Layer-structured two-dimensional nanomaterials are a family of materials with strong covalent bonding within layers and weak van der Waals interaction between layers, whose vertical thickness can be thinned down to few nanometer and even single atomic layer. Bismuth chalcogenides are examples of such two-dimensional materials. Here, we present our discovery of significant enhancement of light transmission through thin nanoplates of layered bismuth chalcogenides by intercalation of copper atoms, which is on the contrary to most bulk materials in which doping reduces the light transmission. This surprising behaviour results from two mechanisms: chemical tuning effect of substantial reduction of material absorption after intercalation and nanophotonic effect of zero-wave anti-reflection unique to ultra-small thickness of nanoplates. We demonstrate that the synergy of these two effects in two-dimensional nanostructures can be exploited for various optoelectronic applications including transparent electrode. The intercalation mechanism allows potential dynamic tuning capability.
Beyond graphene1,2,3,4,5,6, two-dimensional (2D) materials like boron nitride7,8 and a variety of metal chalcogenides9,10,11,12,13 have been shown to host a variety of interesting physical and chemical properties14,15,16,17,18,19,20. As members of this 2D material family, Bi2E3 (E=Se, Te) have been extensively studied for thermoelectrics21,22,23. More recently, they have been discovered to be topological insulators and have caused a great research attention on these materials14,15,16,17. These chalcogenides exhibit a layered, rhombohedral crystal structure as shown in Fig. 1a. Each layer consists of five covalently bonded atomic planes, E-Bi-E-Bi-E, known as a quintuple layer. These quintuple layers are bonded together via van der Waals interaction to form the Bi2E3 crystal. Each quintuple layer has a thickness of about 1 nm. Copper (Cu) intercalated Bi2Se3 has been found to show superconducting behaviour at low temperature24. Recently, we and others have demonstrated the growth of Bi2E3 nanoribbons and nanoplates with thickness down to 3 nm for studying the physics of topological insulator states17,25. Chemical species can be inserted between layered materials via a process known as intercalation26.
In our previous work, we developed a novel chemical approach of zero-valent metal atom intercalation into these nanostructures and demonstrated that a variety of metal atoms can be intercalated27,28, which is different from the historical development of positively charged metal ion intercalation. Very high concentration of Cu atom interaction (up to 60%) has been controllably demonstrated27. As material optical property is strongly dependent on its electronic structure, it is intriguing to tune the optical properties of Bi2E3 with this novel intercalation approach. In the following, we report counter-intuitive optical transparency of Bi2E3 nanoplates induced by Cu intercalation. Simultaneous enhancement of optical transmission and electrical conductivity will enable various applications of these materials.
Material preparation and characterization
Bi2Se3 nanoplates from a few to a few tens of nanometer thick, with a lateral dimension around a few tens of micrometres are synthesized using solvothermal method29. Cu atoms are intercalated into Bi2Se3 nanoplate following our previous procedures27,28. The amount of Cu intercalants can be controlled by varying the reaction time from several minutes to a few hours. In this study, the atomic concentration of Cu we intercalated into the nanoplates ranges from 0 to around 20%. Optical transmission measurements (Fig. 1b) of individual plates before and after intercalation were conducted to compare the changes due to the Cu intercalation. Figure 1c,d provides transmission optical images of the same Bi2Se3 nanoplate with thickness of 8 nm before and after 1 h of Cu intercalation, respectively. The thickness of the plate before intercalation is determined by the atomic force microscopy as shown in Fig. 1e,f. There is no noticeable change in nanoplate thickness after Cu intercalation (Supplementary Fig. 1). Substantial transmission change can be observed directly from the images since the nanoplate looks much brighter after intercalation under the same illumination condition. As a control, we also treated Bi2Se3 samples in the same solvent, but without the Cu salt. There is no observable change in their optical transmission, suggesting that Cu intercalation instead of the solvent makes the nanoplate much more transparent.
