Apr 23, 2024
3:45pm - 4:00pm
Room 343, Level 3, Summit
Yorick Birkholzer1,Anna Park1,Noah Schnitzer1,Evan Krysko1,Jacob Steele1,Hebatalla Elnaggar2,Jelle Ruiters3,Koen Draijer4,Masoud Lazemi4,Qijun Che4,Shigeki Yamada5,Taka-hisa Arima6,Frank de Groot4,David Muller1,Darrell Schlom1,7
Cornell University1,Sorbonne Université2,University of Twente3,University of Utrecht4,Yokohama City University5,University of Tokyo6,Leibniz-Institut für Kristallzüchtung7
Yorick Birkholzer1,Anna Park1,Noah Schnitzer1,Evan Krysko1,Jacob Steele1,Hebatalla Elnaggar2,Jelle Ruiters3,Koen Draijer4,Masoud Lazemi4,Qijun Che4,Shigeki Yamada5,Taka-hisa Arima6,Frank de Groot4,David Muller1,Darrell Schlom1,7
Cornell University1,Sorbonne Université2,University of Twente3,University of Utrecht4,Yokohama City University5,University of Tokyo6,Leibniz-Institut für Kristallzüchtung7
For the realization of the next generation of fast, energy-efficient nanoelectronics, there is a great need for new materials whose electrical and optical conductivities can be sensitively tuned between high (on) and low (off) states by altering a thermodynamic control parameter such as strain or temperature. Unfortunately, most materials are either metallic or insulating and their conductivities cannot be changed substantially. Materials exhibiting a metal-insulator transition (MIT) above room temperature are quite rare, limiting their applicability in devices.<br/><br/>One noteworthy example of such a material is the A-site layer-ordered double perovskite SmBaMn<sub>2</sub>O<sub>6</sub>. While its synthesis in bulk form was reported by Yamada <i>et al.</i> [1], the successful growth of SmBaMn<sub>2</sub>O<sub>6</sub> thin films remained elusive for over a decade. Here, we demonstrate the growth of untwinned epitaxial thin films of phase-pure SmBaMn<sub>2</sub>O<sub>6 </sub>on various single-crystalline oxide substrates using molecular-beam epitaxy (MBE), exploring a wide range of tensile to compressive biaxial strains. The latter has been predicted to host a different ground state based on first-principles calculations by Nowadnick <i>et al. </i>[2]<i>.</i><br/><br/>To stabilize the A-site layer-ordered double perovskite phase, we employ a two-step approach as originally described by Millange <i>et al.</i> for LaBaMn<sub>2</sub>O<sub>6</sub> bulk crystals [3]. The key elements are, first, a high-temperature synthesis step of a brownmillerite-like, oxygen-deficient precursor, and second, a topotactic oxidation at low temperature. Notably, the former requires temperatures higher than 1100 °C that are unattainable in conventional oxide MBE systems. In this study, we utilize a recently installed, high-power CO<sub>2</sub>-laser-based substrate heater at the PARADIM user facility at Cornell University, which allows growth temperatures up to 2000 °C.<br/><br/>Ongoing efforts entail the comprehensive investigation of the structural and spectroscopic properties of epitaxial SmBaMn<sub>2</sub>O<sub>6</sub> thin films as a function of temperature and strain. To this end, we are employing an ensemble of X-ray, optical, and electrical transport techniques, alongside scanning transmission electron microscopy and electron energy-loss spectroscopy. Our aim is to elucidate potential hidden ground states and coupled structural, magnetic, and electronic phase transitions in this MIT compound.<br/><br/><b>References:</b><br/>[1] Yamada, Maeda, Arima, “Successive Electronic Transitions and Anisotropic Properties in a Double-Perovskite SmBaMn<sub>2</sub>O<sub>6</sub> Single Crystal”, <i>J. Phys. Soc. Jpn. </i><b>2012</b>, 81, 113711<br/>[2] Nowadnick, He, Fennie, “Coupled structural distortions, domains, and control of phase competition in polar SmBaMn<sub>2</sub>O<sub>6</sub>”, <i>Phys. Rev. B</i> <b>2019</b>, 100, 195129<br/>[3] Millange, Caignaert, Domengès, Raveau, Suard, “Order-Disorder Phenomena in New LaBaMn<sub>2</sub>O<sub>6-x</sub> CMR Perovskites. Crystal and Magnetic Structure”, <i>Chem. Mater</i> <b>1998</b>, 10, 1974-1983