Magnetic and transport properties of the V2–VI3V2–VI3 diluted magnetic semiconductor Sb2−xMnxTe3Sb2−xMnxTe3
dc.contributor.author | Dyck, Jeffrey S. | en_US |
dc.contributor.author | Švanda, P. | en_US |
dc.contributor.author | Lošt’ák, P. | en_US |
dc.contributor.author | Horák, J. | en_US |
dc.contributor.author | Chen, Wei | en_US |
dc.contributor.author | Uher, Ctirad | en_US |
dc.date.accessioned | 2010-05-06T21:31:46Z | |
dc.date.available | 2010-05-06T21:31:46Z | |
dc.date.issued | 2003-12-15 | en_US |
dc.identifier.citation | Dyck, J. S.; Švanda, P.; Lošt’ák, P.; Horák, J.; Chen, W.; Uher, C. (2003). "Magnetic and transport properties of the V2–VI3V2–VI3 diluted magnetic semiconductor Sb2−xMnxTe3Sb2−xMnxTe3." Journal of Applied Physics 94(12): 7631-7635. <http://hdl.handle.net/2027.42/70033> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/70033 | |
dc.description.abstract | We have measured electrical and magnetic properties of single crystals of Sb2−xMnxTe3Sb2−xMnxTe3 with x=0–0.045x=0–0.045 at temperatures of 2 K to 300 K. Hall effect measurements indicate that each manganese atom donates approximately one hole to the valence band. The magnetic susceptibility is paramagnetic down to 2 K, and both Curie–Weiss and Brillouin analyses show that manganese substitutes for Sb and takes the Mn2+Mn2+ state with S=5/2.S=5/2. Contrary to the case of III–V host matrices, manganese does not stimulate ferromagnetic order in the family of bulk layered V2–VI3V2–VI3 diluted magnetic semiconductors, at least in the range of magnetic impurity and carrier concentrations studied here. © 2003 American Institute of Physics. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 81049 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Magnetic and transport properties of the V2–VI3V2–VI3 diluted magnetic semiconductor Sb2−xMnxTe3Sb2−xMnxTe3 | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Physics, University of Michigan, Ann Arbor, Michigan 48109-1120 | en_US |
dc.contributor.affiliationum | Department of Physics, University of Michigan, Ann Arbor, Michigan 48109-1120 | en_US |
dc.contributor.affiliationother | Faculty of Chemical Technology, University of Pardubice, Čs. Legií Square 565, 532 10 Pardubice, Czech Republic | en_US |
dc.contributor.affiliationother | Joint Laboratory of Solid State Chemistry, Czech Academy of Sciences and University of Pardubice, Studentská 64, 530 09 Pardubice, Czech Republic | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70033/2/JAPIAU-94-12-7631-1.pdf | |
dc.identifier.doi | 10.1063/1.1626803 | en_US |
dc.identifier.source | Journal of Applied Physics | en_US |
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dc.owningcollname | Physics, Department of |
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