Two-dimensional ultrathin gold film composed of steadily linked dense nanoparticle with surface plasmon resonance
© Wang et al.; licensee Springer. 2012
Received: 3 October 2012
Accepted: 29 November 2012
Published: 21 December 2012
Noble metallic nanoparticles have prominent optical local-field enhancement and light trapping properties in the visible light region resulting from surface plasmon resonances.
We investigate the optical spectral properties and the surface-enhanced Raman spectroscopy of two-dimensional distinctive continuous ultrathin gold nanofilms. Experimental results show that the one- or two-layer nanofilm obviously increases absorbance in PEDOT:PSS and P3HT:PCBM layers and the gold nanofilm acquires high Raman-enhancing capability.
The fabricated novel structure of the continuous ultrathin gold nanofilms possesses high surface plasmon resonance properties and boasts a high surface-enhanced Raman scattering (SERS) enhancement factor, which can be a robust and cost-efficient SERS substrate. Interestingly, owing to the distinctive morphology and high light transmittance, the peculiar nanofilm can be used in multilayer photovoltaic devices to trap light without affecting the physical thickness of solar photovoltaic absorber layers and yielding new options for solar cell design.
KeywordsUltrathin gold film Surface plasmon resonance SERS
Noble metal nanoparticles and nanofilms with strong localized surface plasmon resonances (LSPRs) have attracted great interests in fields such as nanoscale photonics, biological sensing [1, 2], surface-enhanced Raman scattering (SERS) [3, 4], photocatalytic and photoelectrochemical processes , and plasmonic absorption enhancement in solar cells [6–19]. The LSPRs arise from the excitation of a collective electron oscillation within the metallic nanostructure induced by the incident light, leading to enormous optical local-field enhancement and a dramatic wavelength-selective photon scattering at the nanoscale [20–23]. The exceptional optical properties introduced by LSPRs have spurred tremendous efforts to design and fabricate highly SERS-active substrates for molecular sensing. The most studied and best established systems are substrates sprayed with Ag or Au colloids that give high SERS signals at some local ‘hot junctions’ . In order to fabricate noble nanoparticle arrays with high SERS activity and improve the uniformity, lithographic techniques have been employed.
We have recently reported a relatively simple approach in fabricating uniform gold nanocrystal-embedded nanofilms via a conventional magnetron sputtering method. In this method, one can more conveniently assemble noble metals with precise gap control in the sub-10-nm regime  than any other method. As a continual effort in supporting the above claim, here we report further evidence such as visible absorption spectra of the Au film on indium tin oxide (ITO) glass substrates, the blend films of poly(3,4-ethylenedioxythiophene) doped with poly(styrenesulfonate) (PEDOT:PSS) and poly(3-hexylthiophene) and [6,6]-phenyl-C61-butyric acid methyl ester (P3HT:PCBM) on ITO glass substrates, and the SERS measurements of molecules adsorbed on gold nanocrystals deposited on ITO glass substrates. Our results suggest that the continuous ultrathin nanofilm can obviously enhance visible-range absorption in the active layer of solar cells and obtain an ultrasensitive SERS-active coating.
The fabrication of continuous ultrathin Au nanofilms
Our approach is based on the formation of Au nanofilms on the buffer layer surface of PEDOT:PSS or on ITO glass utilizing magnetron sputtering deposition of metal atoms. The ITO-coated glass substrate was first cleaned with detergent, then ultrasonicated in acetone and isopropyl alcohol for further cleaning, and subsequently dried in a vacuum oven at 80°C for 3 h. PEDOT:PSS films with thicknesses of 30 nm are prepared via spin coating on top of the ITO glass and cured at 130°C for 10 min in air. On top of the freshly prepared PEDOT:PSS layer, metallic gold are sputtered by magnetron sputtering in an electrical current of 0.38 A, vacuum of 0.15 Pa, Ar flux of 25 sccm, and discharge of 1 s. The ITO/Au nanofilm is fabricated in an identical magnetron sputtering manner.
The SERS measurements were performed at room temperature on a confocal Raman spectrometer with the 514-nm laser focused to a diameter of 1 μm. The incident power was 0.55 mW, and the accumulation time was 10 s.
