cells, [1][2][3][4] but also other types based on small molecule:fullerene [5,6] blends as well as solar cells incorporating singlewalled carbon nanotubes (SWCNTs) [7][8][9][10][11][12][13][14] were investigated with increased efforts. All of these new concepts have been introduced to tackle several drawbacks and outstanding issues related to polymer:fullerene solar cells. [15] Concepts such as small molecule:fullerene active layers aim to use simple, well-defined molecules instead of polymers, which always exhibit a distribution in chain length altering their properties. The application of nonfullerene acceptors allows for more freedom to align the energy levels at the donor-acceptor interface. The incorporation of SWCNTs in OSCs or other organic devices [16][17][18][19] (near-infrared (nIR) detectors, nIR lightemitting diodes (LEDs), and field-effect transistors (FETs)) is based on several advantageous key factors that allow to boost device performances. First, SWCNTs have shown to exhibit a high photochemical stability making them superior to conventional polymers. Second, SWCNTs exhibit a very high charge carrier mobility outperforming conventional organic materials by orders of magnitude. [20,21] The high absorption coefficients in the nIR wavelength regime [22,23] make SWCNTs well suited to IR-sensitive OSCs via a ternary concept or in a binary blend with SWCNTs as the main absorber in the IR region.Previously it was shown that SWCNTs work in a type-II heterojunction scheme acting either as an electron acceptor in combination with a polymer or as the electron donor in combination with C 60 or [6,6]-phenyl-C 61 -butyric acid methyl ester (PCBM). [24] Concerning the combination with C 60 , it was already demonstrated that charge carrier generation and harvesting is highly efficient with internal quantum efficiencies (IQEs) in the range of 85%. [25] The use of nearly monochiral SWCNTs in a bilayer architecture with C 60 facilitated high fill factors (FFs) greater than 60% and a high peak external quantum efficiency (EQE) of 43% at 1050 nm. Employing a bulk heterojunction (BHJ) architecture in combination with multichirality SWCNTs achieved a broad absorption in the nIR with power conversion efficiencies (PCEs) surpassing 3% for all-carbon allotrope absorbers. [24,26] In a recent study performed by Shea et al. [27] on nearly single-chirality (6,5) Current state-of-the-art organic solar cells (OSCs) still suffer from high losses of open-circuit voltage (V OC ). Conventional polymer:fullerene solar cells usually exhibit bandgap to V OC losses greater than 0.8 V. Here a detailed investigation of V OC is presented for solution-processed OSCs based on (6,5) single-walled carbon nanotube (SWCNT): [6,6]-phenyl-C 71 -butyric acid methyl ester active layers. Considering the very small optical bandgap of only 1.22 eV of (6,5) SWCNTs, a high V OC of 0.59 V leading to a low E gap /q − V OC = 0.63 V loss is observed. The low voltage losses are partly due to the lack of a measurable charge transfer state and partly due to th...