Photoluminescence Enhancement of Adsorbed Species on Si Nanoparticles
© Matsumoto et al. 2016
Received: 20 August 2015
Accepted: 27 December 2015
Published: 7 January 2016
We have fabricated Si nanoparticles from Si swarf using the beads milling method. The mode diameter of produced Si nanoparticles was between 4.8 and 5.2 nm. Si nanoparticles in hexane show photoluminescence (PL) spectra with peaks at 2.56, 2.73, 2.91, and 3.09 eV. The peaked PL spectra are attributed to the vibronic structure of adsorbed dimethylanthracene (DMA) impurity in hexane. The PL intensity of hexane with DMA increases by ~3000 times by adsorption on Si nanoparticles. The PL enhancement results from an increase in absorption probability of incident light by DMA caused by adsorption on the surface of Si nanoparticles.
KeywordsSi nanoparticle Si swarf Photoluminescence Absorbance Enhancement Anthracene
Si nanoparticles possess significant properties such as wide-bandgap energies due to the quantum confinement effect [1, 2], large surface area , and high reactivity . Moreover, Si is a safe material, possible to apply to the bio-medical field . Extensive studies have been performed to produce Si nanoparticles using various methods including laser ablation [6, 7], plasma-enhanced chemical vapor deposition (CVD) , hot wire CVD , sputtering , Si implantation , intense pulsed ion beam evaporation , and co-evaporation of SiO plus SiO2 with subsequent heat treatment . These methods require vacuum chambers and are time- and cost-consuming. Si nanoparticles can also be produced by chemical methods such as Zintl reaction and LiAlH reduction of SiCl4 . For a cheap fabrication method of Si nanoparticles, Lam et al.  employed the ball milling method, but only a small fraction of Si powders becomes nanometer size. We have developed a fabrication method of Si nanoparticles from Si swarf (i.e., industrial waste produced during slicing Si ingots) by use of the beads milling method [16, 17].
Si nanoparticles emit visible light under UV irradiation, applicable to light-emitting diodes  and biomarkers . Kang et al.  have shown that various color photoluminescence (PL) can be obtained from Si nanoparticles by varying the size of Si nanoparticles by oxidation.
PL from Si nanoparticles is differently attributed to several causes. In cases where the PL energy strongly depends on the size of Si nanoparticles, it arises most likely from band-to-band transition of Si nanoparticles because the bandgap energy is determined by its size due to the quantum confinement effect [1, 2]. On the other hand, Zhu et al.  and Inada et al.  have attributed PL from Si nanoparticles to energy states of SiO2 (most probably interface states) formed on Si nanoparticles, and in this case, the PL energy does not depend on the size of Si nanoparticles. It is also highly probable that PL is influenced by adsorbed species on Si nanoparticles. Adsorption of alkyl groups on Si nanoparticles is reported to cause blue shift due to prevention of transfer of electron-hole pairs from small (i.e., wide bandgap) to large (i.e., narrow bandgap) nanoparticles . Complicated structured PL spectra, e.g., three-peaked structure, have been observed for Si nanoparticles in hexane, which may arise from adsorbed species [22–24].
In the present study, Si nanoparticles have been fabricated from Si swarf by use of the beads milling method. Si nanoparticles in hexane show PL spectra with four peaks which are attributable to the vibronic structure of 9,10-dimethylanthracene (DMA) impurity in hexane. The PL intensity is increased by ~3000 times by adsorption of DMA on Si nanoparticles, and it is attributed to enhancement of excitation probability of DMA by adsorption on Si nanoparticles.
After cleaning Si swarf, Si nanoparticles were produced by use of the ball milling and beads milling methods. In the case of one-step milling, 0.5-mm zirconia beads were employed. For two-step milling, milling with 0.5-mm zirconia beads and then with 0.3-mm zirconia beads was performed in 2-propanol. Fabricated Si nanoparticles were filtered by use of a Teflon membrane filter, followed by immersion in hexane plus water. In some cases, 2 ml mixed solutions of 70 wt% HNO3 plus 50 wt% HF (HNO3:HF = 1:1 in volume) were added to 5 ml hexane containing Si nanoparticles.
