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Nature communications, v.5, 2014년, pp.3782 -
Zhang, Peng (Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA) , Ma, Lulu (Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA) , Fan, Feifei (Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332, USA) , Zeng, Zhi (Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332, USA) , Peng, Cheng (Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA) , Loya, Phillip E. (Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA) , Liu, Zheng (1] Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA [2] School of Materials Science and Engineering, School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore) , Gong, Yongji (Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA) , Zhang, Jiangnan (Department of Materials Science and NanoEngineer) , Zhang, Xingxiang , Ajayan, Pulickel M. , Zhu, Ting , Lou, Jun
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Perfect graphene is believed to be the strongest material. However, the useful strength of large-area graphene with engineering relevance is usually determined by its fracture toughness, rather than the intrinsic strength that governs a uniform breaking of atomic bonds in perfect graphene. To date, ...
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