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Article http://pubs.acs.org/journal/acsodf
Two-Dimensional Hallmark of Highly Interconnected ThreeDimensional Nanoporous Graphene Iolanda Di Bernardo,† Giulia Avvisati,† Carlo Mariani,† Nunzio Motta,‡ Chaoyu Chen,§ José Avila,§ Maria Carmen Asensio,§ Stefano Lupi,∥ Yoshikazu Ito,⊥,# Mingwei Chen,¶ Takeshi Fujita,¶ and Maria Grazia Betti*,† †
Department of Physics, Sapienza University of Rome, Piazzale Aldo Moro 2, 00185 Rome, Italy School of Chemistry, Physics and Mechanical Engineering and Institute for Future Environments, Queensland University of Technology, 2 George Street, 4000 Brisbane, Australia § Synchrotron SOLEIL, L’Orme des Merisiers, Saint Aubin, 91190 Gif sur Yvette, France ∥ Department of Physics, CNR-IOM, Sapienza University of Rome, Piazzale Aldo Moro 2, 00185 Rome, Italy ⊥ Institute of Applied Physics, Graduate School of Pure and Applied Sciences, University of Tsukuba, 305-8571 Tsukuba, Japan # PRESTO, Japan Science and Technology Agency, 332-0012 Saitama, Japan ¶ Advanced Institute for Materials Research, Tohoku University, 980-8577 Sendai, Japan ‡
S Supporting Information *
ABSTRACT: Scaling graphene from a two-dimensional (2D) ideal structure to a three-dimensional (3D) millimeter-sized architecture without compromising its remarkable electrical, optical, and thermal properties is currently a great challenge to overcome the limitations of integrating single graphene flakes into 3D devices. Herewith, highly connected and continuous nanoporous graphene (NPG) samples, with electronic and vibrational properties very similar to those of suspended graphene layers, are presented. We pinpoint the hallmarks of 2D ideal graphene scaled in these 3D porous architectures by combining the state-of-the-art spectromicroscopy and imaging techniques. The connected and bicontinuous topology, without frayed borders and edges and with low density of crystalline defects, has been unveiled via helium ion, Raman, and transmission electron microscopies down to the atomic scale. Most importantly, nanoscanning photoemission unravels a 3D NPG structure with preserved 2D electronic density of states (Dirac cone like) throughout the porous sample. Furthermore, the high spatial resolution brings to light the interrelationship between the topology and the morphology in the wrinkled and highly bent regions, where distorted sp2 C bonds, associated with sp3-like hybridization state, induce small energy gaps. This highly connected graphene structure with a 3D skeleton overcomes the limitations of small-sized individual graphene sheets and opens a new route for a plethora of applications of the 2D graphene properties in 3D devices.
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INTRODUCTION Graphene is undoubtedly emerging as one of the most promising nanomaterials with high electron mobility, high thermal conductivity, and high tensile strength,1 opening a new perspective for technological applications ranging from electronics to optics, plasmonics, sensors, and biodevices. Recent years have witnessed many breakthroughs in research on graphene, as well as a significant advance in its mass production. Graphene can revolutionize industrial applications when large-area sheets with the same outstanding performance as the ideal suspended graphene are realized. It maximizes the surface area per weight but, for many devices, it is useful to pack the individual two-dimensional (2D) flakes into a threedimensional (3D) arrangement to minimize the volume while increasing its surface area. The employment of a single © 2017 American Chemical Society
graphene sheet in 3D devices is not straightforward, and a strong research effort is oriented toward the design of such 3D architectures,2−4 preserving the remarkable electronic, optical, and transport properties of suspended 2D sheets. The design challenges of 3D nanoporous graphene (NPG) structures are focused on enhancing the surface active areas and on ensuring a topological structure with highly connected layers and negligible density of lattice and edge defects, to engineer physical and chemical properties for the desired functionalities.4,5 A number of methods have been employed to prepare graphene in 3D architectures,6−8 but the undesired density of Received: May 30, 2017 Accepted: July 5, 2017 Published: July 18, 2017 3691
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Figure 1. NPG sample. (a,b) HIM images at different magnifications, taken with helium beam energy E = 25 keV, (c) low-resolution TEM image, (d,e) high-resolution TEM images, and (f) TEM diffraction pattern and zoomed images of the first diffraction spots around (0,0).
