Optical microscopy is one of the most important scientific achievements in the history of mankind, and it is the most widely used technique for exploring the small world. However, as is well known, traditional lens-based optical microscopes suffer from the low imaging resolution λ/2 due to the diffraction limit. To overcome this obstacle, multiple innovative methods have been proposed during the past few decades, such as photoactivatable localization microcopy (PALM), stimulated emission depletion (STEM), surface plasmon polaritons (SPPs) based microscopy, and negative-index metamaterials based microscopy. However, the above methods are either florescence based, or can be only operated in a narrow spectral bandwidth. Here we propose to further push forward the pioneering work of Wang, which uses microspheres to achieve a nanoscope with λ/8-λ/14 imaging resolution. To be specific, we present the schematic of our proposed transmission mode microsphere nanoscope in Fig. 1. The targets under measurement are attached to the bottom side of a thin glass layer, whose upside is illuminated by a white-light source. Microspheres that are put on the top of a gold nanowire array collect the scattering information of the target. If the distance between a point on the surface of the target and the incident point on the surface of the microsphere is smaller than the penetration depth of the evanescent field and meanwhile the scattering angle of a beam from the scatter point fulfills the output propagation condition, the microspheres can collect more information of the target than the traditional microscope. The output propagation beam from the microsphere then couples into the gold nanowire array. The aligned metallic nanowires embedded in dielectric bulk possess strongly anisotropic optical properties with negative permittivity along the nanowire axis and positive permittivity in the transverse plane, which can be used to achieve broadband all-angle negative refraction and superlens imaging. Therefore the gold nanowire array plays the role of a second amplifier and a supplementary collector for collecting the scattering beams that are not collected by the microspheres. In this composite array, the guided mode does not effectively penetrate the gold nanowires and thus most of the energy propagates in the host dielectric medium in between the nanowires, so that the influence of the losses in the gold wires is negligible. The output beam of the array is then picked up by a conventional objective lens and the final image of the target is captured by a charge coupled device (CCD). Simulations will be performed to validate the effectiveness of the proposed configuration.