Thermally, intensifying the phonon scattering is considered to be an effective method to decrease the thermal conductivity (κ lat ), which is generally classified into incorporating extra phonon scattering centers [15] and seeking inherent low lattice thermal conductivity materials. [16,17] The latter representing materials might have a complex crystal structure, [1] heavy constituent elements, [18] intense lattice anharmonicity, [19] and soft chemical bonding. [20] And the extra phonon scattering sources include point defects, nanoprecipitates, grain boundaries, and so on. [21] To date, state-of-the-art TE materials, including Zintl phase, [22] half-Heusler, [23] skutterudite, [24] SiGe, [25] chalcogenides, [8,26] and Bi 2 Te 3 -based compounds, [27] etc., exhibit prominent thermoelectric performance.GeTe is proven to be an eminent mid-temperature thermoelectric material. [28,29] The well-recognized characters of GeTe are multiple valance bands, phase transition, ultrahigh carrier concentration, and high thermal conductivity, which diversify the degrees of freedom to tailor its TE performance. [30][31][32] Counter-doping using aliovalent elements, such as Bi, Sb, and In, [33,34] is a common method to achieve the optimal carrier Thermoelectric materials can achieve the direct conversion between electricity and heat, which has drawn extensive attention in recent decades. Understanding the chemical nature of band structure and microstructure is essential to boost the thermoelectric performance of given materials. Herein, CdSe alloying promotes the evolution of multiple valence bands in GeTe, resulting in the contemporaneous appearance of band convergence and density of state distortion, which benefits the sharply enhanced effective mass from ...