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Difference in gating and doping effects on the band gap in bilayer graphene

  • Scientific Reportsvolume 7, Article number: 11322 (2017)
  • doi:10.1038/s41598-017-11822-9
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A band gap is opened in bilayer graphene (BLG) by applying an electric field perpendicular to the layer, which offers versatility and controllability in graphene-based electronics. The presence of the band gap has been confirmed using double-gated BLG devices in which positive and negative gate voltages are applied to each side of BLG. An alternative method to induce the electric field is electron and hole doping of each side of BLG using electron-transfer adsorbates. However, the generation of the band gap by carrier doping is still under investigation. Here, we determined whether the electron/hole doping can produce the electric field required to open the band gap by measuring the temperature dependence of conductivity for BLG placed between electron-donor self-assembled monolayers (SAMs) and electron-acceptor molecules. We found that some devices exhibited a band gap and others did not. The potentially irregular and variable structure of SAMs may affect the configuration of the electric field, yielding variable electronic properties. This study demonstrates the essential differences between gating and doping.


Control of carrier density is a key issue when engineering the electronic properties of materials. Various phase transitions, such as insulator-metal1,2,3,4, insulator-superconductor5,6,7, and nonmagnetic-magnetic8, 9 transitions have been caused by tuning the carrier density. Two methods are widely used for this purpose. One is a gating method, which accumulates carriers electrostatically using a field-effect transistor (FET) structure. The other is a doping method, based on electron transfer between dopants and target materials. These two methods are generally believed to work in essentially the same way. Indeed, both gating and doping methods have enabled us to induce superconductivity in SrTiO310, 11, MoS212, 13, MoSe214, 15, and LaOBiS216, 17, to name a few.

A double-gate technique using top and bottom gates extends the controllability of electronic states not only by tuning carrier density but also by producing an electric field. When different voltages, Vtg and Vbg, are applied to the top and bottom gates, respectively, the potential difference between the two gates produces an electric field (Fig. 1a). This effect is important, especially in two-dimensional layered materials (2DMs) through which the electric field can penetrate. A notable example is bilayer graphene (BLG), which has two quasi-quadratic bands in contact with each other. This zero-gap semiconductor exhibits a band gap when it was subjected to a perpendicular electric field18, which was confirmed from transport and optical properties19,20,21 for a double-gated FET structure. The effective band gap estimated from transport has been much smaller than that from optical measurement19,20,21,22,23,24,25,26. The origin of the smaller transport gap remains to be clarified, although it can be attributed not only to variable range hopping in gap states19, 22,23,24 but also to one-dimensional conduction through edges25 or domain walls26.

Figure 1
Figure 1

Two methods to generate an electric field. (a) Double-gate method; positive bottom- and negative top-gate voltages produce an upward electric field (left). Energy band diagrams of 2DM and two gate electrodes are illustrated before (middle) and after (right) applying gate voltages. The origin of the electric field is the potential difference between two gate electrodes. (b) Double-dope method; electron-donor SAMs and electron-acceptor molecules can produce an upward electric field (left). Energy band diagrams of 2DM, SAMs and molecules are illustrated before (middle) and after (right) electron transfer. The origin of the electric field is the Fermi level alignment of 2DM, SAMs and the molecules. (c) Schematic of device structure used in this study. BLG is placed on NH2-SAMs. Four-terminal conductivity is compared before and after the deposition of F4TCNQ molecules. Molecular structures of F4TCNQ and NH2-SAMs are shown.

The double-doping method (or electron/hole doping) is also expected to give the same effect in BLG as the double-gating, although the mechanism that produces the electric field is completely different. In the case of double-doping, the electron transfer between dopants and BLG aligns their Fermi levels, thus inducing the electric field (Fig. 1b). For example, n-doping of the bottom layer and p-doping of the top layer can create an electric field directed from the bottom to the top layer, which will open a band gap in BLG.