Morphology of fabricated Au nanofilms
UV–vis absorption spectrum of the Au nanofilm layer on the ITO glass substrates
The effect of UV–vis absorption spectra of the organic photosensitive layer incorporated in thin Au film
The SERS spectra of R6G adsorbed on the surface of the Au nanofilm/glass
To compare the impact of continuous ultrathin gold nanofilms on the absorption of visible light, plasmonic enhancement of the P3HT:PCBM bulk heterojunction system is demonstrated in a spin-cast device with an incorporated continuous ultrathin gold nanofilm thicknesses of 2 nm or so which are chosen to be sufficiently thin to limit the amount of light absorbed before reaching the active layer. The nanofilm incorporated with gold in the active P3HT:PCBM layer is shown to have significantly greater absorbance enhancement than the nanofilm without gold in the entire excitation spectral range in Figure 3. As shown in Figure 2, the optical absorption spectrum of the continuous ultrathin gold nanofilm has high light transmittance and broad surface plasmon resonance band in the wavelength range of 300 to 1,000 nm. Therefore, the results demonstrate that the enhancement of absorption in the wavelength range of 350 to 1,000 nm is due to the surface plasmon resonance absorption. The much higher plasma frequency of Au ensures a better overlap between plasmon resonance and absorption band of organic semiconductors. The light energy is trapped mainly in the P3HT:PCBM layer, leading to enhanced absorption in the active layer.
For the ITO/Au film/PEDOT:PSS/Au film/P3HT:PCBM and ITO/PEDOT:PSS/Au film/PEDOT:PSS/Au film/P3HT:PCBM structures, the plasmon resonance is located at a wavelength range of 350 to 1,000 nm. The plasmonic peak better overlaps the P3HT:PCBM absorption band. These enhancements concerning light absorption in the visible region can be explained by the surface plasmon polariton resonance of metallic nanoparticles in the gold nanofilm. When metallic nanoparticles are in close proximity, their plasmon resonances couple with each other and generate a light-scattering spectrum that depends strongly on the interparticle distance. The two-dimensional distinctive ultrathin continuous gold nanofilms can be used as subwavelength antennas in which the plasmonic near-field is coupled to the organic semiconductor, increasing its effective absorption cross section. A corrugated metallic film on the back surface of the P3HT:PCBM photosensitive layer can couple light into surface plasmon polariton (SPP) modes supported at the metal/P3HT:PCBM organic semiconductor interface as well as guided modes in the organic semiconductor slab. Both the shape and size of metal nanoparticles are key factors in determining the coupling efficiency. The two-layer ultrathin nanofilm increases the nanoparticle density; according to the Mie theory, the extinction coefficient is proportional to the nanoparticle density. Consequently, optical local-field enhancement of the two-layer continuous ultrathin gold nanofilm is stronger than that of the one-layer ultrathin continuous gold nanofilm. Figure 3 embodies the absorbance of the two-layer ultrathin continuous gold nanofilm which far outweighs that of ITO/PEDOT:PSS/Au film/P3HT:PCBM and ITO/Au film/PEDOT:PSS/P3HT:PCBM. In brief, the enhanced efficiency is shown to stem from field enhancement originating both from localized plasmonic resonances and periodic similar nanopatch antenna configuration and SPP modes in the peculiar gold nanofilm.
To investigate the performance for electromagnetic enhancement, SERS spectroscopic measurements were carried out using Rhodamine 6G, a well-characterized test molecule. Spectra obtained from Rhodamine 6G molecules at a concentration of 10−3 to 10−6 M are shown in Figure 4 which exhibit repeatable high SERS sensitivity. The distances between the centers of two adjacent particles and the particle diameter are important parameters affecting SERS activity. This ultrathin continuous gold nanofilm produces a high Raman signal due to its periodic arrangements, high nanoisland density, and control of the gap between the nanostructures in the sub-10-nm regime. The observed SERS efficiency can be explained in terms of interparticle coupling-induced Raman enhancement. Thus, the distinctive continuous gold nanofilm is very effective in providing abundant hot spots for SERS enhancement.
In conclusion, we have produced continuous ultrathin gold nanofilms with high local-field enhancement effect and a high SERS activity. Spectral analysis suggests that the prominent light absorption in organic photosensitive materials and the high SERS activity arise from the near-field effect of localized surface plasmons of nanoparticles. Owing to their distinctive morphology and high light transmittance, continuous ultrathin gold nanofilms can be used in multilayer organic solar cells to trap light without affecting the physical thickness of solar photovoltaic absorber layers and yielding new options for solar cell design. Further work is needed to research two-dimensional distinctive continuous gold nanofilms that are utilized to trap light in solar cells which may be suitable for application to the high photoelectric conversion efficiency of organic solar cells.
