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Meisenheimer PB, Steinhardt RA, Sung SH, Williams LD, Zhuang S, Nowakowski ME, Novakov S, Torunbalci MM, Prasad B, Zollner CJ, Wang Z, Dawley NM, Schubert J, Hunter AH, Manipatruni S, Nikonov DE, Young IA, Chen LQ, Bokor J, Bhave SA, Ramesh R, Hu JM, Kioupakis E, Hovden R, Schlom DG, Heron JT. Engineering new limits to magnetostriction through metastability in iron-gallium alloys. Nat Commun 2021; 12:2757. [PMID: 33980848 PMCID: PMC8115637 DOI: 10.1038/s41467-021-22793-x] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/21/2020] [Accepted: 03/30/2021] [Indexed: 11/09/2022] Open
Abstract
Magnetostrictive materials transduce magnetic and mechanical energies and when combined with piezoelectric elements, evoke magnetoelectric transduction for high-sensitivity magnetic field sensors and energy-efficient beyond-CMOS technologies. The dearth of ductile, rare-earth-free materials with high magnetostrictive coefficients motivates the discovery of superior materials. Fe1-xGax alloys are amongst the highest performing rare-earth-free magnetostrictive materials; however, magnetostriction becomes sharply suppressed beyond x = 19% due to the formation of a parasitic ordered intermetallic phase. Here, we harness epitaxy to extend the stability of the BCC Fe1-xGax alloy to gallium compositions as high as x = 30% and in so doing dramatically boost the magnetostriction by as much as 10x relative to the bulk and 2x larger than canonical rare-earth based magnetostrictors. A Fe1-xGax - [Pb(Mg1/3Nb2/3)O3]0.7-[PbTiO3]0.3 (PMN-PT) composite magnetoelectric shows robust 90° electrical switching of magnetic anisotropy and a converse magnetoelectric coefficient of 2.0 × 10-5 s m-1. When optimally scaled, this high coefficient implies stable switching at ~80 aJ per bit.
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Affiliation(s)
- P B Meisenheimer
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, USA
| | - R A Steinhardt
- Department of Materials Science and Engineering, Cornell University, Ithaca, NY, USA
| | - S H Sung
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, USA
| | - L D Williams
- Department of Materials Design and Innovation, University at Buffalo - The State University of New York, Buffalo, NY, USA
| | - S Zhuang
- Department of Materials Science and Engineering, University of Wisconsin-Madison, Madison, WI, USA
| | - M E Nowakowski
- Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, CA, USA
| | - S Novakov
- Department of Physics, University of Michigan, Ann Arbor, MI, USA
| | - M M Torunbalci
- OxideMEMS Lab, Purdue University, West Lafayette, IN, USA
| | - B Prasad
- Department of Materials Science and Engineering, University of California, Berkeley, CA, USA
| | - C J Zollner
- School of Applied and Engineering Physics, Cornell University, Ithaca, NY, USA
| | - Z Wang
- School of Applied and Engineering Physics, Cornell University, Ithaca, NY, USA
| | - N M Dawley
- Department of Materials Science and Engineering, Cornell University, Ithaca, NY, USA
| | - J Schubert
- Peter Grünberg Institute (PGI-9) and JARA Fundamentals of Future Information Technology, Forschungszentrum Jülich GmbH, Jülich, Germany
| | - A H Hunter
- Michigan Center for Materials Characterization, University of Michigan, Ann Arbor, MI, USA
| | - S Manipatruni
- Components Research, Intel Corporation, Hillsboro, OR, USA
| | - D E Nikonov
- Components Research, Intel Corporation, Hillsboro, OR, USA
| | - I A Young
- Components Research, Intel Corporation, Hillsboro, OR, USA
| | - L Q Chen
- Department of Materials Science and Engineering, Penn State University, State College, PA, USA
| | - J Bokor
- Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, CA, USA
| | - S A Bhave
- OxideMEMS Lab, Purdue University, West Lafayette, IN, USA
| | - R Ramesh
- Department of Materials Science and Engineering, University of California, Berkeley, CA, USA.,Materials Sciences Division, Lawrence Berkeley National Laboratory, CA, USA.,Department of Physics, University of California, Berkeley, CA, USA
| | - J-M Hu
- Department of Materials Science and Engineering, University of Wisconsin-Madison, Madison, WI, USA
| | - E Kioupakis
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, USA
| | - R Hovden
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, USA
| | - D G Schlom
- Department of Materials Science and Engineering, Cornell University, Ithaca, NY, USA.,Kavli Institute at Cornell for Nanoscale Science, Ithaca, NY, USA.,Leibniz-Institut für Kristallzüchtung, Max-Born-Str. 2, Berlin, Germany
| | - J T Heron
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, USA.