crystal and topological defects may strongly reduce the electrical and thermal conductivities and influence the operation of electronic devices. High interconnectivity, low defect density, and tunable nanopore sizes can be obtained by growing high-quality 3D NPG by means of Ni-based chemical vapor deposition (CVD).3 These NPG samples are not constituted by an assembly of graphene flakes, but they contain thousands of suspended graphene planes stacked in a small volume, with a high crystalline order, continuously interconnected in the 3D space, and decorated with pores in the 0.2−2 μm scale,3 and they can be an ideal prototype to engineer highly responsive electronic devices.9,10 The realization of 2D graphene millimeter-sized samples with a large surface area (1200 m2/g)3 into a 3D skeleton overcomes the limitations of the small-scale size of individual graphene flakes11 and can pave a new route for technological applications, if the outstanding 2D electronic properties of graphene are retained in the 3D NPG samples. In this work, we demonstrate with a precise electronic characterization of 3D NPG, by combining high energy and spatially resolved photoelectron and Raman spectroscopy at the submicrometer scale, that the 2D Dirac cone electronic spectral density is dominant in the 3D nanoarchitecture. Nowadays, Raman microscopy is widely recognized as one of the most powerful methods to assess the quality of graphene and carbonbased materials, as it allows to identify the number of interconnected layers, the stacking, the orientation, the density of defects, and the nature of edges, strain, and doping.12−14 Rarely, it has been combined with the state-of-the-art nanoimaging photoemission, sensitive to the electronic structure and to the degree of hybridization, to achieve an all-round and detailed correlation between the electronic, dynamical, and structural properties in carbon-based systems. Herewith, we will employ nanoscanning photoemission at even higher spatial resolution than that of Raman microscopy, to carefully image the degree of sp2 hybridization proper of graphene and, most importantly, the spectral density at the Fermi level as a function of the NPG topology. We exploit the potentialities of these spatially resolved state-of-the-art spectromicroscopies to locally identify in the 3D structure the hallmarks (deviations) of the 2D graphene electronic and
vibrational properties as a function of the topology. In particular, the C 1s core level associated with the pure sp2 hybridization is accompanied with distorted bonds associated to an sp3-like configuration in the wrinkled regions. The accurate control of the electronic state mapping, strictly associated with the morphology of NPG, shows a dominant linear slope of the spectral density of states (DOS) close to the Fermi level with a tiny gap in the wrinkled regions. Moreover, the average electronic response of 3D NPG samples has been firmly established as preserving the 2D graphene properties, corroborating that these 3D NPG architectures can be elected as favorite candidates to integrate and engineer 2D graphene in 3D devices.9
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RESULTS AND DISCUSSION The NPG sample, prepared as detailed in Section 1 of the Supporting Information, after mild annealing in ultrahigh vacuum (UHV) shows high purity and absence of residual contaminants and/or doping, as detected by core-level photoemission spectroscopy (Section 3 of Supporting Information). The free-standing nanoporous 3D graphene sample, depicted by helium ion microscopy (HIM) and transmission electron microscopy (TEM) images reported in Figure 1a−c, presents large flat areas decorated by pores with diameters in the range 0.5−1.0 μm, appearing like a pierced sheet folded in layers with convex and concave curvatures, wrinkles, and interconnected channels without frayed edges. It is worth noticing that the very high surface sensitivity of HIM15 allows the probing of few graphene layers, thus revealing in detail the 3D and complex nature of the sample morphology of the outermost layer. The high crystalline quality of the sample is deduced by high-resolution TEM images taken at different spatial scales, shown in Figure 1d,e, where the hexagonal graphene crystal lattice is well visible over a large scale with a well-defined diffraction pattern (f). The hexagonal moiré superstructure (e) and the parallel straight bands (top-left corner of panel d) found in some regions of the NPG sample suggest the presence of misoriented bilayers. The hexagonal moiré superstructures singled out in the TEM images have periodicities of about 1.4 and 2.4 nm and can be explained by assuming misoriented non-Bernal-stacked AB 3692
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Figure 2. NPG sample. Spatially resolved micro-Raman maps of the 2D/G (a) and D/G (b) Raman peak intensity ratios; 12 × 12 μm2 images formed by 300 × 300 nm2 pixels. Micro-Raman spectrum taken onto a 500 nm-diameter spot (d) with the distribution of the 2D/G integral intensity ratio taken onto a 10 × 10 μm2 area (c).