X-ray diffraction (XRD) measurements were performed using a RIGAKU SmartLab diffractometer. Transmission electron microscopy (TEM) micrographs were observed using a JEOL JEM-3000F microscope at an incident electron energy of 300 keV. Measurements of PL spectra were carried out with a JASCO FP-8500 spectrometer after removal of aggregated and precipitated Si nanoparticles. Ultraviolet and visible light (UV-Vis) absorption spectra were recorded using a JASCO V-670 spectrometer. The PL quantum efficiencies were measured by a Hamamatsu Photonics K.K. Quantaurus-QY absolute PL quantum yields measurement system. The absolute PL quantum efficiencies were calculated from the ratio of a PL photon number to an absorbed photon number. These photon numbers were determined from a differential spectrum between two spectra of hexane solutions with and without Si nanoparticles.These spectra were measured with an integrating sphere to collect photons emitted in all directions into a spectrometer. A downward peak in a differential spectrum was due to the increase in absorption of excitation light caused by the addition of Si nanoparticles, while an upward peak was attributable to PL.
Results and Discussion
Figure 1b shows the volume distribution of Si nanoparticles vs. the diameter estimated from the analysis of the XRD (111) peak shape, obtained using the SLN profile method . For the one-step milling method, the maximum distribution (i.e., mode diameter) was present at 5.2 nm, the median diameter (cf. vertical line A by which the total area is divided into the two same areas) was 10.5 nm, and the average diameter was 13.2 nm. For the two-step milling method, the mode diameter, the median diameter, and the average diameter were estimated to be 4.8, 8.4, and 10.2 nm, respectively.
Figure 2 shows the PL spectra for Si nanoparticles fabricated from Si swarf by use of the beads milling method in hexane. The PL spectra had a peaked structure with peaks at 2.56, 2.73, 2.91, and 3.09 eV. The PL spectra hardly depended on the incident light excitation energy of 3.18–3.76 eV (Fig. 2a). If PL arose from the band-to-band transition of Si nanoparticles, the PL energy would strongly depend on the excitation energy because with an increase in the excitation energy, wider bandgap Si nanoparticles can be excited, leading to PL emission with higher energy. This is not the case, and the observed PL most probably arises from adsorbed species on Si nanoparticles. The PL spectra of Si nanoparticles were very similar to that of DMA (bottom spectrum in Fig. 2a) with peaks at 2.55, 2.75, 2.92, and 3.09 eV. The peaked structure with almost the identical energy separation of ~0.18 eV is due to the vibronic structure of DMA molecules . We conclude that the observed PL with the vibronic structure resulted from DMA impurity in hexane adsorbed on Si nanoparticles.
Figure 2b compares the PL spectra of Si nanoparticles produced by the one-step and two-step milling methods. Both the spectra possessed a peaked structure with nearly the same peak energies. In the case of two-step milling, the PL intensity was approximately twice that for one-step milling.
The same experiment was carried out using Si nanoparticles in 2,2,4-trimethyl pentane (TMP) instead of hexane, but no PL peaks attributable to DMA were observed probably because TMP did not contain DMA. It was also confirmed that PL intensity for vibronic structures increased by the addition of a 2 × 10−8 M DMA solution in hexane. These results clearly show that the vibronic structure arises from DMA molecules adsorbed on Si nanoparticles, and the PL intensity is enhanced by Si nanoparticles.
Spectrum b in Fig. 3 is for hexane without Si nanoparticles. For this spectrum, impurity in hexane was concentrated to 39 times by heating hexane, and the spectrum for unconcentrated hexane was subtracted from the spectrum for concentrated hexane. The structure of the spectrum in the energy region between 2.8 and 3.1 eV could not be determined because of the presence of a Raman peak with a strong intensity at 2.97 eV. The peaked structure nearly the same as those for Si nanoparticles in hexane was observed (cf. vertival dotted lines), but the PL intensity was much lower. From the ratio in the PL intensity for Si nanoparticles in hexane to that for hexane without Si nanoparticles, the PL enhancement factor was determined to be ~3000. Several researchers have observed PL enhancement by the presence of silver particles, and the enhancement is attributed to the plasmonic effect [28, 29]. The observed PL enhancement without Ag is not attributable to the plasmonic effect but to an increase in absorption probability of incident light by DMA due to adsorption on Si nanoparticles, as explained below.
where ψ f and ψ i are the wave functions of final and initial states, respectively, and e r is the dipole moment. The following are possible mechanisms to increase the excitation probability (cf. Fig. 5b): (i) dipole moment is induced by charge transfer between DMA and Si, and (ii) wave functions of DMA are enhanced possibly due to formation of surface resonance state  by overlapping of the wave functions of DMA and Si. Effects (i) and (ii) increase e r and ψ i , respectively, in Eq. (1). Both the effects increase the transition moment. More detailed experimental and theoretical studies are needed to clarify the mechanism of the PL enhancement.
