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Spin Directions in Pure Chromium

dc.contributor.authorWerner, S. A.en_US
dc.contributor.authorArrott, Anthonyen_US
dc.contributor.authorAtoji, M.en_US
dc.date.accessioned2010-05-06T21:52:02Z
dc.date.available2010-05-06T21:52:02Z
dc.date.issued1969-03-01en_US
dc.identifier.citationWerner, S. A.; Arrott, A.; Atoji, M. (1969). "Spin Directions in Pure Chromium." Journal of Applied Physics 40(3): 1447-1449. <http://hdl.handle.net/2027.42/70250>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70250
dc.description.abstractWe have carried out a triple‐axis polarized‐neutron‐beam experiment with polarization analysis of the final beam and magnetic fields to 15 kG applied to a pure Cr single crystal. The purpose was to determine whether the spin axis in the transversely polarized spin‐density wave state (122°K–38.5°C) is confined to the cube edges or whether in sufficient fields it can be made to lie in an arbitrary direction (perpendicular to the wave vector). The experiments show unambiguously that the latter is so. At 25°C, it is slightly more difficult to confine the spins to a single 110 axis than it is to a single 100 axis. At lower temperatures this anisotropy is enhanced. These results along with our previous results for the field dependence of the cube‐edge components using unpolarized neutrons have been analyzed in terms of two different models. Both models have the spins in all directions perpendicular to the wave vector of the spin‐density wave. One is the model of thermal activation of small domains. The other considers a domain structure with wall motion. In both models ansiotropy and magnetic field influence the net number of spins in any given direction.en_US
dc.format.extent3102 bytes
dc.format.extent216548 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleSpin Directions in Pure Chromiumen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumScientific Laboratory, Ford Motor Company, Dearborn, Michiganen_US
dc.contributor.affiliationumScientific Laboratory, Ford Motor Company, Dearborn, Michiganen_US
dc.contributor.affiliationumDepartment of Nuclear Engineering, University of Michigan, Ann Arbor, Michiganen_US
dc.contributor.affiliationotherChemistry Division, Argonne National Laboratory, Argonne Illinoisen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70250/2/JAPIAU-40-3-1447-1.pdf
dc.identifier.doi10.1063/1.1657712en_US
dc.identifier.sourceJournal of Applied Physicsen_US
dc.identifier.citedreferenceS. A. Werner, A. Arrott, and H. Kendrick, Phys. Rev. 155, 528 (1967).en_US
dc.identifier.citedreferenceS. A. Werner, A. Arrott, and M. Atoji, J. Appl. Phys. 39, 671 (1968).en_US
dc.identifier.citedreferenceW. Bindloss, thesis, University of California, Berkeley (1967).en_US
dc.identifier.citedreferenceEquation (5) is obtained by performing a variation on the total energy of the wall in a manner analogous to the classical treatment of a ferromagnetic wall.en_US
dc.owningcollnamePhysics, Department of


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