- Nano Express
- Open Access
Gold nanolayer and nanocluster coatings induced by heat treatment and evaporation technique
© Schaub et al.; licensee Springer. 2013
- Received: 13 March 2013
- Accepted: 13 May 2013
- Published: 22 May 2013
The paper is focused on the preparation and surface characterization of gold coatings and nanostructures deposited on glass substrate. Different approaches for the layer preparation were applied. The gold was deposited on the glass with (i) room temperature, (ii) glass heated to 300°C, and (iii) the room temperature-deposited glass which was consequently annealed to 300°C. The sheet resistance and concentration of free carriers were determined by the van der Pauw method. Surface morphology was characterized using an atomic force microscopy. The optical properties of gold nanostructures were measured by UV–vis spectroscopy. The evaporation technique combined with simultaneous heating of the glass leads to change of the sheet resistance, surface roughness, and optical properties of gold nanostructures. The electrically continuous layers are formed for significantly higher thickness (18 nm), if the substrate is heated during evaporation process. The annealing process influences both the structure and optical properties of gold nanostructures. The elevated temperature of glass during evaporation amplifies the peak of plasmon resonance in the structures, the surface morphology being significantly altered.
- Glass substrate
- Gold coating
- Surface properties
- Thermal annealing
Nanostructured thin films play nowadays a quite significant role in various material science and technology applications. In particular, a considerable attention has been drawn to the structure and properties of thin metal films deposited on non-metal surfaces due to their attractive applications in electronic, magnetic, and optical devices . Gold nanolayers are perspective structures for certain applications due to their unique electrical and optical properties. Gold in the form of thin films is nowadays used in a vast range of applications such as microelectromechanical systems and nanoelectromechanical systems, sensors and electronic textiles, bioengineering, as a generator of nonlinear optical properties, or in devices for surface-enhanced Raman scattering [2–4].
Layers consisting of gold nanoparticles (AuNP) are usually prepared by precipitation from aqueous solutions on various materials, e.g., on etched glass surfaces. The thermal annealing of thin gold films produced by thermal evaporation or sputtering can also lead to a disaggregation into particles [1, 5, 6]. The formation of AuNP from continuous gold layers is driven by the minimization of surface energy and is denoted as solid-state dewetting. All the described methods suffer from the poor adhesion of AuNP to the substrate surface . The electrical resistance measurement shows that the nanoparticles are conductive even at a small metal volume fraction. Due to the aggregation effect, the optical transmission spectra exhibited an enhanced transmission band around 500 nm arising from the surface plasmon resonance. Many authors have developed theories of distortion of crystalline lattice in nanostructures, some of them being applicable on nanoparticles [8–11]. Spherical nanoparticles surrounded ‘by air’ have different behaviors as nanostructures deposited on solid surface [12, 13].
This work is focused on glass substrate and subsequent deposition of Au layer by evaporation. The gold deposition was carried out at room temperature (RT) and at 300°C. Then the samples prepared on the substrate at room temperature in this way were annealed at 300°C. The effects of annealing or deposition on glass substrate with elevated temperature were studied using atomic force microscopy (AFM, for surface morphology and roughness), UV–vis spectroscopy and electrical measurements (for sheet resistance and volume-free charge carrier concentration). The novelty of this research lies in the precise simultaneous study of nanostructures induced by evaporation on heated and non-heated glass substrate and its comparison to subsequently annealed structures. The optical and electrical characterizations connected with the changes in surface morphology induced by the particle surface diffusion bring important new information to this field of research.
Glass substrate (Menzel-Glaser, Braunschweig, Germany) with the dimension 20 × 20 mm2 was used for the present experiments. Vacuum evaporation was performed on Leybold-Heraeus, Univex 450 device (Oerlikon Leybold Vacuum GmbH, Cologne, Germany) with typical parameters: room deposition temperature, total pressure of about 2.10−5 Pa, molybdenum container with source current >5 A. The gold deposition was accomplished at room temperature (25°C) and at 300°C (pressure of 2 × 10−5 Pa) using gold target (purity 99.99%, supplied by Goodfellow Ltd., Huntingdon, Cambridgeshire, UK). The thicknesses of the deposited Au were determined from AFM analysis and were in intervals of 2 to 40 nm. The post-deposition annealing of the gold/glass samples was carried out in air at 300°C (±3°C) for 1 h using a thermostat Binder oven (Binder GmbH, Tuttlingen, Germany). The annealed samples were left to cool in air to room temperature.
For the sheet resistance and concentration of free charge carrier determination of Au layer evaporated onto glass, the van der Pauw method was used. The measurement was accomplished with direct current (dc) and a homogeneous dc magnetic field, with a polarity commutation of both quantities. Keithley 2400 (Keithley Instruments Inc., Cleveland, OH, USA) served as a source of constant current. The voltage response was measured with Keithley 2010 multimeter. The magnetic field (B = 0.4 T) was generated by an electromagnet fed from the Keithley 2440 source. The computer code, working under the LabView 8.5 system (National Instruments, Austin, TX, USA), was used for the experiment control and data evaluation . The values have been obtained from the six independent measurements under previous set-up, and the average values have been introduced in the graph of sheet resistance and the free carrier concentration with error of measurement not exceeding 5%. The values of sheet resistance have been also confirmed by the modified two-point technique  as an alternative method for sheet resistance determination.
