An important task of the scientific community is to provide non-specialized audience with explanations about what is nanoscience. Such explanations can be given during public conferences, seminars in high schools or lab work organized with teachers. And very often, the use of an experimental illustration greatly helps to raise the interest and the curiosity of the public. The present article will describe how the authors have used five simple and visual experiments in chemistry and physics to progressively introduce different audiences into the fascination of nanoscience. One experiment is the synthesis of gold nanoparticles with the Turkevich method and shows the progressive appearance of the ruby-red colour of the nanometric gold particles. The second and third experiments describe the way for modulating their colour and how to include them into a polymer and form a ruby-red coloured plastic film. The fourth experiment shows that starting from these nanoparticles, it is possible to turn them back into a yellow golden film. The last experiment is based on the optical properties of ultra-thin gold films. Using the plasmon resonance, it is possible to demonstrate that gold change colours from yellow to orange and green when a white light beam is shone on the gold interface. These visual experiments cannot be fully interpreted in front of a large audience but serve for rising curiosity.
Many scientists who work in the field of nanoscience have experienced that there is a gap between their daily practice and the comprehension that the common citizen can have of their research. Scientists have been trained to drive their reflections at the nanoscale, and the cutting-edge microscopes they routinely use have made them familiar with the visualization of nano-objects. Transmission electron microscopes were invented as early as 1931, and they are now commonly used to visualize the atomic structure of nanoparticles. More recently, since 1984, the scanning tunnel microscope (STM) makes possible to track individual atoms on a conductive surface and the atomic force microscope (AFM) is able to detect self-organized molecules on even non-conductive substrates. These are just examples of the way a scientist has a kind of privileged access to the “nanoworld”. All these images are truly fascinating, and researchers are probably the first to be mesmerized by the beauty of the world they discover through their various microscopes. Many of these images have been used to draw the attention of the public, of the politics towards our research. Our society is puzzled to discover the amazing nanoworld that is surrounding us, or even within us. As a consequence, the nanoworld has made its way into the public subconscient.
However, once these images have made a first impression in the people’s mind, they need to be explained and commented. Uncontrolled release of images or scientific information can lead to the birth of fears and mistrust towards our scientific work . It is the responsibility of us, scientists, to make sure that the images we release convey a true message and limit the possible distortion. The situation is all the more important that the present status of nanoscience is still being questioned, by the population in most of the European countries at least. Nanoscience is still benefiting a positive image, but this is not sure it will be always so.
Our responsibility for explaining nanoscience
A recent poll issued by a well-known polling agency in France shows that in 2006, only 44 % of the French population has heard about nanoscience or nanotechnology . In 2010, they were 59 % which is a sharp increase within only 4 years. But when one looks closer at the numbers, it turns out that among this proportion of “informed people”, 22 % declare that they know precisely what nanoscience is, whereas 37 % have only a very rough idea. These 37 % should be viewed as “good-willing” citizens who are “ill-informed people” but eager to learn more about science. As scientists, we have a moral obligation to provide them with key concepts and explanation, so that they will turn into the group of “nanoscience-educated people”. An efficient way to do so is probably that some scientists from our communities address the public through general conferences, vulgarization action in high schools, or scientific movies. Probably the most receptive public could be found in general-audience conferences and in high schools. The present article offers some support for colleagues who are ready to dedicate part of their time to this task by giving conferences and lectures. Since the impact of a scientific conference is largely magnified with the help of one or two live experiments, this paper will describe five experiments that can be presented in almost any conference hall without special equipment.
How to use the content of this article?
The aim of the present article is not to draw a typical conference guideline but rather to provide lecturers with experiments that illustrate selected features of nanoscience. The content of this paper will be most useful for teachers who want to introduce nanoscience experiments in their courses or lab teaching. It will also be useful for scientists who are invited to give general-audience conferences. Most of these experiments can be carried out in almost any conference hall, although it is useful to use a webcam and a video projector to magnify the observations. Of course, the most important in a conference is to set up a scenario where the experimental part will be just one aspect of the demonstration. Experimental evidences bring strong arguments in a demonstration. Usually, it is sufficient to present one or two experiments during a talk to definitively capture the public’s attention. To maximize the impact of a conference, it is useful to focus on a few concepts of nanoscience and demonstrate their relevance. This is why, in this article, each experiment is introduced with a few sentences that can give hints towards key concept conveyed by the experiment itself. Finally, these experiments have been tested several times in real conferences , and the details needed to reproduce them are given in the “Experimental” part. No toxic products are used; therefore, no particular security cautions have to be taken. The cost of the experiments is low, especially for the first four ones.