To confirm the Cu intercalation into the nanoplate, we have carried out transmission electron microscopy (TEM) study. Figure 2a is a TEM image of a Bi2Se3 nanoplate. Energy dispersive X-ray spectroscopy measurements are carried out in TEM to determine the ratio of Bi, Se and Cu after the intercalation (Supplementary Fig. 2). Measurements of samples with various amounts of Cu intercalants show that the stoichiometric ratio between Bi and Se remained the same as before intercalation. X-ray diffraction results in ref. 27 have shown that up to 20–30% Cu intercalation causes very small lattice expansion (<1%). Here electron diffraction results (Fig. 2b) also show that the crystal structure of the nanoplates did not change with 22 at% intercalated Cu, which is evident that the host crystal lattice was not distorted by the added Cu atoms. The zero-valent nature of Cu intercalants have been clearly demonstrated in our previous studies27.
To further study the behaviour of such an optical property transition, spectral measurements were carried out to characterize the same individual nanoplates before and after Cu intercalation. The confocal measurement was conducted on single nanoplates to ensure that the detected light is from the nanoplate sample only and not mixed with signals from other area of substrate. The confocal mechanism allows the collection of light from a spot approaching the diffraction limit (<~1 μm), which is much smaller than the lateral size of nanoplates (typically 5–20 μm). All optical transmission data are normalized to the transmission of bare glass substrate.
Figure 2c shows the transmission spectra of Bi2Se3 nanoplates, with 6, 10, 22 nm thicknesses before (black curves) and after (red curves) 1 h of Cu intercalation. Clear thickness dependence of the transmission spectra allows us to compute the optical properties of both intrinsic and Cu-intercalated materials as we will show in the next section. Figure 2d,e plots the transmission versus nanoplate thickness for two different optical wavelengths: 550 nm (visible) and 850 nm (near-IR), respectively. Before Cu intercalation, the optical transmission is relatively low for all thicknesses of nanoplates. In contrast, the transmission increases dramatically for all thicknesses and for all the wavelengths (400–900 nm) measured after Cu interaction. For example, for the bare nanoplates with a thickness of 22 nm, the transmission in visible frequency is only about 20%. After Cu intercalation, the transmission is boosted to over 70% in most part of the visible-near-IR range. Thin plates <10 nm thick become highly transparent (>95%) after Cu intercalation. Moreover, the transmission in long wavelength range is usually more than that in the short one (Fig. 2c–e). Such a feature is preserved even after Cu intercalation, which is a characteristic of the mechanism we provided in the next section. In addition to Bi2Se3 nanoplates, similar optical transmission enhancement after Cu intercalation has also been observed in Bi2Te3 nanoplates, as shown in Fig. 2f.
The behaviour of transmission enhancement is actually caused by combined optical and electronic effects. Below we provide experimental evidence that explains the mechanism of the anomalous reduction of absorption and formulate the light transmission through the nanoplates. The nanoplates’ ultra-small thicknesses, which are much less than the wavelength of light, lead to very unique optical reflectance responses.
Substantial reduction of absorption at optical frequencies can be attributed to an ultra-large Burstein–Moss shift of the bandgap caused by the large amount of free electrons introduced to the material via intercalation of Cu atoms. For degenerately doped semiconductors, increased free electron density will effectively elevate the Fermi level into the conduction band. Therefore, electrons from valence band cannot be excited to the bottom level of the conduction band, but the first unoccupied level above the Fermi level, that is, the effective bandgap has been increased, as shown in Fig. 3a. Compared with the degenerate doping (a few percent or less) of usual semiconductors, the Cu intercalation doping concentration (22%) in 2D materials is much more substantial. The Burstein–Moss shift is expected to be much larger in 2D nanoplates.
A substantial blue shift of plasma edge provided direct evidence of the increasing amount of free electron associated with Cu intercalation. The free electron effect on electrical permittivity can be described by the Drude model30.
where is the angular frequency of plasma oscillations, which is directly dependent on the free carrier concentration N, m* is the effective mass of electrons, ε∞ is the high-frequency dielectric constant and Γ is the damping constant of the free electron plasma. As the frequency of light decreases, real part of the permittivity decreases from positive to large negative values, which provides clear signatures in the reflection of the material. A minimum in reflection is expected close to where the permittivity switches sign from positive to negative31,32. It is then followed by a substantial increase in reflection. Such plasma edge behaviour is observed in the reflection spectra measured on Cu-intercalated Bi2Se3 ribbons, as shown in the reflection measurements in Fig. 3b. As more and more Cu atoms are intercalated, the plasma edge of the material moves toward shorter wavelengths, since the plasma frequency has a blue shift associated with the increasing concentration of free electrons. Our observation is also consistent with the finding that Cu atoms added to interstitial sites provide free electrons to Bi2Se3 system31.