This work is supported by NSFC under grant no. 60977038, the Doctoral Fund of Ministry of Education of China under grant no. 20110092110016, the National Basic Research Program of China (973 Program) under grant no. 2011CB302004, and the Scientific Research Foundation of Graduate School of Southeast University under grant no. YBPY1104.
- Halas NJ, Lal S, Chang WS, Link S, Nordlander P: Plasmons in strongly coupled metallic nanostructures. Chem Rev 2011, 111: 3913–3961. 10.1021/cr200061kView ArticleGoogle Scholar
- Lu XM, Rycenga M, Skrabalak SE, Wiley B, Xia YN: Chemical synthesis of novel plasmonic nanoparticles. Annu Rev Phys Chem 2009, 60: 167–192. 10.1146/annurev.physchem.040808.090434View ArticleGoogle Scholar
- Lal S, Grady NK, Kundu J, Levin CS, Lassiter JB, Halas NJ: Tailoring plasmonic substrates for surface enhanced spectroscopies. Chem Soc Rev 2008, 37: 898. 10.1039/b705969hView ArticleGoogle Scholar
- Zhu SQ, Zhang T, Guo XL, Wang QL, Liu XF, Zhang XY: Fabrication of gold nanoparticle thin film by electrophoretic deposition method. Nanoscale Res Lett in press in press
- Long MC, Jiang JJ, Li Y, Cao RQ, Zhang LY, Cai WM: Effect of gold nanoparticles on the photocatalytic and photoelectrochemical performance of Au modified BiVO4. Nano-Micro Lett 2011, 3(3):171–177.View ArticleGoogle Scholar
- Heidel TD, Mapel JK, Singh M, Celebi K, Baldo MA: Surface plasmon polariton mediated energy transfer in organic photovoltaic. Appl Phys Lett 2007, 91: 093506. 10.1063/1.2772173View ArticleGoogle Scholar
- Wu J, Mangham SC, Reddy VR, Manasreh MO, Weaver BD: Surface plasmon enhanced intermediate band based quantum dots solar cell. Solar Energy Materials & Solar Cells 2012, 102: 44–49.View ArticleGoogle Scholar
- Wang RL, Pitzer M, Fruk L, Hu DZ, Schaadt DM: Nanoparticles and efficiency enhancement in plasmonic solar cells. J Nanoelectron Optoelectron 2012, 7: 322–327.View ArticleGoogle Scholar
- Tvingstedt K, Persson NK, Inganäs O, Rahachou A, Zozoulenko IV: Surface plasmon increase absorption in polymer photovoltaic cells. Appl Phys Lett 2007, 91: 113514. 10.1063/1.2782910View ArticleGoogle Scholar
- Shen H, Bienstman P, Maes B: Plasmonic absorption enhancement in organic solar cells with thin active layers. J Appl Phys 2009, 106: 073109. 10.1063/1.3243163View ArticleGoogle Scholar
- Anthony JM, Kathy LR: Plasmon-enhanced solar energy conversion in organic bulk heterojunction photovoltaics. Appl Phys Lett 2008, 92: 013504. 10.1063/1.2823578View ArticleGoogle Scholar
- Kim CH, Cha SH, Kim SC, Song M, Lee J, Shin WS, Moon SJ, Bahng JH, Kotov NA, Jin SH: Silver nanowire embedded in P3HT:PCBM for high efficiency hybrid photovoltaic device applications. ACS Nano 2011, 5: 3319–3325. 10.1021/nn200469dView ArticleGoogle Scholar
- Yang J, You JB, Chen CC, Hsu WC, Tan HR, Zhang XW, Hong Z, Yang Y: Plasmonic polymer tandem solar cell. ACS Nano 2011, 5: 6210–6217. 10.1021/nn202144bView ArticleGoogle Scholar
- Reilly TH III, Lagemaat JVD, Tenent RC, Morfa AJ, Rowlen KL: Surface-plasmon enhanced transparent electrodes in organic photovoltaics. Appl Phys Lett 2008, 92: 243304. 10.1063/1.2938089View ArticleGoogle Scholar
- Kim SS, Na SI, Jo J, Kim DY, Nah YC: Plasmon enhanced performance of organic solar cells using electrodeposited Ag nanoparticles. Appl Phys Lett 2008, 93: 073307. 10.1063/1.2967471View ArticleGoogle Scholar
