heterojunction (BHJ)-based OSCs with fullerene derivatives acceptors have reached over 11%, [9,10] and nonfullerene-acceptorbased OSC devices even have achieved PCEs over 14%. [11][12][13][14] However, the current photovoltaics performance of OSCs is still in demand to be further improved when compared with other photo voltaic technologies. [15][16][17][18] Single junction OSCs normally suffer from the limited sunlight absorptions and the thermalization loss of photon energy. The tandem concept with stacking two or more subcells in series or parallel connection could address the above issues. [19][20][21][22][23][24][25] For the widely studied series-connected tandem cells, the overall open circuit voltage (V oc ) of the tandem cell is the sum of the V oc values of the subcells if no potential losses in the interconnection layer. [24,25] The current density (J sc ) is generally limited by the subcell with the smallest one. [20,25] In order to pursue high PCEs for the series-connected tandem cell, there are several important factors should be considered synergistically. First, the subcells should have complementary absorptions and well balanced, and high J sc . Second, the two subcells should have minimal energy loss to retain high V oc and thus guarantee the whole high V oc for the tandem devices. Third, the interconnection layer should attain efficient charge extraction and much reduced recombination.In the past decade, great efforts have focused on searching for subcells with efficient light absorptions in a wide range with complementary absorption spectra and minimal absorption overlap. [26][27][28][29][30][31][32] For the fullerene derivatives based devices, it is expected to obtain a well-balanced J sc through appropriate selection of donor materials with different bandgaps since fullerene derivatives have limited absorptions and their contribution on J sc is much smaller than that of the donor materials. To date, PCEs ≈13% have been achieved for the fullenerebased tandem OSCs. [33] The reasons exist in two aspects for the likely ceiling efficiencies of fullerene derivatives based tandem OSCs. [28] The first one is the lack of suitable donor materials, especially narrow bandgap donors utilized for rear cells to achieve the high and balanced J sc for tandem cells. The second one is the general large energy loss of the fullerene The tandem structure is an efficient way to simultaneously tackle absorption and thermalization losses of the single junction solar cells. In this work, a high-performance tandem organic solar cell (OSC) using two subcells with the same donor poly[(2,6-(4,8-bis(5-(2-ethylhexyl)thiophen-2-yl)-benzo[1,2-b:4,5-b′] dithiophene))-alt-(5,5-(1′,3′-di-2-thienyl-5′,7′-bis(2-ethylhexyl)benzo[1′,2′c:4′,5′-c′]dithiophene-4,8-dione))] (PBDB-T) and two acceptors, F-M and 2,9-bis(2-methylene-(3(1,1-dicyanomethylene)benz[f ]indanone))7,12-dihydro-(4,4,10,10-tetrakis(4-hexylphenyl)-5,11-diocthylthieno[3′,2′:4,5]cyclopenta[1,2-b] thieno[2″,3″:3′,4′]cyclopenta[1′,2′:4,5]thieno[2,3-f ][1]benzothiophene (N...