The reflection measurement results can be fitted with the Drude model to obtain the concentration of free electrons in the materials (Supplementary Fig. 3), which yields an extremely high free electron concentration on the order of 1021 cm−3. It is a great advantage of the 2D material systems that a large number of foreign atoms can be added to the van der Waals gap without damaging the host crystal lattice.
Associated with the addition of a plethora of free electrons are the elevation of Fermi level and the increase of effective bandgap, which can be observed through absorption edge measurement. As shown in Fig. 3c, the effective bandgap gradually increases as more Cu atoms are intercalated. With 2-h intercalation of Cu, we observed that the effective optical bandgap has been widened to around 1.1 eV, which is substantial compared with the initial small gap around 0.3–0.5 eV. When the bandgap approaches higher energy scales, material absorption at optical frequencies is substantially decreased. First-principles simulations provide us evidence of the substantial Fermi level shift. As shown in the calculated electronic structure before and after intercalation (Fig. 3d), the Fermi level lies in the bandgap for intrinsic Bi2Se3, but gets deep into the conduction band with Cu intercalation. The calculated separation between Fermi level and the top of the valence band for intercalated samples reaches ~1 eV, consistent with our experimental observation. Unlike previous studies33,34 with small shifts in a very narrow energy range by regular doping, the ultra-large shift due to Cu intercalation here enables dramatic optical property change over a large wavelength range, thus makes such a material system suitable for applications that require substantial optical property tuning.
Figure 4a shows the refractive indices obtained from the experimental data. The transmission of light through the nanoplates has a direct dependence on their thicknesses; therefore the optical properties of the material can be calculated based on transmission data through nanoplates with different thicknesses. Substantial reduction of the imaginary parts of the material’s refractive index after Cu intercalation, as shown in Fig. 4a, indicates the decrease of light absorption. When such an optical property change happens to nanoplates and potentially ultra-thin films, it is further magnified by the interference effect, which is referred to as zero-wave anti-reflection effect here. Considering a light beam passing through a nanoplate with thickness d, it experiences multiple reflections at the top and bottom surfaces of the nanoplates (Fig. 4b). For normally incident light, the total transmitted light can be expressed as follows:
where Et is the electric field amplitude of the transmitted light, E0 is that of the incident light and k is the wavevector of light inside the nanoplate. t1 and t2 are the transmission coefficients at the first and second interface, respectively35.
r1 and r2 are the reflection coefficients at those interfaces.
where n1, n2 and n3 are the refractive indices of the substrate, nanoplate and air, respectively.
Unlike the widely used quarter-wave anti-reflection coatings for many optical devices, here reflections from top and bottom surfaces of bismuth chalcogenide nanoplates have different phase relations due to the refractive index with a non-zero imaginary part and a real part larger than the surrounding media. Figure 4c is a comparison between materials with different absorption capabilities. In the low-absorption case, r1 and r2 have opposite signs (π phase difference). Different orders of transmissions interfere constructively in the thin-film limit, as shown in equation (1). Reflection is suppressed. However, such anti-reflection interference will be damaged when strong absorption is present, because further phase shift is caused by the complex refractive index. The phase change of reflections at both interfaces can be obtained using equation (4), given the refractive indices at different wavelengths. The phase difference between r1 and r2 is away from π. Reflection may even be enhanced as shown in the right panel of Fig. 4c. Therefore, absorption reduction adjusts the phase shifts of the reflections and leads to a more constructive interference condition for optical transmissions through the nanoplates.