The electronic property of doped BLG has been studied in several experiments thus far27,28,29,30, and the presence of a band gap is confirmed in some reports27, 28. An early study with angle-resolved photoemission spectroscopy (ARPES)27 showed that a band gap was actually opened in BLG in which the bottom layer was n-doped by a SiC substrate and the top layer was p-doped by deposition of electron acceptor molecules. Transport and infrared (IR) absorption measurements also demonstrated the existence of a band gap in BLG placed between electron-donor self-assembled monolayers (SAMs) and electron-acceptor molecules28. On the other hand, the band gap was not indicated in other reports29, 30. The Vbg dependence of conductivity was measured in BLG on which K atoms29 or O2 molecules30 were adsorbed. The top layer of BLG was n-doped by K atoms29 or p-doped by O2 molecules30, and the electric field is expected to be induced between the bottom gate and the adsorbates at the charge neutrality point. But neither study indicated the band gap. Thus, the reported results have been inconsistent.

To gain insight into this inconsistency, we studied whether a band gap in BLG is opened with the doping method by measuring the temperature dependence of its transport property. The emergence of a band gap was unambiguously confirmed by the suppression of carrier density at low temperatures, while previous measurements27,28,29,30 have been carried out at room temperature.

Figure 1c illustrates the device structure used in this study. BLG is placed between SAMs and adsorbed molecules. The SAMs were prepared from 10-aminodecyltriethoxysilane, called NH2-SAMs. This has an end group of NH2 which donates an electron to the bottom layer of BLG31. For the other side, typical electron acceptor molecules, 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4TCNQ), were deposited to donate holes to the top layer of BLG. The F4TCNQ molecule is a strong electron acceptor which accumulates nearly 1 hole per molecule at low coverage32. Sandwiched between these molecules, BLG can be influenced by the upwardly directed electric field. The molecular structures of NH2-SAMs and F4TCNQ are shown in Fig. 1c.

First, NH2-SAMs were prepared on SiO2 (300-nm thick)/Si substrates by a liquid-phase method (described in detail elsewhere33). Graphene flakes were deposited on the NH2-SAMs with a cleavage technique34, and BLG was identified by optical contrast35, 36 and Raman spectroscopy37. Electrodes were attached to the flakes in a four-terminal configuration by using electron beam lithography and vacuum evaporation of metals (5-nm thick Cr and 100-nm thick Au). The devices were placed in a cryogenic probe station, and their four-terminal conductivity σ was measured as a function of bottom gate voltage Vbg with decreasing temperature; σ(Vbg) refers to the σ for Vbg. After the transport measurement, the device was transferred to the other chamber in order to deposit F4TCNQ molecules. The deposition was carried out while keeping the substrate at room temperature and the thickness, t, was determined with a thickness monitor. Subsequently, the device was returned to the probe station and the temperature dependence of σ(Vbg) curve was measured again. The process of transport measurement and molecular deposition was repeated in ultrahigh vacuum under 10−6 Pa without exposing the device to air.


Temperature dependence of conductivity

A total of four devices (called samples A1, A2, B1, and B2) were prepared with the same experimental procedure, but samples A1 and A2 (called group A), and samples B1 and B2 (called group B) showed substantially different behavior. Results obtained from samples A1 and B1 are compared in Fig. 2. Figure 2a,b show the temperature dependence of σ(Vbg) before and after the deposition of F4TCNQ molecules. In Fig. 2a,b, the charge neutrality point Vn was initially situated around −65 V. Since Vn is observed at around 0 V in BLG devices prepared on conventional SiO2/Si substrates, the shift of Vn, ΔVn ~ −65 V is due to electron accumulation in BLG from NH2-SAMs. As shown in Fig. 2a,b, Vn shifted to around 0 V after the deposition of F4TCNQ molecules. This shift ΔVn ~ 65 V indicates hole accumulation by F4TCNQ molecules in turn. The electron and hole density transferred from each of the molecules is estimated to be Co|ΔVn|/e ~ 5 × 1012 cm−2, where Co (=11.5 nF cm−2) is the capacitance of a 300-nm thick SiO2 dielectric. Although the σ(Vbg) curves of samples A1 and B1 were similar to each other before the deposition, they showed a distinct difference after the deposition: the σ(Vbg) of sample A1 exhibited a sharp dip, while that of sample B1 was broadened. This phenomenon is discussed later.

