Understanding first-order Raman spectra of boron carbides across the homogeneity range
- 1. Univ Paris Saclay, CEA, Serv Rech Met Phys, F-91191 Gif Sur Yvette, (France)
- 2. CNRS, Lab Anal et Architecture Syst, F-31031 Toulouse 4, (France)
- 3. Inst Polytech Paris, Ecole Polytech, CNRS, Lab Solides Irradies, CEA DRF IRAMIS, F-91120 Palaiseau, (France)
- 4. Univ Paris Saclay, CEA, Lab Jannus, Serv Rech Met Phys, F-91191 Gif Sur Yvette, (France)
Description
Boron carbide, a lightweight, high temperature material, has various applications as a structural material and as a neutron absorber. The large solubility range of carbon in boron, between ≅ to 9 percent and 20 percent, has been theoretically explained by some of us by the thermodynamical stability of three icosahedral phases at low temperature, with respective carbon atomic concentrations: 8.7 percent (B10.5C, named OPO1), 13.0 percent (B6.7C, named OPO2), whose theoretical Raman spectra are still unknown, and 20 percent (B4C), from which the nature of some of the Raman peaks are still debated. We report theoretical and experimental results of the first-order, nonresonant, Raman spectrum of boron carbide. Density functional perturbation theory enables us to obtain the Raman spectra of the OPO1 and OPO2 phases, which are perfectly ordered structures with however a complex crystalline motif of 414 atoms, due to charge compensation effects. Moreover, for the carbon-rich B4C, with a simpler 15-atom unit cell, we study the influence of the low energy point defects and of their concentrations on the Raman spectrum, in connection with experiments, thus providing insights into the sensitivity of experimental spectra to sample preparation, experimental conditions, and setup. In particular, this enables us to propose a new structure at 19.2 percent atomic carbon concentration, B4.2C, that, within the local density approximation of density functional theory (DFT-LDA), lies very close to the convex hull of boron carbide, on the carbon-rich side. This new phase, derived from what we name the '3+1' defect complex, helps in reconciling the experimentally observed Raman spectrum with the theory around 1000 cm-1. Finally, we predict the intensity variations induced by the experimental geometry and quantitatively assess the localization of bulk and defect vibrational modes and their character, with an analysis of 'chain' and 'icosahedral' modes. (authors)
Availability note (English)
Available from doi: http://dx.doi.org/10.1103/PhysRevMaterials.5.063601Additional details
Identifiers
Publishing Information
- Journal Title
- Physical Review Materials
- Journal Volume
- 5
- Journal Issue
- no.6
- Journal Page Range
- p. 063601.1-063601.18
- ISSN
- 2475-9953
INIS
- Country of Publication
- United States
- Country of Input or Organization
- France
- INIS RN
- 55070718
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- APPROXIMATIONS; BORON; BORON CARBIDES; CARBON; DEFECTS; DENSITY FUNCTIONAL METHOD; GEOMETRY; PHASE STABILITY; POINT DEFECTS; RAMAN EFFECT; RAMAN SPECTRA; SAMPLE PREPARATION; SOLUBILITY
- Descriptors DEC
- BORON COMPOUNDS; CALCULATION METHODS; CARBIDES; CARBON COMPOUNDS; CRYSTAL DEFECTS; CRYSTAL STRUCTURE; ELEMENTS; MATHEMATICS; NONMETALS; SEMIMETALS; SPECTRA; STABILITY; VARIATIONAL METHODS
Optional Information
- Notes
- 56 refs.