- Nano Express
- Open Access
Gold nanoparticles deposited on glass: physicochemical characterization and cytocompatibility
© Reznickova et al.; licensee Springer. 2013
Received: 2 April 2013
Accepted: 16 May 2013
Published: 25 May 2013
Properties of gold films sputtered under different conditions onto borosilicate glass substrate were studied. Mean thickness of sputtered gold film was measured by gravimetry, and film contact angle was determined by goniometry. Surface morphology was examined by atomic force microscopy, and electrical sheet resistance was determined by two-point technique. The samples were seeded with rat vascular smooth muscle cells, and their adhesion and proliferation were studied. Gold depositions lead to dramatical changes in the surface morphology and roughness in comparison to pristine substrate. For sputtered gold structures, the rapid decline of the sheet resistance appears on structures deposited for the times above 100 s. The thickness of deposited gold nanoparticles/layer is an increasing function of sputtering time and current. AFM images prove the creation of separated gold islands in the initial deposition phase and a continuous gold coverage for longer deposition times. Gold deposition has a positive effect on the proliferation of vascular smooth muscle cells. Largest number of cells was observed on sample sputtered with gold for 20 s and at the discharge current of 40 mA. This sample exhibits lowest contact angle, low relative roughness, and only mild increase of electrical conductivity.
Gold nanoparticles (GNPs) are currently used as catalysts , and chemical  and plasmonic sensors . They are also used in surface-enhanced Raman scattering  and nonlinear optics . Furthermore, the usage of GNP for diagnosis and even destruction of microorganisms  or AuNP for biological applications [7–9] should be mentioned. Although GNPs are believed to be biologically inert, they can be engineered to possess chemical and biological functionality. GNP exhibits a plasmon resonance (PR) at wavelengths from 510 to 580 nm  leading to enhanced absorption and scattering in this part of the optical spectrum. The PR is affected by the size and shape of the GNP, the type of the supporting substrate (mainly its refractive index) and/or the surrounding material of the gold nanoparticles. The distance between the nanoparticles is also relevant, especially if it is small enough to enable electromagnetic coupling . GNPs are usually prepared by precipitation from aqueous solutions [12, 13] on various materials, e.g., on etched glass surfaces [13, 14]. Thermal annealing of thin gold films produced by evaporation or sputtering  can also lead to a gold aggregation into GNP . The formation of GNP from continuous gold layers is driven by the minimization of the surface energy and is denoted as solid state dewetting . However, all the described methods suffer from the poor adhesion of GNP to the substrate surface .
It is known that the biocompatibility of a substrate is affected, besides of several other factors, by their electrical conductivity, chemical structure, surface morphology, roughness, and wettability (polarity) . In this work, we studied the surface morphology, sheet electrical resistance, contact angle, ultraviolet–visible (UV–vis) spectra, adhesion, and proliferation of living muscle cells on gold structure sputtered on glass surface.
Materials and modification
The gold layers were sputtered on 1.8 × 1.8 cm2 microscopic glass, supplied by Glassbel Ltd., Prague, Czech Republic. The surface roughness of glass, measured over the area of 1×1 μm2 and calculated as an average value from five different measuring positions, was R a = 0. 34 ± 0. 03 nm . The gold sputtering was accomplished on Balzers SCD 050 device from gold target (supplied by Goodfellow Ltd., Huntingdon, England). The deposition conditions were DC Ar plasma, gas purity of 99.995%, sputtering time of 10 to 400 s, current of 10 to 40 mA (discharge power 3 to 15 W), total Ar pressure about 5 Pa, and the electrode distance of 50 mm. The power density of Ar plasma in our case was 0.13 W·cm−2, and the average deposition rate was 0.15 nm s−1. The glass substrate was cleaned with methanol (p.a.) and dried in a stream of N2. The prepared samples were stored at laboratory conditions.
The mean thickness of gold films was measured by gravimetry using Mettler Toledo UMX2 microbalance (Columbus, OH, USA). The thickness was calculated from the sample weights before and after sputtering using gold bulk density.
