To gain insight into the peculiar temperature dependence of the thermoelectric material SnSe, we employ many-body perturbation theory and explore the influence of the electron-phonon interaction on its electronic and transport properties. We show that a lattice dynamics characterized by soft highly-polar phonons induces a large thermal enhancement of the Fröhlich interaction. We account for these phenomena in ab-initio calculations of the photoemission spectrum and electrical conductivity at finite temperature, unraveling the mechanisms behind recent experimental data. Our results reveal a complex interplay between lattice thermal expansion and Fröhlich coupling, providing a new rationale for the in-silico prediction of transport coefficients of high-performance thermoelectrics.The discovery of the record-breaking thermoelectric properties of SnSe has laid a new milestone in the quest for high-efficiency thermoelectric materials [1]. SnSe combines large carrier conductivity σ and Seebeck coefficient S, with highly anharmonic lattice dynamics [2-4]. Anharmonic effects limit the lattice thermal conductivity κ via phonon-phonon scattering, thus contributing to a record-high figure of merit ZT = (S 2 σ/κ)T ∼ 2.6, which may be even further improved through doping and alloying [5][6][7][8].As the operational conditions of thermoelectric devices typically involve large temperatures, a quantummechanical description of the electronic and lattice properties of SnSe across the temperature domain of its thermodynamical stability is key to unravel the microscopic origin of this outstanding thermoelectric performance. Recent experimental investigations have unveiled a pervasive influence of temperature on the electronic and transport properties of SnSe. Angle-resolved photoemission spectroscopy experiments, for instance, have reported (i) a pronounced dependence of the peak linewidth on the sample temperature [9], (ii) the emergence at low temperature of a gap between the first two occupied bands at the Z point, [10][11][12][13], and (iii) a non-monotonic effective-mass renormalization as a function of temperature [14]. Density-functional theory calculations fail at unraveling the origin of these phenomena. Additionally, theoretical predictions based on the Boltzmann formalism indicate an increase of the electrical conductivity with temperature -arising from the thermal excitation of carriers across the Fermi surface -which is in stark contrast with experimental observations, where a pronounced reduction of charge conduction with increasing temperature has been observed [5].These findings seem to suggest a strong interplay between electronic and ionic degrees of freedom. While recent theoretical works have thus far provided a comprehensive investigation, based on first-principles calculations, of quasiparticle bands [15], defect formation energies [16], crystal-lattice dynamics [17], lattice anharmonicities [4], electron-phonon interaction [18], and transport properties [15,19,20], unraveling the origin of the peculiar tempera...