2018
DOI: 10.1016/j.carbon.2018.03.076
|View full text |Cite
|
Sign up to set email alerts
|

Structural characteristics and strain behavior of two-dimensional C3N : First principles calculations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

2
58
1

Year Published

2019
2019
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 113 publications
(61 citation statements)
references
References 52 publications
2
58
1
Order By: Relevance
“…In figure 1, the studied structures in this study are illustrated, which include full carbon 2D structures of graphene (figure 1(a)), phagraphene [56] (figure 1(b)) and haeckelite [57] (figure 1(c)) and carbon-based binary lattices of C 2 N [58] (figure 1(d)), C 3 N [59] or C 3 B (figure 1(f)) and C 7 N 6 [60] (figure 1(f)) and carbon-free MoS 2 (figure 1(g)) and penta-SiP 2 (figure 1(h)). In this study, we also considered the bulk boron arsenide ( figure 1(k)) and silicon (figure 1(m)) lattices to [56] (c) haeckelite [57] (d) C2N [58] (e) C3N [59] or C3B (F) C7N6 [60] examine the accuracy of MTP for reproducing the phonic properties of bulk crystals. The hexagonal lattice constants of graphene, haeckelite, C 2 N, C 3 N, C 3 B, C 7 N 6 and MoS 2 were found to be 2.4674, 7.0869, 8.3277, 4.8605, 5.1735, 6.7949 and 3.1837 Å, respectively.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…In figure 1, the studied structures in this study are illustrated, which include full carbon 2D structures of graphene (figure 1(a)), phagraphene [56] (figure 1(b)) and haeckelite [57] (figure 1(c)) and carbon-based binary lattices of C 2 N [58] (figure 1(d)), C 3 N [59] or C 3 B (figure 1(f)) and C 7 N 6 [60] (figure 1(f)) and carbon-free MoS 2 (figure 1(g)) and penta-SiP 2 (figure 1(h)). In this study, we also considered the bulk boron arsenide ( figure 1(k)) and silicon (figure 1(m)) lattices to [56] (c) haeckelite [57] (d) C2N [58] (e) C3N [59] or C3B (F) C7N6 [60] examine the accuracy of MTP for reproducing the phonic properties of bulk crystals. The hexagonal lattice constants of graphene, haeckelite, C 2 N, C 3 N, C 3 B, C 7 N 6 and MoS 2 were found to be 2.4674, 7.0869, 8.3277, 4.8605, 5.1735, 6.7949 and 3.1837 Å, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…This structure was selected for the evaluation of thermal conductivity by the NEMD simulations. We remind that the C 3 N was fist synthesized by Mahmood et al [59] in 2016 and can be also considered among the most attractive carbon-based 2D materials, which has been extensively explored recently for various applications [67][68][69][70].…”
Section: Resultsmentioning
confidence: 99%
“…Therefore, the motivation rises to design and manufacture other materials without graphene limitations. This issue encouraged the people around the world to design and synthesis novel 2D nanosheets such as borophene [7], phospherene [8], Molybdenum disulfide [9], and carbon nitride [10]. As an example, recently a 2D semiconductor nanosheet so-called twin-graphene was predicted by first-principles calculations with 0.981eV band gap [11].…”
Section: Introductionmentioning
confidence: 99%
“…Mahmood et al [26], reported the first experimental realization of a densely packed and graphene-like carbon-nitride nanomaterials with a C3N stoichiometry. Likely to g-C3N4 and C2N counterparts, C3N is also an intrinsic semiconductor, however thanks to its nonporous atomic lattice C3N can exhibit remarkably high mechanical and thermal conduction properties [27][28][29][30][31][32]. According to the extensive theoretical studies conducted recently, C3N nanosheet can exhibit desirable properties for various applications, like; nanoelectronics [33][34][35][36][37], nanomagnetics [38,39], catalysis [40,41], superconductivity [42], anode materials for Li-ion batteries [43] and hydrogen storage [44].…”
Section: Introductionmentioning
confidence: 99%