create mixed dimensional heterostructures [5] of 2D materials and functional substrates, which provide an even wider opportunity to tailor diverse material functionalities and interface phenomena. In this regard, a very promising substrate is SrTiO 3 (STO), a transition metal oxide with an ABO 3 -type perovskite crystal structure, that has attracted significant attention due to both its unusual bulk properties like high dielectric constant, [6] quantum paraelectricity, [7] and several interface phenomena such as the observation of 2D electron gas at interfaces with oxide insulators [8] and enhancement of superconducting T c at the interfaces with 2D FeSe. [9] The speciality of STO lies in its rich phonon spectrum centered on its AFD structural phase transition [10] (from cubic to tetragonal). The uniqueness of the phonons in STO, specifically the low energy soft phonons when compared to conventional phonons present in most materials lies in the following: i) they arise at a phase transition temperature and their frequency (energy) softens to zero near the transition ii) their intensity increases at low temperatures whereas conventionally phonon intensity decreases at lower temperatures The reduced electrical screening in 2D materials provides an ideal platform for realization of exotic quasiparticles, that are robust and whose functionalities can be exploited for future electronic, optoelectronic, and valleytronic applications. Recent examples include an interlayer exciton, where an electron from one layer binds with a hole from another, and a Holstein polaron, formed by an electron dressed by a sea of phonons. Here, a new quasiparticle is reported, "polaronic trion" in a heterostructure of MoS 2 /SrTiO 3 (STO). This emerges as the Fröhlich bound state of the trion in the atomically thin monolayer of MoS 2 and the very unique low energy soft phonon mode (≤7 meV, which is temperature and field tunable) in the quantum paraelectric substrate STO, arising below its structural antiferrodistortive (AFD) phase transition temperature. This dressing of the trion with soft phonons manifests in an anomalous temperature dependence of photoluminescence emission leading to a huge enhancement of the trion binding energy (≈70 meV). The soft phonons in STO are sensitive to electric field, which enables field control of the interfacial trion-phonon coupling and resultant polaronic trion binding energy. Polaronic trions could provide a platform to realize quasiparticle-based tunable optoelectronic applications driven by many body effects.The last few years have witnessed several extraordinary quantum functionalities emerging at interfaces of van der Waals heterostructures. [1][2][3][4] Recently, there has been a growing interest to