natural power electricity without relying on fossil fuels, and thus a fierce development race is going on to make "clean hydrogen" economically and technologically viable. Advent of hydrogen economy, however, cannot be realized until technical issues related to hydrogen production, transportation, and a storage infrastructure are clear. Ammonia is a highly efficient hydrogen carrier since it can be easily liquefied to store and transport at room temperature, is widely available, is carbon-free, and has hydrogen capacity larger than the liquid hydrogen. [1][2][3][4] Hence, it is strongly motivated to utilize ammonia in fuel cells for the direct conversion of ammonia chemical energy to electricity in a high efficiency. The proton conducting ceramic fuel cells (PCFCs) using protonconducting oxide electrolytes, such as BaZr x Ce 0.8−x Y 0.2 O 3−δ, is promising as a direct ammonia type fuel cell operating at the intermediate temperature (IT) range (400-600 °C) for stationary applications. [4][5][6][7][8][9] Because water formation in PCFCs is mainly progressive at the cathode side, unlike solid oxide fuel cells (SOFCs), and therefore, mixing of the ammonia fuels into the exhaust water is precluded, thereby eliminating repurification of water exhaust and simplifying total systems. Moreover, formation of environmentally hazardous substances NO x at the anode is discouraged if the proton conductivity is much higher than the minor oxide ion conductivity.Although the resistivity and related activation energy of proton conductors are smaller than oxide ion conductors used in SOFCs, the performances of the current PCFCs, however, are far behind the SOFCs even with pure H 2 fuels because of large interfacial polarization due to a lack of suitable cathode [10][11][12][13][14] and the deteriorated microstructural electrolyte. [15][16][17][18] Meanwhile, exceptionally high power output has been reported in the IT range for hydrogen membrane fuel cell (HMFC), [19][20][21][22][23] which comprises a thin proton conducting ceramic electrolyte supported on a dense hydrogen permeable metal anode with the anode reactions driven by separation of the monoatomic hydrogen dissolves into protons and electrons at electrolyte/ nonporous-anode solid-solid interfaces (Figure 1a). Regardless of its simple cell structure, the HMFC based on BaCe 0.8 Y 0.2 O 3 (BCY) thin film and Pd foil has achieved the maximum power density of 1.4 W cm −2 at 600 °C, [19,20] which is still higher than the average performances of recently reported highly efficiency PCFCs at the temperatures. [24][25][26][27] Here, we report on the highly