All glassware and magnetic stirrings used for gold nanoparticle (Au NP) syntheses must be cleaned with freshly prepared aqua regia solution (three parts of conc. HCl and one part of conc. HNO3). The aqua regia can be stored in a glass bottle and reused as long as the orange colour remains. The washing with aqua regia must be handled with care, wearing gloves as well as safety glasses and protective clothing. After that, items must be washed in tap water and then rinsed with distilled water (18.2 MΩ cm resistivity) and dried in air or in an oven.
The same ultrapure distilled water must be used for the preparation of the aqueous solutions. All chemical reagents are purchased from Sigma Aldrich. KAuCl4 can be replaced by HAuCl4. Heptane and ethanol are analytical or reagent grade and are used without purification.
Experiment 1. Synthesis of gold nanoparticles
An aqueous solution of KAuCl4 is heated to the boiling point in an Erlenmeyer, and then, a sodium citrate aqueous solution is added with vigorous magnetic stirring. This solution is heated during about 10 min, and the obtained red solution is finally left cooling. In Table 1, the experimental conditions to obtain Au NPs with two well-defined sizes are given.
Experiment 2. Change of colour by aggregation with salt
At least 0.5 g of NaCl in 10 mL of distilled water is dissolved, or a saturated solution (>360 g/L, i.e. 6.1 mol/L) is used. A small amount (about 3–4 mL) of the Au NPs solution is put in two test tubes. One tube is used as a colour reference. To the other tube, 5–10 drops of the saturated NaCl solution are added. The colour of the solution changes in the second tube. This experiment could be done in a cuvet with the UV–visible spectrum recorded after each addition.
Experiment 3. Polymeric film containing gold nanoparticles
A concentrated solution of poly(vinyl alcohol) (PVA) (1 M in monomer) is prepared by dissolving 440 mg in 10 mL of distilled water. The beaker containing PVA in water is put in a water bath, and the solution is heated to boiling under stirring. The water bath prevents the PVA from sticking on the bottom of the beaker. A homogeneous solution of PVA is obtained after a few tens of minutes. Then, 2 mL of the colloidal Au NPs solution is added to 3 mL of the concentrated PVA solution. After stirring, the mixture is put in a crystallizing dish (of about 3–4 cm in diameter) and heated at 70–80 °C in order to evaporate water. Care should be taken to avoid overheating, since this can lead to non-homogeneous distribution of the Au NPs in the film. A thin film of PVA containing Au NPs is obtained after a few hours of drying.
Au NPs can also be induced directly in PVA solution containing KAuCl4 : PVA acts as reducing and stabilizing agent . The Au NPs are prepared as follows: in a typical experiment, 4 mL of 2.4 mM KAuCl4 aqueous solution is added into 80 mL of 0.24 M (repeating unit) PVA aqueous solution. Then, the mixture is heated at 80 °C for several hours, yielding a purple solution. The film is then prepared in a crystallizing dish as described before.
Experiment 4. Formation of a metallic gold film from colloidal gold nanoparticles
Forty millilitres of an aqueous Au NP solution is centrifugated (around 3,000 rpm, until the supernatant becomes pale pink). The supernatant is then removed, and the concentrated aliquot of Au NPs is redissolved in 0.8 mL of ethanol. A heptane/water biphasic system is prepared in small glassware with ca. 3–4 cm2 of section. In agreement with the densities of these two solvents, the water is located below and the heptane above. The concentrated ethanol solution of Au NPs is then added by small injections in the organic phase near the organic/aqueous interface until a golden film appears at the interface.
Experiment 5. Surface plasmon resonance and the colour of gold
The surface plasmon wave is an electromagnetic wave that arises at the interface between a metal and an insulating medium (dielectric) and whose structure is that of an evanescent wave. It can be seen as a wave confined very close to the metallic surface . In the case of the gold/air interface and at a wavelength of 633 nm, this wave is confined within a 30-nm-thick layer close to the interface and crawls along the gold surface over a distance of 10 μm. Its excitation is possible only with geometries capable of generating large wave vectors parallel to the interface. The most common geometry is the Kretschmann geometry shown in Fig. 1 where the impinging wave is generated by total internal reflection on a glass prism as depicted in Fig. 1b. The gold film should be deposited on this face of the prism. The experiment consists in measuring the reflected intensity as a function of incidence angle when the light is p-polarized. If one measures this intensity when a helium–neon laser in used (λ = 633 nm), the reflected intensity exhibits a sharp minimum for an angle of ca. 30° as plotted in the graph of Fig. 1c . From this plot, it is easy to understand that if the angle is set at 30°, and if a white light beam from a halogen lamp is used instead of a monochromatic laser beam, the red component of light will not be reflected. Therefore, the observed resulting beam will appear green. And by adjusting the angle, it is possible to turn off various colours, and the colour of the observed beam will also vary. This is a typical effect arising from the confinement of an optical wave into a nanometer-thin gold film. A setup that exhibits this effect is described in details in a publication  and is available from a small company as a lab work for master students .
