We study electric transport along an integer quantum Hall edge where the proximity effect is induced due to a coupling to a superconductor. Such an edge exhibits two Majorana-Weyl fermions with different group velocities set by the induced superconducting pairing. We show that this structure of the spectrum results in interference fringes that can be observed in both the two-terminal conductance and shot noise. We develop a complete analytical theory of such fringes for an arbitrary smooth profile of the induced pairing. DOI: 10.1103/PhysRevB.96.241104 Superconductivity and the quantum Hall effect are two celebrated phenomena by which quantum physics is manifested at macroscopic scales. Both exhibit universal characteristics insensitive to the microscopic detail. However, the underlying physics is quite different. Superconductivity arises from a spontaneously broken gauge symmetry and is characterized by a local order parameter. In contrast, the quantum Hall effect is attributed to a much subtler nonlocal topological order.Even though each phenomenon has been studied extensively on its own, combining the two in a single hybrid device has been an experimental challenge [1][2][3][4]. This is because quantum Hall effect requires a strong magnetic field, which is abhorred by superconductors. Nevertheless, a stable proximity effect in the quantum Hall regime has been achieved recently [5][6][7][8][9][10]. The key element of this success is the ability to manufacture a hybrid structure using either superconducting materials with high critical fields or two-dimensional electron gas that exhibits quantum Hall effects in lower magnetic fields. The approach of Ref. [5] was to use NbN contacts, with critical fields higher than 16 T, on a 2-dimensional electron gas in a GaAs quantum well. In contrast, in Refs. [6][7][8][9][10], graphene was used as the two-dimensional electron gas that exhibits quantum Hall effects in lower magnetic fields.This experimental breakthrough offers an opportunity to test the predictions of earlier theoretical works such as the tunneling current from a superconducting point contact into a quantum Hall liquid [11] and the critical current [12] along with the upstream information transfer [13] in a superconductor-normal metal-superconductor (SNS) junction, where the normal metal is in the quantum Hall regime. Furthermore, if one can extend the stable proximity effect into the fractional quantum Hall regime, one might be able to create novel excitations with nontrivial braiding statistics [14][15][16][17].In this Rapid Communication, we focus on the electric transport along the quantum Hall edge with an extended proximity-induced superconducting region. We look into the ν = 1 integer quantum Hall case or the situation where only the outermost edge of a ν > 1 state contributes to transport. We consider the geometry 1 depicted in Fig. 1, where the induced pairing varies smoothly at the interface but dies rapidly away from the proximity-induced superconducting region. Unlike other proximity-induced ...