- Nano Express
- Open Access
Temperature and composition dependent excitonic luminescence and exciton-phonon coupling in CdSeS nanocrystals
© Wu et al.; licensee Springer. 2012
- Received: 7 February 2012
- Accepted: 20 April 2012
- Published: 8 June 2012
The yellow- and red-emitting CdSeS nanocrystals (NCs) synthesized through one-step organometallic synthesis method are uniformly assembled in polymethyl methacrylate (PMMA). A higher-energy emission band originates from band-edge excitonic state appeared at low temperature. With the Se dopant concentration increasing, the luminescent spectra of CdSeS NCs have a red-shifted emission peak and a shorter luminescent lifetime, which is attributed to the existence of trapping state caused by surface defect and Se dopant. CdSeS NC shows a shorter luminescence lifetime and higher energy emission peak in PMMA matrix than that in toluene, indicating that the former is more favorable to transfer energy through exciton-phonon coupling. The upconversion luminescence (UCL) is observed using 800 nm femtosecond laser excitation. The pump power dependence demonstrated UCL spectra of yellow-emitting CdSeS NCs has a slope of 2.2, while that of red-emitting CdSeS NCs has a slope of 1.4. The results demonstrate that the two-photon absorption plays a dominating role when Se concentration of CdSeS NCs is lower, while phonon-assisted UCL by one-photon excitation gradually takes place with the amount of Se dopants increasing.
Various methods of synthesizing semiconductor nanocrystals (NCs) have been investigated in liquid phase, in which NCs are suspended in most organic solvents or aqueous solution, making them less practical for fabrication and integration into optoelectronic devices. Therefore, the solidification of NCs in matrix is prerequisite before the assembling of NCs into electronic and optoelectronic devices. Recently, hybrid organic/inorganic nanocomposites have recently attracted considerable interests due to their promising optoelectronic properties and applications. Blends of conjugated polymers and colloidal semiconductor quantum dots have been advantageously used for light-emitting diodes [1–3], ultrasensitive radiation detection , and solar energy conversion . To realize flexible color conversion or emitting devices, it is desirable to synthesize composite materials consisting of NCs and polymers, in which the thermally stable semiconductor NCs work as the color-emission centers and the transparent polymers as the embedding matrix materials [6, 7]. In addition to this application-driven demand, fundamental physical questions on the coupling between Frenkel excitons in organic molecules and Wannier excitons in inorganic semiconductors have gained enormous attentions .
The alloyed and doped NCs are promising in biological and luminescent bifunctional applications [9–11]. In previous works, the synthesis, basic optical properties, and structural characteristics of doped CdSeS NCs have been reported [12, 13], but the time-resolved luminescent property is lack of investigation. In this work, we describe a simple prepolymerization method to prepare doped NCs/polymethyl methacrylate (PMMA) composite materials with uniform distribution. Taking into account that exciton luminescence is a strongly temperature-dependent process, it should be possible to distinguish mechanism of radiative and nonradiative transition in NCs/PMMA composite materials. Then, the luminescent mechanisms of doped CdS NCs in different host materials are investigated using time-resolved luminescence technique.
