I. Introduction
Thermionic energy converters (TECs) [1], [2] are a class of devices that can conveniently convert the heat energy at relatively high temperatures [3]–[5] into electricity and have attracted considerable attention [6]–[9]. For instance, Wang et al. [10] proposed the model of the vacuum thermionic generator including internal and external irreversible heat losses and gave the optimum design criteria of the device. Gil et al. [11] presented an analytical expression for the current density across an isotype heterojunction valid for arbitrary doping concentration ratios and generalized the standard expression. Choi et al. [12] achieved a micrometer-sized thermionic electron emission source with the maximum current density of 1.2 A/cm2 with full crystallization of the LaB6. Datas [13] established a hybrid thermionic-photovoltaic converter through the combination of the thermionic and photovoltaic energy conversion and offered an alternative approach for thermal energy harvesting. Contrasted with other types of energy conversion devices, TECs have some significant advantages such as the relative simplicity of design and operation [1], high-power density [2], and without mechanically moving parts [10]. The energy conversion efficiency of a TEC is closely dependent on the materials of the cathode working at higher temperatures and the space charge effect [14]–[16]. Besides conventional metals or semiconductors as the cathode, which new materials can be used as the cathode material to more effectively implement thermionic emission? This is a new worthy issue to be investigated [17]–[20].