Various band structure engineering methods have been studied to improve the performance of graphitic transparent conductors; however, none has demonstrated an increase of optical transmittance in the visible range. Here we measure in situ optical transmittance spectra and electrical transport properties of ultrathin graphite (3–60 graphene layers) simultaneously during electrochemical lithiation/delithiation. On intercalation, we observe an increase of both optical transmittance (up to twofold) and electrical conductivity (up to two orders of magnitude), strikingly different from other materials. Transmission as high as 91.7% with a sheet resistance of 3.0 Ω per square is achieved for 19-layer LiC6, which corresponds to a figure of merit σdc/σopt=1,400, significantly higher than any other continuous transparent electrodes. The unconventional modification of ultrathin graphite optoelectronic properties is explained by the suppression of interband optical transitions and a small intraband Drude conductivity near the interband edge. Our techniques enable investigation of other aspects of intercalation in nanostructures.
Two-dimensional (2D) graphene has attracted much interest in fundamental research and technological development due to its extraordinary electrical, mechanical, thermal and optical properties1,2,3,4,5,6. Recently, graphitic films (from monolayer graphene to ultrathin graphite) have been explored as candidates for flexible transparent electrodes for electronics and optoelectronics7,8. An excellent performance of 30 Ω per sq at 90% transmittance has been achieved using doped four-layer chemical-vapour deposition (CVD) graphene9. Bulk materials with 2D-layered structures such as graphite have also been studied and used extensively for electrochemical energy storage based on intercalation10,11,12. Fundamental studies on intercalation in graphite have been extensively carried out13, and nanostructured 2D materials have recently gained much interest14. Reports on the intercalation of various species such as FeCl3 (refs 15, 16), Br17 and Ca18 in few-layer graphene (FLG) have offered a new route to designing and synthesizing graphene-based materials with novel conductive, magnetic or superconductive properties.
It has long been known that the optical transmission of graphite increases on metallization by intercalation with, for example, caesium19. This unusual property results from the unique band structure of the graphene layer; intercalation heavily dopes ultrathin graphite, shifting the Fermi level upward more than any other band engineering method15,19,20,21,22,23,24, suppressing interband optical transitions due to Pauli blocking thus increasing transmittance of light in the visible range. The increase in optical transmittance is expected to be accompanied by an increase in conductivity since the carrier concentration increases on intercalation, an ideal situation for conductive transparent films. All studies to date of doped graphene films as transparent electrodes, however, do not report increased transmission in the visible range. It also has been assumed by some researchers that the transmission of ultrathin graphite can never exceed that of undoped graphene of similar layer numbers25. Moreover, no studies of electrical conductivity and optical transmission have been carried out for lithium-intercalated ultrathin graphite.
Here, we use in situ electronic and optical measurements to understand the electrochemical intercalation process and simultaneously measure the electrical conductivity and optical transmission of exfoliated ultrathin graphite crystallites ranging from 3–60 graphene layers in thickness. On intercalation, we observe a large improvement in the optical transmittance, and at the same time a dramatic increase of sheet conductivity. The Dirac electronic band structure allows for very low electron phonon resistivity even at relatively low carrier concentration26, hence high DC conductivity is achieved with low optical conductivity below the visible range. In addition to elucidating the limits of conductivity and transparency in ultrathin graphite, we expect that the experimental techniques developed here will be broadly useful for studying the intercalation dynamics and correlated optoelectronic properties of other 2D nanomaterials that can be intercalated electrochemically.
Devices for optoelectronic and transport measurements
To simultaneously study the electrical and optical properties of Li-intercalated ultrathin graphite, we design a sandwich-structured cell with electrolyte (1 M LiPF6 in w/w=1/1 ethylene carbonate/diethyl carbonate) that is sealed by bottom and top layers of thin transparent glass. Ultrathin graphite and the lithium source are deposited on the bottom glass layer and connected to separate electrical contacts. Two types of devices are fabricated for our optoelectronic (Fig. 1a–c) and electrical transport (Fig. 1d–f) measurement. Details of the device fabrication are given in the Methods section. In this planar nanoscale half-cell battery (planar nanobattery), Li metal is used as the counter electrode and ultrathin graphite as the working electrode. The intercalation process is controlled by a BioLogic SP-150 electrochemical workstation and the voltage of the planar nanobattery can be measured simultaneously during the electrochemical Li intercalation (Supplementary Fig. 1). The thickness of the ultrathin graphite is determined by an atomic force microscope before cell capsulation.