Figure 2
Figure 2

Comparison of altered transport properties after F4TCNQ deposition. (a,b) Conductivity as a function of bottom gate voltage and its temperature dependence. Conductivity curves are shown for t = 0 and t = 0.2 Å; t = 0 refers to ‘before deposition of F4TCNQ’, while t = 0.2 Å to ‘after deposition of 0.2 Å thick F4TCNQ’. The gate voltage was swept from the negative to the positive value, with no hysteresis observed for either sweep direction. (c,d) Arrhenius plots of the minimum conductivity evaluated from (a) and (b). The solid lines are fitting curves using equation (2). (e,f) Temperature dependence of ON/OFF ratio is shown for t = 0 and t = 0.2 Å. The ON/OFF ratio is defined as σ(V n + 45 V)/σ(V n), and evaluated from (a and b). The solid lines are guides to the eye. All graphs in (a,c and e) are based on sample A1, and those in (b,d and f) are based on sample B1.

The band structure at the charge neutrality point should be sensitively reflected in the minimum conductivity, σmin (=σ(Vn)). In Fig. 2c,d, σmin is plotted on a logarithmic scale as a function of inverse temperature, 1/T, for samples A1 and B1. When the band gap, δ, opens, σmin should be limited by the carrier density thermally excited, n(T)=exp(δ / 2 k B T). Thus, the band gap, if produced, is verified by the enhancement of the slope of the plots in Fig. 2c,d. The slope in the high T range increased in sample A1 after the deposition, while it decreased slightly in sample B1. This result demonstrates the critical difference between the two samples: sample A1 exhibited a band gap, but sample B1 did not, after F4TCNQ deposition.

The difference should also be confirmed by that of ON/OFF ratio between two samples. Figure 2e,f show the temperature dependence of ON/OFF ratio before and after the deposition of F4TCNQ molecules. After the deposition, the ON/OFF ratio increased in sample A1, while it decreased in sample B1. This result can be well explained by different band structure between two samples. The opening of the band gap in sample A1 reduced OFF current to enhance the ON/OFF ratio. This enhancement becomes more prominent at low temperature because of the reduction of carrier density excited at OFF state. On the other hand, the ON/OFF ratio in sample B1 decreased and did not depend on temperature after the F4TCNQ deposition, which indicates no band gap.

Evaluation of a band gap or band overlap

To evaluate band parameters such as a band gap or band overlap numerically, the temperature dependence of the carrier density, n(T), was discussed in detail because σmin is related to n(T) by the equation, σmin(T) = n(T)n. Here, the carrier mobility at the charge neutrality point, μn, is assumed to be constant because the field-effect mobility evaluated from μ e = 1 C O d σ d V b g at electron regimes was independent of T (see Supplementary Fig. S1). Adding up hole and electron density, n(T) is expressed as

n(T)= D h ( E ) [ 1 f ( E ) ] d E + D e ( E ) f ( E ) d E .

Here, Dh(E) and De(E) are the density of states for holes and electrons in BLG. f(E) [ 1 + exp ( E E F k B T ) ] 1 is the Fermi-Dirac distribution function, EF is the Fermi energy, set to be 0 at the charge neutrality point, and kB is the Boltzmann constant. Assuming constant Dh(E) and De(E) of BLG for simplicity:

D h (E)={ D , E δ / 2 0 , E > δ / 2 a n d D e (E)={ 0 , E < δ / 2 D , E δ / 2 ,

the minimum conductivity is obtained from

σ min (T)=2e μ n D k B Tln [ 1 + exp ( δ / 2 k B T ) ] .

Here, a positive δ means a band gap with energy of δ, while negative δ corresponds to a band overlap with energy of −δ. In the low T limit, equation (2) is reduced to σ min 2e μ n D k B Texp( δ 2 k B T ) for δ > 0 and σ min ~e μ n D(δ) for δ < 0. A negative δ can also be the result of Fermi level broadening due to local potential fluctuation38, 39, as discussed later. The experimental data in the range of 125 K ≤ T ≤ 275 K in Fig. 2c,d were fitted with equation (2), and the results are shown with solid lines. The fitting lines show good agreement with experimental data over the entire T range except for the data at t = 0.2 Å of sample A1. The discrepancy at t = 0.2 Å of sample A1 in the low T range is ascribed to the residual conductance due to the variable range hopping, which is noticeable in the presence of a band gap22,23,24. Actually, the δ value of sample A1 increases from −34 to 8.1 meV, indicating the generation of a band gap. On the other hand, the δ of sample B1 decreases from −25 to −37 meV, indicating the enhancement of band overlap. Thus, samples A1 and B1 were affected differently by the deposition of F4TCNQ molecules.

