Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
Thermoelectric Properties of Fe0.2Co3.8Sb12-xTex ... - Physics
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Sharp Raman anomalies and broken adiabaticity at a pressure induced<br />
transition from band to topological insulator in Sb 2 Se 3<br />
Achintya Bera 1 , Koushik Pal 2, 3 , D. V. S. Muthu 1 , Somaditya Sen 4 , Prasenjit Guptasarma 4 ,<br />
U. V. Waghmare 3 , and A. K. Sood 1<br />
1 Department <strong>of</strong> <strong>Physics</strong>, Indian Institute <strong>of</strong> Science, Bangalore-560012, India<br />
2 Chemistry and <strong>Physics</strong> <strong>of</strong> Materials Unit, Jawaharlal Nehru Centre for Advanced Scientific<br />
Research, Bangalore-560064, India<br />
3 Theoretical Sciences Unit, Jawaharlal Nehru Centre for Advanced Scientific Research,<br />
Bangalore-560064, India and<br />
4 Department <strong>of</strong> <strong>Physics</strong>, University <strong>of</strong> Wisconsin-Milwaukee, Wisconsin-53211, USA<br />
Recently discovered three-dimensional Topological insulators (TI) have attracted a lot <strong>of</strong><br />
attention <strong>of</strong> researchers from diverse backgrounds due to robust and exotic phenomena, such<br />
as quantum spin Hall states, arise from the geometric and topological properties <strong>of</strong> the<br />
manifold <strong>of</strong> their electronic states. However, experimental evidence for nontrivial topology <strong>of</strong><br />
electronic states is so far mainly based on the time-reversal symmetry protected chiral surface<br />
states. Signatures <strong>of</strong> the nontrivial topology <strong>of</strong> a TI in its bulk behaviour are subtle, and not<br />
yet identified. Our work presented here establishes that (a) bulk signatures <strong>of</strong> the electronic<br />
topology become significant and detectable as anomalies in the phonon frequency and<br />
linewidth <strong>of</strong> E g Raman mode at an electronic topological transition (specifically in single<br />
crystal Sb 2 Se 3 ), (b) their origin lies in physical mechanisms that involve going beyond<br />
adiabatic approximation as a metallic (vanishing gap) state <strong>of</strong> the bulk appears at the<br />
transition, and (c) they involve electron-phonon couplings some <strong>of</strong> which are not captured by<br />
the standard methods to calculate electronic structure.<br />
References:<br />
[1] Zhang, H. et al. “Topological insulators in Bi 2 Se 3 , Bi 2 Te 3 and Sb 2 Te 3 with a single Dirac<br />
cone on the surface”. Nature Phys. 5, 438-442 (2009).<br />
[2] G.K. Pradhan et al. “Raman signatures <strong>of</strong> pressure induced electronic topological and<br />
structural transitions in Bi 2 Te 3 ”. Solid State Commun. 152, 284–287 (2012)