In situ optoelectronic measurement
The transmittance at a particular wavelength of pristine and Li-intercalated ultrathin graphite can be characterized by analysing the grey-scale images acquired by transmission optical microscopy (Nikon Eclipse Ti-U) using a broadband light source (Thermo Oriel), a monochromator (Spex 500 M), and a charge-coupled device (CCD) camera. A schematic of the in situ transmittance measurement system is shown in Fig. 2a (also see Methods). A series of optical images (550 nm illumination) corresponding to different intercalation stages are shown in Fig. 2d–i, along with a schematic of the lattice structure of LiC6 (Fig. 2h). A clear increase in the transmittance on intercalation can be seen from Fig. 2e–g (also see Supplementary Fig. 2 and Supplementary Movie 1), as discussed below in detail. Furthermore, the optical transmittance change is highly reversible, as shown in Fig. 2i (also see Supplementary Fig. 3).
Our transparent planar nanobattery setup also allows further characterization using Raman microscopy. As shown in Fig. 2j, we examined a series of in situ Raman spectra (Horiba Jobin Yvon with a 633 nm He-Ne laser source), which correspond to different stages of Li-graphite intercalation, with more details discussed in the Supplementary Methods II (Supplementary Fig. 4). The result from our ultrathin graphite samples agrees well with previous studies of bulk samples27, confirming Raman microscopy as one of the tools for differentiating lithiation stages in ultrathin graphite.
We also observed an in situ transmittance change of Li-intercalated ultrathin graphite at different LixC stages by charging the Li-graphite nano-batteries (Fig. 3a), with a constant charging current. The black line represents a typical voltage profile of the Li-graphite nanobattery and the red, green, blue open circles depict the transmittance evolution of ultrathin graphite sheets (dotted regions in the inset of Fig. 3a) with different thicknesses during Li-graphite intercalation. The voltage initially drops rapidly with time until it reaches 0.8 V, where an obvious slope change in the voltage profile is observed. This is due to the decomposition of the electrolyte and a solid electrolyte interphase formation11,27. No obvious change in the transmittance of the ultrathin graphite samples is observed for voltages greater than 0.2 V. A sudden increase in the transmittance (18-layer graphite from 74.4 to 77.2%, 38-layer graphite from 55.9 to 59.2%) occurs after 0.2 V, which we identify with the formation of LiC36 (stage IV)28 from ultrathin graphite sheets. From 0.2 to 0.1 V, a gradual change in the transmittance is observed, presumably due to the formation of LiC27 and LiC18 (ref. 28). As time increases, a second plateau appears in the voltage at ~0.1 V, which we identify with the formation of LiC12 (stage II). At the end of the 0.1 V plateau, we expect that the entire sample has been converted to LiC12, and the transmittance dramatically increased to 85.8% (18-layer) and 71.9% (38-layer). A third voltage plateau appears at a value of ~0.05 V, indicating the formation of LiC6 (stage I). At this stage, the transmittance of the 18-layer sample has increased to 90.9%, and the 38-layer sample has increased to 79.2%. Only two distinct stages are observed for the three-layer sample (from 94.5 to 95.2%, and finally 97.7%), consistent with the fact that there are only two interstitial galleries and hence only stage I and stage II are meaningfully defined. Figure 3b shows the low potential region of the potential versus time trace in which the distinct potential plateaus can be seen more clearly.
The changes in optical transmission in our planar nanobattery allow a direct observation of the lithiation process on an individual ultrathin graphite sheet with excellent spatial and temporal resolution. As shown in Fig. 3c–g, a clear lithiated (LiC36) and dilute stage (LiC72) interface (that is, a lithiation front) is observed within 100 s, and the lithiated area becomes more transparent and the LiC36 area increases linearly with time (Fig. 3h). This agrees well with our electrochemical testing scheme with a constant current charge/discharge process. Thus, our integrated system provides a powerful tool to investigate the intrinsic lithiation kinetics in the two-phase reaction at the nanoscale29.
Thickness and wavelength dependence
We next consider the layer number and wavelength dependence of the in situ optical transmission of individual ultrathin graphite sheets. In Fig. 4a–c, the wavelength dependence of the transmittance is shown in the visible range from 400 to 800 nm for samples of various thicknesses. For pristine ultrathin graphite (Fig. 4a), the transmittance is weakly dependent on the wavelength, consistent with previous reports6; the absorption by ultrathin graphite is approximately Nπα (πα=2.3%), where α is the fine structure constant and N the number of graphene layers. This absorption results from interband transitions in the Dirac spectrum of graphene, which give a nearly constant optical conductivity σ≈πe2/2h where e is the elemental charge and h Planck’s constant. For LiC12 stage (Fig. 4b), the transmittance depends more strongly on wavelength, increasing the most for longest wavelengths. For the LiC6 stage (Fig. 4c), the wavelength-dependent transmittance shows a maximum around 500 nm, and the transmittance of LiC6 is still higher compared with pristine ultrathin graphite. Interestingly, the transmittance of LiC6 still increases compared with LiC12 for wavelengths well below the maximum, while above the transmittance maximum the LiC6 transmittance decreases compared with LiC12.