The σ   − Vbg curves and σmin − 1/T plots for samples A2 and B2 are shown in Supplementary Fig. S2. The values δ for samples A2 and B2 were evaluated from the analysis using equation (2). In Fig. 3, δ values for all four samples are plotted as a function of t. After the first deposition of F4TCNQ, δ increased for both devices in group A, indicated by the closed symbols, while δ decreased for both in group B, indicated by the open symbols. A band gap tends to open in group A, but it does not in group B. With increasing t furthermore, δ decreased to a negative value even for sample A1. To summarize the experimental results, electron and hole doped BLG (or BLG sandwiched by electron-donor SAMs and electron-acceptor molecules) did not always exhibit a band gap even under identical preparation and measurement conditions. This result seems to correspond to previous conflicting reports about the opening of a band gap.

Figure 3
Figure 3

Band parameter as a function of F4TCNQ thickness. The band parameter δ was evaluated using equation (2). Positive and negative δ value means the separation and overlap of the valence and conduction bands, respectively. At t = 0, all δ was negative because of the spatial potential variation (see the main text and Fig. 4a). After the initial deposition of F4TCNQ, δ increased in two samples (samples A1 and A2 are called group A, solid symbols). The positive δ (t = 0.2 Å) in sample A1 means the opening of a band gap. The δ value in sample A2 was also increased but still negative, indicating the decrease in the band overlap or the trend of the band gap opening. In contrast, δ decreased in two samples (samples B1 and B2 called group B, open symbols), indicating the enhancement of the band overlap. With further deposition of F4TCNQ, δ for both samples A1 and B1 decreased. The arrow indicates the boundary at δ(0) ~ −30 meV that distinguishes groups A and B.


We first consider why the behavior of δ(t) is different in groups A and B. It is worth noting that the δ before the deposition of F4TCNQ molecules, δ(0), is smaller in group A than B; the δ(0) values of group A are below −30 meV, while those of group B are above −30 meV (Fig. 3). The values of δ(0) are negative for all samples, which is ascribed to the potential irregularity induced by charged molecules. The molecular density of SAMs33, i.e., the number of NH2-alkylsilane (NH2-AS) per unit area is typically (1–2) × 1014 cm−2, while the electron density transferred from NH2-SAMs is estimated to be 5 × 1012 cm−2 as described before. This means that only one out of 20–40 NH2-ASs donates an electron to the BLG. Consequently, two kinds of molecules are present in NH2-SAMs. One is an ionized molecule that has donated an electron, referred to as NH2+-alkylsilane (NH2+-AS). The other is a neutral molecule which does not donate an electron, referred to as NH2-AS. The potential energy of an electron in BLG is lower near an NH2+-AS than that near an NH2-AS. In this case, both the electrons and holes can contribute to the electric transport even at the charge neutrality point, as seen from Fig. 4a. This situation means that the conduction and valence bands overlap. Thus, the value of −δ(0) shown in Fig. 4a indicates the magnitude of the potential variability in BLG, which is larger in group A than group B (−δ(0) for A > −δ(0) for B).

Figure 4
Figure 4

Potential profiles depending on dopant arrangement. (a) The red line indicates the spatial variation of the potential energy ψ(x) in BLG on NH2-SAMs. NH2 +- and NH2-AS are distinguished by and . ψ(x) shows the minimum on NH2 +-AS and changes spatially in accord with the characteristic screening length l SC,//. The blue curves show the band structure E(k) modified by ψ(x). The horizontal plane indicates the Fermi energy E F at the charge neutrality point around V bg ~ −65 V. At a position far from NH2 +-AS, i.e., the position corresponding to the middle energy diagram, ψ(x) is mainly affected by V bg ~ −65 V. The negative V bg produces a downward electric field to open the band gap. Nonetheless, E F is located at the valence band, producing a hole puddle. However, at a position just above NH2 +-AS, i.e., the position corresponding to the left or right energy diagram, the effect of NH2 +-AS is larger than that of V bg, producing an upward electric field. In this case, E F is located in the conduction band, producing an electron puddle. In this way, both hole and electron puddles contribute to carrier transport at the charge neutrality point. (b) NH2 +-AS and F4TCNQ molecules, denoted by and , are aligned in the normal direction. The horizontal plane indicates E F at the charge neutrality point around V bg ~ 0 V. Two red dashed curves show the potential energy produced by each molecule, which mutually cancel. In this case, the perpendicular electric field produces the band gap, which directly affects the transport property at the charge neutrality point. (c) NH2 +-AS and F4TCNQ molecules are not aligned. The horizontal plane indicates E F at the charge neutrality point around V bg ~ 0 V. When the lateral spacing of two dopants is larger than l SC,//, the potential energy produced by each molecule is not cancelled but varies with location. In this case, the transport property is determined by electron and hole puddles as in (a). The different arrangement in (b and c) originates in the magnitude of potential variation and the screening length l SC,//.

