The chiral p-wave order parameter in Sr2RuO4 would make it a special case amongst the unconventional superconductors. A consequence of this symmetry is the possible existence of superconducting domains of opposite chirality. At the boundary of such domains, the locally supressed condensate can produce an intrinsic Josephson junction. Here, we provide evidence of such junctions using mesoscopic rings, structured from Sr2RuO4 single crystals. Our order parameter simulations predict such rings to host stable domain walls across their arms. This is verified with transport experiments on loops, with a sharp transition at 1.5 K, which show distinct critical current oscillations with periodicity corresponding to the flux quantum. In contrast, loops with broadened transitions at around 3 K are void of such junctions and show standard Little-Parks oscillations. Our analysis demonstrates the junctions are of intrinsic origin and makes a compelling case for the existence of superconducting domains. seems probable, domains or edge currents have not been observed directly. Indications for their existence, however, have been found in transport experiments, which utilize Ru inclusions to form proximity junctions between Sr2RuO4 and a conventional s-wave superconductor [10,11]. A complication in the physics of Sr2RuO4 is that breaking of the tetragonal crystal symmetry due to Ru inclusions or a uniaxial strain can induce a different superconducting state with an enhanced superconducting transition temperature ≈ 3 K [13,14]. Recent experiments suggest that this so-called 3-K phase may exhibit a non-chiral state with a single-component order parameter [15,16]. In this paper, we refer to the multicomponent phase with of around 1.5 K, associated with the pure bulk limit, as the "intrinsic phase" and the possible single-component phase, characterized by ≈ 3 K, as the "extrinsic phase".The vast majority of experiments in the past two decades have been limited to bulk crystals, typically hundreds of microns in dimension. This is partly due to the unavailability of superconducting Sr2RuO4 films. The chiral domains, however, are expected to be no more than a few microns in size [5,11]. Moreover, the time-dependent switching noise observed in transport measurements suggests the domains are mobile [10,11]. We note here that the role of chiral domains resulting in hysteretic behaviour has been discussed in the Bi-Ni bilayer system [12]. The arbitrary configuration of the domains introduces an element of uncertainty.On the other hand, the energy cost associated with a chiral domain wall (ChDW), grows per area [17]. It has been recently discussed that mesoscopic samples made of chiral p-wave superconductors could host multichiral states [18,19], where the two ± chiral components are divided into superconducting domains, separated by ChDWs. This makes mesoscopic structures a promising platform to verify and potentially control the domains.