000019020 001__ 19020
000019020 005__ 20240529111539.0
000019020 0247_ $$2DOI$$a10.1140/epjb/e2011-10567-6
000019020 0247_ $$2WOS$$aWOS:000293705900002
000019020 0247_ $$2MLZ$$aspringerlink:10.1140/epjb/e2011-10567-6
000019020 037__ $$aPreJuSER-19020
000019020 041__ $$aeng
000019020 082__ $$a530
000019020 084__ $$2WoS$$aPhysics, Condensed Matter
000019020 1001_ $$0P:(DE-Juel1)131047$$aXiao, Y.$$b0$$uFZJ
000019020 245__ $$aPhysical properties, crystal and magnetic structure of layered Fe(1.11)Te(1-) (x) Se (x) superconductors
000019020 260__ $$aBerlin$$bSpringer$$c2011
000019020 300__ $$a113-121
000019020 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000019020 3367_ $$2DataCite$$aOutput Types/Journal article
000019020 3367_ $$00$$2EndNote$$aJournal Article
000019020 3367_ $$2BibTeX$$aARTICLE
000019020 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000019020 3367_ $$2DRIVER$$aarticle
000019020 440_0 $$01982$$aEuropean Physical Journal B$$v82$$x1434-6028$$y2
000019020 500__ $$aRecord converted from VDB: 12.11.2012
000019020 520__ $$aThe physical and structural properties of Fe1.11Te and Fe1.11Te0.5Se0.5 have been investigated by means of X-ray and neutron diffraction as well as physical property measurements. For the Fe1.11Te compound, the structure distortion from a tetragonal to monoclinic phase takes place at 64 K accompanied with the onset of antiferromagnetic order upon cooling. The magnetic structure of the monoclinic phase was confirmed to be of antiferromagnetic configuration with a propagation vector k = (1/2, 0, 1/2) based on Rietveld refinement of neutron powder diffraction data. The structural/magnetic transitions are also clearly visible in magnetic, electronic and thermodynamic measurements. For superconducting Fe1.11Te0.5Se0.5 compound, the superconducting transition with T (c) = 13.4 K is observed in the resistivity and ac susceptibility measurements. The upper critical field H (c2) is obtained by measuring the resistivity under different magnetic fields. The Kim's critical state model is adopted to analyze the temperature dependence of the ac susceptibility and the intergranular critical current density is calculated as a function of both field amplitude and temperature. Neutron diffraction results show that Fe1.11Te0.5Se0.5 crystalizes in tetragonal structure at 300 K as in the parent compound Fe1.11Te and no structural distortion is detected upon cooling to 2 K. However an anisotropic thermal expansion anomaly is observed around 100 K.
000019020 536__ $$0G:(DE-Juel1)FUEK412$$2G:(DE-HGF)$$aGrundlagen für zukünftige Informationstechnologien$$cP42$$x0
000019020 536__ $$0G:(DE-Juel1)FUEK415$$aGroßgeräte für die Forschung mit Photonen, Neutronen und Ionen (PNI)$$cP55$$x1
000019020 588__ $$aDataset connected to Web of Science
000019020 650_7 $$2WoSType$$aJ
000019020 7001_ $$0P:(DE-Juel1)130991$$aSu, Y.$$b1$$uFZJ
000019020 7001_ $$0P:(DE-Juel1)VDB84209$$aKumar, C. M. N.$$b2$$uFZJ
000019020 7001_ $$0P:(DE-HGF)0$$aRitter, C.$$b3
000019020 7001_ $$0P:(DE-HGF)0$$aMittal, R.$$b4
000019020 7001_ $$0P:(DE-Juel1)VDB84368$$aPrice, S.$$b5$$uFZJ
000019020 7001_ $$0P:(DE-Juel1)VDB97577$$aPerßon, J.$$b6$$uFZJ
000019020 7001_ $$0P:(DE-Juel1)130572$$aBrückel, T.$$b7$$uFZJ
000019020 773__ $$0PERI:(DE-600)1459068-2$$a10.1140/epjb/e2011-10567-6$$gVol. 82, p. 113-121$$p113-121$$q82<113-121$$tThe @European physical journal / B$$v82$$x1434-6028$$y2011
000019020 8567_ $$uhttp://dx.doi.org/10.1140/epjb/e2011-10567-6
000019020 909CO $$ooai:juser.fz-juelich.de:19020$$pVDB
000019020 9131_ $$0G:(DE-Juel1)FUEK412$$bSchlüsseltechnologien$$kP42$$lGrundlagen für zukünftige Informationstechnologien (FIT)$$vGrundlagen für zukünftige Informationstechnologien$$x0
000019020 9131_ $$0G:(DE-Juel1)FUEK415$$bStruktur der Materie$$kP55$$lGroßgeräteforschung mit Photonen, Neutronen und Ionen$$vGroßgeräte für die Forschung mit Photonen, Neutronen und Ionen (PNI)$$x1
000019020 9132_ $$0G:(DE-HGF)POF3-623$$1G:(DE-HGF)POF3-620$$2G:(DE-HGF)POF3-600$$aDE-HGF$$bForschungsbereich Materie$$lIn-house research on the structure, dynamics and function of matter$$vNeutrons for Research on Condensed Matter$$x0
000019020 9141_ $$y2011
000019020 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000019020 9201_ $$0I:(DE-Juel1)PGI-4-20110106$$gPGI$$kPGI-4$$lStreumethoden$$x0
000019020 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$gJCNS$$kJCNS-2$$lStreumethoden$$x1
000019020 9201_ $$0I:(DE-82)080009_20140620$$gJARA$$kJARA-FIT$$lJülich-Aachen Research Alliance - Fundamentals of Future Information Technology$$x2
000019020 970__ $$aVDB:(DE-Juel1)133739
000019020 980__ $$aVDB
000019020 980__ $$aConvertedRecord
000019020 980__ $$ajournal
000019020 980__ $$aI:(DE-Juel1)PGI-4-20110106
000019020 980__ $$aI:(DE-Juel1)JCNS-2-20110106
000019020 980__ $$aI:(DE-82)080009_20140620
000019020 980__ $$aUNRESTRICTED
000019020 981__ $$aI:(DE-Juel1)JCNS-2-20110106
000019020 981__ $$aI:(DE-Juel1)JCNS-2-20110106
000019020 981__ $$aI:(DE-Juel1)VDB881