Encyclopedie de la recherche sur l'aluminium au Quebec - Edition 2014 | Page 53

TRANSFORMATION ET mechanical//pressure Effect of high APPLICATIONS TRANSFORMATION AND APPLICATIONS and temperature on the plasmon L'EFFET DE LA PRESSION MÉCANIQUE energy of aluminum L'ÉNERGIE DE PLASMON DE ÉLEVÉE ET DE LA TEMPÉRATURE SUR L'ALUMINIUM L’effet de la pression mécanique EFFECT OF HIGH MECHANICAL PRESSURE AND élevée et de la température sur TEMPERATURE ON THE PLASMON ENERGY OF ALUMINUM l'énergie de plasmon de l'aluminium 51 M. Attarian Shandiz and R. Gauvin Department of Materials Engineering, McGill University, Montreal, Quebec, Canada, H3A 0C5. Introduction Model DFT calculations Plasmon excitations, originating from the collective oscillations of the valence electrons in reply to an applied electric field, are the key characteristic of low-loss electron energy loss spectroscopy (EELS) [1]. Plasmon energy is associated with the density of valence electrons and so it can be used to monitor electronic structure of material. There are many studies connecting the plasmon energy to the measurement of other physical and mechanical properties [2]. The mechanical properties such as Young modules have been measured in a clear relationship with plasmon energy [2]. Hence, understanding the effect of physical and thermodynamical parameters on the plasmon energy can be helpful for the investigation of many other electronic structure-related properties of materials. By combination of the free electron model and the equation of state (EOS) based on the pseudo-spinodal theory by Banzona et al [], the pressure and temperature dependency of the plasmon energy was modeled. The EOS suggested by Banoza et al [3] based on pseudo-spinodal method offers a precise EOS for a vast range of temperature and pressure for the solids. The temperature and pressure dependency of plasmon energy can be explained according to our model [4] as: The volume change of crystal is the main reason responsible for the change of valence electron density and plasmon energy in the free electron model. So, to introduce the effect of temperature and pressure for the density functional theory (DFT) calculations of plasmon energy, the temperature and pressure dependency of lattice parameter was employed. In this study, DFT calculations were performed with full potential linear augmented plane wave (FLAPW) method using WIEN2k code [5]. Optical properties and energy loss function (ELF) were computed by the code via random phase approximation (RPA) based on the work of Ambrosch-Draxl and Sofo [6]. Al 15 20 10 5 14 15 16 Energy Loss (eV) 25 0.2 10 K 223 K 473 K 773 K a) 0 13 ' ' G B0 P 3B0 0 N t k B E   B0  B0V0 (eE /T  1) 17 The change in energy loss function of Al by variation of temperature 0 -0.2 -0.4 0 b) Im(-1/) ELF 20 Q(T , P )  1 Ep(eV) Results  1 Q(T2 , P2 )1   Q1 (T1, P1 )1      exp  ' 2  E p (T1, P ) B0 (  1  1) 1   E p (T2 , P2 ) Abe et al Moorthy and Howe DFT calculations 200 400 T (K) 15 10 5 600 0 0 800 The comparison between the results of difference in the plasmon energy from DFT calculations and experiments for Al. Results Al c) 0 GPa 10.7 GPa 30.8 GPa 69.6 GPa 147.5 GPa 10 20 Energy Loss (eV) 30 The change in energy loss function of Al by variation of pressure Conclusion Temperature and pressure dependency of plasmon energy of aluminum can successfully explained based on the results of free electron model and pseudo-spinodal equation of states. DFT calculations based on the lattice parameters variation can also predict the variation of plasmon energy accurately. M. Attarian Shandiz Raynald Gauvin Département de génie des matériaux, Université McGill References Contour plots of difference in valence electron density (Δn) in (1 0 0) plane of Al for a) V/V0=1, b) V/V0=0.8 c) V/V0=0.7 and d) V/V0=0.6 Plasmon energy variation by temperature and pressure according to the results of developed model. [1] R.F. Egerton, Electron Energy-Loss Spectroscopy in the Electron Microscope, third ed. (Springer, New York, 2011). [2] V. P. Oleshko, M. Murayama, J. M. Howe, Microsc. Microanal. 8, 350 (2002). [3] V. G. Baonza, M. Cáceres , J. Núñez, Phys. Rev. B 51, 28 (1995). [4] M. Attarian Shandiz , R. Gauvin, J. Appl. Phys. 116, 163501 (2014) [5] P. Blaha,et al, WIEN2K: An Augmented Plane Wave Plus Local Orbitals Program for Calculating Crystal Properties (2001). [6] C. Ambrosch-Draxl, J. O. Sofo, Comp. Phys. Comm. 175, 1 (2006). Journée des étudiants – REGAL of the free electron model and the equation of state based on the By combination En combinant le modèle des électrons libres et l'équation d'état basée sur la théorie pseudo-spinodale, l’effet de la pression et de la température sur la 18 novembre 2014 dépendance énergétique des plasmons de l'aluminium a été modélisé. P