Note that the potential fluctuation caused by NH2-SAMs affects the top surface of the BLG. This can be understood by considering that the potential energy varies with the characteristic screening length of BLG in the intralayer and interlayer directions. The intralayer screening length, lSC,//, is estimated to be lSC,//κħ2/(gsgvme2) ~ 1.1 nm40, where κ ~ 2.5 is the average background dielectric constant, ħ is the Planck’s constant divided by 2π, gs = gv = 2 is the spin and valley degeneracy, and m = 0.03me is the effective mass in BLG40. The length of lSC,// is less than the average distance between NH2+-ASs, d2 e / ( π C O | Δ V n | ) 5.2 n m (Fig. 4a). Since lSC,// is shorter than d, the spatially inhomogeneous potential is created in BLG as shown in Fig. 4a. On the other hand, the interlayer screening length, lSC,, of few-layer graphene exceeds 2 layers around the charge neutrality point41,42,43. Comparing the screening length, lSC,, and the thickness of BLG shows that the potential fluctuation due to the bottom dopant is not completely screened by BLG but affects the surface of the top layer. This can influence the arrangement of F4TCNQ molecules deposited and thus change the collective electronic properties of the entire construct.

Figure 4b,c illustrate the potential profiles of BLG, which depend on the alignment of the NH2+-AS and F4TCNQ molecules. When the potential fluctuation, −δ(0), is large enough, as in group A, an F4TCNQ molecule, which is ionized to F4TCNQ after accepting an electron, may be trapped by the NH2+-AS as shown in Fig. 4b. Since the two dopants are aligned in the normal direction, the perpendicular electric field is generated to open the band gap. However, when the potential fluctuation, −δ(0), is small, as in group B, F4TCNQ molecules can be adsorbed anywhere without restriction, as in Fig. 4c. In this case, the average lateral distance between randomly deposited NH2+-AS and F4TCNQ molecules is estimated to be d / 2 3.7 n m , which still exceeds the intralayer screening length, lSC,//. Consequently, the potential fluctuation is further enhanced as seen from Fig. 4c, which prevents the opening of a band gap because of the overlapping of potentials as illustrated in Fig. 4c. The difference in molecular alignments shown in Fig. 4b,c depends on whether the F4TCNQ molecule is trapped by the potential drop at the NH2+-AS. The threshold energy for the trapping of the molecules in the potential fluctuation corresponds to thermal energy at room temperature, 26 meV. This estimation shows a good agreement with the experimental boundary around 30 meV (−δ(0) for A > 30 meV, −δ(0) for B < 30 meV) shown in Fig. 3, strongly supporting our discussion.

Thus, the alignment of the NH2+-AS and F4TCNQ molecules via BLG is required for band gap opening. The random deposition of F4TCNQ molecules increases the potential variability, thereby enhancing the potential scattering. The decrease in carrier mobility due to scattering is indicated by the broadening of σ(Vbg) in Fig. 2b. In order to open the maximum energy gap, not only the alignment but also the number of F4TCNQ molecules must be optimized to compensate for the effect of NH2+-AS. As shown in Fig. 3, the excess deposition of F4TCNQ increases −δ even in sample A1, meaning that F4TCNQ molecules in excess of the optimal value only enhance the potential variability.

To generalize our claim and ensure the reproducibility of results, we additionally carried out transport measurement of two devices (samples C1 and C2) which were prepared on SiO2/Si substrate without NH2-SAMs. As shown in Supplementary Fig. S3, the δ(0) value of sample C1 was around −30 meV, and that of sample C2 was less than −30 meV. The δ value of both samples slightly increased after the F4TCNQ deposition, indicating the trend of the band gap opening. The data obtained from samples C1 and C2 seem to follow the scenario derived from other samples (A and B) prepared on NH2-SAMs, supporting our conclusion that the opening of the band gap is determined by δ(0), i.e., the potential variation caused by charged impurities on the substrate governs the electronic property after the deposition of F4TCNQ molecules.

