Strong coupling of two-dimensional semiconductor excitons with plasmonic resonators enables control of light-matter interaction at the subwavelength scale. Here we develop strong coupling in plasmonic nano-gap resonators that allow modification of exciton number contributing to the coupling. Using this system, we not only demonstrate a large vacuum Rabi splitting up to 163 meV and splitting features in photoluminescence spectra, but also reveal that the exciton number can be reduced down to single-digit level (N < 10), which is an order lower than that of traditional systems, close to single-exciton based strong coupling. In addition, we prove that the strong coupling process is not affected by the large exciton coherence size that was previously believed to be detrimental to the formation of plasmon-exciton interaction. Our work provides a deeper understanding of storng coupling in two-dimensional semiconductors, paving the way for room temperature quantum optics applications.Introduction-Two-dimensional (2D) transitional metal dichalcogenides (TMDCs), such as molybdenum disulfide (MoS 2 ) and tungsten disulfide (WS 2 ) have attracted tremendous attention recently [1,2]. These semiconductor nanosheets, when thinned down to monolayers (MLs), become direct bandgap, hosting excitons having ultralarge binding energy[3-5] and very high oscillator strength [2,6], which arise from the strong coulomb interaction and reduced dielectric screening in atomically thin structures. As a result, excitons in TMDC MLs can be tighly bound even at room temperature, producing strong light absorption and photoluminescence (PL). Integrating TMDC MLs with an optical resonator enables fast energy exchange between electromagnetic (EM) resonances and semiconductor excitons, i.e. the strong lightmatter interaction or strong couling, allowing the formation of half-light half-matter quasiparticles, known as polaritons. The strong coupling process not only is of interest for fundamental quantum optics, e.g. Bose-Einstein condensation[7] with superfluid characteritics, but also exhibits a great potential for many compelling applications, e.g. quantum computing [8] and thresholdless semiconductor lasing [9,10].