Substantial reduction in the imaginary part of the refractive index leads to two effects, both of which enhance the transmission of the nanoplates: the reduction of direct absorption and reflection phase shifts at both interfaces that helps the interferential anti-reflection effect as described above. The synergy of these two effects makes the Cu intercalation-induced transparency more substantial.
Such an optical transmission enhancement together with metallic Cu intercalation opens up exciting opportunities for applications such as transparent electrodes. Due to the ultra-high carrier density provided by the Cu intercalants, the Bismuth chalcogenide nanoplates also exhibit very good electrical conductivity even at small thicknesses. Sheet resistance before and after Cu intercalation was measured on single Bi2Se3 nanoplate devices, fabricated by using the standard e-beam lithography and thermally evaporated Cr/Au contacts. Figure 5a shows that contacts remain intact after intercalation and the plate colour changes. As shown in Fig. 5b, the sheet resistances decreased dramatically after intercalation by two to fivefolds. The improvement of both conductivity and transparency is desirable for transparent electrodes. Figure 5c provides the transmission-sheet resistance map of different samples. Materials with properties in the upper left corner of the map are good candidates for transparent electrodes. Our results suggest that Cu intercalation leads to both increased transparency and high conductance. Such a performance is potentially interesting for touch screen applications.
The mechanism described here does not have a strong dependence on the host material as long as carrier density can be greatly changed by metal intercalants. Therefore besides Bi2Se3 and Bi2Te3, similar behaviour may be found in various other 2D material systems through intercalation approaches. And it is particularly attractive to be able to manipulate the positions of the absorption edge and the plasma edge, by controlling the amount of Cu intercalated. In this way, we can flexibly tune the transmission band over a wide range of frequencies from visible to infrared. The high transmittance in infrared further extends the tuning range beyond the wavelength of 1.6 μm where existing transparent conducting oxide materials do not have a good transmittance. Moreover, as extensively studied in electrochemistry26, intercalation and deintercalation in 2D materials can be achieved by electrochemical methods; therefore dynamic tuning of optical properties in a large scale is possible. For example, electrochemical control of photoluminescence in 2D MoS2 nano flakes based on intercalation and deintercalation processes have been studied recently36.
The 2D-layered structure of bismuth chalcogenide materials enables the formation of ultra-thin flat plate and intercalation of large amount of metal atoms. By intercalating Cu atoms into Bi2Se3 and Bi2Te3 nanoplates, we are able to tune the optical and electrical behaviour of such materials. Synergetic effect from chemical tuning and zero-wave anti-reflection leads to substantial optical transmission improvement in those nanoplates, together with enhanced electrical conductivity. The great potential in tuning the physical and chemical properties of such materials will lead to various applications including transparent electrodes, tunable optoelectronic devices.
Solvothermal synthesis of bismuth selenide nanoplates
High-purity polyvinylpyrrolidone (PVP) was first dissolved in ethylene glycol. A mixture of Bi2O3 powder, selenium powder and ethylenediamine tetraacetic acid (EDTA) powder was added to the solution and thoroughly stirred to form a suspension. The suspension was then sealed in a steel autoclave and kept at a temperature in the range of 180–220 °C for 24 h. The lateral dimension of the single-crystalline products was observed to be up to a few tens of micrometres and their thicknesses were typically several to a few tens of nanometres.
Vapour phase growth of bismuth telluride nanoplates
A purity of 99.999% Bi2Te3 powder was heated up in a tube furnace to around 500 °C and transformed to vapour phase. Ar gas flow was applied to the vacuum tube furnace and carried the Bi2Te3 vapour to the end of the furnace where a substrate was placed. As the temperature around the end of the furnace was much lower than the centre part, the molecules in the vapour started to deposit on the substrate and formed ultra-thin triangular or hexagonal nanoplates. Quartz substrate was used to allow the measurement of the transparency of Bi2Te3 nanoplates.
Intercalation of Cu into Bi2Se3 and Bi2Te3 nanoplates
For the consistency of optical measurements, nanoplates were first drop-casted on a glass slide. After drying, they were added into a mixture of 5 ml butanol with 3 mg Tetrakis(acetonitrile)Cu (i) Hexafluorophosphate ([Cu(CH3CN)4]PF6) from Sigma-Aldrich and heated to around 55 °C (ref. 27). The amount of Cu intercalated is controlled by the reaction time.