The PL intensity of Si nanoparticles produced by the two-step milling method with a mode diameter of 4.8 nm is approximately twice that of Si nanoparticles fabricated by the one-step milling method (mode diameter 5.2 nm). From the mode diameter, the ratio in the surface areas of Si nanoparticles fabricated using the one-step and two-step milling methods is estimated to be 1:1.1, and therefore, the difference in the surface area cannot explain the PL intensity ratio of 1:2. The abovementioned effects, effects (i) and (ii), may be enhanced as the size of Si nanoparticles decreases. The great PL enhancement after DMA adsorption for the two-step milling method is most likely due to smaller Si nanoparticles with a higher concentration of active adsorption sites.
The PL quantum efficiencies can be estimated from measurements of the PL intensity divided by the absorbed light intensity. The absorbed light intensity was estimated from the incident light intensity and the integrated light intensity after passing through Si nanoparticle-containing hexane. The PL quantum efficiencies for Si nanoparticles produced by the one-step and two-step milling methods are estimated to be 9 and 15 %, respectively.
The PL intensity is enhanced by ~3000 times by adsorption of DMA on Si nanoparticles. The PL and UV-Vis absorption spectra possess peaked structures, which are attributable to vibronic transitions including vibrational energies of DMA in the ground state and the excited state, respectively. The PL enhancement results from a great increase in light absorption probability of DMA by adsorption on the surface of Si nanoparticles. The structure of the PL spectra is independent of the excitation energy and the size of Si nanoparticles, while the PL intensity strongly depends on the size of Si nanoparticles.
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
- Bulutay C, Ossicini S (2010) Electronic and optical properties of silicon nanocrystals. In: Pavesi L, Turan R (eds) Silicon nanocrytals. Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim, pp 5–38View ArticleGoogle Scholar
- Conibeer G (2010) Applications of Si nanoparticles in photovoltaic solar cells silicon nanocrystals. In: Pavesi L, Turan R (eds) Silicon nanocrytals. Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim, pp 555–61View ArticleGoogle Scholar
- Epur R, Minardi LK, Datta M, Chung SJ, Kumta PN (2013) A simple facile approach to large scale synthesis of high specific surface area silicon nanoparticles. J Solid State Chem 208:93–8View ArticleGoogle Scholar
- Erogbogbo F, Lin T, Tucciarone PM, Lajoie KM, Lai L, Latki GD, Prasad PN, Swihart MT (2013) On-demand hydrogen generation using nanosilicon: splitting water without light, heat, or electricity. Nano Lett 13:451–6View ArticleGoogle Scholar
- O’Farrell N, Houlton A, Horrocks BR (2006) Silicon nanoparticles: applications in cell biology and medicine. Int J Nanomed 1:451–72View ArticleGoogle Scholar
- Watanabe K, Sawada K, Koshiba M, Fujii M, Hayashi S (2002) Photoluminescence decay-dynamics of Si nanoparticles prepared by pulsed laser ablation. Appl Surf Sci 197-198:635–8View ArticleGoogle Scholar
- Makimura T, Kunii Y, Ono N, Murakami K (1988) Silicon nanoparticles embedded in SiO2 films with visible photoluminescence. Appl Surf Sci 127-129:388–92View ArticleGoogle Scholar
- Lacona F, Bongiorno C, Spinella C, Boninelli S, Priolo F (2004) Formation and evolution of luminescent Si nanoclusters produced by thermal annealing of SiOx films. J Appl Phys 95:3723–32View ArticleGoogle Scholar
- Salivati N, An YQ, Downer MC, Ekerdt JG (2009) Hot-wire chemical vapor deposition of silicon nanoparticles on fused silica. Thin Solid Films 517:3481–3View ArticleGoogle Scholar
- Fauchet PM, Ruan J, Chen H, Pavesi L, Negro LD, Cazzaneli M, Elliman RG, Smith N, Samoc M, Luther-Davies B (2005) Optical gain in different silicon nanocrystal systems. Opt Mater 27:745–9View ArticleGoogle Scholar
