Magnetic structure of Y2BaCuO5

I. V. Golosovsky; P. Böni; P. Fischer

doi:10.1016/0038-1098(93)90556-3

Magnetic structure of Y₂BaCuO₅

I. V. Golosovsky, P. Böni, P. Fischer

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Abstract

The antiferromagnetic structure of the Cu spins and the Néel point in Y₂BaCuO₅ were redetermined by neutron powder diffraction. There are two possible collinear models with wave vector k = [0, 1 2, 1 2] and the spins directed along the c-axis. These models cannot be distinguished in powder diffraction. The ordered magnetic moment of the copper atom at saturation amounts to 0.55(3)μ_B.

Original language	English
Pages (from-to)	1035-1037
Number of pages	3
Journal	Solid State Communications
Volume	87
Issue number	11
DOIs	https://doi.org/10.1016/0038-1098(93)90556-3
State	Published - Sep 1993
Externally published	Yes

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10.1016/0038-1098(93)90556-3

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@article{c7fe70b99ffa422daea599b011351607,

title = "Magnetic structure of Y2BaCuO5",

abstract = "The antiferromagnetic structure of the Cu spins and the N{\'e}el point in Y2BaCuO5 were redetermined by neutron powder diffraction. There are two possible collinear models with wave vector k = [0, 1 2, 1 2] and the spins directed along the c-axis. These models cannot be distinguished in powder diffraction. The ordered magnetic moment of the copper atom at saturation amounts to 0.55(3)μB.",

author = "Golosovsky, {I. V.} and P. B{\"o}ni and P. Fischer",

year = "1993",

month = sep,

doi = "10.1016/0038-1098(93)90556-3",

language = "English",

volume = "87",

pages = "1035--1037",

journal = "Solid State Communications",

issn = "0038-1098",

publisher = "Elsevier Ltd.",

number = "11",

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T1 - Magnetic structure of Y2BaCuO5

AU - Golosovsky, I. V.

AU - Böni, P.

AU - Fischer, P.

PY - 1993/9

Y1 - 1993/9

N2 - The antiferromagnetic structure of the Cu spins and the Néel point in Y2BaCuO5 were redetermined by neutron powder diffraction. There are two possible collinear models with wave vector k = [0, 1 2, 1 2] and the spins directed along the c-axis. These models cannot be distinguished in powder diffraction. The ordered magnetic moment of the copper atom at saturation amounts to 0.55(3)μB.

AB - The antiferromagnetic structure of the Cu spins and the Néel point in Y2BaCuO5 were redetermined by neutron powder diffraction. There are two possible collinear models with wave vector k = [0, 1 2, 1 2] and the spins directed along the c-axis. These models cannot be distinguished in powder diffraction. The ordered magnetic moment of the copper atom at saturation amounts to 0.55(3)μB.

UR - http://www.scopus.com/inward/record.url?scp=0027667498&partnerID=8YFLogxK

U2 - 10.1016/0038-1098(93)90556-3

DO - 10.1016/0038-1098(93)90556-3

M3 - Article

AN - SCOPUS:0027667498

SN - 0038-1098

VL - 87

SP - 1035

EP - 1037

JO - Solid State Communications

JF - Solid State Communications

IS - 11

ER -

Magnetic structure of Y₂BaCuO₅

Abstract

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