The sheet resistance of Au layers was examined by Ohm’s method with a picoampermeter Keithley487 (Cleveland, OH, USA). For the measurement, two Au contacts, about 50-nm thick, were deposited on the layer surface by sputtering. The samples with lower resistances (up to 1 MΩ) were measured on the commercially available multimeter UNI-T 83 (Uni-Trend Group Limited, Kowloon, Hong Kong). The electrical measurements were performed at a pressure of about 10 Pa to minimize the influence of atmospheric humidity. The typical error of the sheet resistance measurement did not exceed ±5%.
Static contact angles (CA) of distilled water, characterizing structural and compositional changes caused by the gold deposition, were measured at room temperature at two samples and at seven positions using a Surface Energy Evolution System (SEES, Masaryk University, Brno, Czech Republic). Drops of 8.0 ± 0.2 μl volume were deposited using automatic pipette (Transferpette Electronic Brand, Wertheim, Germany), and their images were taken with 5-s delay. Then, the contact angles were evaluated using the SEES code.
UV–vis absorption spectra were recorded using a Varian Cary 25 Scan UV–vis spectrophotometer (PerkinElmer Inc., Waltham, MA, USA). UV–vis spectra in the range from 300 to 900 nm were taken with 1-nm data step at the scan rate of 240 nm·min−1. The results are presented as difference spectra (delta absorbance) obtained by the substraction of reference spectrum of pristine glass from the spectra of sputtered samples.
The surface morphology of glass and gold-sputtered glass was examined by atomic force microscopy (AFM) using VEECO CP II setup (phase mode);the surface roughness (Ra) was measured in taping mode (Bruker Corp., Madison, WI, USA). Si probe RTESPA-CP with the spring constant 0.9 N m−1 was used. By the repeated measurements of the same region (1 × 1 μm2 in area), we prove that the surface morphology did not change after three consecutive scans.
Cell culture, adhesion, and proliferation
For the study of cell adhesion and proliferation of six samples, gold coated under different conditions, were used. The glass samples were sterilized for 1 h in ethanol (75%), air-dried, inserted into polystyrene 12-well plates (TPP, Trasadingen, Switzerland; well diameter 20 mm), and seeded with vascular smooth muscle cells (VSMCs) derived from the rat aorta using an explantation method . VSMCs were seeded on the samples with the density of 16,000 cells·cm−2 into 3 ml of Dulbecco’s modified Eagle’s minimum essential medium (Sigma, USA, cat. no. D5648), containing 10% fetal bovine serum (Sebak GmbH, Aidenbach, Germany). Cells were cultivated at 37°C in a humidified air atmosphere containing 5% of CO2. The number and the morphology of initially adhered cells were evaluated 24 h after seeding. The cell proliferation activity was estimated from the increase in the cell numbers achieved on the 3rd and 6th days after seeding . The number and the morphology of the cells on the sample surface were then evaluated on microphotographs taken under an Olympus IX 51 microscope (Waltham, MA, USA; objective of 20×, visualized area of 0.136 mm2), equipped with an Olympus DP 70 digital camera. The number of the cells was determined using the image analysis software NIS-Elements (Melville, NY, USA). For each sample type, 20 independent measurements were performed. The number of adhered and proliferated cells was determined from the six samples. One sample of the particular type was used for the determination of the viability of the cells . The determination of cell viability was accomplished on cell viability analyzer (Vi-CELL XR, Beckman Coulter, Fullerton, CA, USA) using elimination test with trypanose blue. This color penetrates through the cell membrane into the dead or damaged cells and accumulates inside. The living cells are not colored. On the base of different coloration, the numbers of living and dead cells are determined, and their viability is evaluated.
