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Abstract
Two-dimensional crystals with angstrom-scale pores are widely considered as candidates for a next generation of molecular separation technologies aiming to provide extreme, exponentially large selectivity combined with high flow rates. No such pores have been demonstrated experimentally. Here we study gas transport through individual graphene pores created by low intensity exposure to low kV electrons. Helium and hydrogen permeate easily through these pores whereas larger species such as xenon and methane are practically blocked. Permeating gases experience activation barriers that increase quadratically with molecules’ kinetic diameter, and the effective diameter of the created pores is estimated as ∼2 angstroms, about one missing carbon ring. Our work reveals stringent conditions for achieving the long sought-after exponential selectivity using porous two-dimensional membranes and suggests limits on their possible performance.
Two-dimensional membranes with angstrom-sized pores are predicted to combine high permeability with exceptional selectivity, but experimental demonstration has been challenging. Here the authors realize angstrom-sized pores in monolayer graphene and demonstrate gas transport with activation barriers increasing quadratically with the molecular kinetic diameter.
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1 University of Manchester, Department of Physics and Astronomy, Manchester, UK (GRID:grid.5379.8) (ISNI:0000000121662407); University of Manchester, National Graphene Institute, Manchester, UK (GRID:grid.5379.8) (ISNI:0000000121662407)
2 University of Antwerp, Department of Physics, Antwerp, Belgium (GRID:grid.5284.b) (ISNI:0000 0001 0790 3681); NANOlab Center of Excellence, Antwerp, Belgium (GRID:grid.5284.b) (ISNI:0000 0001 0790 3681); Izmir Institute of Technology, Department of Photonics, Izmir, Turkey (GRID:grid.419609.3) (ISNI:0000 0000 9261 240X)
3 University of Manchester, Department of Physics and Astronomy, Manchester, UK (GRID:grid.5379.8) (ISNI:0000000121662407)
4 Tsinghua University, Graphene Center, Tsinghua-Berkeley Shenzhen Institute, Tsinghua Shenzhen International Graduate School, Shenzhen, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Tsinghua University, Graphene Center, Institute of Materials Research, Tsinghua Shenzhen International Graduate School, Shenzhen, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178)
5 University of Science and Technology of China, Chinese Academy of Sciences Key Laboratory of Mechanical Behavior and Design of Materials, Department of Modern Mechanics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
6 University of Antwerp, Department of Physics, Antwerp, Belgium (GRID:grid.5284.b) (ISNI:0000 0001 0790 3681); NANOlab Center of Excellence, Antwerp, Belgium (GRID:grid.5284.b) (ISNI:0000 0001 0790 3681)
7 University of Manchester, Department of Physics and Astronomy, Manchester, UK (GRID:grid.5379.8) (ISNI:0000000121662407); University of Manchester, National Graphene Institute, Manchester, UK (GRID:grid.5379.8) (ISNI:0000000121662407); Tsinghua University, Graphene Center, Tsinghua-Berkeley Shenzhen Institute, Tsinghua Shenzhen International Graduate School, Shenzhen, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Tsinghua University, Graphene Center, Institute of Materials Research, Tsinghua Shenzhen International Graduate School, Shenzhen, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178)