In the synthesis of CdSeS NCs, Cd, Se, and S, precursor solutions are prepared separately in three necked flasks. A mixture of CdO, oleic acid, and 1-octadecene is heated at 300°C to get a clear solution used as the Cd precursor. The selenium and sulfur source mixture with different molar ratios in trioctylphosphine is prepared and injected into the hot precursor reaction medium of CdO in solution [14, 15]. The reaction solutions are injected into methanol and then CdSeS NCs powder is generated after evaporation of organic solvent. The dopant incorporation into semiconductors NCs plays an important role in optical and structural characteristics . Doped CdSeS NCs are prepared in TOPO solvent. The Se/S molar ratios are 0.04:1 and 0.10:1 for yellow- and red-emitting NCs, respectively, which are revealed by induced coupled plasma mass spectroscopy. For simplicity, CdSeS NCs with molar ratio (0.04:1) emit yellow light, which are called yellow-emitting NCs; CdSeS NCs with molar ratio (0.10:1) emit red light, which are called red-emitting NCs. The yellow- and red-emitting NCs are dispersed in toluene at a concentration of 1 mg/mL. Under vigorous stirring, 0.2 mL-doped CdSeS NCs in toluene solution are slowly added into the distilled methyl methacrylate , which contains azobisisobutyronitrile of 0.5% in weight. As a prepolymerization process, the MMA-NC solution is first heated in a flask at about 90°C for 20 min to get the suitable viscosity. It is then poured into molds and put into a desiccator at 60°C in vacuum for post polymerization. Generally, the whole process in the desiccator is conducted for more than 20 h. Optical absorption spectra from 3.10 to 1.13 eV with 1-nm step are measured on a Perkin-Elmer Lambda 900 spectrophotometer at room temperature (PerkinElmer, Waltham, MA, USA). Power X-ray diffraction (XRD) spectra are taken on a Philips X'pert diffractometer CdSeS NCs in toluene are deposited onto low-scattering quartz plates, and the solvent is evaporated. Employing a He-Cd laser (λ = 325 nm) as the excitation source, the low temperature photoluminescence (PL) spectroscopy is carried out to characterize the optical properties of CdSeS NCs. We performed steady-state and time-resolved luminescent studies under femtosecond laser excitation. The laser pulses are generated by a Ti: sapphire regenerative amplifier (1 KHz, Spectra Physics, Spitfire, which outputs 130 fs full width at half maximum at the central wavelength of 800 nm. The pump pulses with central wavelength of 3.10 eV are produced by high-level harmonic generation using barium boric oxide nonlinear crystal. Time-resolved luminescence is measured with ICCD (Intensified Charge Coupled Device, Andor, IStar740,) on a spectrometer (Bruker Optics 250IS/SM). The CdSeS NCs are excited by femtosecond pulses at 1.55 or 3.10 eV with a repetition rate of 83 Hz. Instrument response time τ is 2 ns when scattering femtosecond laser pulses are measured. All steady-state and time-resolved luminescent measurements are performed in a darkroom, and samples are placed in sealed cuvette to prevent oxidation.
Absorption and emission properties of CdSeS NCs
Low-temperature luminescent properties of CdSeS NCs
where Eϵ (0) is the transition energy at 0 K, which is blue shifted from the bulk band gap due to quantum confinement effects; αB is the strength of the electron-average phonon coupling; θ is the temperature corresponding to an average phonon energy. The best fitting of yellow-emitting CdSeS NCs (black lines in Figure3a) yields Eϵ (0) = 2.289 eV, αB = 5 meV, and θ = 85 K. The estimated average phonon temperature θ in the sample is lower than the LO phonon temperature (about 305 and 300 K) of cubic CdSe and CdS, indicating that acoustic phonons as well as optical phonons contribute to the red-shift of the emission energy. The θ value contains information about the contribution of the acoustic phonons to the blue shift of band gap emission: the smaller the θ value with respect to the LO phonon energy, the larger the contribution of the acoustic phonons to the band gap broadening through exciton-phonon coupling. The electron-average phonon coupling strength αB is slightly smaller than that of bulk CdSe (36 meV) , which demonstrates that the structure of doped NCs have a more intrinsic exciton picture than pure NCs. The strength of multiple exciton-phonon coupling is enhanced with the increasing Se dopant . Intensities of both the trapping and excitonic emission increased markedly at lower temperature, this effect is attributed to the suppression of phonon-coupled thermal quenching and different sensitivities of temperature dependence between trapping and excitonic state in NCs, while peak shifts at lower energy band are attributed to trapping state in low temperature spectra of CdTe NCs in the previous work [25, 26]. In the doped structures, this can be understood by taking into account a competing influence by a more efficient recombination channel that causes the overall red shift of the absorption and PL peaks with comparison to that of CdS NCs with similar size. The enhancement of luminescence in higher photon energy band at lower temperature is attributed to excitonic state from CdS host NCs. The prominent luminescence is attributed to trapping state originated from the hole wave function spatially localized around the Se defect .