bilayers with a relative angular shift of about 10° and 6°,16 respectively, in agreement with the angular difference between the local multi-spot diffraction pattern reported in Figure 1f (see Section 2 of Supporting Information). The straight band modulation seen in a few zones of the sample (see the top-left zone of Figure 1d) can also be attributed to the moiré modulation induced by parallelogram misfit bilayers,16 owing to the tilted projection as observed by TEM,17 intrinsic to the warped geometry of NPG. The sample appears as constituted by a suspended, interconnected, and continuous graphene layer with misoriented bilayers in some regions. The presence of layers with various distances, stacking, orientations, and degree of π-orbital hybridization can be confirmed by spectromicroscopy analysis. A selected micro-Raman spectrum on the NPG sample taken in 300 nm sized pixels is shown in Figure 2d. At first sight, the low intensity of the “D” Raman peak and the high intensity of the “2D” band suggest the presence of a high-quality graphene sample constituted by a majority of interconnected single layers (SLs). In fact, the “G” band (sp2 C−C stretching mode) is at 1580.6 cm−1 over the whole sample, the “2D” band (doubleresonant second-order mode activated by in-plane breathing of the hexagonal rings) is at 2693.0 cm−1, slightly blue-shifted with respect to SL graphene, and the very small “D” band (activated by the presence of lattice defects) is at 1356 cm−1, as determined by the fitting analysis (detailed in Section 4.1 of the Supporting Information). The symmetric line shape of the “2D” band rules out effects of π-orbital hybridization between adjacent AB Bernal-stacked graphene sheets, which would induce splitting into four components and a definite band asymmetry.13,18 A quality proof of the NPG sample can be obtained by mapping the I2D/IG and ID/IG intensity ratios, whose imaging over a 12 × 12 μm2 area constituted by 300 × 300 nm2 pixels is presented in Figure 2a,b. Large flat areas of hundreds of nanometers are clearly identified for I2D/IG, in agreement with the HIM/TEM images at the same scale. The histogram of the I2D/IG ratio estimated over the whole probed area (Figure 2c) assesses the high average quality of the sample, with a mean value of the distribution of 2.6 and a width (σ = 0.6) reflecting the variety of morphological configurations/orientations in this undoped and contaminant-free NPG sample. This high value of the I2D/IG ratio is consistent with the presence of one-to-two layers of planar graphene, though curvatures in NPG may influence its absolute value. Uniaxial and biaxial strain effects in the hexagonal lattice in graphene-based systems have been proposed to justify variations of the Raman peak positions associated with the hexagonal lattice change.19,20 Tensile (compressive) strain can
induce a phonon softening (stiffening), leading to a red (blue) shift and broadening of the “2D” and “G” bands. We observe a small stiffening of the “2D” band, compatible with a slight compressive strain on the order of 0.3%,21 likely to be attributed to the drying process after NPG growth. Different orientations between adjacent misoriented bilayers can induce Raman band broadening,18,22−25 in very good agreement with the high-resolution TEM images (Figure 1d,e). Thus, the symmetric line shape of the “2D” band with a wider width (54 cm−1) than that expected at SL graphene can be associated with the coexistence of continuous SL graphene with some regions of disoriented non-Bernal-stacked bilayers,18,22−25 owing to NPG preparation on Ni below 1000 °C,22 that can generate turbostratically stacked bilayers.22,26−28 The non-homogeneous grainy ID/IG imaging, mirroring the defect distribution density, is inversely proportional to the I2D/ IG image in terms of brighter versus darker regions (Figure 2a,b).29 This mapping unveils a very low defect intensity, with the presence of 5−7 lattice distortions from pure hexagons only in the complementary regions where the I2D/IG intensity ratio is lower, confirming the high-spatial-resolution TEM images.3 These defects, despite appearing with a very low density, are intrinsically associated with the curvature necessary to warp graphene into the 3D NPG structure, as previously reported in refs 2 3, and 9. The D/G intensity ratio can also be directly related to the average crystallite size (i.e., average distance between two defects/edges), according to the