Semiconductive Nanocrystals and Quantum Dots:
An Introduction

Semiconductors and their influence on our lives

In the current age of electronics, we heavily depend on semiconductor based devices. Semiconductors are at the core of every diode, transistor, LED and processor. Therefore, many devices that we use on a daily basis, such as mobile phones, computers, credit cards etc. require semiconductors.1-2 Thus, they have a monumental impact on society. In addition to consumer electronics, semiconductors are also extremely important with regard to sustainable energy, as current solar energy technology is based on semiconductors.

A semiconductor’s properties lie somewhere between those of a conductor (like metals) and those of an insulator (glass, most plastics). The electric conductivity of a semiconductor thus also lies somewhat between that of conductors and insulators, hence the name “semi-conductor”. By combining semiconductors with different conductivities, which is often done by taking a single semiconductor and doping different regions with different elements, one can create a semiconductor junction. These semiconductor junctions direct the flow of electrons (electricity), and therefore can be used for the two most important components in electronics: diodes and transistors. In a diode, a semiconductor junction is used to create a near infinite resistance in one direction, and a near zero resistance in the other, thus ensuring that the conductivity can only flow in one direction. A transistor is a (multi) semiconductor junction which allows the direction of the current to be switched towards different “terminals“. Furthermore, a semiconductor junction can amplify the current in a transistor. Semiconductors are also excellent materials for converting light into electricity and vice versa, making them great materials for use in light emitting devices (LEDs, lasers) and light absorption devices (solar cells, light detectors etc.). Semiconductors can also exhibit other interesting properties. For example, they are heat sensitive which also allows them to be used in heat sensors.

Due to the extremely high demand for more powerful devices, and the desire to make them smaller, the research field of semiconductor materials is constantly looking for semiconductors with new compositions as well as new ways of implementing them. One approach to carrying out these goals is to make semiconductors in the form of colloidal nanocrystals (NCs), which not only decreases their size, allowing for smaller devices, but also allows for a new way of manipulating the properties of semiconductors.

Small nanocrystals have a big impact

As is the case for semiconductors, our daily lives depend on material properties. For instance, we require conductive materials for electron transport, transparent materials for windows, and brightly colored materials for paintings. All these properties are material dependent. For instance, we use copper for conductive materials since copper is a good electron conductor, and we use silicon dioxide (SiO2) for windows since SiO2 as it is transparent. We use other materials that strongly interact with light for instance in paintings, like The Great Wave off Kanagawa by Hokusai or the the Starry Night, by Vincent van Gogh, in which Prussian blue (named after the Prussian army who used the blue pigment to dye their uniforms) (Fe4[Fe(CN)6]3) is used to represent dark, deep blue.3-4 In all the aforementioned cases, the material properties, such as e.g. conductivity, melting point, colour, etc., do not depend on the size or shape of the used material. However, when one starts to look at material properties at the nano-scale (1-100 nm, or 0.000000001 - 0.0000001 meter), in a range where the amount of atoms start to be limited, certain material properties start to become size dependent, and they can differ greatly from the properties of their bulk sized counterparts. This extra property tunability has driven the scientific community, especially the field of semiconductors, to go “nano”, as it would allow for an extra tunability of the material properties. For instance, one can envision modifying the nano-size of materials in order to alter the optical and conductive properties, rather than having to change the composition of a metal, or the molecular structure of an organic molecule.

These colloidal semiconductor NCs have been synthesized and studied for at least the last three decades. Now, in 2018, we have an excellent understanding of how the nanoscale influences semiconductors, and we have access to a plethora of different compositions with a very great size and shape control on the nanoscale. Furthermore, the field has moved to colloidal NCs, meaning that the NCs can be synthesized as small, stable, solid NCs in a solution. This does not only allow for more control over the size during the synthesis (the NCs can be precisely tuned to the size of an atom), but also has a large processability advantage, as colloidal NC solutions can be deposited using simple deposition techniques like inkjet printing or spray painting. All these advancements have pushed these NCs from being the subject of fundamental lab studies to being employed in several types of applications today, such as light emitters in TVs (as is shown in figure 1).5 Current colloidal semiconductor NCs also have the capacity to be used in a wide range of applications in the future, such as solar cells, LEDs, lasers, luminescent solar concentrators.6 They are also extremely important with regard to advancements in nano-biotechnology, and they can be used in drug delivery techniques, in vivo imaging and photothermal cancer therapy treatments.7-8