As well as we know, the ionic radius of S2− is 0.17 nm, whereas that of Se2 is 0.18 nm. Se2− ions are mostly injected into crystal lattice and substitute the site of S2- ions because of good crystal matching. Several Se2 ions in the CdS NCs create a distribution of traps within a band gap as impurity states, which leads to a red-shifted narrow emission compared to that of pure CdS NCs. The light emission of pure CdS NCs are mostly in the blue to green spectral range; however, luminescence emission may be extended to UV and near-infrared spectral range through element-doping method. Although Se element with only a small quantity (molar ratios of Se to S are 4.0% and 10%) is in the form of CdSeS NCs, the trapping energy level due to Se impurity and surface defects is dominant on luminescence of CdSeS NCs. With the amount of Se2− ions in CdSeS NCs increasing, the lowest impurity state is further lowered in energy gap. In order to further verify the assumption, we need to consider that the temperature dependence of the energy gap is usually similar to the bulk semiconductor one, except for a temperature-independent energy offset due to the quantum confinement.
Host and composition dependent time-resolved luminescence of CdSeS NCs
Here, Se-doped NCs, in which the dopant atoms form a defect state, spatially localizes only the holes and traps electron. Hole wave function overlaps with carriers in valence band, which enhances the electronic potential and shifts up the position of valence band. With more Se incorporation, simple trapping states evolutes to a trapping energy band. One of the optical transition routes always happened between conduction band minimum (CBM) and the highest level of trapping band. When Se dopant concentration achieves a critical value, trapping energy band will merge into valance band maximum (VBM). The band gap decreases because of stronger overlap of the hole wave functions due to more Se dopant.
The biexponential fitting strongly implies the involvement of other excited states in this luminescence process for CdSeS NCs in both host materials. These energy levels are more likely to be of the surface nature. In the previous study, an intensity-dependent energy level can explain the red shift of the emission peak using infrared femtosecond laser excitation , where two excited states are higher-lying optical-allowed state and a lower-lying surface state with a triplet origin. Here, we show that a few atoms of Se incorporated in each dot can have a significant effect not only on the linear but also on the nonlinear properties of the entire nanocomposites .
In Figure4a, we can see that CdSeS NCs in PMMA has a blue shift about 2 nm with comparison to that in toluene, it is due to the oxidation of surface during the prepolymerization process. However, its luminescence has a shorter lifetime and is presumably originated from exciton-phonon coupling in NCs/PMMA. Since surface oxidation changes the position of surface-trapping state in energy gap, it is another point of view which causes a large increase in the local dielectric constant relative to the PMMA medium (ϵ PMMA = 2.60). Toluene has a slightly lower dielectric constant (ϵ toluene = 2.38) than PMMA and could result in an increase of the emission energy in the larger NCs . PMMA as a host for exciton-phonon coupling and relatively small distance between neighboring NCs in PMMA enhance the possibility of a direct carrier transfer. It is reasonable that enhancement of excitonic state emission occurs when the host material form toluene to PMMA. Certain media, e.g., a PMMA polymer, destroy the perfection of the ligands capping, thus inducing a reduction of lifetime τave. PMMA media induces a surrounding with a relatively high dielectric constant which differs from other organic media. The lifetime of the NCs embedded in PMMA and water solution is thus scaled by a factor of from that measured in toluene solution. But simple simulations are not helpful for analysis of luminescent property because of intrinsic energy level structure. In general, trapping state emissions have longer radiative lifetimes due to lower transition probability relative to band-edge excitonic combination. The average lifetime of NCs/PMMA becomes shorter than that of dispersed in toluene. We adopt long-lived species to investigate the dependence of detection photon energy of CdSeS NCs, because faster components in biexponential decay usually reflect the excitonic recombination process of an electron and a hole. The long lifetime decay component becomes shorter from 24.2to 16.2 ns with the change of host material from dispersed in toluene to PMMA. Obviously, the lifetime (1 2 ns) of band-edge PL does not depend on detection wavelengths shown in Figure4. However, the long-lived species, which is attributed to surface or trapping state , rebounds to investigate the mechanism of luminescence in detail. The long lifetime component becomes longer from 12.5to 19.9 ns with the change of detection energies from 2.3to 2.1 eV. Therefore, the average PL lifetime increases steadily with increased QDs size. The wavelength dependence of the luminescence decay indicates that surface excitonic emission indicates the difference between the populations of different sizes of NCs. The larger NCs, which emit at the longer wavelength, have surface state emission with a longer lifetime. We suggest that the PMMA form a strongly coupled electronic bath that forms the environment controlling energetic fluctuations and, hence, irradiative trapping kinetics in the CdSeS NCs. The NCs/PMMA composites can be applied to fiber communication and all-optical limiting switching and electroluminescence. The work on the application of luminescent NCs/PMMA composite for brand new solid state lighting devices and optical limiting is in progress.
