High frequency impedance inverse in MTJ junction
| dc.citation.epage | 1904 | en_US |
| dc.citation.issue | 2 | en_US |
| dc.citation.spage | 1903 | en_US |
| dc.citation.volume | 310 | en_US |
| dc.citation.woscount | 0 | |
| dc.contributor.author | Hsieh, L. C. | en_US |
| dc.contributor.author | Huang, Y. W. | en_US |
| dc.contributor.author | Han, X. F. | en_US |
| dc.contributor.author | Zeng, Z. M. | en_US |
| dc.contributor.author | Chien, W. C. | en_US |
| dc.contributor.author | Peng, T. Y. | en_US |
| dc.contributor.author | Lo, C. K. | en_US |
| dc.contributor.author | Yao, Y. D. | en_US |
| dc.contributor.department | 材料科學與工程學系 | zh_TW |
| dc.contributor.department | Department of Materials Science and Engineering | en_US |
| dc.date.accessioned | 2014-12-08T15:14:33Z | |
| dc.date.available | 2014-12-08T15:14:33Z | |
| dc.date.issued | 2007-03-01 | en_US |
| dc.description.abstract | The magnetoimpedance effect of magnetic tunnel junction ( MTJ) was investigated at room temperature in the frequency ranged from 100 Hz to 15 MHz. The MR loop with a ratio of 9.49% at 5MHz switches to - 11.51% at 7 MHz, respectively. This indicates the MR loop reverse shape and sign around 6 MHz. This inverse MR effect is explained by the impedance competition among Resistor- Inductor series circuit and Capacitor part. (c) 2006 Elsevier B. V. All rights reserved. | en_US |
| dc.identifier.doi | 10.1016/j.jmmm.2006.10.1097 | en_US |
| dc.identifier.issn | 0304-8853 | en_US |
| dc.identifier.journal | JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS | en_US |
| dc.identifier.uri | http://dx.doi.org/10.1016/j.jmmm.2006.10.1097 | en_US |
| dc.identifier.uri | https://ir.lib.nycu.edu.tw/handle/11536/11065 | |
| dc.identifier.wosnumber | WOS:000247720400007 | |
| dc.language.iso | en_US | en_US |
| dc.subject | MTJ | en_US |
| dc.subject | inverse | en_US |
| dc.subject | impedance | en_US |
| dc.title | High frequency impedance inverse in MTJ junction | en_US |
| dc.type | Article | en_US |