HAL Id: jpa-00205798
https://hal.archives-ouvertes.fr/jpa-00205798
Submitted on 1 Jan 1964
HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.
L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.
Neutron diffraction investigation of U3O8
B.O. Loopstra
To cite this version:
B.O. Loopstra. Neutron diffraction investigation of U3O8. Journal de Physique, 1964, 25 (5), pp.429-
430. �10.1051/jphys:01964002505042900�. �jpa-00205798�
429.
NEUTRON DIFFRACTION INVESTIGATION OF U3O8 By B. O. LOOPSTRA (1),
Reactor Centrum Nederland, Petten, the Netherlands.
Résumé. 2014 Un échantillon polycristallin d’U3O8 orthorhombique a été étudié par diffraction
neutronique afin d’essayer d’expliquer certaines différences apparues lors de deux études précé- dentes faites l’une sur un monocristal aux rayons X et l’autre par diffraction neutronique. Le groupe
d’espace est Amm2 - (C142v). Les atomes d’uranium sont entourés par six oxygènes en contact
situés à des distances comprises entre 2,07 et 2,23 Å ; les atomes d’uranium ont un septième
voisin oxygène situé à 2,44 Å pour U1 et 2,71 Å pour U2.
Abstract.
2014A polycrystalline sample of orthorhombic U3O8 has been investigated by neutron
diffraction in order to resolve discrepancies between previous single crystal X-ray and powder
neutron investigations. The spacegroup is found to be Amm2 - (C142v). The uranium atoms
are surrounded by six oxygens in close contact at distances between 2.07 and 2.23 Å, with a
seventh oxygen at 2.44 Å for the U1 and at 2.71 Å for the U2 atoms.
LE JOURNAL DE PHYSIQUE 10ME 25, MAI 1964,
A polycrystalline sample of orthorhombic U308
has been investigated by neutron diffraction in order to resolve discrepancies between a previous single crystal X-ray investigation (Chodura and
FIG. 1.
(1) Work sponsored jointly by Reactor Centrum Neder-
land, The Netherlands, and Institutt for Atomenergi, Noway.
Mal~) and a powder neutron diffraction inves-
tigation (Andresen), the difference with the pre- vious investigation being a much higher resolution.
In the present investigation the unit cell axes were found to be a
=4.148 ~., b
=11.966 A
and c
=6.717 us. Here, the axes are chosen in
accordance with the usual space group designation.
The cell dimensions agree with Andresen’s data,
but Chodura and Maly find an a-axis ot double length. No trace is found in the neutron diagram
of this nor of the monoclinic splitting of the reflec- tions, also noticed by Chodura and Mal~. In
agreement with both previous investigations, the
cell is centered in the (100) face. This leaves as possible space groups A222(D2), A2mm(Cg§), Amm2(C2") and Ammm(D"). A fourier projec-
tion along the a-axis, made with the Okl neutron
intensities up to (015) as observed values and with Andresen’s parameters to obtain the calculated signs, shows clearly that the correct space group is Amm2. From this point on the structure was
refined by trial and error methods down to
TABLE
PARAMETERS U30, (Amm2)
In the final structure (see figure and table) each uranium atom is surrounded by six oxygens at
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01964002505042900
430
distances between 2.07 and 2.23 A. One out of the three uranium atoms of U308 has a seventh
oxygen at 2.44 A, the other two have a seventh
oxygen at 2.71 A. This would seem in agreement with the composition U6+ U2+ O8 .
The full paper will appear in Acta Crystallo- graphica.
°
Discussion
Dr IBERS.
-Pouvez-vous expliquer le blocage apparent d’un atome par une anisotropie de vibra-
tion ? Comment traitez-vous 1’agitation ther- mique ?
Dr LOOPSTRA. - Les facteurs de temperature isotropes sont appliqu6s a U (2But = 0,46 ui2) et
0 (2Bo = 1,38 ~.2). L’anisotropie de vibration
devrait être très grande pour l’oxyg6ne en (0, 1/2)
dans la projection de Fourier, et, cependant n’ex- pliquerait pas pourquoi le pic (U + 0) en (0, 0)
serait si peu élevé.
Dr BERTAUT. - Dr Ibers pense a un modele d’oscillateur anharmonique. On pourrait v6rifier
par une simple experience. Avez-vous fait un dia- gramme a très basse temperature ?
Dr LOOPSTRA.
-Non.
Dr. HOLTZBERG. - Avez-vous fait des mesures
de densité ? Elles sont excellentes pour verifier la
stoechiométrie.
zDr LOOPSTRA.
-Non.
~
’