Figures 4d,e show the optical transmittance for pristine and intercalated ultrathin graphite sheets as a function of layer number. For both 550 and 800 nm, a clear increase of the optical transmittance is seen after intercalation, both for LiC12 and LiC6. For 550 nm wavelength (Fig. 4d), the transmittance increases monotonically with Li concentration; for LiC6 versus pristine ultrathin graphite, the transmittance increase can be as high as 55% (for a sample of 60–80 layers). For 800 nm wavelength (Fig. 4e), the transmittance for all measured thicknesses first increases (LiC12) and then decreases (LiC6); for LiC12 versus pristine ultrathin graphite, the transmittance has an increase up to twofold (for a sample more than 100 layers). We also observed that in thicker sheets (insets of Fig. 4d,e), the transmittance of LiC6 increases less and starts to approach the value of its pristine state at both wavelengths of 550 and 800 nm, that is, at 550 nm for 90-layer thickness the transmittance at LiC6 state starts to approach the value of LiC12 state and approaches the value of pristine state at about 150 layers, and for 800 nm wavelength the transmittance of LiC6 becomes lower than the value of pristine state with layer number greater than 60. In situ optical measurements in reflective mode are also shown in Supplementary Fig. 5, further confirming the wavelength-dependent optical properties of lithiated ultrathin graphite.
Drude and interband contribution
The changes in optical transmittance in the visible range described above can be qualitatively understood as follows. The result of the Li intercalation is electron doping due to the low electrochemical potential of Li metal. As shown in Fig. 4f, intercalation of Li heavily dopes the ultrathin graphite, shifting up the Fermi level. The magnitude of Fermi level shift is associated with the carrier density, which increases monotonically with lithium concentration. The doping concentration is as high as ~6 × 1014 cm−2 per layer for LiC6, corresponding to EF≈1.5 eV30, higher than the highest doping that can be achieved in graphene with electrolytic gating24. The increase in Fermi energy leads to the suppression of interband optical transitions for photon energies ω<2EF, thus decreasing the optical conductivity and increasing the transmission. As doping increases, however, intraband (Drude) conductivity becomes important, decreasing the transmission for ħω<ħ/τ (where τ is the carrier relaxation time) due to the electron–longitudinal optical (LO) phonon interaction. Thus, we expect that the transmission of ultrathin graphite is enhanced with doping for a window of photon energies ħ/τ<ħω<2EF.
This phenomenon has been observed previously in gated monolayer and FLG samples, where doping levels were much lower than explored here and the window occurred in the infrared31. A decrease in the absorption coefficient is also observed in graphite intercalation compounds by Hennig et al.19 In Li-intercalated graphite, the window manifests as a minimum in reflectivity occurring near 740 nm for bulk LiC12 and 440 nm for bulk LiC6 (ref. 32). The reflectivity minimum previously observed for bulk LiC6 corresponds reasonably well to our observation of a transmission maximum near 500 nm (Fig. 4c). For LiC12, the transmission maximum may occur at a longer wavelength than our experiment accesses, and we observe only an enhancement of long-wavelength transmission. Thus, we conclude that the overall reduction in interband transitions by Pauli blocking is responsible for the transmission increase, and the higher Drude conductivity of more strongly doped LiC6 is responsible for the observed reduction in transmission at long wavelength and the non-monotonic doping dependence of transmission at these wavelengths.
Further insight into these results is gained by examining the optical transmittance in terms of the optical conductivity. On a substrate with refractive index n, the transmittance of ultrathin graphite with optical (sheet) conductivity σopt=σ1+iσ2, relative to that of the bare substrate, can be expressed as33:
where Z0 is the free space impedance. Li et al.31 and Stauber et al.34 reported the optical conductivities of doped monolayer graphene in the IR range. For ħω<2EF, that is, below the Pauli blocking edge, σ1>>σ2; σ1 is large due to LO phonon emission and σ2 passes through zero near the plasma edge (ε1=0; also see the Supplementary Methods IV) so that the transmission reaches a maximum. Therefore, near the transmission maximum, σopt~σ1.
