2009
DOI: 10.1038/nmat2572
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Giant Zeeman splitting in nucleation-controlled doped CdSe:Mn2+ quantum nanoribbons

Abstract: Doping of semiconductor nanocrystals by transition-metal ions has attracted tremendous attention owing to their nanoscale spintronic applications. Such doping is, however, difficult to achieve in low-dimensional strongly quantum confined nanostructures by conventional growth procedures. Here we demonstrate that the incorporation of manganese ions up to 10% into CdSe quantum nanoribbons can be readily achieved by a nucleation-controlled doping process. The cation-exchange reaction of (CdSe)(13) clusters with Mn… Show more

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Cited by 231 publications
(179 citation statements)
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“…A similar phenomenon was also observed by Yao and coworkers on the Zn 0.98 Co 0.02 O NWs [78]. The substitutional incorporation of Mn ions up to 10% into CdSe quantum nano-ribbons was also readily achieved by Yu and coworkers via a nucleation-controlled doping process [79].…”
Section: Magnetic Semiconductor Nanostructuressupporting
confidence: 74%
“…A similar phenomenon was also observed by Yao and coworkers on the Zn 0.98 Co 0.02 O NWs [78]. The substitutional incorporation of Mn ions up to 10% into CdSe quantum nano-ribbons was also readily achieved by Yu and coworkers via a nucleation-controlled doping process [79].…”
Section: Magnetic Semiconductor Nanostructuressupporting
confidence: 74%
“…This value is much larger than that reported for nanoparticles in organic solution (0.5 emu g −1 for x = 3%). [ 14 ] Unlike Mn-doped II-VI nanocrystals, [ 1,2,7,17 ] the PL emission from the Mn dopants in PbS is either not observed or else is much weaker than the QD PL emission ( Figure 3 a,b): the weak Mn-related PL band is centered at ≈1.9 eV at room temperature, at higher energies relative to the much stronger PL emission wileyonlinelibrary.com www.particle-journal.com www.MaterialsViews.com of the nanocrystals (see Figure 3 b). Also, while the Mn-related PL band does not change with x , the QD PL emission tends to blueshift with increasing x : for PbS QDs with no Mn, the PL band is centered at E QD = 1.08 eV ( λ = 1150 nm) at T = 295 K; increasing Mn results in a monotonic energy blue-shift of the PL emission up to a value of E QD = 1.40 eV ( λ = 885 nm) at x = 18% (see Figure 3 a).…”
Section: Doi: 101002/ppsc201300184mentioning
confidence: 98%
“…[1][2][3] In particular, 3 d transition metal ions (Mn, Co, etc.) with their d -shell electronic confi gurations can imprint a nanocrystal with magnetic properties of relevance for innovative applications ranging from bio-imaging [ 4,5 ] to spintronics.…”
Section: Doi: 101002/ppsc201300184mentioning
confidence: 99%
“…12,13,[36][37][38][39][40] Most prominently, a strong quantum-confinement-induced change in the fundamental nature of the conduction-band-electron ( e CB − ) -Mn 2+ exchange (s-d exchange) interaction has been described both theoretically 36,37 and experimentally. 37,[41][42][43][44][45] According to k·p-model descriptions of Mn at finite k vectors. 36,37 This mixing has been proposed to turn on strong antiferromagnetic kinetic s-d exchange coupling that dominates over the weaker ferromagnetic potential s-d exchange coupling in DMS QDs and quantum wells (QWs).…”
Section: Introductionmentioning
confidence: 99%