Nanoplate optical transmission and reflection measurements
Bi2Se3 nanoplate suspension was first drop-casted on glass substrate and their optical transmissions were measured using a Nikon C1 confocal microscope. The spectra were analysed using the Princeton Instruments Acton SpectraPro 2300i spectrograph and Pixis 1024 Si CCD detector. Reflection spectra were measured using Bruker Hyperion 2000 infrared microscope and IFS-125/HR Fourier transform infrared spectrometer.
First-principles density functional theory calculations are performed to obtain the electronic band structure of the undoped Bi2Se3 and the Cu-intercalated Bi2Se3 for both bulk (Fig. 3d) and a few quintuple layer cases (Supplementary Figs 4,5). We use the Hohenberg–Kohn density functional theory with the generalized-gradient approximation and the projector augmented-wave method as implemented in Vienna Ab initio Simulation Package (VASP). Intercalated Cu atoms are at the tetrahedral sites in the van der Waals gap of Bi2Se3, which lead to the lowest energy configuration. Spin-orbit coupling effect is included in the band structure calculations. The band structures are plotted along the high-symmetry directions K-Γ-M in the reciprocal space of the hexagonal lattice.
How to cite this article: Yao, J. et al. Optical transmission enhacement through chemically tuned two-dimensional bismuth chalcogenide nanoplates. Nat. Commun. 5:5670 doi: 10.1038/ncomms6670 (2014).
Novoselov, K. S. et al. Electric field effect in atomically thin carbon films. Science 306, 666–669 (2004).
Zhang, Y., Tan, Y.-W., Stormer, H. L. & Kim, P. Experimental observation of the quantum Hall effect and Berry’s phase in graphene. Nature 438, 201–204 (2005).
Wang, F. et al. Gate-variable optical transitions in graphene. Science 320, 206–209 (2008).
Chen, C.-F. et al. Controlling inelastic light scattering quantum pathways in graphene. Nature 471, 617–620 (2011).
Seol, J. H. et al. Two-dimensional phonon transport in supported graphene. Science 328, 213–216 (2010).
Chen, S. et al. Thermal conductivity of isotopically modified graphene. Nat. Mater. 11, 203–207 (2012).
Pacile, D., Meyer, J. C., Girit, C. O. & Zettl, A. The two-dimensional phase of boron nitride: few-atomic-layer sheets and suspended membranes. Appl. Phys. Lett. 92, 133107 (2008).
Kobayashi, Y., Kumakura, K., Akasaka, T. & Makimoto, T. Layered boron nitride as a release layer for mechanical transfer of GaN-based devices. Nature 484, 223–227 (2012).
Wilson, J. A. & Yoffe, A. D. The transition metal dichalcogenides discussion and interpretation of the observed optical, electrical and structural properties. Adv. Phys. 18, 193–335 (2012).
Marseglia, E. A. Transition metal dichalcogenides and their intercalates. Int. Rev. Phys. Chem. 3, 177–216 (2012).
Oriakhi, C. O. & Lerner, M. M. inHandbook of Layered Materials (eds Auerbach S. M., Carrado K. A., Dutta P. K. CRC Press (2004).
Coleman, J. N. et al. Two-dimensional nanosheets produced by liquid exfoliation of layered materials. Science 331, 568–571 (2011).
Tenne, R. Inorganic nanotubes and fullerene-like nanoparticles. Nat. Nanotechnol. 1, 103–111 (2006).
Zhang, H. et al. Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface. Nat. Phys. 5, 438–442 (2009).
Chen, Y. L. et al. Experimental realization of a three-dimensional topological insulator, Bi2Te3 . Science 325, 178–181 (2009).
Zhang, Y. et al. Crossover of the three-dimensional topological insulator Bi2Se3 to the two-dimensional limit. Nat. Phys. 6, 584–588 (2010).
