One group of 2D layered materials is the transition metal dichalcogenides (TMDs) with MX 2 structure, where M denotes a transition metal such as Mo, W, Re, Nb, etc. and X ascertains a chalcogen atom, namely, S, Se, and Te. Unlike graphene's single carbon atomic-thick layer, a monolayer of TMDs consists of X-M-X sandwiches which are interacted by interlayer weak van der Waals forces and strong in-plane covalent bonding between atoms. As a result of their interesting and diverse structural, electronic, optical, mechanical, chemical, and thermal properties, this class of materials is still a topic of many recent scientific studies. [1][2][3][4][5][6][7] Particularly, MoS 2 shows a potential application in 2D nanoscale technology. [1,[8][9][10] The bandgap of MoS 2 semiconductor undergoes from indirect 1.29 eV (bulk) to direct 1.90 eV (monolayer) transitions. [5] The monolayer MoS 2 contains large specific surface areas, strong visible light-absorbing ability, and extreme flexibility against the bulk MoS 2 . [6,11] Such intriguing properties make MoS 2 a perfect alternative material for numerous applications such as photocatalysts, [12,13] photodetectors, [14,15] field-effect transistors, [16] solar cells, [17] and biomedical purposes [18,19] as well as optical fiber sensors (OFS). [10,20] The latter is a well-known sensor due to high sensitivity, noise and electromagnetic interference immunity, compact size, low cost, and multiplex capability. The OFS applications based on Fabry-Pérot interferometer (FPI) include industry, environment, medical care, homeland security, and defense. A simple and low-cost ultrasensitive configuration has been shown to upgrade FPI-acoustic OFS. Owing to high strength, flexibility, and relatively small Young's modulus, the MoS 2 membrane significantly improves the sensor sensitivity against others. [10]