The surface morphology of glass and Au-metalized glass was examined using AFM in tapping mode under ambient conditions with a CP II Veeco microscope (Bruker Corp., Santa Barbara, CA, USA). An etched Si probe (doped with P), RTESPA-CP, with spring constant of 20 to 80 N m−1 was used. The average mean roughness (Ra) represents the arithmetic average of the deviations from the center plane of the samples. All samples have been measured repeatedly at three different areas on two samples; the error in the surface roughness measurement did not exceeded 7%.
The UV–vis spectra were measured using a PerkinElmer Lambda 25 spectrometer (PerkinElmer Inc., Waltham, MA, USA) in the spectral range from 330 to 1100 nm. Rutherford backscattering (RBS) analyses were performed on Tandetron 4130MC accelerator (Center of Accelerators and Nuclear Analytical Methods, Nuclear Physics Institute of the ASCR, Řež, Czech Republic) using 1.7 MeV 4He ions. The RBS measurement was realized at the CANAM infrastructure. The measurements were performed in IBM geometry with incident angle 0°, and laboratory scattering angle of 170°. The typical energy resolution of the spectrometer was FWHM = 15 keV. The RBS spectra were evaluated using SIMNRA and GISA softwares.
Electrical properties of Au structures
The influence of gold nanocluster formation has been also extensively studied  on mica. A phenomenological study was carried out to find a reliable way for the gold thin film preparation. The following parameters have been focused on: annealing time of the substrate before deposition of the gold film, deposition rate of the gold film, substrate temperature before and during evaporation and annealing time after the deposition . Deposition of Au films on mica with the deposition temperature 500°C led to the similar structures that we achieved on glass heated to 300°C, where pores and whiskers have been observed .
The gold nanocluster formation on glass substrate is strongly influenced by the physical processes of vapor-deposited thin gold films on glass substrate . The processes which can alter the layer’s growth may be, e.g., chemical or plasma modification of the substrate  or gold and glass wettability . The bonds between the gold clusters and the glass substrates are usually weak, and their wettability is relatively bad. It was reported that the gold nuclei diffusion on the surface is increased, as well as their coalescence, when its wettability is poor . On the contrary, if the wettability of gold for the substrate is improved (chemical modification of the surface), the interactions between the two materials are globally stronger, and both the diffusion and coalescence of the metal clusters are disfavored .
Surface plasmon resonance (SPR) can be described as a collective oscillation of electrons in solid or liquid stimulated by incident light. The condition for the resonance appearance is established when the frequency of light photons matches the frequency of surface electrons oscillating against the restoring force of the positive nuclei. This effect when occurring in nanometer-sized structures is called localized surface plasmon resonance. Surface plasmons have been used to enhance the surface sensitivity of several spectroscopic measurements including fluorescence, Raman scattering, and second harmonic generation. Also, SPR reflectivity measurements can be used to detect molecular adsorption, such as polymers, DNA or proteins, and molecular interaction studies .
The shift of the curves in extinction spectra can be explained by the coupling of the electromagnetic field between surface plasmons excited in gold nanoparticles of different densities and sizes. The shift of surface plasmon resonance towards higher wavelengths has been observed for the gold nanolayer deposited on heated substrate to 300°C, while no shift has been observed for Au nanolayer deposited under RT and those consecutively heated. According to the shift in sheet resistance and different morphologies observed by atomic force microscopy, it can be concluded that for Au nanolayer deposited under 300°C, the insulating layer between gold nanoclusters causes shift of the surface plasmon resonance peak, as was observed e.g. in  for graphene and Au nanoparticles.
On the basis of the achieved results, it can be concluded that electrically continuous metal nanolayers with very low surface roughness can be prepared by evaporation on the substrate at elevated temperature. These structures also exhibit peaks of plasmon resonance up to Au thickness of 10 nm. The combination of surface plasmon resonance together with low surface roughness may find applications in the construction of biosensors for the detection of mycotoxins . On the contrary, structures with different densities of gold nanoclusters prepared by the technique of evaporation at RT or consequently annealed can be of a great contribution for the construction of biosensors and DNA detection .
The different surface properties of thermally annealed gold nanostructures in comparison to those evaporated onto heated substrate has been described. The heating of glass during the evaporation results in dramatic changes of the surface morphology and roughness. The substrate heating leads to the decrease of surface roughness for higher Au thickness, the electrical properties being also strongly influenced, the structure being more homogeneous. The electrically continuous layer is formed for the thicknesses above 20 nm. The shift of this threshold in comparison to structures evaporated and consequently annealed is probably caused by the surface diffusion in combination with local gold melting. The thermal annealing, on the contrary, leads to the creation of relatively large ‘spherolytic and hummock-like’ structures in the gold layer. The globular structure is strongly amplified by the thermal annealing probably due to local surface melting of gold nanoparticles during the process. The optical properties and appearance of peak of plasmon resonance for different thicknesses of Au structures are strongly influenced by prior glass heating.
This work was supported by the Grant Agency of the CR under the project no. P108/10/1106 and P106/09/0125.
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