Results and discussion
Surface roughness R a of glass with gold film sputtered for different sputtering times and discharge currents
Surface roughness (nm)
Glass/Au (20 s)
Glass/Au (150 s)
Glass substrates sputtered with gold for different sputtering times and at different discharge currents were studied. The thickness of the deposited gold film is an increasing function of the sputtering time and the discharge current. Linear dependence between the sputtering time and the layer thickness is evident even in the initiatory stage of nanoparticles/layer growth. A rapid decline of the sheet resistance is observed on gold films deposited for the times above 100 s. The contact angle is a slowly increasing function of the sputtering time for discharge currents from 10 to 30 mA. After the formation of continuous gold coverage, the samples exhibit hydrophobic character. The UV–vis absorbance of gold films increase with increasing sputtering time and discharge current and film thickness. Gold deposition leads to dramatic changes in the surface morphology and roughness in comparison to pristine glass substrate. AFM images prove the creation of separated gold islands in initial deposition phase and a continuous gold coverage for longer deposition times. Gold deposition has a positive effect on the proliferation of vascular smooth muscle cells. The largest number of cells was observed on sample sputtered with gold for 20 s and at the discharge current of 40 mA. This sample exhibits lowest contact angle, low relative roughness, and only mild increase of electrical conductivity. Under the present experimental conditions, the specific contribution of individual factors to cell interaction with the substrate cannot be classified separately. The gold/glass structures studied in this work could find an application as biosensors.
This work was supported by the GACR under project P108/12/G108.
- Chen M, Goodman DW: Catalytically active gold: from nanoparticles to ultrathin films. Accounts Chem Res 2006, 39: 739–746. 10.1021/ar040309dView ArticleGoogle Scholar
- Ruiz AM, Cornet A, Sakai G, Shimanoe K, Morante IR, Yamazoe NY: Cr-doped TiO2gas sensor for exhaust NO2monitoring. Sensor Actuat B-Chem 2003, 93: 509–518. 10.1016/S0925-4005(03)00183-7View ArticleGoogle Scholar
- Fernandez CD, Manera MG, Spadarecchia J, Maggioni G: Study of the gas optical sensing properties of Au-polyimide nanocomposite films prepared by ion implantation. Sensor Actuat B-Chem 2005, 111: 225–229.View ArticleGoogle Scholar
- Hrelescu C, Sau TK, Rogach AL, Jäckel F, Feldmann J: Single gold nanostars enhance Raman scattering. Appl Phys Lett 2009, 94: 153113. 10.1063/1.3119642View ArticleGoogle Scholar
- Hosoya Y, Suga T, Yanagawa T, Kurokawa Y: Linear and nonlinear optical properties sol–gel-derived Au nanometer-particle-doped alumina. J Appl Phys 1997, 81: 1475–1480. 10.1063/1.363983View ArticleGoogle Scholar
- Pissuwan D, Cortie CH, Valenzuela SM, Cortie MB: Functionalised gold nanoparticles for controlling pathogenic bacteria. Trends Biotechnol 2010, 28: 207–213. 10.1016/j.tibtech.2009.12.004View ArticleGoogle Scholar
- Dreaden EC, Alkilany AM, Huang X, Murphy CJ, El-Sayed MA: The golden age: gold nanoparticles for biomedicine. ChemSoc Rev 2012, 41: 2740–2779.View ArticleGoogle Scholar
- Giljohann DA, Seferos DS, Daniel WL, Massich MD, Patel PC, Mirkin CA: Gold nanoparticles for biology and medicine. Angew Chem Int Ed 2010, 49: 3280–3294. 10.1002/anie.200904359View ArticleGoogle Scholar
- Švorčík V, Kasálková N, Slepička P, Záruba K, Bačáková L, Pařízek M, Ruml T, Macková A: Cytocompatibility of Ar plasma-treated and Au nanoparticle-grafted PE. Nucl Instrum Meth B 2009, 267: 1904–1910. 10.1016/j.nimb.2009.03.099View ArticleGoogle Scholar