We then modelled the optical transmittance based on optical conductivity with a Drude contribution from the free carriers and an interband contribution that turns on for ħω>2EF due to Pauli unblocking, that is, σopt(ω)=σD+σib. The conductivity is modelled as N layers of graphene. The Drude sheet conductivity can be written as2 , where n2D is the carrier density per layer, m the effective mass, γ=1/τ is the carrier relaxation rate, and N is the number of layers. The thermal broadening of the Pauli blocking leads to35 , and the imaginary part of σib is obtained from Kramers–Kronig relation. The details of the modelling are presented in the Supplementary Methods IV. Figure 4g shows a schematic of σ1/Nσ0 versus the photon energy from the model for N-layer ultrathin graphite before and after Li intercalation. σ1 in the visible range significantly decreases on Li intercalation, which leads to a large increase in the optical transmittance. The modelled transmittances of both 8-layer and 83-layer ultrathin graphite (Fig. 4h, solid curves) closely resemble the corresponding experimental data, and the sharpening of the transmission maximum for thicker films is a consequence of the plasma edge as discussed in the Supplementary Methods IV (Supplementary Fig. 6).
In order to understand the prospects for highly transparent Li-intercalated ultrathin graphite for conducting transparent electrode applications, we adapted our planar nanobattery setup for in situ conductivity measurements of ultrathin graphite during electrochemical cycling. We transferred ultrathin graphite onto predeposited electrical contacts in a Hall-bar arrangement (Fig. 5a inset, see also Supplementary Figs 7–9). Figure 5a shows the room temperature sheet resistance Rs for ultrathin graphite samples with different thickness before intercalation as well as intercalated to LiC12 and LiC6. As expected, all intercalated ultrathin graphite samples invariably exhibit a lower resistivity compared with their pristine state (also see Supplementary Fig. 10). Note that RS measured on both stage I and II is inversely proportional to the sample thickness (before intercalation) as indicated by the dashed lines. Considering the expansion of the graphite-layer spacing during Li intercalation36, we can estimate that ρ(LiC6)~3.1 × 10−6 and ρ(LiC12)~1.4 × 10−5 Ω cm−1. The intrinsic limit of the conductivity for doped graphene at room temperature is set by electron–acoustic phonon scattering and is approximately σdc,phonon=33 mS per layer26,37 for Fermi energies in the linear portion of the band structure, while we observe a DC sheet conductivity σdc≈11 mS per layer in LiC6. At the high doping levels present in LiC6, we expect significant band curvature and reduction in the Fermi velocity, likely reducing the limiting conductivity. In addition, disorder may play a role. Thus, our approach within a factor of ~3 to the limiting conductivity value for the graphene Dirac band is impressive.
In order to elucidate the type and density of charge carriers, we investigated the Hall resistance at perpendicular magnetic fields. The linear Rxy (B) curves with negative slope (Fig. 5b) indicate that charge carriers are electrons for a 4-nm thick FLG device after Li intercalation. The carrier density nH is readily determined by a measurement of the Hall coefficient RH=Rxy/B, where RH is related to nH by nH=1/eRH. With the information of expanded thickness of Li-intercalated ultrathin graphite, our measurements reveal that bulk nH ranges from 3 × 1021 to 7 × 1021 cm−3 for LiC12 and from 1.5 × 1022 to 3.5 × 1022 cm−3 for LiC6, with no observable dependence on sample thickness, as shown in Fig. 5c. These values compare reasonably well with the full ionization values of 1.7 × 1022 cm−3 for LiC6 and 9.0 × 1021 cm−3 for LiC12, which are indicated in Fig. 5c as guidelines. Figure 5d shows the temperature dependence of the sheet resistance. Rs(T) is metallic, that is, RS decreases with decreasing T, for samples at LiC6 state, while LiC12 exhibits a moderate temperature dependence, and pristine samples always exhibited weakly non-metallic behaviour consistent with previous studies3. The strong decrease in RS with lowering T for LiC6 is consistent with phonon-limited conduction and further corroborates that we have approached the phonon-limited conductivity in Li-intercalated ultrathin graphite21.
Transparent electrode performance
In the race to find better transparent electrodes, researchers have investigated numerous candidate materials25,38,39,40,41. Figure 6a shows the transmittance versus sheet resistance of Li-intercalated ultrathin graphite as well as other high-performance transparent conducting materials, including other carbon-based materials15,42, and the best commercial indium tin oxide electrodes40,43. In previous doped graphene studies, an improvement in the electrical conductivity was observed; however, little or no change of transmittance in the visible range was obtained9,15. When σ1>>σ2 and n=1, to compare the performance of a freestanding film in vacuum, Equation (1) becomes:
where the sheet resistance is Rs=1/σdc. Thus, at a given sheet resistance, the transmission is determined by the ratio σdc/σopt, which can be used as the Figure of Merit (FOM) to characterize the performance of a transparent conductor.
