dc.description.abstract |
Magnetlc ordering In two series of mixed spinel oxide systems have been investigated
by neutron diffraction studies as iUlicliom; of composition and temperature. The
~y~tem, .,ladied arc (i) Zn,Mgll, .,Ni",FcI04 with composition, x = 00, 02, [) 4, 0.6
and (ii) CO,MllhAh,Fc).7,O, wilh composition, x = 0.2, 0.4, 06, 08. The samples
were prepared in the ceramic Sintering method. The chemical structures of the systems
have been determined by X-ray and neutron diffraction and the two re'lilts are
compared. Bulk magnetization for each of the compllSlllOns urlhe (wo systems were
measured <it room temperature using a Vibrating Sample Magnelometer (VSM), in
order to have a preliminary idea of the overall magnetic properties of the system The
detail magnetic behavior of the system is found out from the ncutron diffraction
measurement> on them at a serics of temperatures buth above and below the
respective Curie temperatures. For system (i) neutron diffraction measurements were
done in the temperature range 15K,,; T ,,; 823K. For ,y,tem (ii) the neutron
mea,urements were also performed at a number of temperatures '-anging from 773K
down to 15K
For system (i) the observed sublattlCe moment, do not follow the ~rnooth trend as
expected in collinear ferrimagnetic :;tmcture, A ,Iuggi,h and ~lep like behavior in the
temperature dependence of the magnetic moment ha:; been ob:.erved below Tc which
manifests the pre~ence of spin clusters superimpo,ed on the inJinite magnctic
netwurk. For the ~amplc \vith x = 0 6 the ordered moment in the 13sublattice reduces
dra:;tically indicating the presence of strong lloncollmeanty in the B ~ite. But the
absence of (200) rellection in thc neutron patterns at all temperatures suggests that
there is no long range spatial ordering of the transver,e spin components However,
for this sample thcre is con~iderahle broadening of the (111) dlffractron peak at 15K
due to the diffuse ,ignal The presence of this dlffuse scattering and the decrease in
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the B site moment at temperatures below SOKindicate that a re-entrant or semi-spingla:;
s like :;tructure 1\ more probable for the composition with x = 0.6 The results are
described qualitatively in the light of the eXisting tbcorie~ and experimental
observation:;
FOI system (ii). it appear:; that it ]Jo:;:;esse:;a long range ferrimagnetic ordering at
x '" 0 6 along with some randomly canted :;pin components At x ~ 0 8, a 8eml-;pin
gla:;s beiJaVlllr 'WaSobserved The laller composition e"hibits three tran:;itions' at
temperatures higher than lOOK,there is formation of magnelic ,pin c1u,ters showing
,uper-paramagnetic type behavior before the true pawm;lgnetlC region is reaehed at
about 200K, a ferrimagnetLc long-range ordering is observed in the temperature range
lOOKto SOK; and ]jnally below SOKthere is freezIng of the magnetic 8pin cluster8,
The competitIOn between the long range ferrimagnetie order and the fluctuating :;mall
spin clusters has been probed through developing a computer program and fitting the
(Ill) Blagg dim-action peaks in the diffraction patterns al different temperatures lor
the composition with x = 0.8 |
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