- Nano Express
- Open Access
Ferromagnetism in sphalerite and wurtzite CdS nanostructures
© Yang et al.; licensee Springer. 2013
- Received: 27 November 2012
- Accepted: 22 December 2012
- Published: 7 January 2013
Room-temperature ferromagnetism is observed in undoped sphalerite and wurtzite CdS nanostructures which are synthesized by hydrothermal methods. Scanning electron microscopy and transmission electron microscopy results indicate that the sphalerite CdS samples show a spherical-like shape and the wurtzite CdS ones show a flower-like shape, both of which are aggregated by lots of smaller particles. The impurity of the samples has been ruled out by the results of X-ray diffraction, selected-area electron diffraction, and X-ray photoelectron spectroscopy. Magnetization measurements indicate that all the samples exhibit room-temperature ferromagnetism and the saturation magnetization decreases with the increased crystal sizes, revealing that the observed ferromagnetism is defect-related, which is also confirmed by the post-annealing processes. This finding in CdS should be the focus of future electronic and spintronic devices.
- CdS nanostructures
- Hydrothermal methods
- Room-temperature ferromagnetism
- Sulfur vacancies
Since the first discovery of ferromagnetism (FM) in Mn-doped GaAs , great effort has been paid to search for intrinsic dilute magnetic semiconductors (DMSs) with Curie temperatures (Tc) at or above room temperature (RT) by doping semiconductors with transition metals (TMs) [2, 3]. During the past few years, room-temperature ferromagnetism (RTFM) has been reported in TM-doped DMSs experimentally. Nevertheless, the mechanism of the observed FM remains controversial theoretically, which mainly includes experimental artifacts, segregation of secondary ferromagnetic phases, magnetic clusters, and indirect exchange mediated by carriers, electrons, and holes associated with impurities that are related to the observed RTFM [4–7]. Subsequently, RTFM has also been observed in undoped semiconducting or insulating (such as HfO2, In2O3, MgO, ZnO, SnO2, etc.) [8–12], where nominal magnetic ions are not present, and the term ‘d 0 FM’ [13, 14] was suggested to summarize these cases. It is strongly believed that the point defects in semiconductors or insulators have an open-shell electronic configuration, which can indeed confine the compensating charges in molecular orbitals, forming a local magnetic moment. Recently, experiment results show that the size of the lower dimensional systems, such as film thickness or diameter of nanoparticles, has an effect on the vacancy concentration as well as their magnetic behavior [15, 16]. The results are also supported by theoretical works which show the effects of curvature, confinement, and size on various properties of nanocrystals [17, 18]. Obviously, the surface-to-volume atomic ratio will be increased significantly with the decreased size of nanocrystals. Since the surface has a broken atomic symmetry and it often has higher anisotropy, new surface states that differ from their bulk form are established, which play a crucial role in controlling the electronic, optical, and other properties of nanocrystals.
CdS, belonging to the II-VI compound family, has a considerably important application such as in optoelectronic devices, photocatalysts, solar cells, optical detectors, and nonlinear optical materials [19–25]. If RTFM were achieved in CdS, it would be a potential candidate in the fabrication of new-generation magneto-optical and spintronic devices. Remarkably, lots of investigations have demonstrated FM with Tc above room temperature observed in transition metal ion (such as Fe, Co, Cr, Mn, and V)-doped CdS-based low-dimensional materials [26–30]. Recently, Pan et al. demonstrated that FM can be realized in CdS with C doping via substitution of S which can be attributed to the hole-mediated double-exchange interaction . Li et al. also studied a Cu-doped CdS system by first-principles simulation and predicted that the system shows a half-metallic ferromagnetic character and the Tc of the ground state is above RT . Meanwhile, Ren et al. indicated that Pd doping in CdS may lead to a long-range ferromagnetic coupling order, which results from p d exchange coupling interaction . Moreover, Ma et al. studied the magnetic properties of non-transition metal/element (Be, B, C, N, O, and F)-doped CdS and explained the magnetic coupling by p p interaction involving holes . In this paper, we report the observation of size-dependent RTFM in CdS nanostructures (NSs). The CdS NSs in sphalerite and wurtzite structures were synthesized by hydrothermal methods with different sulfur sources. The structure and magnetic properties of the samples were studied.