 

Figure 1: Semiconductor nanocrystals and their use in ultra-high definition TVs. (a) Example of solutions containing colloidal semiconductor NCs with different sizes, resulting in a range of different colors. (b) Samsung Ultra High Definition (SUHD) TV using InP NCs as emitters, resulting in one of the best TVs that is currently on the market in terms of color purity. Taken from ref.5

A brief history of colloidal nanocrystals

Although the field of colloidal semiconductor NCs started to gain attention in the 1980s, particles with properties that are tunable on the nanoscale, especially metals, have been used for thousands of years. One of the most reported and visual examples is stained glass, which dates back to the middle ages.5, 9 Medieval stained glass artists knew that baking their glass with gold and silver salts at different temperatures or for different amounts of times resulted in different colored stained glasses (even though the composition remained the same).5, 9-10 Using silver salt, they could for instance produce every primary color (blue, yellow and red). Similarly, they created red, green and orange by using gold salts. Therefore, mixing silver and gold gave them access to any color that they needed to stain their windows. In a similar way, ceramics with different bright colors were made in Italy during the Renaissance period (i.e. during the 15th and early 16th century), using only different copper and silver salts, resulting in a wide variety of colors.11-12 These ceramics, called Deruta ceramics (derived from the name of the small town Deruta, in the region of Umbria, Italy), were therefore a result of differently sized copper and silver NCs. Of course, at this time, the scientific reason behind the production of these different colors was not known. Nevertheless, this is a perfect example of the tunable properties of materials in NC form. In fact, the use of “nanoparticles” as single coloring agents can be traced back even earlier in history: lead sulfide NCs (about 5 nm) were used by the ancient Egyptians to dye their hair,13 and iron nanoparticles were used in the Bronze Age to dye pottery red.14 In retrospect, we now know that, in each of these cases, different reaction temperatures and times resulted in differently sized and shaped copper, silver, gold or iron NCs, all of which exhibited different colors due to their nano-size.10-12, 14

Although the use of NCs may go back centuries, the first reported scientific study on size dependent optical properties dates back to 1857, when Michael Faraday tried to study the relationship between gold (and other metal) layers of different thicknesses and light.15 In these experiments, he accidentally created different colored solutions while trying to mount gold leafs onto microscope slides. Based on these observations, he concluded that “known phenomena appeared to indicate that a mere variation in the size of its particles gave rise to a variety of resultant colors” and that “reflexion, refraction, absorption etc. depended upon such relations, there was reason to expect that these functions would change sensibly by the substitution of different sized particles”. Nowadays, we know that the different colors of metal particles stem from the so-called Localized Surface Plasmon Resonance (LSPR) effect, which, in turn, originates from the collective oscillation of electrons at the surface of the particles. This effect is highly sensitive to the surface of the NC, therefore it is highly size and shape dependent. The discovery that the electronic structure of NCs can change came a century later, when small nanometer-sized copper chloride and silver iodide, which will than were referred to as ‘crystallites’, were embedded into NaCl matrices in a very similar way as to how the medieval stained glass artists made their stain glass windows.16-17 For these crystallites, it was observed that the bandgap depended on their size, and, thus, on changes in the electronic structure of the NCs. One of the first theoretical models describing the relation between the electronic properties of semiconductors and size dates back to the 1960s, when Evens and Young correlated the changing optical properties of thin layered MoS2 with the changes in its electronic structure.18 Twenty years later, in the 1980s, the first models of small spherical semiconductor NCs, so called ‘Quantum dots (QDs)’, were published (figure 2a-c).19-21 One of the major breakthroughs with regard to linking the experimental data with theoretical models was achieved as a result of the quick pace at which advancements were made in the synthesis of colloidal PbS and CdSe NCs.22-23 One obstacle that was still limiting the linking of experimental data with theoretical models was the accurate determination of the NCs size (and shape), especially in the smaller size range of 1-10 nm. To this end, the discovery and development of the transmission electron microscope (TEM, which was first demonstrated by Max Knoll and Ernst Ruska in 1931, but it did not reach the required resolution until the 1970s-1980s, in 1986, Ernst Ruska was awarded the Nobel Prize in Physics “for his fundamental work in electron optics, and for the design of the first electron microscope.") gave researchers the final boost they needed to link the experimental data with theoretical models, as it directly gave “images” of NCs (figure 2d). Another major breakthrough was in 1993, when the Bawendi’s group reported a synthetic procedure that was able to produce (nearly) monodisperse colloidal CdSe NCs, reaching near atomic precision (figure 2e-g).24 Over the following decades, the research field of colloidal semiconductor NCs quickly expanded and matured into a large research community. Today, the synthesis field has expanded to encompass different materials, such as PbSe, CuInS2, InAs, Cu2-xS, ZnS and many other semiconductors, and it has achieved a large range of sizes and shapes.6 Furthermore, highly complex binary NCs, consisting of multiple semiconductor domains, can be synthesized resulting in an extreme high tunability of the NC’s properties.25-26 Moreover, the field has matured and started to move from fundamental research towards applications, with NCs being studied for use in a wide range of applications such as LEDs, lasers, solar cells and cancer treatments.6, 27

