2017
DOI: 10.1103/physrevb.95.039903
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Publisher's Note: Interpenetrating graphene networks: Three-dimensional node-line semimetals with massive negative linear compressibilities [Phys. Rev. B 94, 245422 (2016)]

Abstract: with an incorrect version of Fig. 2 and an error in the caption of Fig. 10. The second line of the caption to Fig. 10 should read as ". .. two-dimensional electronic band dispersion in Z11. (a) The Fermi. .. ." The caption has been corrected and Fig. 2 has been replaced as of 27 December 2016. The text and figure are correct in the printed version of the journal.

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Cited by 5 publications
(5 citation statements)
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“…The combined variation of bonding fraction and the spatial arrangement of the tetrahedra and triangles formed by sp 3 or sp 2 bonds make some of the BC structures different from diamond or graphite. Their motifs are similar to those which have already been reported in pure carbon structures [40][41][42][43][44][45][46] , and classified as "interpenetrating graphene networks" (IGN ) 40 or "carbon honeycombs" (CHC ) 46 . We have grouped these structures under the general keywords tubulanes.…”
Section: Structures : Thermodynamics and Prototypessupporting
confidence: 81%
“…The combined variation of bonding fraction and the spatial arrangement of the tetrahedra and triangles formed by sp 3 or sp 2 bonds make some of the BC structures different from diamond or graphite. Their motifs are similar to those which have already been reported in pure carbon structures [40][41][42][43][44][45][46] , and classified as "interpenetrating graphene networks" (IGN ) 40 or "carbon honeycombs" (CHC ) 46 . We have grouped these structures under the general keywords tubulanes.…”
Section: Structures : Thermodynamics and Prototypessupporting
confidence: 81%
“…Unlike relativistic high-energy physics, the violation of Lorentz invariance for type-II Weyl points reveals the unnecessary restriction of Lorentz symmetry in condensed matter systems [26]. Nevertheless type-I and II Weyl points share the same topological characteristics, and the two can be transformed from one to the other by a Lifshitz transition [27,28], and their Fermi surfaces, which are crucial to magnetic properties and carrier transport, can be drastically different [29,30].Because of its rich bonding chemistry, a carbon network provides a natural platform in the search for new topological matter [31][32][33], since carbon has many forms of allotropes ranging from one (1D) to three (3D)dimension [34][35][36][37][38][39][40]. Here, the presence of topological properties originates from graphene as a two-dimensional (2D) topological matter [41], with nanoribbons serving as building blocks for the carbon allotropes.…”
mentioning
confidence: 99%
“…Because of its rich bonding chemistry, a carbon network provides a natural platform in the search for new topological matter [31][32][33], since carbon has many forms of allotropes ranging from one (1D) to three (3D)dimension [34][35][36][37][38][39][40]. Here, the presence of topological properties originates from graphene as a two-dimensional (2D) topological matter [41], with nanoribbons serving as building blocks for the carbon allotropes.…”
mentioning
confidence: 99%
“…Even before and also after the emerging of graphene studies, there have been many theoretical proposals and studies about such 3DGraphene polymeric structures. 28−30 Importantly, in addition to the unique electronic and mechanical properties derived from graphene, 31,32 most of these proposed graphene based networks, including that with sp 2 −sp 3 hybridized structures, are thought to be highly stable. While the ordered (crystalline) 3DGraphene materials have not been proved/ prepared completely, some materials with the proposed network structures but in the amorphous form have been reported, and indeed they demonstrate many excellent and unique properties.…”
Section: ■ Fabrication and Preparation Of 3dgraphenementioning
confidence: 99%