when they are in close proximity [5,7]. The weak couplings between the plasmon and exciton resonances can lead to the induced transparency, enhanced absorption, increased emission, and increased optical nonlinearity [4,[8][9][10][11][12][13]. The strong plasmon-exciton couplings will modify the responses of the plasmon and exciton modes. J aggregates can strongly couple with the surface plasmon polariton [14][15][16] or the localized surface plasmon resonance (LSPR) [17,18] leading to new hybridized plasmon-exciton states (plexcitons). The dispersion curves of two plexcitonic modes show an avoided crossing, which is known as Rabi splitting [5]. Fofang et al. [19,20] further reported the enhanced and tunable nonlinear optical properties in the Au nanoshell-J aggregate complexes. As a quantum emitter (QE) locates at the center of a dimer nanoantenna, a Rabi splitting has been found in the scattering spectrum [21]. It was also found that the interaction between the quantum emitter and the gap plasmon can result in a Fano resonance in the metallic dimer-QE system [22]. In addition, Marinica et al. [23] found that the electron transfer of the excited electron into the metal can decrease the lifetime of the exciton in the QE.Recently, Manassah [24] investigated the electrodynamics of CuCl-coated Ag nanoshells. Semiconductor CuCl exhibits a strong Z 3 exciton line at about 3.202 eV [7,25]. The plasmon-exciton couplings in the Ag-CuCl nanoshell lead to a splitting of the excitonic line and a shift in LSPR. In the dimer including a CuCl nanosphere and an Ag nanosphere, the exciton resonances of the CuCl nanosphere interact with the SP resonances of the Ag nanoparticles resulting in the induced transparency and slow light effect [8]. We also found that the plasmon-exciton couplings in the Ag nanoshell with a semiconductor CuCl core can lead to the Rabi splitting and the induced transparency by changing the geometry of the CuCl-Ag nanoshell [26]. To Abstract The plasmon-exciton couplings in Ag-CuClcoated nanowires (ACNWs) have been investigated by using the scattering theory and the finite element method. It is found with increasing the shell thickness that the dipole plasmon resonance of the Ag nanowire can be tuned through the exciton resonance in the CuCl shell. The strong coupling between the plasmon resonance in the Ag nanowire and the exciton resonance in the CuCl shell leads to two new hybridized plexcitonic modes. The dispersion curves of the plexcitonic modes in the ACNWs are studied, and the obtained splitting energy is about 88 meV. We further find that the destructive interference between the plasmon and exciton resonances results in the plasmon-exciton induced transparency. As the TE wave propagates through the ACNW array, an extraordinary transmittance can be found in the ACNW array at the scattering dip of the ACNW.