As shown in Fig. 6a, we fit the data for our Li-intercalated FLG devices to Equation (1) using σdc/σopt as a fitting parameter, and fitting result gives σdc/σopt=920 (fitting details also see Supplementary Figs 11 and 12). For the best sample at LiC6 state, we measured transmittance of 91.7% and 3.0 Ω per sq, obtaining σdc/σopt=1400. Figure 6b shows the best measured σdc/σopt for the material systems shown in Fig. 6a; σdc/σopt for our LiC6 exceeds that of FeCl3-intercalated FLG (σdc/σopt=235)15 and the best commercial transparent electrode indium tin oxide (σdc/σopt=118)40. In fact, σdc/σopt of few-layer LiC6 exceeds that for all other carbon-based materials, and as far as we can determine, it is the highest for any uniform thin film. Higher transparency at a given conductivity has only been achieved in inhomogenous conductors such as metal nanowire networks44, which may not be suitable for many applications. It also exceeds the intrinsic limit for doped graphene9,25,38 previously expected ignoring the increased transparency due to Pauli blocking. The sheet resistance and transparency easily meet the need for optoelectronic device applications where 90% and 10 Ω per sq is required. Thus, we expect that electrochemically intercalated FLG is promising for applications where the highest DC conductivity at a given optical transparency is needed.
To demonstrate the feasibility of ultrathin graphite as transparent electrode for industrial applications, we successfully fabricated stable millimeter-scale devices using encapsulated commercially obtained CVD-grown thin graphite (see Methods and Supplementary Fig. 13). Comparison of two 40- and 80-nm thick devices before and after Li intercalation are shown in Fig. 7a,b. Transmittance spectra are also characterized before and after Li intercalation, as shown in Fig. 7c, which are very similar to the results of single exfoliated ultrathin graphite sheets. Changes in the sheet resistance was also measured for 40-nm-thick devices by the Van der Pauw method (see Supplementary Fig. 14). The sheet resistances of three different devices dropped drastically on complete lithiation from 35.4, 47.7, 57.0 Ω per sq (graphite) to 3.0, 3.9, 1.7 Ω per sq (LiC6), respectively. The 1.7 Ω per sq correspond to a single layer sheet resistance of 200 Ω per sq, only 2.3 times larger than the single flake value (87.3 Ω per sq) from our experiment, leads to a FOM of 400.
We discuss the ultimate limits to conductivity and transparency of doped graphene-based systems. Previous studies25 of graphene as a transparent conductor have ignored changes in the optical conductivity, assuming it remains limited by interband transitions and is fixed at σopt=σib≈Nπe2/2h=Nσ0, with N the number of layers, as discussed above. For phonon-limited conduction at room temperature, σdc=Nσdc,phonon where. σdc,phonon=33 mS26,37. This predicts a maximum value of σdc/σopt≈550, while our intercalated ultrathin graphite significantly exceeds this value. However, as noted previously, below the Pauli blocking edge σopt is the free carrier Drude conductivity that can be smaller than σib. Optical measurements on doped monolayer graphene gives f≡σ1/σ0≈0.3 below the interband edge for EF≈0.3 eV31. Assuming this value of f implies σdc/σopt≈1,800 in reasonable agreement with our best observation; however, there are no experimental results on the magnitude of σ1 and hence f for the EF≈1.5 eV conditions of our intercalated graphene. Theory predicts that the Drude optical conductivity for frequencies above the LO phonon frequency is limited by the electron–LO phonon relaxation rate, γ=1/τLO (ref. 34). At the higher EF of our experiments, the electron phonon scattering rate will be stronger because of the larger electronic density of states (~EF), but the high frequency Drude conductivity falls off as σ1~EF γ/(γ2+ω2)~EF γ/ω2. This suggests that σ1 and hence f at ω≤2EF are approximately independent of EF so that f≡σ1/σ0≈0.3 may also be valid at EF ≈1.5 eV, and our estimate of the intrinsic limit of σdc/σopt≈1,800 is reasonable. Thus, we believe that our real devices approach the ultimate limits of transparency at a given conductivity for the doped graphene system.