- Gupta R, Dyer MJ, Weimer WA: Preparation and characterization of surface plasmon resonance tunable gold and silver films. J Appl Phys 2002, 92: 5264–5271. 10.1063/1.1511275View ArticleGoogle Scholar
- De G, Bhattacharyya S: Au nanoparticles in alumina sols and coatings. J Mater Chem 2008, 18: 2816–2824. 10.1039/b802156bView ArticleGoogle Scholar
- Vakarelski IU, Chan DYC, Nonoguchi T, Shinto H, Higashitani K: Assembly of gold nanoparticles into microwire networks induced by drying liquid bridges. Phys Rev Lett 2009, 105: 058303.View ArticleGoogle Scholar
- Kealley CS, Cortie MB, Maaruf AI, Xu XD: The versatile colour gamut of coatings of plasmonic metal nanoparticles. Phys Chem Chem Phys 2009, 11: 5897–5902. 10.1039/b903318aView ArticleGoogle Scholar
- Xu X, Cortie MB, Stevens M: Effect of glass pre-treatment on the nucleation of semi-transparent gold coatings. Mater Chem Phys 2005, 94: 266–274. 10.1016/j.matchemphys.2005.04.044View ArticleGoogle Scholar
- Schrank C, Eisenmenger-Sittner C, Neubauer E, Bangert H, Bergauer A: Solid state de-wetting observed for vapor deposited copper films on carbon substrates. Thin Solid Films 2004, 459: 276–281. 10.1016/j.tsf.2003.12.143View ArticleGoogle Scholar
- Švorčík V, Siegel J, Šutta P, Mistrík J, Janíček P, Worsch P, Kolská Z: Annealing of gold nano-structures sputtered on glass substrate. Appl Phys A 2011, 102: 605–610. 10.1007/s00339-010-6167-1View ArticleGoogle Scholar
- Müller CM, Spolenak R: Microstructure evolution during dewetting in thin Au films. Acta Mater 2010, 58: 6035–6045. 10.1016/j.actamat.2010.07.021View ArticleGoogle Scholar
- Worsch C, Wisniewski W, Kracker M, Rüssel R: Gold nanoparticles fixed on glass. Appl Surf Sci 2012, 258: 8506–8513. 10.1016/j.apsusc.2012.05.010View ArticleGoogle Scholar
- Bacakova L, Filova E, Pařízek M, Ruml T, Švorčík V: Modulation of cell adhesion, proliferation and differentiation on materials designed for body implants. Biotechnol Adv 2011, 29: 739–767. 10.1016/j.biotechadv.2011.06.004View ArticleGoogle Scholar
- Kim KS, Ryu CM, Park CS, Sur GS, Park CE: Investigation of crystallinity effects on the surface of oxygen plasma treated low density polyethylene using X-ray photoelectron spectroscopy. Polymer 2004, 44: 6287–6295.View ArticleGoogle Scholar
- Švorčík V, Zehentner J, Rybka V, Slepička P, Hnatowicz V: Characterization of thin gold layers on polyethyleneterephthalate: transition from discontinuous to continuous, homogenous layer. Appl Phys A 2002, 75: 541–544. 10.1007/s003390101024Google Scholar
- Chopra K: Thin Film Phenomena. New York: Wiley; 1969.Google Scholar
- Hodgman CD: Handbook of Chemistry and Physics: A Ready-Reference Book of Chemical and Physical Data. Cleveland: CRC press; 1975.Google Scholar
- Hiemenz PC, Rajagopalan R: Principles of colloid and surface chemistry. New York: Marcel Dekker; 1997.Google Scholar
- Doremus RH: Optical properties of thin mettalic films in island form. J ApplPhys 1966, 37: 2775–2782. 10.1063/1.1782121View ArticleGoogle Scholar
- Švorčík V, Slepička P, Švorčíková J, Špírková M, Zehentner J, Hnatowicz V: Characterization of evaporated and sputtered thin Au layers on PET. J Appl Polym Sci 2006, 99: 1698–1704. 10.1002/app.22666View ArticleGoogle Scholar
- Jacobs T, Morent R, Geyter ND, Dubruel P, Leys C: Plasma surface modification of biomedical polymers: influence on cell-material interaction. Plasma Chem Plasma Process 2012, 32: 1039–1073. 10.1007/s11090-012-9394-8View ArticleGoogle Scholar
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