CdS NSs were synthesized by hydrothermal methods. In a typical procedure for the synthesis of sphalerite CdS samples, 0.15 M cadmium chloride (CdCl2 · 2.5H2O) and 0.15 M sodium thiosulfate (Na2S2O3 · 5H2O) were added into 40 mL deionized water. After stirring for 30 min, the mixed solution was transferred into a Teflon-lined stainless steel autoclave of 50-mL capacity. After being sealed, the solution was maintained at 90°C for 2, 4, 6, and 8 h, which were denoted as S1, S2, S3, and S4, respectively. The resulting solution was filtered to obtain the samples. To eliminate the impurity ions, the products were further washed with deionized water for several times and then dried in air at 60°C. Wurtzite CdS were synthesized with different sulfur sources. In this method, 0.2 M cadmium chloride (CdCl2 · 2.5H2O) and 0.2 M thioacetamide (CH3CSNH2) were added into 40 mL deionized water. After stirring, the cloudy solution was transferred into a Teflon-lined stainless steel autoclave of 50-mL capacity. After being sealed, the solution was maintained at 60°C for 4, 6, 8, and 10 h, which were denoted as S5, S6, S7, and S8, respectively. The as-formed wurtzite CdS NSs were filtered, washed with deionized water, and then dried in air at 40°C.
X-ray diffraction (XRD; X’Pert PRO PHILIPS with Cu Kα radiation, Almelo, The Netherlands) was employed to study the structure of the samples. The morphologies of the samples were obtained using a scanning electron microscope (SEM; Hitachi S-4800, Chiyoda-ku, Japan). Microstructures of the samples were characterized using a transmission electron microscope (TEM; Tecnai TMG2F30, FEI, Hillsboro, OR, USA) and high-resolution TEM (HRTEM) equipped with selected-area electron diffraction (SAED) and energy-dispersive X-ray spectrum (EDS). The measurements of static magnetic properties were made using a Quantum Design MPMS magnetometer based on a superconducting quantum interference device (SQUID; San Diego, CA, USA). Electron spin resonance (ESR; JEOL, JES-FA300, microwave frequency is 8.984 GHz, Akishima-shi, Japan) spectra were recorded to study the dynamic magnetic properties of the samples. The chemical bonding state and the compositions of the samples were determined by X-ray photoelectron spectroscopy (XPS; VG Scientific ESCALAB-210 spectrometer, East Grinstead, UK) with monochromatic Mg Kα X-rays (1,253.6 eV). The thermogravimetric and differential thermal analysis (TG-DTA; DuPont Instruments 1090B, Parkersburg, VA, USA) was employed to obtain the variation of mass and phase transition details of the samples during argon annealing.
ESR was performed to further characterize the magnetic properties of the sphalerite CdS NSs. Figure 5c depicts the ESR results measured at different temperatures from 90 to 300 K for sample S1. It can be seen that the sample shows resonance signals with applied magnetic field from 0 to 500 mT. The center magnetic fields (Hcenter) for the sample are far from 321 mT which characterize a free electron (g = 2.0023), indicating that the sample has obvious FM , and the ferromagnetic coupling between the moments increase with the decreasing temperature. According to the theory of ferromagnetic resonance , the relationship between resonance field and microwave frequency in the ferromagnetic resonance is hν = gμB · H, where h, ν, g, μB, and H are the Planck constant, frequency of the applied microwave magnetic field, g-factor, Bohr magnetron, and resonance magnetic field, respectively. In FM materials, the orbital angular momentum quenching in the crystal field and g-factor is 2.0023; the resonance field is made up of applied field Ha and magnetocrystalline anisotropy field Hk: H = Ha + Hk. If we define Ha as H and attribute the change of Hk to the g-factor, which is defined as an effective g-factor (geff), then the ferromagnetic resonance relationship changes to hν = geffμB · Ha. Hk will increase with the decreasing temperature, and then geff will get higher. In sample S1, the geff increases from 2.54 to 2.74 as the temperatures decrease from RT to 90 K. The results in Figure 5d indicate that the variation of ΔH (=321 mT − Hcenter, which represents the position of the resonance peak) measured at different temperatures is consistent with that of Ms in the samples.
