. 2023 Sep 6;15(38):45212–45228. doi: 10.1021/acsami.3c07476

Table 3. Comparison of Short-Circuit Current Density (J_sc) from J–V Curves and EQE Measurements and Hole Mobility (μ_h) of the Hole Transport Layers (HTLs) with and without Carbon Nanomaterials (CNMs).

HTL	J_sc (mA cm^–2)^a	J_sc (mA cm^–2)^b	μ_h (10^–3 cm² V^–1 s^–1)^c
w/o CNMs	20.5	20.4	4.10
CNHs-Cz	21.5	21.2	6.91
CNHs-TPA	22.0	22.1	7.32
SWCNTs-Cz	21.1	20.9	7.07
SWCNTs-TPA	21.9	21.8	7.69
DWCNTs-Cz	20.8	20.7	6.39
DWCNTs-TPA	21.9	21.7	7.22

From the J–V curves.

From EQE measurements.

From SCLC method.

Table 3. Comparison of Short-Circuit Current Density (Jsc) from J–V Curves and EQE Measurements and Hole Mobility (μh) of the Hole Transport Layers (HTLs) with and without Carbon Nanomaterials (CNMs).