Two-dimensional (2D) superconductors (SCs) with Ising spin-orbit coupling are regarded as a central ingredient for the topological protection of spin-triplet Cooper pairs and, thereby, Majorana fermions. Here, we fabricate non-local magnon devices to examine how such 2D Ising superconductivity affects the conversion efficiency of magnon spin to quasiparticle charge in superconducting flakes of 2H-NbSe 2 transferred onto ferromagnetic insulating Y 3 Fe 5 O 12 . Comparison with a reference device based on a conventionally paired superconductor shows that the Y 3 Fe 5 O 12 -induced exchange spinsplitting in the NbSe 2 flake is hindered by its inherent spin-orbit-field, which, in turn, limits the transition-state enhancement of the spin-to-charge conversion efficiency. Our out-of-equilibrium study highlights the significance of symmetry matching between underlying Cooper pairs and exchange-induced spin-splitting for the giant transitionstate spin-to-charge conversion and may have implications towards proximity-engineered spin-polarized triplet pairing via tuning the relative strength of exchange and spin-orbit fields in ferromagnetic insulator/2D Ising SC bilayers. Ising Cooper pairing governs out-of-equilibrium spin-to-charge conversion characteristics.materials provide new platforms to explore novel physical phenomena in various geometries (22), including van der Waals (vdW) heterostructures with a twist, and in proximity combination with magnetic vdW flakes and/or thin films (23,24). Because excited QPs and Cooper pairs in the superconducting condensate state are intimately correlated (1-6), studies of non-equilibrium QP spin properties in such 2D SCs are of fundamental importance for understanding equilibrium spin-polarized triplet Cooper pairing (1-6) and the possible stabilization of Majorana fermions (25-27). 2D superconductivity has been recently discovered in monolayer transition metal dicalcogenides (TMDs) (17) such as gated 2H-MoS2 (18,19) and 2H-NbSe2 (20). Interestingly, the in-plane (IP) upper critical field 𝜇 0 𝐻 𝑐2 ∥ is found to far exceed the Pauli paramagnetic limit of isotropic Bardeen-Cooper-Schrieffer (BCS) SCs 𝜇 0 𝐻 𝑃 𝐵𝐶𝑆 ≈ 1.84Tc (28), where Tc is the superconducting transition temperature. Such an enhancement of 𝜇 0 𝐻 𝑐2 ∥ is explained by Ising spin-orbit coupling (SOC) (17-21), rooted in the broken IP crystal inversion symmetry plus the large SOC due to heavy transition metal atoms in TMDs. The Ising SO field 𝜇 0 𝐻 𝑆𝑂 (as large as several hundred Tesla in the monolayer limit) (17-21) strongly pins Cooper pair spins at K and K' points of the hexagonal Brillouin zone to opposite out-of-plane (OOP) directions over IP applied magnetic fields. This stabilizes OOP Cooper pairing and forms so-called Ising superconductivity (17-21).We here investigate how the 2D Ising superconductivity influences the transition-state enhancement of magnon spin to QP charge conversion in a superconducting flake of 2H-NbSe2(20,29-31) (Fig. 1A) and compare its efficiency with a conventional superconducting thin film of ...