Experiment 1. Synthesis of gold nanoparticles
While gold is known since a long time for its golden colour so appealing in jewellery, gold is also used since antiquity as red dye. For instance, Au NPs have been found in several red glasses or on porcelains decorated with red or pink enamels dating from ancient times, for instance, in Roman glassworks (such as the famous Lycurgus Cup dating from the fourth century CE) or in the Chinese “Famille Rose” porcelain dating from the eighteenth century [9–11]. Indeed, bulk gold reflects the yellow colour and appears golden-coloured, whereas at the nanoscale gold appears generally red. Michael Faraday, fascinated by this ruby colour of colloidal gold solutions, was the first scientist who has discovered that the optical properties of gold colloids differ from those of the corresponding bulk metal. He reported on the first synthesis of Au NPs in solution in 1857 . These colloids were obtained by reduction of gold salts by white phosphorous . Later, the specific colours of metal colloids were explained by Mie .
This phenomenon is due to the well-known plasmon resonance also called local surface plasmon resonance (LSPR), which can be explained by a confinement of the electromagnetic wave associated with the light inside the NPs. Indeed, when its wavelength is greater than the size of the NPs, the whole NP feels a uniform and oscillating electric field, and consequently electrons oscillate in phase. Nevertheless, this collective oscillation of the electrons is constrained by the reduced dimensions of the NP in which they are confined, leading to a significant absorption of the wavelengths around green. Then, NPs appear with the complementary colour, which is red.
This experiment introduces the audience into the idea that at the nanoscale, basic properties, such as colour, turn out to be very different from what happens in the “macro-world”. Therefore, nanoscience focuses on properties linked not only to a material but to its specific size. And sometimes, the changes of properties at the nanoscale have consequences visible at our human scale. In the present case, the assembly of gold atoms into NPs of ca. 1,000 atoms changes the colour of gold. This message is always puzzling for non-scientific audience.
Nowadays, among the different ways of synthesis of spherical Au NPs, Turkevich’s method is the most known and the easiest to perform . This method is based on the reduction of an Au(III) salt by sodium citrate, as described in the experimental part (experiment 1). The reaction starts by boiling a gold salt aqueous solution (pale yellow). A few minutes after the addition of sodium citrate, the mixture becomes firstly uncoloured, then grey, violet, and finally burgundy red (Fig. 2a). In this reaction, the sodium citrate is used not only as reducing agent, but also as stabilizing agent. Indeed, its stabilizing role restrains the growth of the NPs and controls the NP diameter. Thus, the size of the NPs can be modulated by changing the concentration of the gold salt solution and the ratio of the quantity of gold salt to the quantity of sodium citrate [16, 17]. The sizes of the NPs described in this experiment are 15 and 30 nm and has been verified by transmission electronic microscopy (TEM) (Fig. 2b)
Diffusion (or scattering) of light by the Au NPs can be evidenced with a laser beam pointed to the solution (Fig. 2c) and can be compared with a similar experiment using an aqueous solution containing an organic red dye (rhodamine or Congo red for instance) for which diffusion is not detectable (Fig. 2d). When light is scattered by single molecules such as dye molecule, the efficiency of the phenomenon is very low (usually quantified with the scattering cross section) and is barely visible by eyes (Fig. 2d). However, this cross section grows as the volume of the object, and with a particle of 30 nm whose diameter is 100 times larger than a molecule (volume 106 larger), the scattering process becomes easily visible as demonstrated in Fig. 2c. Moreover, Fig. 2c shows that if the laser wavelength is tuned to the plasmon resonance, the scattering is even stronger. The green laser beam is quickly damped when going through the NP suspension, whereas the red laser light is scattered less efficiently, but over a longer path.
Many other chemical methods of synthesis exist  and can lead to different shapes of NPs: nanorods [19, 20], nanopyramids , nanocubes, etc. Physical chemical syntheses such as photolytic and radiolytic methods can also be used, and generally lead to a better control of the size of the NPs [18, 22, 23]. Chemical and optical properties of Au NPs depend on their size, their shape, their aggregation state and their local environment. Such Au NPs have applications for example in catalysis (oxidation of CO), medicine (photothermal therapy and radiotherapy), plasmonics and electronics [9, 24, 25].
