The honeycomb antiferromagnet BaCo 2 (AsO 4 ) 2 , in which small in-plane magnetic fields (H1 ≈ 0.26 T and H2 ≈ 0.52 T at T = 1.8 K < T N ≈ 5.4 K) induce two magnetic phase transitions, has attracted attention as a possible candidate material for the realization of Kitaev physics based on the 3d element Co 2+ . Here, we report on the change of the transition temperature T N and the critical fields H1 and H2 of BaCo 2 (AsO 4 ) 2 with hydrostatic pressure up to ∼ 20 kbar, as determined from magnetization and specific heat measurements. Within this pressure range, a marginal increase of the magnetic ordering temperature is observed. At the same time, the critical fields are changed significantly (up to ∼ 25 -35 %). Specifically, we find that H1 is increased with hydrostatic pressure, i.e., the antiferromagnetic state is stabilized with hydrostatic pressure, whereas H2, which was previously associated with a transition into a proposed Kitaev spin liquid state, decreases with increasing pressure. These results put constraints on the magnetic models that are used to describe the low-temperature magnetic properties of BaCo 2 (AsO 4 ) 2 .
I. INTRODUCTIONThe search for quantum spin liquids, a particularly exotic state of matter, has seen a boost over the last 15 years by the postulation of (i) the analytically exactly solvable Kitaev model [1] that hosts a spin-liquid ground state, as well as (ii) the Jackeli-Khaliullin approach to design Kitaev interactions in real materials [2]. The latter initially involved spin-orbitcoupled d 5 ions in an octahedral environment in Mott insulators, in which the combination of crystal field effects and spin-orbit coupling coupling generates an effective j eff = 1/2 moment. These moments are then coupled via bond-dependent ferromagnetic Ising interactions that are the central ingredient of the Kitaev model. Following these discoveries, the research concentrated on material realizations based on heavy, 4d and 5d, transition metals [3] due to their inherently large spin-orbit coupling. Prominent examples include Na 2 IrO 3 [4], α-Li 2 IrO 3 [5] and α-RuCl 3 [6]. All the listed materials show antiferromagnetic order at finite temperatures [7,8], which is thought to obscure the observation of the putative Kitaev spin liquid. The emergence of magnetic order is believed to originate from the presence of sizable non-Kitaev interactions [9, 10], such as nearest-neighbor and third nearest-neighbor Heisenberg couplings as well as off-diagonal couplings. The existence of these couplings is generally attributed to the spatial extent of the 4d and 5d orbitals which promotes longer-