TY - JOUR
T1 - Luminescent and ferromagnetic CdS:Mn2+/C core-shell nanocrystals
AU - Bhattacharyya, Sayan
AU - Estrin, Y.
AU - Rich, D. H.
AU - Zitoun, D.
AU - Koltypin, Yuri
AU - Gedanken, A.
PY - 2010/12/23
Y1 - 2010/12/23
N2 - The Mn-doped CdS nanocrystals encapsulated by carbon (Cd 1-xMnxS/C) were synthesized by a one-step, kinetically controlled, solid-state reaction under autogenic pressure at elevated temperatures. The ∼50 nm wurtzite Cd1-xMnxS core was encapsulated by a 5-11 nm disordered carbon shell, and with the increase in Mn concentration, a gradual change from isotropic nanocrystals to one-dimensional nanorods was observed. Electron paramagnetic resonance studies showed that Mn2+ could be efficiently doped into the CdS lattice up to a Mn:Cd atomic ratio of 0.012. The 0.9-1.8 atomic % manganese-doped CdS samples were found to be ferromagnetic at room temperature, and the magnetic moment did not saturate even at 2 K, likely due to the coexistence of superparamagnetic fractions and antiferromagnetic coupling between the Mn2+ spins. The lowest-doped samples (Mn:Cd = 0.009 and 0.012) display the highest magnetic moments (4.43 ± 0.04 and 4.52 ± 0.04 μB/Mn), respectively. The more concentrated samples exhibit weaker magnetic moments (2.85 ± 0.03 μB/Mn for Mn:Cd = 0.018) as a result of antiferromagnetic coupling between Mn2+ second neighbors. Cathodoluminescence spectroscopy experiments were performed from 50 to 300 K to assess the temperature dependence of emissions related to the CdS near band edge, the Mn intra d-shell4T1 → 6A 1 transition, defectrelated surface state transitions, and the effect of surface passivation with carbon. The temperature-dependent spectral line shape variations, the emission intensities, and energies of the various components were examined for each Mn doping density to evaluate the incorporation of Mn2+ into the host CdS nanocrystal lattice.
AB - The Mn-doped CdS nanocrystals encapsulated by carbon (Cd 1-xMnxS/C) were synthesized by a one-step, kinetically controlled, solid-state reaction under autogenic pressure at elevated temperatures. The ∼50 nm wurtzite Cd1-xMnxS core was encapsulated by a 5-11 nm disordered carbon shell, and with the increase in Mn concentration, a gradual change from isotropic nanocrystals to one-dimensional nanorods was observed. Electron paramagnetic resonance studies showed that Mn2+ could be efficiently doped into the CdS lattice up to a Mn:Cd atomic ratio of 0.012. The 0.9-1.8 atomic % manganese-doped CdS samples were found to be ferromagnetic at room temperature, and the magnetic moment did not saturate even at 2 K, likely due to the coexistence of superparamagnetic fractions and antiferromagnetic coupling between the Mn2+ spins. The lowest-doped samples (Mn:Cd = 0.009 and 0.012) display the highest magnetic moments (4.43 ± 0.04 and 4.52 ± 0.04 μB/Mn), respectively. The more concentrated samples exhibit weaker magnetic moments (2.85 ± 0.03 μB/Mn for Mn:Cd = 0.018) as a result of antiferromagnetic coupling between Mn2+ second neighbors. Cathodoluminescence spectroscopy experiments were performed from 50 to 300 K to assess the temperature dependence of emissions related to the CdS near band edge, the Mn intra d-shell4T1 → 6A 1 transition, defectrelated surface state transitions, and the effect of surface passivation with carbon. The temperature-dependent spectral line shape variations, the emission intensities, and energies of the various components were examined for each Mn doping density to evaluate the incorporation of Mn2+ into the host CdS nanocrystal lattice.
UR - http://www.scopus.com/inward/record.url?scp=79951708648&partnerID=8YFLogxK
U2 - 10.1021/jp107083f
DO - 10.1021/jp107083f
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SN - 1932-7447
VL - 114
SP - 22002
EP - 22011
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 50
ER -