Experiment 2. Colour change of nanoparticles by aggregation with a salt
Upon addition of NaCl, the initially red colour of the Au NP solution turn to blue grey (experiment 2).
This experiment illustrates the extreme sensitivity of the coloration property with phenomena occurring at the nanoscale: if NPs are driven close to each other, the plasmon resonance is altered, and the colour changes (Fig. 3a, b).
The surface of Au NPs is charged. This induces repulsive forces between the NPs preventing them from aggregation: the energy barrier is too strong for interaction to occur between particles. However, upon addition of NaCl, this energy barrier is reduced allowing the Au NPs to interact and aggregate. Dissolved salts, or electrolytes in general, are able to screen the repulsive electrostatic forces caused by the citrate layer: indeed, the positive charges of the electrolyte associate with the negative charges on the surfaces of the NPs. Cryo-TEM experiments, which consist in freezing the NPs after deposition onto an analysis grid by dipping it in a cooling media (liquid nitrogen), allowing to clearly show initially well-dispersed Au NPs in solution (before addition of NaCl) and their aggregation after addition of NaCl, but the nanoparticles keep their shape (Fig. 3c, d). This aggregation causes surface plasmon coupling which induces a shift in the surface plasmon resonance to a higher wavelength, resulting in a change in colour of the solution from red to blue in our case (Fig. 3a). These experiments can be done in an optical cell, and with a spectrophotometer, and students can monitor the NP aggregation by the UV–visible absorption of the solution (Fig. 3b). The students can then associate the absorbed wavelength with the observed colour of the solution.
These experiments show that individual small Au NPs appear red; however, when the particles aggregate together, the plasmon resonances can couple, and the colour changes to blue.
This property is used to develop biosensors. Au NPs can be easily functionalized. Thus, binding of Au NPs to biomolecules offers a promising approach for facile tracking of desired targets in aqueous samples. Antibody/antigen pairs can selectively link to the NPs. By modifying the surfaces of the NPs to incorporate these biomolecules, binding events can be detected by a change in solution colour. The most familiar example of NPs in sensing is the home pregnancy test based on detection of the hormone pregnancy (β-HCG hormone) . Tests for DNA detection take also advantage of surface plasmon resonance changes . For example, one kind of DNA test looks for certain bases. In this test, NPs are present as large aggregates displaying a blue colour. If the complementary DNA base is present, the NPs will preferentially bind to that base instead of each other, and the aggregates will dissolve inducing a deep red colour. We can detect the colour changes associated with DNA binding in about 2 min, making for a rapid assay. Au NPs functionalized with antibodies can be also used for rapid detection of virus (such as A/H5N1) . Another example is the use of Au NPs for sensitive diagnostic tests and novel treatments in the detection of Alzheimer’s disease by finding a protein in spinal fluid .
Experiment 3. Polymeric film containing gold nanoparticles
A thin film of Au NPs dispersed in PVA can be obtained by simply drying the gold colloid in the presence of dissolved PVA (at high concentration) (experiment 3). Au NPs will be randomly distributed within the PVA film (TEM images not shown here). The film appears purple, because the index of refraction of the medium surrounding the Au NPs is changed: from n = 1.33 (in aqueous solution) to n ∼ 1.7 (in the PVA film) (Fig. 4).
This experiment demonstrates that Au NPs keep their unusual optical properties, even outside of the preparation solution. It makes possible to use their nanoscale properties for various applications in the daily life. Indeed, composite materials made of NPs and polymeric matrices are suitable candidates for biomedical applications, magnetic storage, optoelectronic and electronic devices.
Experiment 4. Formation of a metallic gold film from colloidal gold nanoparticles
While Au NPs are generally red, can we obtain again a golden appearance if we build bulk gold by aggregating and coalescing a lot of NPs? The experiment proposed in this part consists in the formation of a golden metallic film at the interface between two immiscible liquids (Fig. 5), using a colloidal Au NP solution (experiment 4).
This experiment consists in using a water/heptane biphasic system and adding an ethanol solution of colloidal Au NPs at the interface between the two immiscible liquids . Indeed, when Au NPs are redissolved in ethanol, the surface charge density of the NPs decreases, most likely due to the competitive adsorption of alcohol with citrate on the NPs. The solubility of the Au NPs in the aqueous phase is decreased when they diffuse towards the water/heptane interface. Moreover, when a water-miscible solvent with a lower dielectric constant, such as ethanol, is added at the interface, the interfacial energy between the two phases decreases even more, leading to the formation of the mirror-like gold film at the interface .
