Inelastic neutron scattering reveals a broad continuum of excitations in Pr2Zr2O7, the temperature and magnetic field dependence of which indicate a continuous distribution of quenched transverse fields (∆) acting on the non-Kramers Pr 3+ crystal field ground state doublets. Spin-ice correlations are apparent within 0.2 meV of the Zeeman energy. A random phase approximation provides an excellent account of the data with a transverse field distribution ρ(∆) ∝ (∆ 2 + Γ 2 ) −1 where Γ = 0.27(1) meV. Established during high temperature synthesis due to an underlying structural instability, it appears disorder in Pr2Zr2O7 actually induces a quantum spin liquid.Instead of a discrete set of states that satisfy all interactions, frustrated spin systems support a high density of low energy states from which novel collective phenomena may emerge at temperatures (T ) well below the bare interaction strengths.[1] A prominent example is quantum spin ice (QSI).[2] By introducing quantum spin fluctuations to classical spin ice through transverse inter-spin interactions, it has been proposed that a quantum spin liquid (QSL) phase with gapless photon-like excitations can be realized. [2] Several materials have been examined in the search for QSI including Yb 2 Ti 2 O 7 and Tb 2 Ti 2 O 7 , but so far there is no experimental evidence for salient features such as low energy electrodynamics.[2] Instead unanticipated features have been discovered including a very strong dependence of physical properties on sample quality. In a recent study of Tb 2+x Ti 2−x O 7+y it was found that a change in the Tb/Ti molar ratio as small as 0.005 can tune the samples between an ordered and a disordered phase.[3] While such sensitivity is a distinguishing feature of systems with a high density of low energy states, there is so far no clear understanding of the microscopic mechanisms involved. Can this be explained in terms of small changes of the exchange interactions in the pseudo-spin-1/2 Hamiltonian[2] for materials near phase boundaries or are there new pieces of the puzzle yet to be discovered? Further insight into these questions will not only help clarify the complicated magneto-structural properties of specific materials, but may guide the broader search for QSL materials.In this paper we show quenched structural disorder acts as a transverse field on the non-Kramers Pr 3+ ion in Pr 2 Zr 2 O 7 (PZO) and in competition with exchange interactions induces a spatially correlated and disordered singlet ground state. A previous neutron study of PZO revealed weak diffuse elastic scattering with pinch points indicative of spin-ice correlations.[4] Here we show magnetic excitations in PZO are composed of two parts: a lower energy regime that is driven by inter-spin correlations, and a momentum transfer (q) independent higher energy part driven by quenched transverse fields. A nearest neighbor spin ice model augmented by random transverse fields provides an excellent account of these observations and points to the realization of a newly proposed QSL [...