Peng, H. et al. Aharonov-Bohm interference in topological insulator nanoribbons. Nat. Mater. 9, 225–229 (2010).
Radisavljevic, B., Radenovic, A., Brivio, J., Giacometti, V. & Kis, A. Single-layer MoS2 transistors. Nat. Nanotechnol. 6, 147–150 (2011).
Mak, K. F., He, K., Shan, J. & Heinz, T. F. Control of valley polarization in monolayer MoS2 by optical helicity. Nat. Nanotechnol. 7, 494–498 (2012).
Peng, H. et al. Topological insulator nanostructures for near-infrared transparent flexible electrodes. Nat. Chem. 4, 281–286 (2012).
Ioffe, A. F. Semiconductor Thermoelements and Thermoelectric Cooling Infosearch (1957).
Goldsmid, H. J. Thermoelectric Refrigeration Plenum Press (1964).
Mishra, S. K., Satpathy, S. & Jepsen, O. Electronic structure and thermoelectric properties of bismuth telluride and bismuth selenide. J. Phys. Condens. Mat. 9, 461–470 (1997).
Hor, Y. S. et al. Superconductivity in CuxBi2Se3 and its implications for pairing in the undoped topological insulator. Phys. Rev. Lett. 104, 057001 (2010).
Kong, D. et al. Few-layer nanoplates of Bi2Se3 and Bi2Te3 with highly tunable chemical potential. Nano Lett. 10, 2245–2250 (2012).
Whittingham, M. S. Electrical energy storage and intercalation chemistry. Science 192, 1126–1127 (1976).
Koski, K. J. et al. High-density chemical intercalation of zero-valent copper into Bi2Se3 nanoribbons. J. Am. Chem. Soc. 134, 7584–7587 (2012).
Koski, K. J. et al. Chemical intercalation of zero-valent metals into 2D layered Bi2Se3 nanoribbons. J. Am. Chem. Soc. 134, 13773–13779 (2012).
Kong, D., Koski, K. J., Cha, J. J., Hong, S. S. & Cui, Y. Ambipolar field effect in Sb-doped Bi2Se3 nanoplates by solvothermal synthesis. Nano Lett. 13, 632–636 (2013).
Ashcroft, N. W. & Mermin, N. D. Solid State Physics Brooks Cole (1976).
Vaško, A., Tichý, L., Horák, J. & Weissenstein, J. Amphoteric nature of copper impurities in Bi2Se3 crystals. Appl. Phys. A 5, 217–221 (1974).
Tichý, L. & Horák, J. Nonparabolicity of the conduction band and anisotropy of the electron effective mass in n-Bi2Se3 single crystals. Phys. Rev. B 19, 1126–1131 (1979).
Burstein, E. Anomalous optical absorption limit in InSb. Phys. Rev. 93, 632–633 (1954).
Deppe, D. G., Gerrard, N. D., Pinzone, C. J., Dupuis, R. D. & Schubert, E. F. Quarter-wave Bragg reflector stack of InP-In0.53Ga0.47As for 1.65 mu m wavelength. Appl. Phys. Lett. 56, 315–317 (1990).
Jackson, J. D. Classical Electrodynamics Wiley (1998).
Wang, Y. et al. Electrochemical control of photoluminescence in 2DMoS2 nanoflakes. ACS Nano 7, 10083–10093 (2013).
Y.C. acknowledges the support by the Department of Energy, Office of Basic Energy Sciences, Materials Sciences and Engineering Division, under contract DE-AC02-76-SFO0515.
The authors declare no competing financial interests.
About this article
Cite this article
Yao, J., Koski, K., Luo, W. et al. Optical transmission enhacement through chemically tuned two-dimensional bismuth chalcogenide nanoplates. Nat Commun 5, 5670 (2014). https://doi.org/10.1038/ncomms6670
This article is cited by
Nature Reviews Materials (2022)
Intercalation as a versatile tool for fabrication, property tuning, and phase transitions in 2D materials
npj 2D Materials and Applications (2021)
Recent progress on in situ characterizations of electrochemically intercalated transition metal dichalcogenides
Nano Research (2019)
Nature Communications (2018)