Imprimir Resumo


The 27th AIRAPT International Conference on High Pressure Science and Technology
Abstract

Poster


16:30

Baric evolution of room-temperature structural properties of MAl2Si2 (M=Ca, Ba, Sr)

Authors:
Stamatios Strikos (UFRJ - Universidade Federal do Rio de Janeiro) ; Mohammed El Massalami (UFRJ - Universidade Federal do Rio de Janeiro) ; Boby Joseph (S.C.P.A - Elettra - Sincrotrone Trieste) ; Frederico G. Alabarse (S.C.P.A - Elettra - Sincrotrone Trieste) ; George Valadares (UFAC - Universidade Federal do Acre) ; Deyse G. Costa (UFV - Universidade Federal de Viçosa) ; Rodrigo B. Capaz (UFRJ - Universidade Federal do Rio de Janeiro)

Abstract:

Recently, we studied, both experimentally and theoretically, the thermal and baric evolution of linear-in-field magnetoresistive (LMR) properties of the layered, compensated, and semimetallic CaAl2Si2.1 One of our results indicates that the thermal and baric evolution of LMR curves manifest various transition/ crossover events (based on which a detailed P-T phase diagram was constructed). The origin of these transition/ crossover events is not clear, most probably due to structural or electronic phase transitions.2 To gain more insight on these events, we carried out both theoretical and experimental investigation on the baric evolution of the crystalline and electronic structures of CaAl2Si2 and, for comparison, on all MAl2Si2 (M=Sr, Ba). Theoretically, while the calculated electronic structures (e.g. NEF density of states at EF ) do not manifest any anomalous feature, the ab initio calculations predict a monotonic reduction of the lattice parameters and, in addition, various structural phase transitions: e.g. P-3m1 to I4/mmm at Pc = 8 GPa for M=Ca, P-3m1 to I4/mmm at 5 GPa for M=Sr, and finally Pnma to I4/mmm at 4 GPa for M=Ba. We measured room-temperature pressure-dependent diffractograms up to 9 GPa. With no adjustable parameters, the baric evolution of lattice parameters confirms the corresponding theoretically calculated lattice parameters curves. Nevertheless, no phase transition is observed within the measured pressure range which was limited by the then available beamtime. We discuss the discrepancy regarding the predicted structural phase transitions.