Tuinstra−Koenig relation:30 La (nm) = 2.4 × 10−10 × λ4 × IG/ID. In this NPG sample, average La results about 225 nm (λ being 532 nm), in agreement with the typical size of the structures as observed in the aforementioned microscopy data. The Raman spectra demonstrate that the NPG 3D architecture is indeed very similar to that of ideal decoupled and suspended graphene layers, with a low density of defects over all of the NPG specimen. These results have been verified also for NPG samples with smaller nanopore size, although the intensity of the “D” Raman peak is slightly higher in this case because of a larger curvature gradient in the pore regions (see Section 4.2 of Supporting Information).3,18 The topology as observed by HIM, TEM, and Raman microspectroscopy allows us to define this 3D NPG architecture as composed by highly interconnected graphene sheets, where only a slight compressive strain and the presence of rotational misoriented bilayer graphene are observed. These lines of evidence and the absence of interface interactions, frayed borders, and edge defects could provide a novel route to exploit this 3D NPG with the desirable electronic properties of an ideal suspended 2D graphene. However, only a spatially resolved analysis of the electronic states via the very surface-sensitive nanoscanning photoelectron 3693
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linear spectral density toward the Fermi level, reflecting the typical lineshape measured on suspended graphene.32 It is worth noting that these data are very surface sensitive, owing to the chosen photon energy (hν = 350 and 100 eV, for the C 1s and VB data, respectively) guaranteeing a photoelectron kinetic energy at the minimum escape depth (only few Å).33 The photoemission data are therefore related to non-interacting graphene layers at the surface of the NPG sample. Although the averaged spatial signal shows the dominant 2D signatures of suspended graphene, the spatial distribution of the hallmarks of graphene is essential to disentangle the chemical, optical, transport, and electronic properties of NPG structures. In the following, both chemical imaging and electronic imaging, using high energetic and spatial resolution nanoscanning photoemission, have been combined to determine directly the sp2/sp3 degree of hybridization throughout the sample as well as its relation with the DOS at the Fermi level. Recently, high energy and angular resolution nanoscanning photoemission measurements of core levels and valence band at a given momentum, with a spatial resolution of a few hundred nanometer scale, have been made possible,34−36 combining information on the chemical sensitivity and hybridization state (core levels), with the spectral density close to the Fermi level (valence band) at the same scale. In the last decade, disentangling the actual carbon chemical state in sp2-based nanostructures (such as C nanotubes)37,38 with a resolution down to few hundred nanometers has been a great challenge. This innovative spectromicroscopy approach applied to the NPG sample paves the way for imaging electronic states at new frontiers because a combined analysis of both the C 1s and the spectral density close to EF for graphene structures at the nanoscale is still lacking. The spatially resolved C 1s mapping of the NPG sample taken on 300 × 300 nm2 size pixels is shown in Figure 4. At this
spectroscopy can verify whether NPG presents the properties of 2D graphene and whether we can associate different hybridization states and electronic spectral DOS with the different spatial zones of the actual NPG samples, namely, at flat and at bent/wrinkled regions. The precise topological and structural description obtained by HIM and TEM together with Raman mapping does not give univocal hallmarks of the electronic properties of 2D NPG. The spatially integrated C 1s and valence band spectra of the NPG sample compared with those taken on HOPG are shown in Figure 3a,b. The C 1s centroid (Figure 3a) is located almost
Figure 3. (a) Spatially integrated C 1s spectrum of the NPG sample and of highly oriented pyrolitic graphite (HOPG) shown for comparison (gray line), photon energy of 350 eV; C 1s intensity spatial mapping (50 × 50 μm2 pixel size) reported in the inset and (b) spatially integrated valence-band spectrum of the NPG sample and of HOPG shown for comparison (gray line), photon energy of 100 eV; in the inset, zoomed region around the Fermi level.
