the nanocarbon itself. In fact, it is known that the electrical properties of CNTs [ 23,24 ] and graphene [ 25 ] are strongly infl uenced by light, hence this inherent behavior of the nanocarbons needs to be considered for TPM on nanocarbon-based hybrids and composites.The photoresponse of CNTs has generated considerable debate during the last few decades and only recently its bolometric nature has been experimentally confi rmed. [ 26 ] The theory implies that light illumination of CNTs creates excitons with unusually high binding energies, [ 27 ] which cannot directly contribute to the photoconductivity. In this scenario, they have to dissociate thermally, therefore locally heating up the nanocarbon matrix. The increase in temperature leads to an increase in conductivity of the CNTs (in contrast to 3D metals, as explained by the Luttinger liquid model for 1D conductors. [ 28,29 ] ) and results in additional photocurrent.This knowledge, however, has not yet been implemented into practice and standard photocurrent measurements on nanocarbon hybrids and composites are still conducted without considering the photoresponse of bare CNTs. Here we report a new technique, which we describe as dual excitation transient photocurrent measurement (DETPM). This technique allows for distinguishing the bolometric effect (i.e., intrinsic conductivity change due to heat produced by light irradiation) from a potential photoexcited charge transfer in CNTs-based hybrids. We have tested this technique on two high-performance hybrids, CNT-TiO 2 and CNT-Ta 2 O 5 , and explicitly demonstrate the presence of the charge transfer from the semiconductor to the nanocarbon in both the cases.We synthesized the CNT-Ta 2 O 5 hybrid via a modifi ed sol-gel process and the CNT-TiO 2 hybrid via atomic layer deposition process (details of synthesis are in the Experimental Section and characterization in ESI). We aimed to create hybrids with a high degree of conformal coating and an extended interface between the CNTs and the metal oxide to maximize the interfacial charge transfer. SEM images of both hybrids in Figure S1 (Supporting Information) confi rm the presence of uniform coating on the nanocarbon surface and demonstrate homogeneity of the samples. As further revealed by high-resolution transmission electron microscopy (HRTEM) in Figure 1 b,c a tight interface between the two components was established in both the cases. Importantly, all samples used for the TPM were prepared in the form of free-standing macroscopic membranes to eliminate any substrate contribution. In a typical DETPM experiment, a macroscopic membrane, containing either pure CNTs (i.e., reference) or the CNT-based hybrids, was connected to two electrodes as shown in Figure 2 a and a small bias was applied to establish a constant current.