Path-integral Monte Carlo calculations have been performed to study the 4 He adsorption on γ-graphyne, a planar network of benzene rings connected by acetylene bonds. Assuming the 4 Hesubstrate interaction described by a pairwise sum of empirical 4 He-carbon interatomic potentials, we find that unlike α-graphyne, a single sheet of γ-graphyne is not permeable to 4 He atoms in spite of its large surface area. One-dimensional density distributions computed as a function of the distance from the graphyne surface reveal a layer-by-layer growth of 4 He atoms. A partially-filled 4 He monolayer is found to exhibit different commensurate solid structures depending on the helium coverage; it shows a C 2/3 commensurate structure at an areal density of 0.0491Å −2 , a C 3/3 structure at 0.0736Å −2 , and a C 4/3 structure at 0.0982Å −2 . While the promotion to the second layer starts beyond the C 4/3 helium coverage, the first 4 He layer is found to form an incommensurate triangular solid when compressed with the development of the second layer. PACS numbers: 67.25.bd, 67.25.bh, For the past few decades, a system of 4 He atoms adsorbed on a substrate has been intensively studied to investigate physical properties of low-dimensional quantum fluids. Carbon allotropes have often been chosen as substrates for this purpose because they provide strong enough interactions for 4 He adsorbates to show multiple distinct layered structures [1]. As a result of the interplay between 4 He-4 He and 4 He-substrate interaction, these helium adlayers are known to exhibit rich phase diagrams including various commensurate and incommensurate solids. On the surface of graphite, a monolayer of 4 He atoms is crystallized to a C 1/3 commensurate solid at an areal density of 0.0636Å −2 and goes through various domain structures before freezing into an incommensurate triangular solid as the helium coverage increases [2,3] . Similar quantum phase transitions were predicted for the 4 He monolayer on a single graphene sheet [4][5][6]. While no superfluidity has been observed in the first 4 He layer, the second layer on graphite does show finite superfluid response at intermediate helium coverages as first revealed by torsional oscillator measurements of Crowell and Reppy [3]. Whether this second-layer superfluid phenomenon is related to two-dimensional supersolidity is still an ongoing issue pursued heavily by some experimentalists.The 4 He adsorption on the surface of a carbon allotrope other than graphite or graphene has recently been investigated. While 4 He atoms adsorbed on the interstitials or the groves of carbon nanotube bundles showed characteristics of one-dimensional quantum fluid [7,8], a series of theoretical calculations predicted well-distinct layered structures for 4 He atoms adsorbed on the outer surfaces of fullerene molecules with each near-spherical helium layer exhibiting various quantum states depending on the number of 4 He adatoms [9][10][11][12]. More recently, graphynes, sp-sp 2 hybridized two-dimensional networks of carbon atoms...