from over 11% [1,2] and 12% [3] up to over 13% now [4] in either tandem or single junction solar cells from benzo [1,2-b:4,5-b′] dithiophene (BDT)-based polymers as the donor material in photovoltaic (PV) devices, their limiting open-circuit voltage (V oc , below 1.00 V) is still one of the key obstacles to achieve ideally high PV performance with minimized trade-off on another characteristic features of the OPV devices, i.e., the short-circuit current density (J sc ). For the first two single junction polymer solar cells (PSCs) with PBDB-T/3,9-bis(2-methylene-(3-(1,1-dicyanomethylene)-indanone))-5,5,11,11-tetrakis(4-hexylphenyl)-dithieno[2,3-d:2′,3′-d′]-s-indaceno[1,2-b:5,6-b′]dithiophene (ITIC) and PBDT-T/IT-M as active layer materials, respectively, their photon energy loss (defined as E Loss = E g − eV oc , [5,6] whereas E g refers to the band gap energy difference between the energy level of highest occupied molecular orbital (HOMO) and lowest unoccupied mole cular orbital (LUMO)) has been pronounced as 0.66 and 0.69 eV, respectively, which is still above the empirically optimized level of 0.60 eV. [7] Despite their breaking PCE values, these nonideally low E Loss still reflect the imperfect molecular design of the PBDB-T backbone structure for ideal control on their HOMO/LUMO levels.