5%. The minimum transmission of the samples in the visible and the near-infrared range is over 85%, completely meeting the optical condition of transparent conducting films. Theoretically, the transparency of graphene drops quickly with thickness [8]. However, the this website actual measured transparency of graphene is not closely obeying it. For instance, Wang et al. reported that the transparency of GO is over 80% in 550-nm white light for 22 to 78 nm of thickness [27]. The high transparency of our samples is attributed

to the graphene films being composed of many graphene flakes, which allowed light transmission from the tiny pits between flakes. Moreover, the pits between graphene flakes make the actual average thickness often much smaller than

the measured thickness because of the resolution AG-881 in vivo of the AFM instrument. Figure 4 The light transmission rate of the graphene samples. (a) Transmission of the graphene films in the 400- to 800-nm range. (b) Transmission of the graphene films in the 1,000- to 3,000-nm range. The optical transmittance of the graphene films is over 85% in the visible range of 400 to 800 nm. The surface current–voltage (I-V) behaviors of the 1, 3, and 5 min graphene films were measured by means of Hall effect measurement, as shown in Figure 5a,b,c. The four measuring electrodes a, b, c, and d were arranged on the surface of the graphene www.selleckchem.com/products/ganetespib-sta-9090.html films in a square with a side length of 1 cm, as shown the inset in Figure 5a. For the graphene deposited Farnesyltransferase for 1 min, we can see that the I-V behaviors between the four points are not a characteristic of a linear relation, but of a nonlinear property. Especially, I-V bc and I-V cd lines were largely shifted from the linear relation. This is because the graphene on quartz does not form a continuous film but islands by a short time. With deposition time increasing to 3 and 5 min, the graphene islands collected each other to become a continuous film, and then the I-V properties become linear, as shown in Figure 5b,c. I-V da in Figure 5b is far from the other lines which may be caused by the asymmetry

of the four points. The I-V behaviors in Figure 5c all closely obey Ohm’s law. The linear I-V relations of the graphene surface show films with good conductivity. Figure 5 The surface I – V behaviors of the 1, 3, and 5 min graphene samples. (a) 1 min sample. The inset shows the electrodes’ layout on the surface of the graphene film. (b) 3 min sample. (c) 5 min sample. The thickness of the graphene films with deposition time is shown in Figure 6a. We can see that the thickness linearly increases with time. Then we investigated the electron mobility, conductivity, and sheet resistance with the thickness of the graphene films, as shown in Figure 6b,c. The electron mobility is 2.3 × 102, 5.1 × 104, and 9.5 × 104 cm2/V/s for 1, 3, and 5 min samples, respectively.