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Hunter AH, Araullo-Peters V, Gibbons M, Restrepo OD, Niezgoda SR, Windl W, Flores KM, Hofmann DC, Marquis EA. Three-dimensional imaging of shear bands in bulk metallic glass composites. J Microsc 2016; 264:304-310. [PMID: 27513447 DOI: 10.1111/jmi.12443] [Citation(s) in RCA: 8] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/29/2016] [Revised: 05/17/2016] [Accepted: 06/08/2016] [Indexed: 11/30/2022]
Abstract
The mechanism of the increase in ductility in bulk metallic glass matrix composites over monolithic bulk metallic glasses is to date little understood, primarily because the interplay between dislocations in the crystalline phase and shear bands in the glass could neither be imaged nor modelled in a validated way. To overcome this roadblock, we show that shear bands can be imaged in three dimensions by atom probe tomography from density variations in the reconstructed atomic density, which density-functional theory suggests being a local-work function effect. Imaging of near-interface shear bands in Ti48 Zr20 V12 Cu5 Be15 bulk metallic glass matrix composite permits measurement of their composition, thickness, branching and interactions with the dendrite interface. These results confirm that shear bands here nucleate from stress concentrations in the glass due to intense, localized plastic deformation in the dendrites rather than intrinsic structural inhomogeneities.
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Affiliation(s)
- A H Hunter
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, Michigan, U.S.A
| | - V Araullo-Peters
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, Michigan, U.S.A
| | - M Gibbons
- Department of Materials Science and Engineering, The Ohio State University, Columbus, Ohio, U.S.A
| | - O D Restrepo
- Department of Materials Science and Engineering, The Ohio State University, Columbus, Ohio, U.S.A
| | - S R Niezgoda
- Department of Materials Science and Engineering, The Ohio State University, Columbus, Ohio, U.S.A
| | - W Windl
- Department of Materials Science and Engineering, The Ohio State University, Columbus, Ohio, U.S.A
| | - K M Flores
- Department of Mechanical Engineering and Materials Science, Institute of Materials Science and Engineering, Washington University, St. Louis, Missouri, U.S.A
| | - D C Hofmann
- Jet Propulsion Laboratory/California Institute of Technology, Pasadena, California, U.S.A
| | - E A Marquis
- Department of Materials Science and Engineering, University of Michigan, Ann Arbor, Michigan, U.S.A
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Abstract
Acid and alkali secretion have been examined together with prostaglandin E2 production in response to two mucosal protective drugs, colloidal bismuth subcitrate and sucralfate. Doses of colloidal bismuth subcitrate in the therapeutic range (120 and 1200 mg) had no effect on alkali secretion or luminal PGE2 output when perfused into the stomach of human volunteers. Similarly, in the anaesthetised rat, neither gastric acid nor duodenal alkali secretions were influenced by iv (12 mg/kg) or topical (120 mg/ml) administration of colloidal bismuth subcitrate. In contrast, perfusion of the human stomach with 1 g sucralfate stimulated bicarbonate output by 50%, a response which was unaffected by indomethacin (25 mg/h). A rise of 64% in gastric PGE2 output after sucralfate was, however, prevented by indomethacin pretreatment. Alkali secretion by rat duodenum was also increased by sucralfate but the response depended on the basal secretory rate. Low basal secretors (less than 3 mumol) showed a 75% stimulation whereas rats with high basal secretory rates (greater than 3 mumol) showed no significant response. All duodenal preparations regardless of basal secretory rate showed a stimulation of bicarbonate output with topical PGE2. The results suggest that enhancement of gastroduodenal bicarbonate secretion may play a role in the protective action of sucralfate but is unlikely to explain mucosal protection by colloidal bismuth subcitrate.
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Affiliation(s)
- C J Shorrock
- Department of Gastroenterology, Hope Hospital, University of Manchester School of Medicine, Salford
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