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Gas transport controlled graphene synthesis via jig gap: Nucleation - PowerPoint PPT Presentation

Gas transport controlled graphene synthesis via jig gap: Nucleation and growth study Seong-Yong Cho, Ki-Ju Kim, Hyun-Mi Kim, Do-Joong Lee, Min-Hyun Lee and Ki-Bum Kim Department of Materials Science and Engineering Seoul National University


  1. Gas transport controlled graphene synthesis via jig gap: Nucleation and growth study Seong-Yong Cho, Ki-Ju Kim, Hyun-Mi Kim, Do-Joong Lee, Min-Hyun Lee and Ki-Bum Kim Department of Materials Science and Engineering Seoul National University

  2. Polycrystalline nature of graphene growth Random nucleation in graphene CVD Grain boundaries nucleation C. Mattevi, et al ., J. Mater. Chem. 21 , 3324 (2011) Electrical properties in polycrystalline graphene Q. Yu et al. , Nature Mater. 10 , 443 (2011) Understanding on growth mechanism and controlling method is required 2

  3. Jig concept for gas transport study • Graphene CVD appears relatively simple, but obtaining a high quality graphene is another issue. • Both the kinetics on nucleation and growth should be well understood and controlled. Jig is an excellent tool to observe gas transport effect in graphene growth by controlling boundary layer thickness in CVD system. Gas conductance control was observed directly. Jig effect on pre-annealing: Reduction of copper sublimation 3

  4. Effect of jig gap on graphene growth Dendritic to polygon shape evolution 5 mm 0 mm 2 mm 10 mm 20 mm 50 µm Nucleation and growth behavior in jig gap Lateral distance from jig entrance (mm) 5 0 1 2 3 7 10 15 20 1 mm 500 µm Jig gap 200 µm 100 µm 50 µm 4

  5. Analysis on nucleation and growth Areal coverage vs. distance Normalization 𝑫 = 𝒍 𝑩 C : gas conductance 𝑴 A : area L : length k/k’ : constant ≈ 𝒍 ′ 𝑬 𝑴 D L : lateral distance 𝑬 𝒘 D V : vertical distance Gas conductance was successfully controlled by manipulating jig gap. Universal conductance parameter D L /D V governs graphene coverage. Grain size variation Nuclei density variation 𝑶 ∗ = 𝒐 𝒕 𝒇𝒚𝒒(− ∆𝑯 ∗ 𝒍𝑼 ) N* : equilibrium concentration of critical nuclei n s : density of nucleation site ∆𝐻 ∗ : function of degree of supersaturation k : Boltzmann constant Variation of gas conductance via jig gap controls grain size of graphene, but nuclei density was independent of gas transport control. S. Y. Cho K. J. Kim et al ., MRS 2012 Fall S. Y. Cho K. J. Kim et al ., RSD Advances 3, 26376 (2013) 5

  6. Summary • Reduction of copper surface : static vapor condition limits the sublimation and re- deposition of Cu which make Cu surface smoother • Morphology of graphene grain : because of carbon source depletion and continuous etching of hydrogen, graphene grain shape shifted from dendritic to polygon • Coverage of graphene : coverage of graphene show general behavior to the parameter, D L /D V , which is gas conductance • Grain size and nuclei density of graphene : grain size of graphene is the function of gas conductance whereas nuclei density is not. The nuclei density itself considered to related with the nucleation site, heterogeneous nucleation behavior of graphene. 6

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