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Statements

Subject Item
n2:RIV%2F60076658%3A12640%2F09%3A00010047%21RIV10-MSM-12640___
rdf:type
skos:Concept n10:Vysledek
dcterms:description
We studied the structural, spin-polarized electronic band structures, density of states, and magnetic properties of the diluted magnetic semiconductors (DMSs) Cd1-xMnxS and Cd1-xMnxS in zinc blende phase (B3) with 25% Mn by using the ab initio method. The calculations were performed by using the full potential linearized augmented plane wave plus local orbitals (FP-L/APW+lo) method within the spin-polarized density functional theory and the local spin density approximation (LSDA). Calculated electronic band structures and the density of states of these DMSs are discussed in terms of the contribution of Mn 3d(5)4s(2), Cd 4d(10)5s(2), S 3s(2)3p(4), and Se 4s(2)4p(4) partial density of states and we also compute the local magnetic moments. We estimated the spin-exchange splitting energies, Delta(x)(d) and Delta(x)(p-d), produced by the Mn 3d states, and we found that the effective potential for the minority spin is more attractive than that for the majority spin. We determine the s-d exchange constant N- We studied the structural, spin-polarized electronic band structures, density of states, and magnetic properties of the diluted magnetic semiconductors (DMSs) Cd1-xMnxS and Cd1-xMnxS in zinc blende phase (B3) with 25% Mn by using the ab initio method. The calculations were performed by using the full potential linearized augmented plane wave plus local orbitals (FP-L/APW+lo) method within the spin-polarized density functional theory and the local spin density approximation (LSDA). Calculated electronic band structures and the density of states of these DMSs are discussed in terms of the contribution of Mn 3d(5)4s(2), Cd 4d(10)5s(2), S 3s(2)3p(4), and Se 4s(2)4p(4) partial density of states and we also compute the local magnetic moments. We estimated the spin-exchange splitting energies, Delta(x)(d) and Delta(x)(p-d), produced by the Mn 3d states, and we found that the effective potential for the minority spin is more attractive than that for the majority spin. We determine the s-d exchange constant N-
dcterms:title
Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase
skos:prefLabel
Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase
skos:notation
RIV/60076658:12640/09:00010047!RIV10-MSM-12640___
n3:aktivita
n12:V
n3:aktivity
V
n3:cisloPeriodika
20
n3:dodaniDat
n13:2010
n3:domaciTvurceVysledku
Reshak, Ali Hussain
n3:druhVysledku
n4:J
n3:duvernostUdaju
n15:S
n3:entitaPredkladatele
n11:predkladatel
n3:idSjednocenehoVysledku
342964
n3:idVysledku
RIV/60076658:12640/09:00010047
n3:jazykVysledku
n9:eng
n3:klicovaSlova
FLIP RAMAN-SCATTERING; FERROMAGNETISM; EXCHANGE; ENERGY; ZNMNS; CDSE
n3:klicoveSlovo
n5:EXCHANGE n5:ENERGY n5:FLIP%20RAMAN-SCATTERING n5:CDSE n5:ZNMNS n5:FERROMAGNETISM
n3:kodStatuVydavatele
US - Spojené státy americké
n3:kontrolniKodProRIV
[DF858933E56C]
n3:nazevZdroje
Journal of Physical Chemistry A
n3:obor
n16:BO
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
6
n3:rokUplatneniVysledku
n13:2009
n3:svazekPeriodika
113
n3:tvurceVysledku
Nazir, S. Ikram, N. Shaukat, A. Reshak, Ali Hussain Saeed, Y. Tanveer, M.
n3:wos
000266093500027
s:issn
1089-5639
s:numberOfPages
6
n14:organizacniJednotka
12640