The M H curves for the post-annealing samples and the variation of their Ms are shown in Figure 8c,d, respectively. It can be seen that the Ms of the samples decrease continuously after post-annealing at 200°C and 400°C. However, the Ms increases with the increasing annealing temperature when the annealing temperature exceeds 400°C. The chemical composition calculated from the XPS result shows that Cd and S have an atomic ratio of 76.7:23.3 for sample S1 after being annealed at 800°C, which indicates that the density of sulfur vacancies gets higher than that of the as-prepared sample. As the analysis of the above annealing progresses, it can be understood that argon annealing at a temperature lower than 400°C results in crystal grain reconstruction and growth which compensates the sulfur vacancies. However, when the annealing temperature gets higher, the sample begins to decompose and promotes large amount of vacancies. Subsequently, the exchange interaction between these different concentrations of sulfur vacancies changes the Ms. Note that changes of Ms for the wurtzite-structure samples after post-annealing processes have the same variation as those for the sphalerite ones above. The post-annealing results further clarify the role of sulfur vacancies in triggering the RTFM in undoped CdS [34, 41].
In summary, well-crystalline CdS NSs both in sphalerite and wurtzite were synthesized by simple hydrothermal methods. The NSs were self-aggregated into spherical and flower shapes, respectively. Intrinsic FM is observed in the samples by the magnetic hysteresis loops and prominent ferromagnetic resonance signals. The mechanism of RTFM from sulfur vacancies is proposed. Moreover, the magnetization value can be tuned by changing the concentration of sulfur vacancies, which is affected by the particle size and annealing condition. These findings not only demonstrate that pure CdS shows tunable RTFM, but also suggest that introduction of sulfur vacancies can be a significant way to mediate the d 0 FM.
This work is supported by the National Basic Research Program of China (grant no. 2012CB933101), the NSFC (grant nos. 11034004 and 51202101), the National Science Fund for Distinguished Young Scholars (grant no. 50925103), and the Fundamental Research Funds for the Central Universities (no. lzujbky-2012-28).
- Ohno H, Shen A, Matsukura F, Oiwa A, Endo A, Katsumoto S, Lye Y: (Ga, Mn)As: a new diluted magnetic semiconductor based on GaAs. Appl Phys Lett 1996, 69: 363. 10.1063/1.118061View ArticleGoogle Scholar
- Dave N, Pautler BG, Farvid SS, Radovanovic PV: Synthesis and surface control of colloidal Cr3+-doped SnO2 transparent magnetic semiconductor nanocrystals. Nanotechnology 2010, 21: 134023. 10.1088/0957-4484/21/13/134023View ArticleGoogle Scholar
- Wu ZY, Chen FR, Kai JJ, Jian WB, Lin JJ: Fabrication, characterization and studies of annealing effects on ferromagnetism in Zn1−xCoxO nanowires. Nanotechnology 2006, 17: 5511–5518. 10.1088/0957-4484/17/21/036View ArticleGoogle Scholar
- Jin Z, Murakami M, Fukumura T, Matsumoto Y, Ohtomo A, Kawasaki M, Koinuma H: Combinatorial laser MBE synthesis of 3d ion doped epitaxial ZnO thin films. J Cryst Growth 2000, 214: 55–58.View ArticleGoogle Scholar
- Cho YM, Choo WK, Kim H, Kim D, Ihm YE: Effects of rapid thermal annealing on the ferromagnetic properties of sputtered Zn1-x(Co0.5Fe0.5)xO thin films. Appl Phys Lett 2002, 80: 3358–3360. 10.1063/1.1478146View ArticleGoogle Scholar
