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arxiv: 1409.2743 · v1 · pith:C7I32FQVnew · submitted 2014-09-09 · ❄️ cond-mat.str-el · cond-mat.mtrl-sci· cond-mat.supr-con

Sr_(0.9)K_(0.1)Zn_(1.8)Mn_(0.2)As₂: a ferromagnetic semiconductor with colossal magnetoresistance

classification ❄️ cond-mat.str-el cond-mat.mtrl-scicond-mat.supr-con
keywords colossalmagnetoresistanceunderferromagneticmagneticsemiconductorandersonbulk
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A bulk diluted magnetic semiconductor (Sr,K)(Zn,Mn)$_{2}$As$_{2}$ was synthesized with decoupled charge and spin doping. It has a hexagonal CaAl$_{2}$Si$_{2}$-type structure with the (Zn,Mn)$_{2}$As$_{2}$ layer forming a honeycomb-like network. Magnetization measurements show that the sample undergoes a ferromagnetic transition with a Curie temperature of 12 K and \revision{magnetic moment reaches about 1.5 $\mu_{B}$/Mn under $\mu_0H$ = 5 T and $T$ = 2 K}. Surprisingly, a colossal negative magnetoresistance, defined as $[\rho(H)-\rho(0)]/\rho(0)$, up to $-$38\% under a low field of $\mu_0H$ = 0.1 T and to $-$99.8\% under $\mu_0H$ = 5 T, was observed at $T$ = 2 K. The colossal magnetoresistance can be explained based on the Anderson localization theory.

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