Upconversion luminescence of CdSeS NCs
Overall, the optical properties of CdSeS NCs are found to be radically different from the binary NCs and to a certain extent from those reported for other ternary NCs. The involvement of trapping state due to anion dopant makes these materials of many potential interests in quantum dot laser and solar cell conversion.
We synthesized a CdSeS NCs/PMMA composite using prepolymerization method. PMMA, a transparent material in the visible spectral range, is chosen as the embedding matrix for the NCs. The steady-state and time-resolved luminescence of Se-doped CdS NCs has been studied. The long lifetime component of CdSeS NCs in PMMA is shorter than that dispersed in toluene. We have described a model for impurity doping in semiconductor CdSeS NCs based in terms ideas of low temperature and composition dependence of luminescence. The model shows that Se dopant, which are used to control emission wavelength, play another important role by affecting energy structure. By choosing a suitable composition of NCs with special size, our model can offer a route to rational optimization of doped NCs and tailor the PL spectrum of the composite devices in the visible spectral range.
This research is partially supported Natural Scientific Foundation of Heilongjiang Province (F201032, QC2011C008), Natural Scientific Foundation of Dalian City (2010J21DW020), Heilongjiang Province Postdoctoral Science Foundation (LBH-Q09032, LBH-Z10047), We gratefully acknowledge the key laboratory of Electronics Engineering, College of Heilongjiang province and and high-level Team Project (Hdtd2010-15) of Heilongjiang University. We also thank Dr. Wei Xie in the research institute of organic chemistry providing CdSeS NCs to support this research.
- Colvin VL, Schlamp MC, Alivisatos AP: Light-emitting-diodes made from cadmium selenide nanocrystals and a semiconducting polymer. Nature 1994, 370: 354–357. 10.1038/370354a0View ArticleGoogle Scholar
- Dabbousi BO, Bawendi MG, Onitsuka O, Rubner MF: Electroluminescence from Cdse quantum-dot polymer composites. Appl Phys Lett 1995, 66: 1316–1318. 10.1063/1.113227View ArticleGoogle Scholar
- Lee J, Sundar VC, Heine JR, Bawendi MG, Jensen KF: Full color emission from II-VI semiconductor quantum dot-polymer composites. Adv Mater 2000, 12: 1102–1105. 10.1002/1521-4095(200008)12:15<1102::AID-ADMA1102>3.0.CO;2-JView ArticleGoogle Scholar
- Campbell IH, Crone BK: Quantum-dot/organic semiconductor composites for radiation detection. Adv Mater 2006, 18: 77–79. 10.1002/adma.200501434View ArticleGoogle Scholar
- Bao H, Habenicht BF, Prezhdo OV, Ruan XL: Temperature dependence of hot-carrier relaxation in PbSe nanocrystals: an ab initio study. Phys Rev B 2009, 79: 235306–235312.View ArticleGoogle Scholar
- Song H, Lee S: Photoluminescent (CdSe) ZnS quantum dot-polymethylmethacrylate polymer composite thin films in the visible spectral range. Nanotechnology 2007, 18: 055402–055407. 10.1088/0957-4484/18/5/055402View ArticleGoogle Scholar