In summary, we have designed a methodology via a planar nanobattery for in situ study of the electrical and optical properties of individual ultrathin graphite sheets during electrochemical intercalation and deintercalation. Metallic-like temperature-dependent transport is observed in Li-intercalated ultrathin graphite with conductivities approaching the acoustic phonon limit at room temperature and is comparable to good metals. Due to the unusual band structure of graphene, Li intercalation can simultaneously increase the DC electrical conductivity and increase optical transmission in the visible, allowing Li-intercalated FLG to achieve an unprecedented FOM σdc/σopt=920, significantly higher than any other material and approaching the ultimate limit expected for doped graphene systems. Our technique will allow similar studies to be carried out in other 2D materials. Furthermore, the methodology reported in this study can be applied to in situ investigations of the intercalation process with good spatial and temporal resolution in materials for electrochemical energy storage applications.
Device fabrication for electrochemical/optical measurements
Pristine ultrathin graphite sheets from monolayer to 50 nm (~150 layers) are first obtained by mechanical exfoliation of Kish graphite onto 0.2 mm thick glass substrates (Fisher Scientific), followed by deposition of electrical contacts (50 nm copper) on top of the selected ultrathin graphite sheets using a shadow mask technique in electron beam evaporator. The device is then transferred into a glove box filled with argon gas, and a small lithium pellet is deposited onto an isolated electrical contact, followed by the addition of a small amount of electrolyte (LiPF6 in EC:DEC w-w=1:1) to cover the region with both ultrathin graphite and lithium pellet. At last, the centre region with electrolyte/lithium/ultrathin graphite is covered by another piece of 0.2 mm thick glass and sealed by polydimethylsiloxane, as shown in Fig. 1c.
Device fabrication for electrical transport measurements
During the Li intercalation process, the volume of ultrathin graphite gradually expands because of the insertion of lithium atoms. The layer spacing of LiC6 is ~10% larger than that of pristine graphite36. Therefore, the narrow metal electrodes fabricated by the normal method of thermal evaporation on top of ultrathin graphite usually crack after intercalation. Here, we use a lithography-free fabrication method shown in Fig. 1d–f. The 50-nm thick copper Hall-bar/lithium-contact electrodes are prepatterned on a blank glass wafer. A uniform exfoliated ultrathin graphite sheet is then transferred onto the top of the electrodes aligned by a micromanipulator. The rest of the device fabrication is the same as described above. Using this method, ultrathin graphite sheets are attached to the top of the electrodes and can expand freely during Li intercalation.
Fabrication of large-scale CVD graphene devices
CVD ultrathin graphite on nickel foil (2″ × 2″) is obtained from Graphene Supermarket and cut into 1.5 × 1.5 cm pieces. A solution based (1 M FeCl3 in deionized water as etchant, Sigma Aldrich) etching/transfer method is then carried out to transfer ultrathin graphite onto transparent substrates (for example, glass and polyethylene terephthalate). A gel electrolyte film is prepared by mixing P (VDF-HFP)/Acetone/deionized water (w:w:w=1:19:1, Sigma Aldrich) as a mixed solution. The electrolyte is then drop-cast on glass and ready for use after drying in a vacuum oven (MTI Corp.). A sandwiched device structure of glass/ultrathin graphite/gel electrolyte/polyethylene terephthalate is assembled in an argon-filled glove box. The transmittance of the device is measured by a UV–vis spectrometer (PerkinElmer Lambda 35).
In situ optical transmission measurements
A system based on a transmission optical microscope (Nikon Eclipse Ti-U) combined with a CCD camera is used to acquire transmission data. Microscope objectives with × 5 and × 20 magnification are used depending on the size of the sample. A beam of light at particular wavelength from a monochromator (Spex 500 M, 0.2 nm bandwidth) passes through the transmission optical microscope and is then projected onto the 1,392 × 1,040 lines of the grey CCD camera. Intensity is then extracted from images taken by CCD camera and is normalized to the signal obtained through a region of bare substrate close to the sample to give the transmission at that wavelength. Such analysis results in a weak overestimate of transmittance for ultrathin graphite embedded in an electrolyte solution; however, if we focus on the highly transparent samples (more than 90%), the difference is negligible (~1%).
An electrochemical workstation (Biologic SP-150) is used to control charge/discharge of the Li-ultrathin graphite nanobattery and measure the time-dependent potential on intercalation (lithiation) and deintercalation (delithiation). Details are also discussed in Supplementary Methods I.
How to cite this article: Bao, W. et al. Approaching the limits of transparency and conductivity in graphitic materials through lithium intercalation. Nat. Commun. 5:4224 doi: 10.1038/ncomms5224 (2014).