- Kaminski A, Sarma SD: Polaron percolation in diluted magnetic semiconductors. Phys Rev Lett 2002, 88: 247202.View ArticleGoogle Scholar
- Coey JMD, Venkatesan M, Fitzgerald CB: Donor impurity band exchange in dilute ferromagnetic oxides. Nat Mater 2005, 4: 173–179. 10.1038/nmat1310View ArticleGoogle Scholar
- Venkatesan M, Fitzgerald CB, Coey JMD: Thin films: unexpected magnetism in a dielectric oxide. Nature 2004, 430: 630. 10.1038/430630aView ArticleGoogle Scholar
- Huang LM, Århammar C, Moysés AC, Silvearv F, Ahuja R: Tuning magnetic properties of In2O3 by control of intrinsic defects. Europhys Lett 2010, 89: 47005. 10.1209/0295-5075/89/47005View ArticleGoogle Scholar
- Kapilashrami M, Xu J, Rao KV, Belova L, Carlegrim E, Fahlman M: Experimental evidence for ferromagnetism at room temperature in MgO thin films. J Phys Condens Matter 2010, 22: 345004. 10.1088/0953-8984/22/34/345004View ArticleGoogle Scholar
- Xing G, Wang D, Yi J, Yang L, Gao M, He M, Yang J, Ding J, Sum TC, Wu T: Correlated d0 ferromagnetism and photoluminescence in undoped ZnO nanowires. Appl Phys Lett 2010, 96: 112511. 10.1063/1.3340930View ArticleGoogle Scholar
- Wang C, Wu Q, Ge HL, Shang T, Jiang JZ: Magnetic stability of SnO2 nanosheets. Nanotechnology 2012, 23: 075704. 10.1088/0957-4484/23/7/075704View ArticleGoogle Scholar
- Coey JMD, Venkatesan M, Stamenov P, Fitzgerald CB, Dorneles LS: Magnetism in hafnium dioxide. Phys Rev B 2005, 72: 024450.View ArticleGoogle Scholar
- Coey JMD: d0 ferromagnetism. Solid State Sci 2005, 7: 660–667. 10.1016/j.solidstatesciences.2004.11.012View ArticleGoogle Scholar
- Nguyen HH, Joe S, Virginie B: Observation of ferromagnetism at room temperature in ZnO thin films. J Phys Condens Matter 2007, 19: 036219. 10.1088/0953-8984/19/3/036219View ArticleGoogle Scholar
- Xu X, Xu C, Dai J, Hu J, Li F, Zhang S: Size dependence of defect-induced room temperature ferromagnetism in undoped ZnO nanoparticles. J Phys Chem C 2012, 116: 8813–8818. 10.1021/jp3014749View ArticleGoogle Scholar
- Pemmaraju CD, Sanvito S: Ferromagnetism driven by intrinsic point defects in HfO2. Phys Rev Lett 2005, 94: 217205.View ArticleGoogle Scholar
- Pan H, Feng YP, Wu QY, Huang ZG, Lin J: Magnetic properties of carbon doped CdS: a first-principles and Monte Carlo study. Phy Rev B 2008, 77: 125211.View ArticleGoogle Scholar
- Ruxandra V, Antohe S: The effect of the electron irradiation on the electrical properties of thin polycrystalline CdS layers. J Appl Phys 1998, 84: 727. 10.1063/1.368129View ArticleGoogle Scholar
- Hullavarad NV, Hullavarad SS, Karulkar PC: Cadmium sulphide (CdS) nanotechnology: synthesis and applications. J Nanosci Nanotechnol 2008, 8: 3272. 10.1166/jnn.2008.145View ArticleGoogle Scholar
- Huynh WU, Dittmer JJ, Alivisatos AP: Hybrid nanorod-polymer solar cells. Science 2002, 295: 2425–2427. 10.1126/science.1069156View ArticleGoogle Scholar
- Oladeji IO, Chow L: Synthesis and processing of CdS/ZnS multilayer films for solar cell application. Thin Solid Films 2005, 474: 77–83. 10.1016/j.tsf.2004.08.114View ArticleGoogle Scholar
- Tenne R, Nabutovsky VM, Lifshitz E, Francis AF: Unusual photoluminescence of porous CdS (CdSe) crystals. Solid State Commun 1992, 82: 651–654. 10.1016/0038-1098(92)90055-EView ArticleGoogle Scholar
- Su B, Choy KL: Electrostatic assisted aerosol jet deposition of CdS, CdSe and ZnS thin films. Thin Solid Films 2000, 361: 102–106.View ArticleGoogle Scholar
