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ALFA II-HIFIELD Proyect #II0147FI

ALFA II-HIFIELD Proyect #II0147FI

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<strong>ALFA</strong> <strong>II</strong>-<strong>HIFIELD</strong><br />

<strong>Proyect</strong> #<strong>II</strong>0147FI<br />

“Advanced Materials in H.M.F”<br />

V.Sagredo A<br />

L.M. De Chalbaud; L.Betancourt<br />

Magnetism Group<br />

ULA-Mérida<br />

Mérida-VENEZUELA


Tentative research lines<br />

• A) Colossal magneto-resistance<br />

in chromium chalcogenide<br />

compounds<br />

• B) Variable range-hopping<br />

conduction in semiconductors


MAGNETORESISTANCE IN<br />

FeCr 2 S 4


MAGNETIZATION and M.S. in<br />

FeCr 2 S 4


MAGNETORESISTANCE IN<br />

MANGANITES


MAGNETIZATION IN<br />

MANGANITES


A) Colossal Magneto-Resistance<br />

The discovery of the colossal MR phenomenon<br />

in perovskite Mn oxides of .R 1-x<br />

B x<br />

MnO 3<br />

Where R: rare earth and B a divalent cation.<br />

Has generated wide attention due a variety of<br />

interesting physical properties and their potential<br />

for technological applications.<br />

In this type of materials is long known to exist<br />

the metal-insulator transition.


Important property<br />

It is important to note that CMR does not saturate<br />

until applied fields at least of the order of 6 T where<br />

the MR, when normalized to the high field resistance,<br />

can exceed that of GMR by orders of magnitude. It<br />

has been suggested that the field scale over which<br />

CMR materials can be applied will be pushed to<br />

lower values by field- amplification or spin-valve<br />

techniques.


Chromium chalcogenides<br />

A.P.Ramirez et. Al in Science (97) proposed<br />

investigate spinel structure chalcogenide compounds<br />

with composition AB 2<br />

X 4<br />

where A and B are<br />

transition elements occupying tetrahedral and<br />

octahedral sites respectively and X is a chalcogen.<br />

FeCr 2 S 4


Differences from perovskite oxides<br />

i) There are many ferromagnetic members of this<br />

family, there is the possibility of varying both<br />

anion as well cation species while maintained the<br />

spinel structure.<br />

ii<br />

Unlike in the perovskite where the A-cation<br />

acts mainly to donate charge and control the unit<br />

cell volume, in the spinels it is common to have<br />

A-cation derived states near the Fermi level.


B) Variable range hopping<br />

conduction in semiconductors<br />

Chromium diluted chalcogenide<br />

compounds as FeCr 2-x Al x S 4 have<br />

shown that Al favors the fluctuation<br />

of Coulomb potential.<br />

This effect produces an increase of<br />

resistivity and the transport behavior<br />

transits from MP transport to the<br />

VRH process


Cr based chalcogenide<br />

spinels<br />

FeCr 2 S 4<br />

CoCr 2 S 4<br />

Diluted ACr 2-x <strong>II</strong>I x S 4 compounds<br />

Examples: CdCr 2-x Ga x Se 4<br />

CdCr 2-x In x S 4

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