Figure 1.2. Overview of some of the most important advancements in the history of colloidal semiconductor nanocrystals. (a) Absorption spectra of different sized CuCl NCs. (b) Plotted exciton absorption of CuCl vs. NC size. (c) Calculated quantum confinement effect of different semiconductors. (d) TEM image of 2 nm PbS cluster. (e) Optical absorption of 1.2 – 11.5 nm CdSe NCs in hexane. (f) High resolution TEM image of 8 nm CdSe NCs. (g) Monolayer of 5,1 nm diameter CdSe crystallites showing short-range hexagonal close packing. Taken with permission from ref.19, 21, 24, 28

References

1.            Semiconductors Shaping Society. The Electrochemical Society, https://www.electrochem.org/semiconductors-shaping-society.

2.            Enabling the Hyperconnected Age: The Role of Semiconductors. Oxfor Economics, https://www.oxfordeconomics.com/recent-releases/enabling-the-hyperconnected-age-the-role-of-semiconductors.

3.            Molecule of the Week Archive, Prussian Blue. https://www.acs.org/content/acs/en/molecule-of-the-week/archive/p/prussian-blue.html 2017.

4.            Philip McCouat, Prussian Blue and Its Partner in Crime. Journal of Art in Society, www.artinsociety.com 2014.

5.            What Do Medieval Stained Glass and Suhd Tv’s Quantum Dot Technology Have in Common? https://www.samsung.com/global/tv/blog/stained-glass-and-quantum-dot-technology/ 2016.

6.            Kovalenko, M. V., et al., Prospects of Nanoscience with Nanocrystals. ACS Nano 2015, 9, 1012-1057.

7.            Nasirzadeh, K., et al., Inorganic Nanomaterials; a Brief Overview of the Applications and Developments in Sensing and Drug Delivery. J. Appl. Biotechn. Rep. 2016, 395-402.

8.            Li, C., A Targeted Approach to Cancer Imaging and Therapy. Nat. Mater. 2014, 13, 110.

9.            Odom, T. W., Printable Stained Glass. Nat. Nanotechnol. 2012, 7, 550.

10.          Freestone, I., et al., The Lycurgus Cup — a Roman Nanotechnology. Gold Bull. 2007, 40, 270-277.

11.          Padovani, S., et al., Copper in Glazes of Renaissance Luster Pottery: Nanoparticles, Ions, and Local Environment. J. Appl. Phys. 2003, 93, 10058-10063.

12.          Ball, P., Renaissance Potters Were Nanotechnologists. Nature, doi:10.1038/news030623-17 2003.

13.          Walter, P., et al., Early Use of PbS Nanotechnology for an Ancient Hair Dyeing Formula. Nano Lett. 2006, 6, 2215-2219.

