journal article·2015-09

Self‐Assembled Epitaxial Core–Shell Nanocrystals with Tunable Magnetic Anisotropy

Sheng‐Chieh Liao, Yong‐Lun Chen, Wei‐Cheng Kuo, Jeffrey Cheung, Wei‐Cheng Wang, Xuan Cheng, Yi‐Ying Chin, Yu‐Ze Chen, Heng‐Jui Liu, Hong‐Ji Lin, Chien‐Te Chen, Jeng‐Yih Juang, Yu‐Lun Chueh, Valanoor Nagarajan, Ying‐Hao Chu, Chih‐Huang Lai

Small· Volume 11· Issue 33
Publisher page

Abstract

Epitaxial core-shell CoO-CoFe2 O4 nanocrystals are fabricated by using pulsed laser deposition with the aid of melted material (Bi2 O3 ) addition and suitable lattice mismatch provided by substrates (SrTiO3 ). Well aligned orientations among nanocrystals and reversible core-shell sequence reveal tunable magnetic anisotropy. The interfacial coupling between core and shell further engineers the nanocrystal functionality.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Multiferroics and related materials · Copper-based nanomaterials and applications · Magnetic Properties and Synthesis of Ferrites

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

Affiliations

Department of Materials Science & Engineering National Tsing Hua University Hsinchu 30013 Taiwan

Department of Materials Science & Engineering National Chiao Tung University Hsinchu 30010 Taiwan

Department of Electrophysics National Chiao Tung University Hsinchu 30010 Taiwan

School of Materials Science and Engineering University of New South Wales Sydney 2052 Australia

Graduate Program for Science and Technology of Accelerator Light Source National Chiao Tung University Hsinchu 30010 Taiwan

National Synchrotron Radiation Research Center Hsinchu 30076 Taiwan

References (27)

Show source-provided references
1. 10.1021/jp027835b10.1021/jp027835b ↗
2. 10.1021/ja036174910.1021/ja0361749 ↗
3. 10.1088/0957-4484/21/1/01530210.1088/0957-4484/21/1/015302 ↗
4. 10.1002/smll.20110115710.1002/smll.201101157 ↗
5. 10.1002/adma.20100026010.1002/adma.201000260 ↗
6. 10.1021/nl101181e10.1021/nl101181e ↗
7. 10.1021/ja067422e10.1021/ja067422e ↗
8. 10.1021/ja071428210.1021/ja0714282 ↗
9. 10.1103/PhysRevB.78.17441410.1103/PhysRevB.78.174414 ↗
10. 10.1103/PhysRevLett.99.14720110.1103/PhysRevLett.99.147201 ↗
11. 10.1021/cm202895910.1021/cm2028959 ↗
12. 10.1103/PhysRevLett.84.610210.1103/PhysRevLett.84.6102 ↗
13. 10.1021/nl501917210.1021/nl5019172 ↗
14. 10.1103/PhysRevLett.103.25610310.1103/PhysRevLett.103.256103 ↗
15. 10.1002/adfm.20120106610.1002/adfm.201201066 ↗
16. 10.1103/PhysRevB.35.684710.1103/PhysRevB.35.6847 ↗
17. Goldman A. · 1990
18. 10.1063/1.170282010.1063/1.1702820 ↗
19. 10.1007/BF0266730610.1007/BF02667306 ↗
20. 10.1063/1.476674810.1063/1.4766748 ↗
21. 10.1021/nn101012310.1021/nn1010123 ↗
22. 10.1016/0022-5088(81)90004-710.1016/0022-5088(81)90004-7 ↗
23. 10.1080/1040843970824125910.1080/10408439708241259 ↗
24. 10.1007/s12274-010-1001-910.1007/s12274-010-1001-9 ↗
25. 10.1109/TMAG.2012.220088410.1109/TMAG.2012.2200884 ↗
26. The interface‐to‐ferrimagnetic volume‐ratio (S = Ainter/VFiM) of type I nanocrystals is calculated by following equation: whererandbrepresent theVcore/Vshelland length of 100] edge of core–shell nanocrystals respectively.
27. 10.1016/j.physrep.2005.08.00410.1016/j.physrep.2005.08.004 ↗