- Kochergin V, Neely L, Jao CY, Robinson HD: Aluminum plasmonic nanostructures for improved absorption in organic photovoltaic devices. Appl Phys Lett 2011, 98: 133305. 10.1063/1.3574091View ArticleGoogle Scholar
- Zhu JF, Xue M, Shen HJ, Wu Z, Kim S, Ho JJ, Aram HA, Zeng BQ, Wang KL: Plasmonic effects for light concentration in organic photovoltaic thin films induced by hexagonal periodic metallic nanospheres. Appl Phys Lett 2011, 98: 151110. 10.1063/1.3577611View ArticleGoogle Scholar
- Spyropoulos GD, Stylianakis M, Stratakis E, Kymakis E: Plasmonic organic photovoltaics doped with metal nanoparticles. Phot Nano Fund Appl 2011, 9: 184–189. 10.1016/j.photonics.2010.09.001View ArticleGoogle Scholar
- Atwater HA, Polman A: Plasmonics for improved photovoltaic devices. Nat Mater 2010, 19: 205–213.View ArticleGoogle Scholar
- Stewart ME, Anderton CR, Thompson LB, Maria J, Gray SK, Rogers JA, Nuzzo RG: Nanostructured plasmonic sensors. Chem Rev 2008, 108: 494–521. 10.1021/cr068126nView ArticleGoogle Scholar
- Gao SY, Koshizaki N, Tokuhisa H, Koyama E, Sasaki T, Kim JK, Ryu J, Kim DS, Shimizu Y: Highly stable Au nanoparticles with tunable spacing and their potential application in surface plasmon resonance biosensors. Adv Funct Mater 2010, 20: 78–86. 10.1002/adfm.200901232View ArticleGoogle Scholar
- Zhang XY, Hu A, Zhang T, Lei W, Xue XJ, Zhou YH, Duley WW: Self-assembly of large-scale and ultrathin silver nanoplate films with tunable plasmon resonance properties. ACS Nano 2011, 5: 9082–9092. 10.1021/nn203336mView ArticleGoogle Scholar
- Zhang XY, Zhang T, Zhu SQ, Wang LD, Liu XF, Wang QL, Song YJ: Synthesis and optical spectra investigation of silver nanochains and nanomeshworks. Nanoscale Res Lett 2012, 7: 596. 10.1186/1556-276X-7-596View ArticleGoogle Scholar
- Nie S, Emory SR: Probing single molecules and single nanoparticles by surface-enhanced Raman scattering. Science 1997, 275: 1102–1106. 10.1126/science.275.5303.1102View ArticleGoogle Scholar
- Wang LD, Zhang T, Zhang XY, Li RZ, Zhu SQ, Wang LN: Synthesis of ultra-thin gold nanosheets composed of steadily linked dense nanoparticle arrays using magnetron sputtering. J Nanosci Nanotechnol in press in press
- Doremus RH: Optical properties of thin metallic films in island form. J Appl Phys 1966, 37: 2775. 10.1063/1.1782121View ArticleGoogle Scholar
- Yang YM, Qiu T, Ou HL, Lang XZ, Xu QY, Kong F, Zhang WJ, Chu PK: Modulation of surface-enhanced Raman spectra by depth selective excitation of embedded indium tin oxide nanoisland arrays. J Phys D: Appl Phys 2011, 44: 215305. 10.1088/0022-3727/44/21/215305View ArticleGoogle Scholar
- Qiu T, Zhang WJ, Lang XZ, Zhou YJ, Cui TJ, Chu PK: Controlled assembly of highly Raman-enhancing silver nanocap arrays templated by porous anodic alumina membranes. Small 2009, 5: 2333–2337. 10.1002/smll.200900577View ArticleGoogle Scholar
- Qiu T, Wu XL, Shen JC, Chu PK: Silver nanocrystal superlattice coating for molecular sensing by surface-enhanced Raman spectroscopy. Appl Phys Lett 2006, 89: 131914. 10.1063/1.2357548View ArticleGoogle Scholar
- Hutter E, Fendler JH: Exploitation of localized surface plasmon resonance. Adv Mater 2004, 16: 1685–1706. 10.1002/adma.200400271View ArticleGoogle Scholar
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