Experiment 5. Surface plasmon resonance and the colour of gold
The usual colour of bulk gold is yellow, which itself is a non-usual property for metals since they are all grey except gold and copper. This yellow colour is due to the so-called interband transitions of gold that occur in the blue region of the visible spectrum . As a consequence, the reflected light is deprived of its blue component and appears yellow. However, when the thickness of a gold layer decreases down to the nanometer scale, light behaves differently. This phenomenon can be shown in a demonstrative way in the case of the surface plasmon resonance using the setup described in Figs. 1a and 5a. The gold thin film which is attached on the prism should be illuminated with a beam light from a white light lamp. The excitation beam enters the prism through one face, and the reflected beams exits through another face and is observed on a screen (Fig. 6a, b). The experiment consists in slowly rotating the prism: the beam reflected from the thin film goes through a range of different colours that can be easily viewed on a white screen and that are absolutely unusual for gold. This change of colour of a reflected beam is the visible manifestation of the presence of the surface plasmon wave . The energy at one wavelength of the impinging wave is transferred to the surface plasmon wave, and the reflected beam is strongly attenuated. As a consequence, this wavelength is missing in the reflected beam, and the observed colour changes (Fig. 6c). For example, if the angle of the rotation stage is set at 30° in our setup, the surface plasmon wave is generated for the red wavelength, and the reflected beam will be green (complementary colour to red). It helps demonstrate that light behaves very differently when interacting with nano-objects. This experiment can also lead the audience to plasmonics and to the fabrication of some kinds of ultra-sensitive biosensors. An impressive way to demonstrate that this plasmon wave is a very sensitive sensor is to blow gently towards the gold film. The slight optical index change induced by the air flow makes the colours fluctuate. It can help in understanding that if a layer of molecules adsorbs on the gold film, the index change will also be detected by the surface plasmon wave.
A set of five easy experiments has been proposed as an introduction to key concepts of nanoscience targeting a public audience of non-specialists. They are all based on the use of gold either as nanoparticles or in nanometric thin films. The main message is that usual material exhibits unexpected properties when one of their dimensions is nanometric. This article explores more specifically the colour modulations of gold at the nanometric size. The first four experiments are based on gold nanospheres of 15 to 30 nm in diameter that are prepared according to the Turkevich method. In this case, gold adopts a magnificent ruby-red colour. Experiments 1, 2, and 3 describe the chemical preparation, the way for modulating their colour and how to include them into a polymer film. Experiment 4, based on the use of immiscible liquids, is a striking experiment that shows that starting from these nanoparticles, it is possible to turn them back into a gold film that recovers its conventional yellow colour. Finally, the last experiment plays with the optical properties of the surface plasmon wave. These experiments can be used for teaching in lab courses with undergraduate students after some adaptation. Of course when used in conferences, they are always capturing the public attention if they are conducted as live experiments, although it demands some training so that the effect comes up at the right moment. This is always a very rewarding feeling for us scientists to be able to raise a fascination for scientific work and contribute to attract young people into the scientific community.
It has to be noted that some experiments proposed in this paper have been tested many times with success in school, in partnership with the Nano-School (www.nano-ecole.fr) project. This action aims to educate young people about nanoscience and give them some basics. These experiences around gold nanoparticles are particularly suitable in this context. This partnership has also helped to develop a kit for synthesizing nano particles, for teachers of middle and high schools (www.jeulin.fr).
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The authors thank Patricia Beaunier (Laboratoire de Réactivité de Surface, Université Pierre et Marie Curie) for the TEM observations and Jean-Michel Guigner (Institut de Minéralogie et de Physique des Milieux Condensés, Université Pierre et Marie Curie) for the Cryo-TEM studies. Finally, this paper is in debt to Don Eigler, a prominent physicist, known for his pioneering work in STM. One of the authors attended a keynote given by Don Eigler in 2006 in Basel (Switzerland) entitled “Computation in Small Structures: a Long Road to an Uncertain Destination”. The content of the conference was totally unexpected since Don Eigler did not talk about computation at all, but about the urgent need for scientists to address the issue of informing the public, the journalists, the companies and the politics. This paper shows that his call has been heard.
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Pluchery, O., Remita, H. & Schaming, D. Demonstrative experiments about gold nanoparticles and nanofilms: an introduction to nanoscience. Gold Bull 46, 319–327 (2013). https://doi.org/10.1007/s13404-013-0122-9
- Gold nanoparticles
- Plasmon resonance
- Gold nanofilms