Finally, we consider the origin of the different values of δ(0) in different devices. Since the devices were prepared in the same manner, some uncontrollable factors may affect δ(0). For example, when BLG is transferred onto the NH2-SAMs using the micromechanical cleavage technique34, the spacing between BLG and NH2-SAMs may change depending on devices owing to the flexibility of the alkyl chains in NH2-SAMs. In this case, the smaller the spacing, the larger the −δ(0). Additional factors originating in the interaction of NH2-SAMs and BLG such as corrugation44 of the BLG may also affect the potential fluctuation, −δ(0). One possible solution to open the band gap in BLG under any conditions is to deposit F4TCNQ molecules at low temperature. The molecules will tend to be trapped at NH2+ sites and thus to promote the band gap opening, since the low thermal energy suppresses molecular motion.

In conclusion, we studied the electronic states of BLG, both surfaces of which were decorated with electron transfer molecules. The temperature dependence of conductivity showed that the band gap was opened in some devices and was not in others, which seems consistent with previous inconsistent results. We have concluded that the difference originates in local potential variations due to dopant molecules. The effect of the potential variation on BLG is significant because of the long interlayer and short intralayer screening length in BLG. Furthermore, our results show an important difference between gating and doping methods. Compared with the gating method, the doping method is more sensitive to the potential irregularities caused by the dopants. In the gating method using a conventional 300-nm thick SiO2 dielectric, the effect of local potential variations is averaged out. When very thin gate dielectrics such as an electric-double layer are used, the effect of potential irregularities becomes important even in the gating method. Our study of the microscopic arrangement of molecular dopants and its controllability is significant for the application of an electron-transfer molecule for the ultimate small gate electrode. The findings may open new avenues for the nano-technological development of molecular electronics.


Device preparation

NH2-SAMs were prepared on a SiO2/Si substrate as in the previous report33. Its uniformity was confirmed by measuring the contact angle of a water droplet placed on the NH2-SAMs. The contact angle was 81.2(9)°, which was larger than the values reported previously33, indicating the uniformity of NH2-SAMs. BLG devices on NH2-SAMs were prepared by the conventional microfabrication technique using electron beam lithography, Elionix Inc., ELS-S50.


Transport measurement was carried out in a cryogenic probe station that is combined with a chamber for molecular deposition (Riko International LTD, i-series ultrahigh vacuum microprobe and chamber). In advance of the measurement, the devices were annealed at 373 K in a vacuum for over 1 hour in order to eliminate adsorbed atmospheric gases such as H2O or O2 molecules. Four-terminal conductivity was measured using a semiconductor device analyzer, Agilent B1500A. The devices were transferred from the probe system to the other vacuum chamber, in which F4TCNQ molecules were deposited on the devices under a pressure of 10−6 Pa.

Data availability

All data generated or analysed during this study are included in this published article (and its Supplementary Information files).

Additional information

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  1. 1.

    Rosenbaum, T. F. et al. Metal-insulator transition in a doped semiconductor. Phys. Rev. B 27, 7509–7523 (1983).

  2. 2.

    McWhan, D. B., Menth, A., Remeika, J. P., Brinkman, W. F. & Rice, T. M. Metal-insulator transitions in pure and doped V2O3. Phys. Rev. B 7, 1920–1931 (1973).

  3. 3.

    Evers, F. & Mirlin, A. D. Anderson transitions. Rev. Mod. Phys. 80, 1355–1417 (2008).

  4. 4.

    Imada, M., Fujimori, A. & Tokura, Y. Metal-insulator transitions. Rev. Mod. Phys. 70, 1039–1263 (1998).

  5. 5.

    Saito, Y., Nojima, T. & Iwasa, Y. Highly crystalline 2D superconductors. Nature Rev .Mater. 2, 16094, (2016).

  6. 6.

    Bollinger, A. T. et al. Superconductor-insulator transition in La2-xSrxCuO4 at the pair quantum resistance. Nature 472, 458–460 (2011).

  7. 7.