14.          Colomban, P., The Use of Metal Nanoparticles to Produce Yellow, Red and Iridescent Colour, from Bronze Age to Present Times in Lustre Pottery and Glass: Solid State Chemistry, Spectroscopy and Nanostructure. J. Nano Res. 2009, 8, 109-132.

15.          Faraday, M., Experimental Relations of Gold (and Other Metals) to Light. Philos. Trans. Royal Soc. 1857, 147, 145-181.

16.          Gross, E. F.; Kapliansky, A. A., A Spectroscopic Study of Absorption and Luminescence of Cuprous Chloride, Introduced into a Crystal of Rock Salt. Opt. Spektrosk. 1957, 2, 204-209.

17.          Berry, C. R., Structture and Opticcal Absorption of AgI Microcrystals. Phys. Rev. B 1967, 161, 848-851.

18.          Evans, B. L.; Young, P. A., Exciton Spectra in Thin Crystals: The Diamagnetic Effect. Proc. Phys. Soc. 1967, 91, 475.

19.          Ekimov, A. I.; Onushchenko, A. A., Quantum Size Effects in 3-Dimensional Microscopic Semiconductor Crystals. Jetp Lett. 1981, 34, 345-349.

20.          Efros, A. L., Interband Absorption of Light in a Semiconductor Sphere. Sov. Phys. Semicond. 1982, 16, 772-775

21.          Brus, L., Electronic Wave Functions in Semiconductor Clusters: Experiment and Theory. J. Phys. Chem. 1986, 90, 2555-2560.

22.          Brennan, J. G., et al., Bulk and Nanostructure Group II-VI Compounds from Molecular Organometallic Precursors. Chem. Mater. 1990, 2, 403-409.

23.          Steigerwald, M. L., et al., Surface Derivatization and Isolation of Semiconductor Cluster Molecules. J. Am. Chem. Soc. 1988, 110, 3046-3050.

24.          Murray, C. B., et al., Synthesis and Characterization of Nearly Monodisperse CdE (E = Sulfur, Selenium, Tellurium) Semiconductor Nanocrystallites. J. Am. Chem. Soc. 1993, 115, 8706-8715.

25.          Donega, C. d. M., Synthesis and Properties of Colloidal Heteronanocrystals. Chemical Society Reviews 2011, 40, 1512-1546.

26.          Burda, C., et al., Chemistry and Properties of Nanocrystals of Different Shapes. Chem. Rev. 2005, 105, 1025-1102.

27.          Talapin, D. V., et al., Prospects of Colloidal Nanocrystals for Electronic and Optoelectronic Applications. Chem. Rev. 2010, 110, 389-458.

28.          Brus, L. E., Electron–Electron and Electron‐Hole Interactions in Small Semiconductor Crystallites: The Size Dependence of the Lowest Excited Electronic State. J. Chem. Phys. 1984, 80, 4403-4409.

29.          Akkerman, Q. A., et al., Genesis, Challenges and Opportunities for Colloidal Lead Halide Perovskite Nanocrystals. Nat. Mater. 2018, 17, 394-405.

30.          Hirose, K., et al., Perovskite in Earth’s Deep Interior. Science 2017, 358, 734-738.

31.          Correa-Baena, J.-P., et al., Promises and Challenges of Perovskite Solar Cells. Science 2017, 358, 739-744.

32.          Stranks, S. D.; Snaith, H. J., Metal-Halide Perovskites for Photovoltaic and Light-Emitting Devices. Nat. Nano. 2015, 10, 391-402.

33.          Lee, M. M., et al., Efficient Hybrid Solar Cells Based on Meso-Superstructured Organometal Halide Perovskites. Science 2012, 338, 643-647.

34.          Protesescu, L., et al., Nanocrystals of Cesium Lead Halide Perovskites (CsPbX3, X = Cl, Br, and I): Novel Optoelectronic Materials Showing Bright Emission with Wide Color Gamut. Nano Lett. 2015, 15, 3692-3696.

The QD Lab at LMU


Dr. Q. A. Akkerman, Group Leader

Chair for Photonics and Optoelectronics

Nano-Institute Munich, Department of Physics

Ludwig-Maximilians-University Munich

80539 Munich, Germany

Q.Akkerman@lmu.de