001     56059
005     20180211162411.0
024 7 _ |2 DOI
|a 10.1143/JJAP.45.L416
024 7 _ |2 WOS
|a WOS:000237571200022
037 _ _ |a PreJuSER-56059
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Applied
100 1 _ |a Fukushima, T.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a Spinodal decomposition under layer by layer growth condition and high Curie temperature quasi-one-dimensional nano-structure in dilute magnetic semiconductors
260 _ _ |a Tokyo
|b Inst. of Pure and Applied Physics
|c 2006
300 _ _ |a
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|0 0
|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Japanese Journal of Applied Physics Part 2: Letters
|x 0021-4922
|0 8483
|y 12
|v 45
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a We show that spinodal decomposition under layer by layer crystal growth condition leads to characteristic quasi-one-dimensional nano-structures in dilute magnetic semiconductors (DMS). It is found that the DMS systems can form rather large clusters with highly anisotropic shape even for low concentrations. It is suggested that the blocking phenomena in the super-paramagnetism, the magnetic dipole-dipole interaction and the network of the one-dimensional structures should be considered to understand the magnetism in DMS. Based on the present simulations, we propose that the delta-doping method can be effective approach to realize high Curie temperature.
536 _ _ |a Kondensierte Materie
|c P54
|2 G:(DE-HGF)
|0 G:(DE-Juel1)FUEK414
|x 0
588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
653 2 0 |2 Author
|a dilute magnetic semiconductor
653 2 0 |2 Author
|a spinodal decomposition
653 2 0 |2 Author
|a layer by layer growth
653 2 0 |2 Author
|a one-dimensional structure
653 2 0 |2 Author
|a super-paramagnetism
653 2 0 |2 Author
|a blocking phenomena
653 2 0 |2 Author
|a magnetic anisotropy
653 2 0 |2 Author
|a dipole-dipole interaction
700 1 _ |a Sato, K.
|b 1
|0 P:(DE-HGF)0
700 1 _ |a Katayama-Yoshida, H.
|b 2
|0 P:(DE-HGF)0
700 1 _ |a Dederichs, P. H.
|b 3
|u FZJ
|0 P:(DE-Juel1)130612
773 _ _ |a 10.1143/JJAP.45.L416
|g Vol. 45
|q 45
|0 PERI:(DE-600)2006801-3
|t Japanese journal of applied physics
|v 45
|y 2006
|x 0021-4922
856 7 _ |u http://dx.doi.org/10.1143/JJAP.45.L416
909 C O |o oai:juser.fz-juelich.de:56059
|p VDB
913 1 _ |k P54
|v Kondensierte Materie
|l Kondensierte Materie
|b Materie
|z entfällt bis 2009
|0 G:(DE-Juel1)FUEK414
|x 0
914 1 _ |a Nachtrag
|y 2006
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k IFF-TH-III
|l Theorie III
|d 31.12.2006
|g IFF
|0 I:(DE-Juel1)VDB32
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970 _ _ |a VDB:(DE-Juel1)87603
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980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)PGI-2-20110106


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