journal article·2014-04-08

Specific Heat of (GeTe)x(Sb2Te3)1–x Phase-Change Materials: The Impact of Disorder and Anharmonicity

Peter Zalden, Karl Simon Siegert, Stéphane Rols, Henry E. Fischer, Franziska Schlich, Te Hu, Matthias Wuttig

Chemistry of Materials· Volume 26· Issue 7
Publisher page

Abstract

Phase-change materials (PCM) are bad glass formers, and their rapid crystallization is accompanied by a drastic change in optical and electrical properties, which opens opportunities for novel nonvolatile data storage devices. Many of these materials are located on the pseudobinary line between GeTe and Sb 2 Te 3 and form a metastable rock-salt-like atomic arrangement in which Te atoms occupy one of the two sublattices and the other is randomly filled with Ge and Sb atoms as well as vacancies. The resulting disorder has profound impact on, for example, transport properties, causing disorder-induced localization of charge carriers. Here we discuss the impact of disorder on thermal properties. We have investigated several PCMs from the pseudobinary line between GeTe and Sb 2 Te 3 . A significant enhancement of the specific heat is found for the disordered rock-salt-like phase compared with the ordered trigonal phase, in which Ge and Sb atoms occupy separate layers. The magnitude of this enhancement is correlated with the fraction of stoichiometric vacancies in the Ge/Sb sublattice. The additional contribution to the specific heat is shown to consist of a reversible fraction and an irreversible fraction, which are attributed to anharmonic lattice dynamics and irreversible vacancy ordering, respectively. These findings underline the prominent role of vacancy ordering in electrical and thermal transport.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Phase-change materials and chalcogenides · Chalcogenide Semiconductor Thin Films · Advanced Thermoelectric Materials and Devices

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

I. Physikalisches Institut (IA), RWTH Aachen University, 52056 Aachen, Germany

Institut Laue-Langevin, 6 rue Jules Horowitz, B.P. 156, 38042 Grenoble cedex 9, France

SLAC, Stanford Institute for Materials and Energy Sciences, 2575 Sand Hill Road, Stanford, California 94025, United States

JARA − Fundamentals of Future Information Technology, RWTH Aachen University, 52056 Aachen, Germany

Funding

Deutsche Forschungsgemeinschaft

References (28)

Show source-provided references
1. Wuttig M. · Nat. Mater. · 2007 · 6 · 82410.1038/nmat2009 ↗
2. Burr G. W. · J. Vac. Sci. Technol., B · 2010 · 28 · 22310.1116/1.3301579 ↗
3. Lencer D. · Adv. Mater. · 2011 · 23 · 203010.1002/adma.201004255 ↗
4. Siegrist T. · Nat. Mater. · 2011 · 10 · 20210.1038/nmat2934 ↗
5. Zhang W. · Nat. Mater. · 2012 · 11 · 95210.1038/nmat3456 ↗
6. Matsunaga T. · Acta Crystallogr. · 2004 · 60 · 68510.1107/S0108768104022906 ↗
7. Wuttig M. · Nat. Mater. · 2007 · 6 · 12210.1038/nmat1807 ↗
8. Matsunaga T. · Jpn. J. Appl. Phys. · 2004 · 43 · 470410.1143/JJAP.43.4704 ↗
9. Sittner E.-R. · Physica Status Solidi (a), · 2013 · 210 · 14710.1002/pssa.201228397 ↗
10. Lyeo H. K. · Appl. Phys. Lett. · 2006 · 89 · 15190410.1063/1.2359354 ↗
11. Matsunaga T. · Inorg. Chem. · 2006 · 45 · 223510.1021/ic051677w ↗
12. Ibach, H.; Lüth, H.Solid-State Physics: An Introduction to Principles of Materials Science,4th ed.Springer:Berlin, 2009; p148.10.1007/978-3-540-93804-0 ↗
13. Höhne, G. W. H.; Hemminger, W. F.; Flammersheim, H.J.Differential Scanning Calorimetry;Springer:Berlin, 2003; p153.10.1007/978-3-662-06710-9 ↗
14. Schwabl, F.Statistische Mechanik;Springer:Berlin, 2006; p89.10.1007/3-540-31097-5 ↗
15. Park I. · Thin Solid Films · 2008 · 517 · 84810.1016/j.tsf.2008.08.194 ↗
16. Kalb J. · J. Appl. Phys. · 2003 · 94 · 490810.1063/1.1610775 ↗
17. Njoroge W. K. · J. Vac. Sci. Technol., A · 2002 · 20 · 23010.1116/1.1430249 ↗
18. Institut Laue-Langevin. Instrumental description of IN4.http://www.ill.eu/instruments-support/instruments-groups/instruments/in4c/description/instrument-layout/(accessed Apr 15, 2013) .
19. Large Array Manipulation Program (LAMP).http://www.ill.eu/instruments-support/computing-for-science/cs-software/all-software/lamp/(accessed March 7, 2014).
20. Reichardt, W.MUPHOCOR: A Fortran Program To Determine the Phonon Density of States from Neutron Scattering Experiments.Primärberichte des Kernforschungszentrums Karlsruhe:Karlsruhe, Germany, 1984.
21. Kuwahara M. · Jpn. J. Appl. Phys. · 2007 · 46 · 390910.1143/JJAP.46.3909 ↗
22. Matsunaga T. · J. Appl. Phys. · 2008 · 103 · 3511
23. Matsunaga T. · Adv. Funct. Mater. · 2011 · 21 · 223210.1002/adfm.201002274 ↗
24. Kolobov A. V. · Nat. Mater. · 2004 · 3 · 70310.1038/nmat1215 ↗
25. Jones, W.; March, N. H.Theoretical Solid State Physics, Vol. 1: Perfect Lattices in Equilibrium;Dover Publications:Mineola, NY, 1985; p237.
26. Sokolov A. P. · J. Phys.: Condens. Matter · 1999 · 11 · A213
27. Orava J. · Nat. Mater. · 2012 · 11 · 27910.1038/nmat3275 ↗
28. Salinga M. · Nat. Commun. · 2013 · 4 · 237110.1038/ncomms3371 ↗