- Zhang CX, O’Brien S, Balogh L: Comparison and stability of CdSe nanocrystals covered with amphiphilic poly(amidoamine) dendrimers. J Phys Chem B 2002, 106(40):10316–10321. 10.1021/jp014241kView ArticleGoogle Scholar
- Stoferle T, Scherf U, Mahrt RF: Energy transfer in hybrid organic/inorganic nanocomposites. Nano Lett 2009, 9: 453–456. 10.1021/nl8034465View ArticleGoogle Scholar
- Santangelo SA, Hinds EA, Vlaskin VA, Archer PI, Gamelin DR: Bimodal bond-length distributions in cobalt-doped CdSe, ZnSe, and Cd1-xZnxSe quantum dots. J Am Chem Soc 2007, 129: 3973–3978. 10.1021/ja068260pView ArticleGoogle Scholar
- Swafford LA, Weigand LA, Bowers MJ, McBride JR, Rapaport JL, Watt TL, Dixit SK, Feldman LC, Rosenthal SJ: Homogeneously alloyed CdSxSe1-(x)nanocrystals: synthesis, characterization, and composition/size-dependent band gap. J Am Chem Soc 2006, 128: 12299–12306. 10.1021/ja063939eView ArticleGoogle Scholar
- Kwak WC, Kim TG, Chae WS, Sung YM: Tuning the energy bandgap of CdSe nanocrystals via Mg doping. Nanotechnology 2007, 18: 205702–205709. 10.1088/0957-4484/18/20/205702View ArticleGoogle Scholar
- Yu DQ, Chen X, Zhang HQ, Hu LZ, Sun JC, Qiao SS, Sun KT, Zhu JX: Anomalous temperature dependent photoluminescence properties of CdSxSe1−xquantum dots. Science China: Physics, Mechanics & Astronomy 2010, 53: 1842–1846. 10.1007/s11433-010-4099-6Google Scholar
- Ouyang JY, Vincent M, Kingston D, Descours P, Boivineau T, Zaman MB, Wu XH, Yu K: Noninjection, one-pot synthesis of photoluminescent colloidal homogeneously alloyed CdSeS quantum dots. J Phys Chem C 2009, 113: 5193–5200. 10.1021/jp8110138View ArticleGoogle Scholar
- Al-Salim N, Young AG, Tilley RD, McQuillan AJ, Xia J: Synthesis of CdSeS nanocrystals in coordinating and noncoordinating solvents: solvents role in evolution of the optical and structural properties. Chem Mater 2007, 19: 5185–5193. 10.1021/cm070818kView ArticleGoogle Scholar
- Chong SV, Suresh N, Xia J, Al-Salim NI, Idriss H: TiO2nanobelts/CdSSe quantum dots nanocomposite. J Phys Chem C 2007, 111: 10389–10393. 10.1021/jp072579uView ArticleGoogle Scholar
- Yu WW, Qu LH, Guo WZ, Peng XG: Experimental determination of the extinction coefficient of CdTe, CdSe, and CdS nanocrystals. Chem Mater 2003, 15: 2854–2860. 10.1021/cm034081kView ArticleGoogle Scholar
- Langer DW, Park YS, Euwema RN: Phonon coupling in edge emission and photoconductivity of Cdse Cds and Cd (SexS1-X). Phys Rev 1966, 152: 788–796. 10.1103/PhysRev.152.788View ArticleGoogle Scholar
- Cao YC, Wang JH: One-pot synthesis of high-quality zinc-blende CdS nanocrystals. J Am Chem Soc 2004, 126: 14336–14337. 10.1021/ja0459678View ArticleGoogle Scholar
- Seitz F: Low temperature luminescence of inorganic solids. Trans Faraday Soc 1939, 35: 79–87.View ArticleGoogle Scholar
- Huang K, Rhys A: Theory of light absorption and non-radiative transitions in F-centres. Proceedings of the Royal Society of London Series a-Mathematical and Physical Sciences 1950, 204: 406–423. 10.1098/rspa.1950.0184View ArticleGoogle Scholar
- Joshi A, Narsingi KY, Manasreh MO, Davis EA, Weaver BD: Temperature dependence of the band gap of colloidal CdSe/ZnS core/shell nanocrystals embedded into an ultraviolet curable resin. Appl Phys Lett 2006, 89: 131907–131909. 10.1063/1.2357856View ArticleGoogle Scholar