at the same binding energy (BE; 284.4 eV) attained at HOPG (284.3 eV), with a broader lineshape likely to be attributed to the presence of C 1s multicomponent at higher BE.31 The angle-integrated photoelectron spectroscopy valence band data (Figure 3b) allow the identification of both the σ-band, at about 7.7 eV BE, the π-band, centered at about 3.1 eV BE, and a
Figure 4. Spatially resolved C 1s core-level mapping of the NPG sample on 12 × 12 μm2 area, constituted by 300 × 300 nm2 pixels, taken with 350 eV photon energy, is reported in panel (a), showing the typical tubular-shaped structures of the sample. The C 1s spectrum spatially averaged over the mapping is plotted in panel (d), whose two components are fitted with sp2-like (284.4 eV) and sp3-like (285.1 eV) peaks, after subtraction of a Shirley background (dashed lines). The sp2-like and sp3-like mappings are obtained by energy integrating (0.6 eV energy windows) around either 284.4 or 285.1 eV BE, and they are reported in panels (b) and (c), respectively. The C 1s core-level spectra with the dominant sp2-like component (red star in the total mapping a) and with a more intense sp3-like component (blue star in the total mapping a) are reported in panels (e) and (f), respectively. The tubular-shaped structures of the sample are also reflected in the sp2-like mapping (e) representative of the flatter areas, whereas the sp3-like mapping (f) associated with the highly bent/wrinkled regions highlight their complementary spatial distribution. Color scales of maps are normalized to the maximum intensity of the corresponding peak. 3694
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Figure 5. Spatially resolved valence band taken at 100 eV photon energy on the NPG sample with 300 nm spatial resolution. Left panel (a) intensity map of the valence band signal taken over 300 × 300 nm2 pixels in 12 × 12 μm2 sized zone. Center (b) and right (c) panels: spectral DOS in the low-BE region taken at flat area (b) and edge (c) zones marked by red and blue stars, respectively, in the mapping; insets: zoomed energy regions close to EF, showing either a linearly decreasing (b) or an edge-like DOS toward EF (c); data (dotted lines) with superimposed linear fit (b) or linear + Gaussian fit multiplied by the steplike Fermi−Dirac distribution function (c).
The most important spectroscopic signature of 2D graphene is the linear DOS toward the Fermi level, reflecting the Dirac cone band. A detailed spatial mapping can correlate the sample topology to the DOS close to the Fermi level, which could have consequences on the electrical/thermal conductivities of the NPG. Spatially resolved DOS photoelectron spectroscopy data of the NPG sample taken in the first few electronvolts below the Fermi level (EF) in a 12 × 12 μm2 spot, with a high spatial resolution at the submicrometer scale (300 × 300 nm2), are shown in Figure 5a. A point-to-point analysis of the spatially resolved spectra reveals the dominance of data with the following characteristics: (i) a spectral density with a common linear shape toward EF, in agreement with the expected DOS for ideal graphene with a Dirac cone dispersion,32 (ii) a peak at about 3.1 eV owing to the 2p-π states, and (iii) a bump associated with σ−π states at higher BE. In few regions, corresponding to the edges of the tubular-shaped forms of the mapping, we observe a reduction in the 2p-π state, which is more intense in pure sp2 hybridization, and it is expected to be reduced as the distortion toward sp3like bonds progresses, as in hydrogenated graphene.44 In Figure 5b,c, we present two exemplary VB spectra taken in flat and bent/wrinkled regions of that spectroscopy mapping. By focusing on the binding energies right below EF, a linear fit perfectly matches the DOS in the flat regions of the sample (inset of Figure 5b), whereas the same kind of fit does not match appropriately the complementary regions (inset to Figure 5c). We suggest these regions to be related to the wrinkled/highly bent areas of the NPG sample, where the presence of the distortion leads to sp3-like hybridized states. By adding a Gaussian contribution to the linear spectral density and multiplying the curve by the edge-like Fermi−Dirac distribution function calculated at 80 K, we observe a tiny finite DOS contribution at a few tenths of electronvolts below the Fermi level. In summary, the DOS mapping corroborates the spatial resolved spectroscopic results obtained from the sp2-like and sp3-like bonds in Figure 5. Certainly, the feature at ≈3.1 eV BE, with sp2-like character, shows a dominant distribution with areas of the order of several micrometer size. By mapping the total spectral density, the sp2-like distribution persists, indicating that the DOS of the NPG sample is dominated by the electronic 2D graphene-like character. Interestingly,
