“…The systems with the space group of P 6 3 / mmc , such as the Ising ferromagnet FeCr 2 Te 4 , the topological superconductor BaSn 3 , and the ferromagnetic nodal-line semimetal candidate Fe 3 GeTe 2 , have recently attracted essential interest, presumably due to the special crystalline symmetry, , which makes these systems promising topological nontrivial materials and worthy of both theoretical and experimental investigation. , Furthermore, the structure of NdCrGe 3 consists of chains of face-sharing Cr-centered octahedra, 1 ∞ [CrGe 6/2 ], aligned along the c axis, separated by Nd atoms. The chains expand infinitely along the c direction [Figure (a,b)], exhibiting 1D features. , The Nd atoms are coordinated by 12 Ge atoms in an anticuboctahedral geometry. , Owing to the 1D crystal structure and the P 6 3 / mmc space group, NdCrGe 3 should be a potentially fruitful system in further theoretical and experimental research. − Previously, the single crystals of LnCrGe 3 (Ln = rear earths), which were as tiny as 0.5 mm, were fabricated, and the basic magnetic properties were measured but based on polycrystalline samples . We have investigated the critical behavior and magnetocaloric of PrCrGe 3 single crystal around the ferromagnetic transition…”