INTRODUCTION Controlled assembly of nanoparticles (NPs) within a polymer matrix can create novel nanostructured materials with enhanced properties. [1][2][3][4] This is of particular interest in the case of anisotropically shaped nanorods (NRs), because the collective electrical and optical properties of their organizations depend strongly on both their aspect ratio (AR) and directional assembly.5-11 Self-assembly of block copolymers (BCPs) can direct the position of the NRs, their orientation, and three-dimensional assembly. [12][13][14][15][16] Despite their interesting and attractive properties, much fewer studies on the morphological behavior of BCP/NR assembly have been conducted when compared with BCP/NP system. 6,[17][18][19][20][21][22] The influence of the AR values of the NRs on their positioning in the BCP domain and on their morphological behavior has been theoretically simulated; [23][24][25] however, it is still an open question experimentally. Although the assembly of NPs in BCP domains can be relatively well understood by the interplay of entropy loss of the chains to accommodate the NPs and enthalpic interactions between the NPs and BCPs, 26,27 other factors including the anisotropic geometry, rotational freedom, and NR-NR interactions should be considered for the NR positioning within the BCP domains.The self-assembly of BCPs confined in a three-dimensional emulsion particle can produce novel structured materials that are not available in bulk. 28,29 Their morphological behavior is strongly dependent on the interfacial interactions between the BCP emulsions and the surrounding media. [30][31][32] Therefore, the effect of NR location on the morphological transition of BCP domains can be systematically investigated if the NRs are used as surfactants, and thus involved in tuning the interfacial properties of the BCP particles. In particular, the role of the NP surfactants should be emphasized in affecting the morphology of the BCP particles because the interfacial interactions are greatly amplified by the high surface area of the particles. Recently, controlling the position of NPs at the interface between the BCP particle and the surrounding media led to a dramatic change in the internal morphology and overall shape of the BCP particles by tuning their interfacial properties. [33][34][35] For example, we achieved precise positioning of size-controlled Au NPs in the BCP particles and controlled the interfacial properties at selective locations on the particle surface, generating the interesting morphological transitions of the BCP particles. 33 Herein, we exploited the particles of polystyrene-b-poly(4-vinylpyridine) (PS-b-P4VP) BCPs to investigate the AR effect of NRs on their location in the BCP domains and on the internal morphology and the overall shape of the BCP particles. The lengths (l) of the CuPt NRs were tuned from 2.6 to 40 nm with a fixed width (w) of 2.6 nm, thus producing five different AR values of 1, 3, 6, 10, and 15. To generate strong favorable interaction between the NRs and th...