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Volumn 79, Issue 8 PART 2B, 1996, Pages 6013-6015

Negative remanence in magnetic nanostructures

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Indexed keywords


EID: 5244239990     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.362137     Document Type: Article
Times cited : (19)

References (22)
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    • J. I. Gittleman, Y. Goldstein, and Bozowski, Phys. Rev. B 5, 3609 (1972); B. Abeles, P. Sheng, M. D. Couts, and Y. Arie, Adv. Phys. 24, 407 (1975); B. Abeles, H. L. Pinch, and J. I. Gittleman, Phys. Rev. Lett. 35, 247 (1975).
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    • J. I. Gittleman, Y. Goldstein, and Bozowski, Phys. Rev. B 5, 3609 (1972); B. Abeles, P. Sheng, M. D. Couts, and Y. Arie, Adv. Phys. 24, 407 (1975); B. Abeles, H. L. Pinch, and J. I. Gittleman, Phys. Rev. Lett. 35, 247 (1975).
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  • 4
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    • note
    • A remanent magnetic field is usually positive in a superconductor due to the trapped flux. But this trapped positive field in the superconducting solenoid could lead to a negative field of the order of 10 G in the sample space. This can cause error due to a finite dM/dH. In our experiments, Pd standard was measured subsequently and the results shown in the insert of Fig. 1 was after the field correction. However, we are not absolutely sure if such a correction is sufficient due to the remaining field error of about 1.5 G in our set-up and a large dM/dH for the sample than the Pd standard.
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    • Y. Xu, B. Zhao, and X. Yan, this conference
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    • Ph.D. Thesis, University of Nabraska, Lincoln
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    • note
    • The same results can be obtained by considering bound current density at the interfaces.


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