    Lee, P. A., Nagaosa, N. & Wen, X.-G. Doping a Mott insulator: physics of high-temperature superconductivity. Rev. Mod. Phys. 78, 17–85 (2006).

  8. 8.

    Yamada, Y. et al. Electrically induced ferromagnetism at room temperature in cobalt-doped titanium dioxide. Science 332, 1065–1067 (2011).

  9. 9.

    Ohno, H. et al. Electric-field control of ferromagnetism. Nature 408, 944–946 (2000).

  10. 10.

    Ueno, K. et al. Electric-field-induced superconductivity in an insulator. Nature Mater. 7, 855–858 (2008).

  11. 11.

    Schooley, J. F. et al. Dependence of the superconducting transition temperature on carrier concentration in semiconducting SrTiO3. Phys. Rev. Lett. 14, 305–307 (1965).

  12. 12.

    Ye, J. T. et al. Superconducting dome in a gate-tuned band insulator. Science 338, 1193–1196 (2012).

  13. 13.

    Rao, G. V. S., Shafer, M. W., Kawarazaki, S. & Toxen, A. M. Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides. J. Solid State Chem. 9, 323–329 (1974).

  14. 14.

    Shi, W. et al. Superconductivity series in transition metal dichalcogenides by ionic gating. Sci. Rep. 5, 12534, doi:1038/srep12534 (2015).

  15. 15.

    Miao, X. et al. Emergence of superconductivity in (NH3)yMxMoSe2 (M: Li, Na and K). Sci. Rep. 6, 29292, doi:1038/srep29292 (2016).

  16. 16.

    Mizuguchi, Y. et al. Superconductivity in novel BiS2-based layered superconductor LaO1-xFxBiS2. J. Phys. Soc. Jpn. 81, 114725 (2012).

  17. 17.

    Uesugi, E., Nishiyama, S., Goto, H., Ota, H. & Kubozono, Y. Electrostatic electron-doping yields superconductivity in LaOBiS2. Appl. Phys. Lett. 109, 252601 (2016).

  18. 18.

    McCann, E. Asymmetry gap in the electronic band structure of bilayer graphene. Phys. Rev. B 74, 161403(R) (2006).

  19. 19.

    Oostinga, J. B., Heersche, H. B., Liu, X., Morpurgo, A. F. & Vandersypen, L. M. K. Gate-induced insulating state in bilayer graphene devices. Nature Mater. 7, 151–157 (2008).

  20. 20.

    Zhang, Y. et al. Direct observation of a widely tunable bandgap in bilayer graphene. Nature 459, 820–823 (2009).

  21. 21.

    Mak, K. F., Lui, C. H., Shan, J. & Heinz, T. F. Observation of an electric-field-induced band gap in bilayer graphene by infrared spectroscopy. Phys. Rev. Lett. 102, 256405 (2009).

  22. 22.

    Taychatanapat, T. & Jarillo-Herrero, P. Electronic transport in dual-gated bilayer graphene at large displacement fields. Phys. Rev. Lett. 105, 166601 (2010).

  23. 23.

    Miyazaki, H., Tsukagoshi, K., Kanda, A., Otani, M. & Okada, S. Influence of disorder on conductance in bilayer graphene under perpendicular electric field. Nano Lett. 10, 3888–3892 (2010).

  24. 24.

    Kanayama, K. & Nagashio, K. Gap state analysis in electricfield-induced band gap for bilayer graphene. Sci. Rep. 5, 15789, doi:1038/srep15789 (2015).

  25. 25.

    Zhu, M. J. et al. Edge currents shunt the insulating bulk in gapped graphene. Nat. Commun. 8, 14552, doi:1038/ncomms14552 (2017).

  26. 26.

    Ju, L. et al. Topological valley transport at bilayer graphene domain walls. Nature 520, 650–655 (2015).

  27. 27.

    Coletti, C. et al. Charge neutrality and band-gap tuning of epitaxial graphene on SiC by molecular doping. Phys. Rev. B 81, 235401 (2010).

  28. 28.

    Park, J. et al. Single-gate bandgap opening of bilayer graphene by dual molecular doping. Adv. Mater. 24, 407–411 (2012).

  29. 29.

    Xiao, S., Chen, J.-H., Adam, S., Williams, E. D. & Fuhrer, M. S. Charged impurity scattering in bilayer graphene. Phys. Rev. B 82, 041406(R) (2010).

