2009
DOI: 10.1103/physrevb.80.033201
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Magnetic polaron percolation on a rutile lattice: A geometrical exploration in the limit of low density of magnetic impurities

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Cited by 7 publications
(13 citation statements)
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“…Magnetization saturation value M S depends on the magnetic moments of oxygen vacancies V(O) and Fe 3+ ions and their amounts N 1 and N 2 , respectively, in the infinite cluster as M S  = | S 1 N 1  −  S 2 N 2 |, that is in a complete agreement with Ref. [20]. …”
Section: Discussionsupporting
confidence: 89%
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“…Magnetization saturation value M S depends on the magnetic moments of oxygen vacancies V(O) and Fe 3+ ions and their amounts N 1 and N 2 , respectively, in the infinite cluster as M S  = | S 1 N 1  −  S 2 N 2 |, that is in a complete agreement with Ref. [20]. …”
Section: Discussionsupporting
confidence: 89%
“…Here, M S is the saturation magnetization, H is a static magnetic field, and V 0 is the volume of infinite (in fact, closured over a nanoparticle surface) magnetic cluster. Saturation magnetization was defined in accordance with the formula (7) from [ 20 ]: …”
Section: Introductionmentioning
confidence: 99%
“…At the same time the important role played by the defect concentration in determining the magnetic properties became evident, making them strongly dependent on the preparation technique and intrinsic disorder 8. Among the possible models the bound magnetic polarons (BMPs) model, has received great attention in recent years 7–15. The basic idea is the polarization of TM ion spins by a localized defect.…”
Section: Introductionmentioning
confidence: 99%
“…For low TM concentrations or even for undoped material this model is hardly usable due to the small number of transition ions in the polaron sphere. The contribution of the defect itself has to be considered 11, 12, 15. Therefore, any information about magnetic ion and/or defect states, obtained with specific experimental methods, is very valuable.…”
Section: Introductionmentioning
confidence: 99%
“…It is often assumed (see, e.g., refs. ) that the localized carriers created with an oxygen vacancy can be described by a wavefunction such as Ψtrue(rtrue)=true(π aB3true)1/2 exptrue(r/aBtrue) where a B can be regarded as a polaron radius and the interaction between localized carriers (and their spin) can be discussed in the frame of polaron percolation theory. In particular, in the anatase‐type lattice, assuming a first nearest neighbor (NN) cation–cation interaction, the percolation occurs when 27.9% of Ti atoms have a magnetic moment .…”
Section: Resultsmentioning
confidence: 99%