TY - JOUR
T1 - Synthesis of graphene and graphene nanostructures by ion implantation and pulsed laser annealing
AU - Wang, Xiaotie
AU - Berke, Kara
AU - Rudawski, Nicholas G.
AU - Venkatachalam, Dinesh K.
AU - Elliman, Robert G.
AU - Fridmann, Joel
AU - Hebard, Arthur F.
AU - Ren, Fan
AU - Gila, Brent P.
AU - Appleton, Bill R.
N1 - Publisher Copyright:
© 2016, American Institute of Physics Inc. All rights reserved.
PY - 2016/7/14
Y1 - 2016/7/14
N2 - In this paper, we report a systematic study that shows how the numerous processing parameters associated with ion implantation (II) and pulsed laser annealing (PLA) can be manipulated to control the quantity and quality of graphene (G), few-layer graphene (FLG), and other carbon nanostructures selectively synthesized in crystalline SiC (c-SiC). Controlled implantations of Si- plus C- and Au+ ions in c-SiC showed that both the thickness of the amorphous layer formed by ion damage and the doping effect of the implanted Au enhance the formation of G and FLG during PLA. The relative contributions of the amorphous and doping effects were studied separately, and thermal simulation calculations were used to estimate surface temperatures and to help understand the phase changes occurring during PLA. In addition to the amorphous layer thickness and catalytic doping effects, other enhancement effects were found to depend on other ion species, the annealing environment, PLA fluence and number of pulses, and even laser frequency. Optimum II and PLA conditions are identified and possible mechanisms for selective synthesis of G, FLG, and carbon nanostructures are discussed.
AB - In this paper, we report a systematic study that shows how the numerous processing parameters associated with ion implantation (II) and pulsed laser annealing (PLA) can be manipulated to control the quantity and quality of graphene (G), few-layer graphene (FLG), and other carbon nanostructures selectively synthesized in crystalline SiC (c-SiC). Controlled implantations of Si- plus C- and Au+ ions in c-SiC showed that both the thickness of the amorphous layer formed by ion damage and the doping effect of the implanted Au enhance the formation of G and FLG during PLA. The relative contributions of the amorphous and doping effects were studied separately, and thermal simulation calculations were used to estimate surface temperatures and to help understand the phase changes occurring during PLA. In addition to the amorphous layer thickness and catalytic doping effects, other enhancement effects were found to depend on other ion species, the annealing environment, PLA fluence and number of pulses, and even laser frequency. Optimum II and PLA conditions are identified and possible mechanisms for selective synthesis of G, FLG, and carbon nanostructures are discussed.
UR - http://www.scopus.com/inward/record.url?scp=85003944950&partnerID=8YFLogxK
U2 - 10.1063/1.4955137
DO - 10.1063/1.4955137
M3 - Article
SN - 0021-8979
VL - 120
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 2
M1 - 025105
ER -