E.F. Bertaut
Centre national de la recherche scientifique
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Featured researches published by E.F. Bertaut.
Solid State Communications | 1967
E.F. Bertaut; J. Chappert; J. Mareschal; J.P. Rebouillat; J. Sivardière
Resume TbFeO 3 de structure perovskite (groupe Pbnm) est etudie par diffraction neutronique, mesures magnetiques et effet Mossbauer. A 97°K les spins du fer sont ordonnes suivant le mode G x appartenant a la representation Γ 4 ; a 4, 2°K les spins du terbium sont ordonnes suivant les modes F x et C y (Γ 2 ), et ceux du fer suivant G z couples dans la meme representation Γ 2 ; a 1, 5°K on observe les modes A x et G y (Γ 8 ) pour le terbium et un mode G (probablemennt G x ϵΓ 4 ) decouple du terbium pour le fer. Les temperatures de Neel des trois structures magnetiques sont respectivement 681°K 8, 4°K et 3, 1°K.
Journal of Applied Physics | 1966
E.F. Bertaut; G. Bassi; G. Buisson; P. Burlet; J. Chappert; A. Delapalme; J. Mareschal; G. Roult; R. Aleonard; R. Pauthenet; J.P. Rebouillat
In orthorhombic CrRO3 (R=rare earth and Y), Cr spins are ordered in a G mode between TN 282°K for R=La, to 112°K for R=Lu. The rare‐earth ordering is coupled to the Cr‐spin ordering, with the exception of terbium. In the magnetoelectric compound Fe1.15Ga0.85O3, four sites are available for cations, one of these mainly occupied by Ga. Neutron‐diffraction and magnetic‐susceptibility measurements give evidence of a ferrimagnetic ordering. Tetragonal FeS shows no evidence for magnetic ordering by neutron diffraction and Mossbauer effect down to 1.7°K. The CrS‐MnS solid solution has NaCl type. First kind of facecentered magnetic ordering is observed.
Solid State Communications | 1965
E.F. Bertaut; P. Burlet; J. Chappert
Resume Le FeS tetragone ( a = 3, 768 A , c = 5, 039 A , groupe P 4/ nmm ) a du FeII dans un milieu tetraedrique. Etudie par diffraction de neutrons et par leffet Mossbauer, il nindique aucun signe dordre magnetique a des temperatures aussi basses que 1, 7°K. Ce comportement, ajoute a labsence de toute conductibilite metallique, indique une forte co-valente. De la chaleur au-dessus de 160°C transforme, avec une contraction du volume, la variete tetragone instable en une forme hexagonale, dune facon exothermique.
Solid State Communications | 1970
U. König; E.F. Bertaut; Y. Gros; M. Mitrikov; G. Chol
Abstract For the normal spinel ZnFe2O4 one indicates colinear and non colinear spin arrangements which are equally compatible with neutron diffraction powder intensities, observed at 4.2 K. A quadrupolar splitting, observed by Mossbauer effect, favours the non colinear model which belongs to the Shubnikov group pl 4 The Neel temperature is about 10K. Magnetic moment values of Fe3+ are abnormally low.
Solid State Communications | 1967
E.F. Bertaut; G. Buisson; S. Quezel-Ambrunaz; G. Quezel
The magnetic structure of BiMn2O5 (group Pbam) observed at 4, 2° K corresponds to a propagation vector k = [12 0 12]. From the irreducible representations associated with k in the space group Pbam, one deduces all possible magnetic couplings and one proposes non-colinear structure models, which are checked by calculation.
Journal of Applied Physics | 1962
R. Aleonard; E.F. Bertaut; M. C. Montmory; R. Pauthenet
In the pyrochlore compounds Ru2M2O7 (where M=Pr, Nd, Gd, Tb, Dy, Ho, and Y), RuIV contributes to the Curie constant 1 instead of the value 3 which would be expected for a d4 state with g=2 and j=2.
Solid State Communications | 1970
F. Tcheou; E.F. Bertaut; H. Fuess
Abstract Canting of the rare earth moments at low temperature for DyIG, ErIG and YbIG is evidenced. The canting angles and the moments are refined and compared with theoretical predictions.
Solid State Communications | 1971
M Nasr-Eddine; E.F. Bertaut
Resume Nous avons determine par diffraction de rayons-X, entre 5 et 360K, les variations des parametres a, b et c de la maille. La variation thermique de laimantation a ete precisee par diffraction neutronique. Grâce a ces mesures, nous avons calcule d T N /d P = 0, 73. 10 -9 degre cm 2 dyne -1 , en bon accord avec les mesures experimentales directes. Le modele de Bean et Rodbell est generalise par lintroduction dune energie anisotrope de deformation, laquelle permet la justification theorique de la nature de premier ordre de la transition a T N
Solid State Communications | 1967
E.F. Bertaut; Paulette Burlet
The solid solutions MnxCr1−x S show a considerable magnetic short range order above TN. The analysis of the diffused intensity for the composition x = 0.33 allows the estimation of spin correlations and of exchange integrals J1 ⋍ -4.5°K, J2 ⋍ + 6°K which are compatible with the observation below TN of a long range order of the first kind, i.e. with the positive second neighbour interactions.
Solid State Communications | 1967
R.R. Chevalier; G. Roult; E.F. Bertaut
Resume Alors que letude par effet Mossbauer de solutions solides (Mn 2 O 3 ) 1−x (Fe 2 O 3 ) x suggere lexistence de deux transitions magnetiques dans Mn 2 O 3 , lune vers 80°K, lautre vers 25°K, la variation thermique des intensites des raies magnetiques (100) (110) et (111) etudiees par diffraction neutronique montre dans Mn 2 O 3 lexistence dune transition a 90°K et dune autre vers 50°K (et non pas 25°K).