- Brus LE: Quantum crystallites and nonlinear optics. Appl Phys A 1991, 53: 465–474. 10.1007/BF00331535View ArticleGoogle Scholar
- Ladizhansky V, Lyahovitskaya V, Vega S: 113Cd NMR study of transferred hyperfine interactions in the dilute magnetic semiconductors Cd1-xCoxS and Cd1-xFexS and impurity distribution in Cd0.994Co0.006S. Phy Rev B 1999, 60: 8097–8104. 10.1103/PhysRevB.60.8097View ArticleGoogle Scholar
- Delikanli S, He S, Qin Y, Zhang P, Zeng H, Zhang H, Swihart M: Room temperature ferromagnetism in Mn-doped CdS nanorods. Appl Phys Lett 2008, 93: 132501. 10.1063/1.2982583View ArticleGoogle Scholar
- Srivastava P, Kumar P, Singh K: Room temperature ferromagnetism in magic-sized Cr-doped CdS diluted magnetic semiconducting quantum dots. J Nanopart Res 2011, 13: 5077–5085. 10.1007/s11051-011-0488-7View ArticleGoogle Scholar
- Kim DS, Cho YJ, Park J, Yoon J, Jo Y, Jung MH: (Mn, Zn) co-doped CdS nanowires. J Phys Chem C 2007, 111: 10861–10868.View ArticleGoogle Scholar
- Herbich M, Mac W, Twardowski A, Demianiuk M: Role of the Jahn-Teller effect of the V2+ center in the magnetic anisotropy of Cd1-xVxS and Cd1-xVxSe. Phy Rev B 1999, 59: 2726–2730. 10.1103/PhysRevB.59.2726View ArticleGoogle Scholar
- Li P, Zhang C, Lian J, Gao S, Wang X: First-principles study on electronic and magnetic properties of Cu-doped CdS. Solid State Commun 2011, 151: 1712–1715. 10.1016/j.ssc.2011.07.042View ArticleGoogle Scholar
- Ren M, Zhang C, Li P, Song Z, Liu X: The origin of ferromagnetism in Pd-doped CdS. J Magn Magn Mater 2012, 324: 2039–2042. 10.1016/j.jmmm.2012.02.006View ArticleGoogle Scholar
- Ma Y, Dai Y, Huang B: Magnetism in non-transition-metal doped CdS studied by density functional theory. Comput Mater Sci 2011, 50: 1661–1666. 10.1016/j.commatsci.2010.12.025View ArticleGoogle Scholar
- Gao D, Yang G, Zhang J, Zhu Z, Si M, Xue D: d0 ferromagnetism in undoped sphalerite ZnS nanoparticles. Appl Phys Lett 2011, 99: 052502. 10.1063/1.3622303View ArticleGoogle Scholar
- Coey JMD, Mlack JT, Venkatesan M, Stamenov P: Magnetization process in dilute magnetic oxides. IEEE Trans Magn 2010, 46: 2501.View ArticleGoogle Scholar
- Huang B, Liu Y, Wang J, Zhang R, Zhang L, Zhang L, Mei L: Magnetic properties and giant magnetoresistance in Fe0.35(In2O3)0.65 granular film. J Phys Condens Matter 2003, 15: 47–53. 10.1088/0953-8984/15/2/305View ArticleGoogle Scholar
- Xin Y, Lu J, Stampe PA, Kenney RJ: Crystallographically orientated fcc Co nanocrystals in rutile TiO2 thin films. Appl Phys Lett 2006, 88: 112512. 10.1063/1.2172011View ArticleGoogle Scholar
- Lee S, Shon Y, Kim DY, Kang TW, Yoon CS: Enhanced ferromagnetism in H2O2-treated p-(Zn0.93Mn0.07)O layer. Appl Phys Lett 2010, 96: 042115. 10.1063/1.3294635View ArticleGoogle Scholar
- Aksu S, Bacaksiz E, Parlak M, Yılmaz S, Polat I, Altunbaş M, Türksoy M, Topkaya R, Özdoğan K: Structural, optical and magnetic properties of Mn diffusion-doped CdS thin films prepared by vacuum evaporation. Mater Chem Phys 2011, 130: 340–345. 10.1016/j.matchemphys.2011.06.046View ArticleGoogle Scholar
- Zelaya-Angel O, Lozada-Morales R: Sphalerite-wurtzite phase transformation in CdS. Phys Rev B 2000, 62: 13064–13069. 10.1103/PhysRevB.62.13064View ArticleGoogle Scholar
- Madhu C, Sundaresan A, Rao CNR: Room-temperature ferromagnetism in undoped GaN and CdS semiconductor nanoparticles. Phys Rev B 2008, 77: 201306.View ArticleGoogle Scholar
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