Geim, A. K. & Novoselov, K. S. The rise of graphene. Nat. Mater. 6, 183–191 (2007).
Castro Neto, A. H., Guinea, F., Peres, N. M. R., Novoselov, K. S. & Geim, A. K. The electronic properties of graphene. Rev. Mod. Phys. 81, 109–162 (2009).
Das Sarma, S., Adam, S., Hwang, E. H. & Rossi, E. Electronic transport in two-dimensional graphene. Rev. Mod. Phys. 83, 407–470 (2011).
Lee, C., Wei, X., Kysar, J. W. & Hone, J. Measurement of the elastic properties and intrinsic strength of monolayer graphene. Science 321, 385–388 (2008).
Balandin, A. A. Thermal properties of graphene and nanostructured carbon materials. Nat. Mater. 10, 569–581 (2011).
Mak, K. F., Ju, L., Wang, F. & Heinz, T. F. Optical spectroscopy of graphene: from the far infrared to the ultraviolet. Solid State Commun. 152, 1341–1349 (2012).
Bonaccorso, F., Sun, Z., Hasan, T. & Ferrari, A. C. Graphene photonics and optoelectronics. Nat. Photon. 4, 611–622 (2010).
Kim, K. S. et al. Large-scale pattern growth of graphene films for stretchable transparent electrodes. Nature 457, 706–710 (2009).
Bae, S. et al. Roll-to-roll production of 30-inch graphene films for transparent electrodes. Nat. Nano 5, 574–578 (2010).
Whittingham, M. S. The Role of ternary phases in cathode reactions. J. Electrochem. Soc. 123, 315–320 (1976).
Aurbach, D. et al. The study of electrolyte-solutions based on ethylene and diethyl carbonates for rechargeable li batteries.2. Graphite-electrodes. J. Electrochem. Soc. 142, 2882–2890 (1995).
Xiao, J. et al. Exfoliated MoS2 nanocomposite as an anode material for lithium ion batteries. Chem. Mater. 22, 4522–4524 (2010).
Dresselhaus, M. S. & Dresselhaus, G. Intercalation compounds of graphite. Adv. Phys. 30, 139–326 (1981).
Sun, Y., Wu, Q. & Shi, G. Graphene based new energy materials. Energy Environ. Sci. 4, 1113–1132 (2011).
Khrapach, I. et al. Novel highly conductive and transparent graphene-based conductors. Adv. Mater. 24, 2844–2849 (2012).
Kim, N., Kim, K. S., Jung, N., Brus, L. & Kim, P. Synthesis and electrical characterization of magnetic bilayer graphene intercalate. Nano Lett. 11, 860–865 (2011).
Hwang, J., Carbotte, J. P., Tongay, S., Hebard, A. F. & Tanner, D. B. Ultrapure multilayer graphene in bromine-intercalated graphite. Phys. Rev. B 84, 041410 (2011).
Kanetani, K. et al. Ca intercalated bilayer graphene as a thinnest limit of superconducting C6Ca. Proc. Natl Acad. Sci. USA 109, 19610–19613 (2012).
Hennig, G. R. Optical Transmission of graphite compounds. J. Chem. Phys. 43, 1201–1206 (1965).
Li, Z. Q. et al. Dirac charge dynamics in graphene by infrared spectroscopy. Nat. Phys. 4, 532–535 (2008).
Yan, J., Zhang, Y., Kim, P. & Pinczuk, A. Electric field effect tuning of electron-phonon coupling in graphene. Phys. Rev. Lett. 98, (2007).
Wang, F. et al. Gate-variable optical transitions in graphene. Science 320, 206–209 (2008).
Zhang, Y. et al. Direct observation of a widely tunable bandgap in bilayer graphene. Nature 459, 820–823 (2009).
Efetov, D. K. & Kim, P. Controlling electron-phonon interactions in graphene at ultrahigh carrier densities. Phys. Rev. Lett. 105, (2010).
De, S. & Coleman, J. N. Are there fundamental limitations on the sheet resistance and transmittance of thin graphene films? ACS Nano 4, 2713–2720 (2010).
Pietronero, L., Strässler, S., Zeller, H. R. & Rice, M. J. Electrical conductivity of a graphite layer. Phys. Rev. B 22, 904–910 (1980).
Inaba, M. et al. In-situ raman-study on electrochemical li-intercalation into graphite. J. Electrochem. Soc. 142, 20–26 (1995).
Ohzuku, T., Iwakoshi, Y. & Sawai, K. Formation of lithium-graphite intercalation compounds in nonaqueous electrolytes and their application as a negative electrode for a lithium ion (shuttlecock) cell. J. Electrochem. Soc. 140, 2490–2498 (1993).
