2012
DOI: 10.1016/j.jmmm.2012.03.039
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Effects of high-temperature annealing on magnetic properties of V-doped GaN thin films grown by MOCVD

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Cited by 6 publications
(4 citation statements)
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“…The optimized lattice parameters were not significantly affected by the implementation of the isolated magnetic MLs and were about the same as obtained for bulk GaN (a ¼ 3.22 Å and c/a ¼ 1.63); this fact agrees with previous experimental 17 and theoretical works. 22 In the second part of this work, we focus our attention on the electronic properties of GaN/V and GaN/Cr, the only DMHs with FM ground state (among the seven studied ones). The standard SDFT-GGA leads to a charge density overdelocalization of d orbitals and to an underestimation of the energy gap.…”
mentioning
confidence: 99%
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“…The optimized lattice parameters were not significantly affected by the implementation of the isolated magnetic MLs and were about the same as obtained for bulk GaN (a ¼ 3.22 Å and c/a ¼ 1.63); this fact agrees with previous experimental 17 and theoretical works. 22 In the second part of this work, we focus our attention on the electronic properties of GaN/V and GaN/Cr, the only DMHs with FM ground state (among the seven studied ones). The standard SDFT-GGA leads to a charge density overdelocalization of d orbitals and to an underestimation of the energy gap.…”
mentioning
confidence: 99%
“…We obtained for the GaN/V DMH a T c ¼ 1394 K, and for GaN/ Cr DMH a T c ¼ 555 K. There are in the litterature results only for bulk systems. In 2012, three different papers pointed ferromagnetism for bulk GaVN above RT: one of them is an experimental work 22 (which measured T c ¼ 350 K), and the other two are theoretical works, which predicted T c > RT 42 and T c > 350 K. 42 Concerning bulk GaCrN, many experimental measurements have pointed [43][44][45][46][47] a T c lying in the interval 320 K to 460 K. Our results for 2D GaN/V and GaN/ Cr system follow the trend already observed for bulk GaVN 22,42,48 and GaCrN: [43][44][45][46][47]49 above RT T c . Contrasting DMHs approach with the usual DMSs, regarding the same materials, the main difference is that DMHs present a 2D region of extremely high concentration of TM atoms, which, in principle, can favor magnetic ordering, thus leading to higher Curie temperatures, in agreement with our previous results.…”
mentioning
confidence: 99%
“…Extensive theoretical studies have been discussed this phenomenon in III-V DMSs and investigate their half-metallic ferromagnetic behaviour. They conclude that III-V DMSs are from the better candidates of spintronic applications [22][23][24][25][26][27][28][29][30][31][32][33][34][35] InP and BP crystallized in a face-centred cubic at zincblend structure with space group of F 43m and coordinate in tetrahedral symmetry. Their lattice parameters are 5.868 and 4.538Å, respectively, for InP and BP.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, extensively studies have been investigated to control the properties of (DMS)s as Ti-doped AlP [5], Ca doped AlP [6], Cr doped AlP [7], Ga 1−x Mn x N and Ga 1−x Mn x As [8], p-type (Ga, Fe)N [9], V doped AlN [10], Cr-doped GaP [11], V-doped GaN [12], V-doped GaN [13], Mn-doped III-V [14], doped GaAs (Zinc Blende) [15], Ga 1-x Mn x P and Ga 1-x Mn x As [16], V-doped GaN [17], Cr-doped AlP [18], Cu -doped ZnO [19].…”
Section: Introductionmentioning
confidence: 99%