  30. 30.

    Sato, Y., Takai, K. & Enoki, T. Electrically controlled adsorption of oxygen in bilayer graphene devices. Nano Lett. 11, 3468–3475 (2011).

  31. 31.

    Yan, Z. et al. Controlled modulation of electronic properties of graphene by self-assembled monolayers on SiO2 substrates. ACS Nano 5, 1535–1540 (2011).

  32. 32.

    Akiyoshi, H. et al. Carrier accumulation in graphene with electron donor/acceptor molecules. Adv. Electron. Mater. 1, 1500073 (2015).

  33. 33.

    Kobayashi, S. et al. Control of carrier density by self-assembled monolayers in organic field-effect transistors. Nature Mater. 3, 317–322 (2004).

  34. 34.

    Novoselov, K. S. et al. Electric field effect in atomically thin carbon films. Science 306, 666–669 (2004).

  35. 35.

    Uesugi, E., Goto, H., Eguchi, R., Fujiwara, A. & Kubozono, Y., Electric double-layer capacitance between an ionic liquid and few-layer graphene. Sci. Rep. 3, 01595, doi:1038/srep01595 (2013).

  36. 36.

    Blake, P. et al. Making graphene visible. Appl. Phys. Lett. 91, 063124 (2007).

  37. 37.

    Ferrari, A. C. et al. Raman spectrum of graphene and graphene layers. Phys. Rev. Lett. 97, 187401 (2006).

  38. 38.

    Martin, J. et al. Observation of electron-hole puddles in graphene using a scanning single-electron transistor. Nature Phys. 4, 144–148 (2008).

  39. 39.

    Deshpande, A., Bao, W., Zhao, Z., Lau, C. N. & LeRoy, B. J. Mapping the Dirac point in gated bilayer graphene. Appl. Phys. Lett. 95, 243502 (2009).

  40. 40.

    Sarma, S. D., Adam, S., Hwang, E. H. & Rossi, E. Electronic transport in two-dimensional graphene. Rev. Mod. Phys. 83, 407–480 (2011).

  41. 41.

    Miyazaki, H. et al. Inter-layer screening length to electric field in thin graphite film. Appl. Phys. Express 1, 034007 (2008).

  42. 42.

    Kuroda, M. A., Tersoff, J. & Martyna, G. J. Nonlinear screening in multilayer graphene systems. Phys. Rev. Lett. 106, 116804 (2011).

  43. 43.

    Lee, N. J. et al. The interlayer screening effect of graphene sheets investigated by Kelvin probe force microscopy. Appl. Phys. Lett. 95, 222107 (2009).

  44. 44.

    Meyer, J. C. et al. The structure of suspended graphene sheets. Nature 446, 60–63 (2007).

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This work was partly supported by Grants-in-aid (26105004, 26400361 and 17K05500) from MEXT. This work was also supported by JST ACT-C Grant Number JPMJCR12YW, by the Program for Advancing Strategic International Networks to Accelerate the Circulation of Talented Researchers from JSPS (R2705), and by the Program for Promoting the Enhancement of Research Universities. The authors would like to express their gratitude to Prof. M. Mifune and Prof. N. Ikeda for Raman spectroscopy and atomic force microscopy (AFM) measurements, respectively.

Author information


  1. Research Institute for Interdisciplinary Science, Okayama University, Okayama, 700-8530, Japan

    • Takaki Uchiyama
    • , Hidenori Goto
    • , Hidehiko Akiyoshi
    • , Ritsuko Eguchi
    •  & Yoshihiro Kubozono
  2. Hanamaki Satellite, Research Center for Industrial Science, Iwate University, Iwate, 025-0312, Japan

    • Takao Nishikawa
  3. Faculty of Science and Engineering, Iwate University, Iwate, 020-8551, Japan

    • Hiroshi Osada


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H.G. supervised the study in collaboration with Y.K. T.N. and H.O. prepared NH2-SAMs on SiO2/Si substrates. T.U. and H.A. prepared BLG devices and measured their transport properties with help from R.E. The experimental data were analyzed by H.G., T.U. and H.A. H.G. wrote the manuscript by discussing the results with all authors.

Competing Interests

The authors declare that they have no competing interests.

Corresponding author

Correspondence to Hidenori Goto.

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