Hard, transparent, sp3-containing 2D phase formed from few-layer graphene under compression
暂无分享,去创建一个
Jesse S. Smith | J. Kong | T. Palacios | R. Comin | M. Hempel | X. Ji | L. G. Cançado | Ang-Yu Lu | A. B. de Oliveira | M. Mazzoni | C. Su | R. S. Alencar | C. Occhialini | R. J. Batista | M. J. Matos | Alysson A. Pinto | A. Souza | Diego L. Silva | Luiz G. Pimenta Martins | Ricardo Pablo
[1] Yan-Kai Tzeng,et al. Synthesis of Atomically Thin Hexagonal Diamond with Compression. , 2020, Nano letters.
[2] Omar P. Vilela Neto,et al. Raman spectroscopy analysis of number of layers in mass-produced graphene flakes , 2020 .
[3] A. P. Santos,et al. A semi-automated general statistical treatment of graphene systems , 2020, 2D Materials.
[4] R. D. Rodriguez,et al. The correlation between electrical conductivity and second-order Raman modes of laser-reduced graphene oxide. , 2019, Physical chemistry chemical physics : PCCP.
[5] K. Momeni,et al. Mechanochemistry of Stable Diamane and Atomically Thin Diamond Films Synthesis from Bi- and Multilayer Graphene: A Computational Study , 2019, The Journal of Physical Chemistry C.
[6] H. Mao,et al. Large bandgap of pressurized trilayer graphene , 2019, Proceedings of the National Academy of Sciences.
[7] P. Puech,et al. Low temperature, pressureless sp2 to sp3 transformation of ultrathin, crystalline carbon films , 2019, Carbon.
[8] E. Riedo,et al. Layer dependence of graphene-diamene phase transition in epitaxial and exfoliated few-layer graphene using machine learning , 2019, 2D Materials.
[9] R. Ruoff,et al. Chemically induced transformation of chemical vapour deposition grown bilayer graphene into fluorinated single-layer diamond , 2019, Nature Nanotechnology.
[10] B. Neves,et al. Compression-Induced Modification of Boron Nitride Layers: A Conductive Two-Dimensional BN Compound. , 2018, ACS nano.
[11] E. Riedo,et al. Ultrahard carbon film from epitaxial two-layer graphene , 2018, Nature Nanotechnology.
[12] J. Kong,et al. Raman evidence for pressure-induced formation of diamondene , 2017, Nature Communications.
[13] S. Reich,et al. Precise determination of graphene functionalization by in situ Raman spectroscopy , 2017, Nature Communications.
[14] Zhi-Pan Liu,et al. Graphite to Diamond: Origin for Kinetics Selectivity. , 2017, Journal of the American Chemical Society.
[15] Bo Xu,et al. Recent Advances in Superhard Materials , 2016 .
[16] Kenji Watanabe,et al. Electronic transport of encapsulated graphene and WSe2 devices fabricated by pick-up of prepatterned hBN. , 2015, Nano letters.
[17] P. Sorokin,et al. Converting Chemically Functionalized Few-Layer Graphene to Diamond Films: A Computational Study , 2015 .
[18] G. Kalosakas,et al. Raman spectroscopy of graphene at high pressure: Effects of the substrate and the pressure transmitting media , 2013 .
[19] Yuejian Wang,et al. Crystal structure of graphite under room-temperature compression and decompression , 2012, Scientific Reports.
[20] Stefan Goedecker,et al. Crystal Structure of Cold Compressed Graphite , 2012 .
[21] Konrad Herrmann,et al. Hardness Testing: Principles and Applications , 2011 .
[22] S. Goedecker,et al. Crystal structure of cold compressed graphite. , 2011, Physical review letters.
[23] B. Neves,et al. Room‐Temperature Compression‐Induced Diamondization of Few‐Layer Graphene , 2011, Advanced materials.
[24] A. Balandin. Thermal properties of graphene and nanostructured carbon materials. , 2011, Nature materials.
[25] Ado Jorio,et al. Raman Spectroscopy in Graphene Related Systems , 2011 .
[26] Dianzhong Li,et al. Intrinsic Correlation between Hardness and Elasticity in Polycrystalline Materials and Bulk Metallic Glasses , 2011, 1102.4063.
[27] Yoshiyuki Kawazoe,et al. Low-Temperature Phase Transformation from Graphite to s p 3 Orthorhombic Carbon , 2011 .
[28] L. Chernozatonskii,et al. Influence of Size Effect on the Electronic and Elastic Properties of Diamond Films with Nanometer Thickness , 2011, 1103.6210.