- Malikova L, Krystek W, Pollak FH, Fred H, Dai N, Cavus A, Tamargo MC: Temperature dependence of the direct gaps of ZnSe and Zn0.56Cd0.44Se. Phys Rev B 1996, 54: 1819–1824. 10.1103/PhysRevB.54.1819View ArticleGoogle Scholar
- Lautenschlager P, Garriga M, Logothetidis S, Cardona M: Interband critical-points of gas and their temperature-dependence. Phys Rev B 1987, 35: 9174–9189. 10.1103/PhysRevB.35.9174View ArticleGoogle Scholar
- Shen Q, Kobayashi J, Diguna LJ, Toyoda T: Effect of ZnS coating on the photovoltaic properties of CdSe quantum dot-sensitized solar cells. J Appl Phys 2008, 103: 084304–084308. 10.1063/1.2903059View ArticleGoogle Scholar
- Wuister SF, Donega CDM, Meijerink A: Luminescence temperature antiquenching of water-soluble CdTe quantum dots: role of the solvent. J Am Chem Soc 2004, 126: 10397–10402. 10.1021/ja048222aView ArticleGoogle Scholar
- Nonoguchi Y, Nakashima T, Kawai T: Size- and temperature-dependent emission properties of zinc-blende CdTe nanocrystals in ionic liquid. J Phys Chem C 2007, 111: 11811–11815. 10.1021/jp073152qView ArticleGoogle Scholar
- Avidan A, Oron D: Large blue shift of the biexciton state in tellurium doped CdSe colloidal quantum dots. Nano Lett 2008, 8: 2384–2387. 10.1021/nl801241mView ArticleGoogle Scholar
- Kim D, Mishima T, Tomihira K, Nakayama M: Temperature dependence of photoluminescence dynamics in colloidal CdS quantum dots. J Phys Chem C 2008, 112: 10668–10673. 10.1021/jp8009172View ArticleGoogle Scholar
- Liu LP, Peng Q, Li YD: An effective oxidation route to blue emission CdSe quantum dots. Inorg Chem 2008, 47: 3182–3187. 10.1021/ic702203cView ArticleGoogle Scholar
- Javier A, Magana D, Jennings T, Strouse GF: Nanosecond exciton recombination dynamics in colloidal CdSe quantum dots under ambient conditions. Appl Phys Lett 2003, 83: 1423–1425. 10.1063/1.1602159View ArticleGoogle Scholar
- Wu WZ, Qu W, Ye HA, Zheng ZR, Yang YQ: Photoluminescent spectroscopic and kinetic studies on green-emitting CdSeS quantum dot/polymethyl methacrylate composite. J. Non-Cryst. Solids. 2010, 356: 1016–1020. 10.1016/j.jnoncrysol.2010.01.022View ArticleGoogle Scholar
- Franzl T, Muller J, Klar TA, Rogach AL, Feldmann J: CdSe:Te nanocrystals: band-edge versus Te-related emission. J Phys Chem C 2007, 111: 2974–2979. 10.1021/jp067166sView ArticleGoogle Scholar
- Potyrailo RA, Leach AM: Selective gas nanosensors with multisize CdSe nanocrystal/polymer composite films and dynamic pattern recognition. Appl Phys Lett 2006, 88: 134110–134112. 10.1063/1.2190272View ArticleGoogle Scholar
- Wang XY, Qu LH, Zhang JY, Peng XG, Xiao M: Surface-related emission in highly luminescent CdSe quantum dots. Nano Lett 2003, 3: 1103–1106. 10.1021/nl0342491View ArticleGoogle Scholar
- Poles E, Selmarten DC, Micic OI, Nozik AJ: Anti-Stokes photoluminescence in colloidal semiconductor quantum dots. Appl Phys Lett 1999, 75: 971–3. 10.1063/1.124570View ArticleGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.