Crystal Structure of Cold Compressed Graphite

: Through a systematic structural search we found an allotrope of carbon with Cmmm symmetry which we predict to be more stable than graphite for pressures above 10 GPa. This material, which we refer to as Z-carbon, is formed by pure sp(3) bonds and it provides an explanation to several features in experimental x-ray diffraction and Raman spectra of graphite under pressure. The transition from graphite to Z-carbon can occur through simple sliding and buckling of graphene sheets. Our calculations predict that Z-carbon is a transparent wide band-gap semiconductor with a hardness comparable to diamond.

[1]  Peter J. Eng,et al.  Bonding Changes in Compressed Superhard Graphite , 2003, Science.

[2]  Zhao,et al.  X-ray diffraction data for graphite to 20 GPa. , 1989, Physical review. B, Condensed matter.

[3]  Franccois Bottin,et al.  Large scale ab initio calculations based on three levels of parallelization , 2007, 0707.3405.

[4]  G. Scuseria,et al.  Restoring the density-gradient expansion for exchange in solids and surfaces. , 2007, Physical review letters.

[5]  W. Aulbur,et al.  Quasiparticle calculations in solids , 2000 .

[6]  S. Goedecker Minima hopping: an efficient search method for the global minimum of the potential energy surface of complex molecular systems. , 2004, The Journal of chemical physics.

[7]  S. Goedecker,et al.  Relativistic separable dual-space Gaussian pseudopotentials from H to Rn , 1998, cond-mat/9803286.

[8]  P. Loubeyre,et al.  Properties of diamond under hydrostatic pressures up to 140 GPa , 2003, Nature materials.

[9]  Hui Wang,et al.  Superhard monoclinic polymorph of carbon. , 2009, Physical review letters.

[10]  Takashi Miyake,et al.  Body-centered tetragonal C4: a viable sp3 carbon allotrope. , 2010, Physical review letters.

[11]  Wataru Utsumi And Takehiko Yagi,et al.  Light-Transparent Phase Formed by Room-Temperature Compression of Graphite , 1991, Science.

[12]  Artem R. Oganov Modern Methods of Crystal Structure Prediction: OGANOV:CRYSTAL - METHODS O-BK , 2010 .

[13]  Stefan Goedecker,et al.  Crystal structure prediction using the minima hopping method. , 2010, The Journal of chemical physics.

[14]  Xavier Gonze,et al.  A brief introduction to the ABINIT software package , 2005 .

[15]  S. Louie,et al.  Structural and electronic properties of carbon in hybrid diamond-graphite structures , 2005 .

[16]  R. Baughman,et al.  A carbon phase that graphitizes at room temperature , 1997 .

[17]  F. P. Bundy,et al.  Hexagonal Diamond—A New Form of Carbon , 1967 .

[18]  Xavier Gonze,et al.  Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional perturbation theory , 1997 .

[19]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[20]  A. Kuznetsov,et al.  Raman scattering from turbostratic graphitelike BC4 under pressure , 2007 .

[21]  Artem R. Oganov,et al.  Modern methods of crystal structure prediction , 2011 .

[22]  David N. Jamieson,et al.  The Raman spectrum of nanocrystalline diamond , 2000 .

[23]  Yoshiyuki Kawazoe,et al.  Low-Temperature Phase Transformation from Graphite to s p 3 Orthorhombic Carbon , 2011 .

[24]  Syassen,et al.  Graphite under pressure: Equation of state and first-order Raman modes. , 1989, Physical review. B, Condensed matter.

[25]  Pekka Koskinen,et al.  Structural relaxation made simple. , 2006, Physical review letters.

[26]  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.

[27]  Siyuan Zhang,et al.  Hardness of covalent crystals. , 2003, Physical review letters.