2018
DOI: 10.1007/s10948-018-4948-5
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Electronic Structures and Ferromagnetic Properties of 3d (Cr)-Doped BaSe Barium Selenide

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Cited by 16 publications
(11 citation statements)
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“…The thermodynamic stability and the possibility of synthesizing the structure Sr 0.875 Mn 0.125 O are resolved by the formation and cohesive energy, [ 40,41 ] to validate the phase stability of the Sr 0.875 Mn 0.125 O structure, we have computed the formation and cohesive energies employing the following formula [ 12,13,16–20,42–60 ] EformSr0.875Mn0.125O=EtotalSr0.875Mn0.125O0.875EsolidSr+0.125EsolidMn+EsolidO$$\begin{eqnarray} E_{form}^{S{r}_{0.875}M{n}_{0.125}O} = E_{total}^{S{r}_{0.875}M{n}_{0.125}O} - \left[ {0.875E_{solid}^{Sr} + 0.125E_{solid}^{Mn} + E_{solid}^O} \right]\nonumber\\ \end{eqnarray}$$ EcohSr0.875Mn0.125O=0.875EatomSr+0.125EatomMn+EatomOEtotalSr0.875Mn0.125O$$\begin{eqnarray} E_{coh}^{S{r}_{0.875}M{n}_{0.125}O} = \left[ {0.875E_{atom}^{Sr} + 0.125E_{atom}^{Mn} + E_{atom}^O} \right] - E_{total}^{S{r}_{0.875}M{n}_{0.125}O}\nonumber\\ \end{eqnarray}$$…”
Section: Resultsmentioning
confidence: 99%
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“…The thermodynamic stability and the possibility of synthesizing the structure Sr 0.875 Mn 0.125 O are resolved by the formation and cohesive energy, [ 40,41 ] to validate the phase stability of the Sr 0.875 Mn 0.125 O structure, we have computed the formation and cohesive energies employing the following formula [ 12,13,16–20,42–60 ] EformSr0.875Mn0.125O=EtotalSr0.875Mn0.125O0.875EsolidSr+0.125EsolidMn+EsolidO$$\begin{eqnarray} E_{form}^{S{r}_{0.875}M{n}_{0.125}O} = E_{total}^{S{r}_{0.875}M{n}_{0.125}O} - \left[ {0.875E_{solid}^{Sr} + 0.125E_{solid}^{Mn} + E_{solid}^O} \right]\nonumber\\ \end{eqnarray}$$ EcohSr0.875Mn0.125O=0.875EatomSr+0.125EatomMn+EatomOEtotalSr0.875Mn0.125O$$\begin{eqnarray} E_{coh}^{S{r}_{0.875}M{n}_{0.125}O} = \left[ {0.875E_{atom}^{Sr} + 0.125E_{atom}^{Mn} + E_{atom}^O} \right] - E_{total}^{S{r}_{0.875}M{n}_{0.125}O}\nonumber\\ \end{eqnarray}$$…”
Section: Resultsmentioning
confidence: 99%
“…In recent times, considerable scientists have concentrated their investigation on diluted magnetic III-V and II-VI for spintronics employment. [12][13][14][15][16][17][18][19][20][21][22][23] The manganese ion Mn +3 has a 3d 4 electronic configuration, while the configuration of the Mn +4 ion has 3d 3 . Due to a strong Hund magnetic coupling (J H ) between the spin moments carried by the electrons of each orbital (J H ≈ 2-3 eV), the manganese ions are in a high spin configuration, and for its magnetic properties, Manganese is the most favorable element as a dopant in semiconductors.…”
Section: Introductionmentioning
confidence: 99%
“…These significant parameters describe, respectively, the exchange interaction between the conduction electron carriers and Ti − 3d states (conduction band), and the exchange interaction between the holes and Ti − 3d states (valance band). The N 0⍺ , and N 0β exchange constants can be computed using the following expressions [47]:…”
Section: -5-magnetic Propertiesmentioning
confidence: 99%
“…Where ΔE C = E(↓) − E(↑) and ΔE V = E(↓) − E(↑) are the conduction band-edge and the valence band-edge spin-splittings, respectively, of Ca 1−x Ti x S compounds at the Γ symmetry point of the band structures. < S > represents the half total magnetic moment of Ti atom [47] and x is the concentration of titanium impurity. The calculated exchange constants for both potentials are tabulated in Table 5.…”
Section: -5-magnetic Propertiesmentioning
confidence: 99%
“…In most cases, magnetic semiconductors have low Curie temperatures. Interest in DMSs was recently aroused by theoretical and experimental work on semiconductors [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]. DMS based on the transition element doped and on semiconductors has two important characteristics.…”
Section: Introductionmentioning
confidence: 99%