- Morales-Sánchez A, Leyva KM, Aceves M, Barreto J, Domínguez C, Luna-López JA, Carrilo J, Pedraza J (2010) Photoluminescence enhancement through silicon implantation on SRO-LPCVD films. Mater Sci Eng B 174:119–22View ArticleGoogle Scholar
- Choi BJ, Lee JH, Yatsui K, Yang SC (2007) Preparation of silicon nanoparticles for device of photoluminescence. Surf Coat Technol 201:5003–6View ArticleGoogle Scholar
- Steveler E, Rinnert H, Vergnat M (2014) Photoluminescence properties of Nd-doped silicon oxide thin films containing silicon nanoparticles. J Lumin 150:35–9View ArticleGoogle Scholar
- Kang Z, Liu Y, Lee ST (2011) Small-sized silicon nanoparticles: new nanolights and nanocatalysts. Nanoscale 3:777–91View ArticleGoogle Scholar
- Lam C, Zhang YF, Tang YH, Lee CS, Bello I, Lee ST (2000) Large-scale synthesis of ultrafine Si nanoparticles by ball milling. J Crystal Growth 220:466–70View ArticleGoogle Scholar
- Matsumoto T, Maeda M, Furukawa J, Kim WB, Kobayashi H (2014) Si nanoparticles fabricated from Si swarf by photochemical method. J Nanopart Res 16:2240-1-7Google Scholar
- Maeda M, Imamura K, Matsumoto T, Kobayashi H (2014) Fabrication of Si nanoparticles from Si swarf and application to solar cells. Appl Surf Sci 312:39–42View ArticleGoogle Scholar
- Di D, Perez-Wurfl I, Wu L, Huang Y, Marconi A, Tengattini A, Anopchenko A, Pavesi L, Conibeer G (2011) Electroluminescence from Si nanocrystal/c-Si heterojunction light-emitting diodes. Appl Phys Lett 99:251113-1-4View ArticleGoogle Scholar
- Zhu Y, Wang H, Ong PP (2000) Evidence of photoluminescence related to subsurface Si–O–Si bonds in sputtered silicon nanoparticles. Solid State Commun 116:427–9View ArticleGoogle Scholar
- Inada M, Nakagawa H, Umezu I, Sugimura A (2003) Effects of hydrogenation on photoluminescence of Si nanoparticles formed by pulsed laser ablation. Mater Sci Eng B 101:283–5View ArticleGoogle Scholar
- Ryabchikov YV, Alekseev SA, Lysenko V, Bremond G, Bluet JM (2013) Photoluminescence of silicon nanoparticles chemically modified by alkyl groups and dispersed in low-polar liquids. J Nanopart Res 15:1535-1-9Google Scholar
- Imamura M, Nakamura J, Fujimasa S, Yasuda H, Kobayashi H, Negishi Y (2011) Photoluminescence dynamics of organic molecule-passivated Si nanoclusters. Eur Phys J D 63:289–92View ArticleGoogle Scholar
- Portolés MJL, Nieto FR, Soria DB, Amalvy JI, Peruzzo PJ, Mártire DO, Kotler M, Holub O, Gonzalez MC (2009) Photophysical properties of blue-emitting silicon nanoparticles. J Phys Chem C 113:13694–702View ArticleGoogle Scholar
- Dobrovolskas D, Mickevičius J, Tamulaitis G, Reipa V (2009) Photoluminescence of Si nanocrystals under selective excitation. J Phys Chem Solid 70:439–43View ArticleGoogle Scholar
- Ida T, Shimazaki S, Hibino H, Toraya H (2006) Diffraction peak profiles from spherical crystallites with lognormal size distribution. J Appl Cryst 36:1107–15View ArticleGoogle Scholar
- Ohno K (1978) Simple calculations of Franck-Condon factors for electronic transition bands of polyacenes. Chem Phys Lett 53:571–7View ArticleGoogle Scholar
- Henβge A, Acker J, Müller C (2006) Titrimetric determination of silicon dissolved in concentrated HF–HNO3-etching solutions. Talanta 68:581–5View ArticleGoogle Scholar
- Mertens H, Biteen JS, Atwater H, Polman A (2006) Polarization-selective plasmon-enhanced silicon quantum-dot luminescence. Nano Lett 6:2622–5View ArticleGoogle Scholar
- Tamamitsu H, Saitow K (2014) Local enhancement effect in the photoluminescence intensity of Si quantum dots: single Medusa-type particles investigated by in situ microscope spectrometer. Chem Phys Lett 591:37–42View ArticleGoogle Scholar
- Barraza-Jimenez D, Flore-Hidalgo A, Glossman-Mintnik D (2009) Theoretical analysis of anthracene and its carbonyl and carboxyl derivatives using DFT and TD-DFT. J Mol Struct (THEOCHEM) 894:64–70View ArticleGoogle Scholar
- Oura K, Lifshits VG, Saranin AA, Zotov AV, Katayama M (2003) Surface science. Springer-Verlag Berlin Heiderberg, New York, p 267View ArticleGoogle Scholar