Dimiev, Ayrat M. et al. Direct real-time monitoring of stage transitions in graphite intercalation compounds. ACS Nano 7, 2773–2780 (2013).
Holzwarth, N. A. W., Louie, S. G. & Rabii, S. Lithium-intercalated graphite: self-consistent electronic structure for stages one, two, and three. Phys. Rev. B 28, 1013–1025 (1983).
Li, Z. Q. H. et al. Dirac charge dynamics in graphene by infrared spectroscopy. Nat. Phys. 4, 13 (2008).
Basu, S. et al. Synthesis and properties of lithium-graphite intercalation compounds. Mater. Sci. Eng. 38, 275–283 (1979).
Wu, S. et al. Temperature dependence of the far-infrared magnetotransmission of YBa2Cu3O7-delta films. Phys. Rev. B 54, 13343–13347 (1996).
Stauber, T., Peres, N. M. R. & Castro Neto, A. H. Conductivity of suspended and non-suspended graphene at finite gate voltage. Phys. Rev. B 78, 085418 (2008).
Peres, N. M. R. Colloquium: the transport properties of graphene: an introduction. Rev. Mod. Phys. 82, 2673–2700 (2010).
Dahn, J. R., Fong, R. & Spoon, M. J. Suppression of staging in lithium-intercalated carbon by disorder in the host. Phys. Rev. B 42, 6424–6432 (1990).
Chen, J.-H., Jang, C., Xiao, S., Ishigami, M. & Fuhrer, M. S. Intrinsic and extrinsic performance limits of graphene devices on SiO2 . Nat. Nanotech. 3, 206–209 (2008).
Tung, V. C. et al. Low-temperature solution processing of graphene-carbon nanotube hybrid materials for high-performance transparent conductors. Nano Lett. 9, 1949–1955 (2009).
Rathmell, A. R., Minh, N., Chi, M. & Wiley, B. J. Synthesis of oxidation-resistant cupronickel nanowires for transparent conducting nanowire networks. Nano Lett. 12, 3193–3199 (2012).
Lee, J.-Y., Connor, S. T., Cui, Y. & Peumans, P. Solution-processed metal nanowire mesh transparent electrodes. Nano Lett. 8, 689–692 (2008).
Ramesh, P. et al. Electro-oxidized epitaxial graphene channel field-effect transistors with single-walled carbon nanotube thin film gate electrode. J. Am. Chem. Soc. 132, 14429–14436 (2010).
Hellstrom, S. L. et al. Strong and stable doping of carbon nanotubes and graphene by MoOx for transparent electrodes. Nano Lett. 12, 3574–3580 (2012).
Hecht, D. S., Hu, L. & Irvin, G. Emerging transparent electrodes based on thin films of carbon nanotubes, graphene, and metallic nanostructures. Adv. Mater. 23, 1482–1513 (2011).
Wu, H. et al. A transparent electrode based on a metal nanotrough network. Nat. Nanotech. 8, 421–425 (2013).
The work is supported by Energy Research Frontier Center (EFRC) funded by DOE, Office of Science, BES under Award # DESC0001160 and the U.S. ONR MURI programme. This work is partially supported by NSF-CMMI Award #1300361. J.N.M. acknowledges the startup support from University of Maryland. M.S.F. acknowledges support from an ARC Laureate Fellowship. We acknowledge the support of the Maryland Nanocenter. We thank Dr Karen Gaskell, Joe Murray and Joe Villeneuve for technical assistance for this experiment. We also thank Jiaqi Dai for making Cover Art and Colin Preston for reading the manuscript and useful comments.
The authors declare no competing financial interests.
Supplementary Figures 1-14, Supplementary Methods and Supplementary References (PDF 1383 kb)
This video recorded by a transmission optical microscope shows a dynamic evolution of lithiation interface during electrochemical intercalation in multilayer graphene. (MOV 4511 kb)
About this article
Cite this article
Bao, W., Wan, J., Han, X. et al. Approaching the limits of transparency and conductivity in graphitic materials through lithium intercalation. Nat Commun 5, 4224 (2014). https://doi.org/10.1038/ncomms5224
This article is cited by
Nature Chemistry (2023)
Nature Communications (2023)
Performance and reliability improvement in intercalated MLGNR interconnects using optimized aspect ratio
Scientific Reports (2022)
Nature Nanotechnology (2022)
Multispectral graphene-based electro-optical surfaces with reversible tunability from visible to microwave wavelengths
Nature Photonics (2021)