of 2D materials, [3][4][5] providing opportunity for understanding the adhesion and mechanical properties of these atomically thin materials. The bubbles of 2D materials have also been demonstrated to own potential applications in electronics and photonics. [6][7][8] For example, scanning tunneling microscopy measurements have verified the presence of enormous pseudo-magnetic fields in highly strained graphene nanobubbles, [7] offering a new basis for exploration of extremely high magnetic field regimes in a condensedmatter environment. Georgiou et al. [6] have demonstrated that the curvature of graphene can be tuned by applying an external electric field, showing potential application for optical lenses. Bao et al. [8] have reported that there is strong nonlinear light-matter interaction in graphene nanobubbles, resulting in optical bistability effect at cavity resonance. Interference-induced Raman enhancement [9] and oscillations [10] have also been observed in graphene bubbles.Like graphene, atomically thin WS 2 crystal is also a mechanically exceptional material, which can be grown or transferred on various substrates. [11][12][13][14] On top of that, it is semiconductor, undergoing a transition from indirect to direct bandgap after thinning to monolayer. [15] In addition, monolayer WS 2 shows strong photoluminescence (PL) with high efficiency and narrower emission linewidth. [16] Due to these superior properties, monolayer WS 2 has shown promising applications in electronics, spintronics, valleytronics, and optoelectronic, [17][18][19] such as field-effect transistors, [20,21] photodetectors, [22,23] magnetoluminescence devices, [24] and valleytronic devices. [25] Monolayer WS 2 crystal, whose bandgap and lattice vibrations are highly sensitive to external conditions like strain, [26,27] pressure, [28] temperature, [29,30] and electric field, [31] is also a perfect model material for PL and Raman studies. [16,32,33] Although numerous studies and research on atomically thin WS 2 crystals have been carried out, there has been no experimental observation on WS 2 bubble so far, much less its properties.In the present work, huge amount of monolayer WS 2 (1L WS 2 ) bubbles are created in large-scale CVD-grown WS 2 WS 2 monolayer crystals have been grown in a large scale by chemical vapor deposition on SiO 2 (300 nm)/Si substrates, and via high-temperature treatment under protection of Ar or N 2 gas flow after growth, huge amount of monolayer WS 2 bubbles have been successfully created in a shape of spherical cap and widely distributed sizes. Optical and fluorescence images reveal obvious interference rings on the monolayer WS 2 bubbles of large sizes. In line scans and mapping images of photoluminescence (PL) and Raman, oscillatory behaviors have been observed not only for peak intensity but also for peak position and width. It is easy to understand that the oscillatory PL and Raman peak intensities originate from constructive and destructive interference on the bubble's surface, while the oscillatory peak positio...