[29] M. M. Lucchese,et al. Evolution of the Raman spectra from single-, few-, and many-layer graphene with increasing disorder , 2010 .
[30] Takashi Miyake,et al. Body-centered tetragonal C4: a viable sp3 carbon allotrope. , 2010, Physical review letters.
[31] J. Coleman,et al. High-pressure Raman spectroscopy of graphene , 2009 .
[32] Hugen Yan,et al. Phonon softening and crystallographic orientation of strained graphene studied by Raman spectroscopy , 2009, Proceedings of the National Academy of Sciences.
[33] Hui Wang,et al. Superhard monoclinic polymorph of carbon. , 2009, Physical review letters.
[34] K. Novoselov,et al. Control of Graphene's Properties by Reversible Hydrogenation: Evidence for Graphane , 2008, Science.
[35] A. Ferrari,et al. Raman spectroscopy of graphene and graphite: Disorder, electron phonon coupling, doping and nonadiabatic effects , 2007 .
[36] S. Louie,et al. Structural and electronic properties of carbon in hybrid diamond-graphite structures , 2005 .
[37] V. Crespi,et al. Collective stabilization of hydrogen chemisorption on graphenic surfaces , 2003 .
[38] Peter J. Eng,et al. Bonding Changes in Compressed Superhard Graphite , 2003, Science.
[39] Anton Kokalj,et al. Computer graphics and graphical user interfaces as tools in simulations of matter at the atomic scale , 2003 .
[40] D. Sánchez-Portal,et al. The SIESTA method for ab initio order-N materials simulation , 2001, cond-mat/0104182.
[41] John Robertson,et al. Resonant Raman spectroscopy of disordered, amorphous, and diamondlike carbon , 2001 .
[42] S. Stuart,et al. A reactive potential for hydrocarbons with intermolecular interactions , 2000 .
[43] M. Hanfland,et al. EQUATION OF STATE OF ICE VII UP TO 106 GPA , 1997 .
[44] J. Badding,et al. Quenchable Transparent Phase of Carbon , 1997 .
[45] Burke,et al. Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.
[46] I. Hutchings,et al. The rôle of particle properties in the erosion of brittle materials , 1996 .
[47] Steve Plimpton,et al. Fast parallel algorithms for short-range molecular dynamics , 1993 .
[48] Utsumi,et al. High-pressure in situ x-ray-diffraction study of the phase transformation from graphite to hexagonal diamond at room temperature. , 1992, Physical review. B, Condensed matter.
[49] Wataru Utsumi And Takehiko Yagi,et al. Light-Transparent Phase Formed by Room-Temperature Compression of Graphite , 1991, Science.
[50] Martins,et al. Efficient pseudopotentials for plane-wave calculations. , 1991, Physical review. B, Condensed matter.
[51] Syassen,et al. Optical reflectivity of graphite under pressure. , 1989, Physical review. B, Condensed matter.
[52] Syassen,et al. Graphite under pressure: Equation of state and first-order Raman modes. , 1989, Physical review. B, Condensed matter.
[53] Peter M. Bell,et al. Calibration of the ruby pressure gauge to 800 kbar under quasi‐hydrostatic conditions , 1986 .
[54] S. Nosé. A unified formulation of the constant temperature molecular dynamics methods , 1984 .
[55] Leonard Kleinman,et al. Efficacious Form for Model Pseudopotentials , 1982 .
[56] Stanley Block,et al. Hydrostatic limits in liquids and solids to 100 kbar , 1973 .
[57] Joseph Callaway,et al. Inhomogeneous Electron Gas , 1973 .
[58] W. Kohn,et al. Self-Consistent Equations Including Exchange and Correlation Effects , 1965 .
[59] H G Drickamer,et al. Carbon: A New Crystalline Phase , 1963, Science.
[60] F. Birch. Finite Elastic Strain of Cubic Crystals , 1947 .
[61] P. Puech,et al. Towards a better understanding of the structure of diamanoïds and diamanoïd/graphene hybrids , 2020 .
[62] A. G. S. Filho,et al. Raman scattering studies of graphene under high pressure , 2017 .
[63] Yoshiyuki Kawazoe,et al. Low-temperature phase transformation from graphite to sp3 orthorhombic carbon. , 2011, Physical review letters.
[64] John W. Anthony,et al. Handbook of mineralogy , 1990 .
[65] P. M. Halleck,et al. Compression and bonding of ice VII and an empirical linear expression for the isothermal compression of solids , 1975 .
[66] S. J. PERRY,et al. Low Temperature , 1881, Nature.