scale, we clearly identify everywhere in the probed area two components in the C 1s feature, fitted by two asymmetric pseudo-Voigt (Gaussian and Lorentzian) curves, the dominant component centered at 284.4 (sp2-like) and the smaller component centered at 285.1 eV, whose energy value suggests its attribution to a distortion of the perfect sp2 bonds of graphene toward an sp3-like hybridization state.39−41 The relative intensity ratio of the two components varies in the mapping, depending on the topology of the NPG zone. To correlate the bond distortion with the morphology of the NPG sample, the intensity spatial mappings generated by selecting the energy regions centered on the main component at 284.4 (sp2-like) and on the component at 285.1 (sp3-like) are reported in Figure 4 (middle and right panels, respectively). The images are obtained by integrating the data in a 0.6 eV energy window around 284.4 and 285.1 eV. While we observe the same general diagonal-shaped structures in both images (dominated by the main sp2 component), the sp3-like component prevails in the border areas of the elongated tubular regions. Wrinkles and highly bent regions are indeed expected to induce some of the carbon atoms to partially warp the sp2 bonding and rehybridize toward an sp3-like configuration, generating a high BE weight in the spectra. We exclude everywhere in the sample the presence of contaminants or oxidation, as revealed in the survey photoemission spectrum shown in Section 3 of the Supporting Information. Furthermore, the absence of a low-BE component associated with unsaturated in-plane C bonds42,43 points out the irrelevant density of edge defects, in agreement with the low “D” band intensity in the Raman spectra. The absence of frayed contours with armchair and/or zigzag edges confirms the bicontinuous topology, as suggested by Ito et al.4 The nanospectroscopy images in Figure 4 demonstrate that the very 2D graphene properties dominate in the NPG sample, with the prominent sp2 C 1s peak and the presence of a small component owing to distorted bonds. We notice that the same analysis carried out on an NPG sample with smaller pore size and higher curvature gradients reveals a slight intensity increase in the sp3-like component, as reported in Section 4.3 of the Supporting Information, but the dominant planar hybridization state is preserved. 3695
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were 1.3 Å. Further details are provided in the Supporting Information. The spectromicroscopy photoemission experiments were carried out at the ANTARES beamline (SOLEIL synchrotron radiation facility). The nano-X-ray photoelectrom spectroscopy (XPS) microscope is equipped with two Fresnel zone plates for beam focusing, whereas higher diffraction orders were eliminated, thanks to an order selection aperture. The sample was placed on a precision positioning stage located at the common focus point of the hemispherical Scienta R4000 analyzer (whose energy resolution is 0.005 eV) and the Fresnel zone plates, and this experimental setup was used both for the collection of point-mode spectra and imaging-mode spectra. In this mode, the photo-emitted electron intensity from the desired energy range is collected over the sample to form a 2D image resolved at the submicrometer range (pixel size of 300 × 300 nm2). Core-level and valence band spectra were taken with 350 and 100 eV photon energy, respectively. The analyzer pass energy was set to 100 eV (200 eV) for the spatially unresolved (resolved) mode. After insertion in UHV, the NPG sample was degassed at 500 °C for 2 h to minimize contamination from the environment. The base pressure of the UHV chamber was kept in the range 10−10 mbar, whereas the sample was cooled via liquid nitrogen (≃89 K) to avoid damaging the sample via radiation pressure.
mapping regions where that feature is less intense are able to show where the sp3-like bonds are present. Furthermore, these results enlighten the powerful approach of nanoscale photoemission, able to precisely unravel and discriminate the coexistence of even small sp3-like deformations in NPG materials strongly dominated by the 2D hallmark of graphene-like structures. In fact, the continuous topology, the absence of defects and sharp edges, and the linear spectral density can ensure a 2D graphene-like electrical conductivity (104 S/m)3 and mobility (5000 cm2/V/s)9 of these NPG sample.
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CONCLUSIONS These Raman and photoemission nanospectromicroscopy studies unveil that the NPG 3D structure is indeed very similar to that of ideal decoupled graphene layers. Thanks to the stateof-the-art nano-photoemission spectroscopy, we are able to correlate local electronic structures with the different spatial regions in a single component sample. The bicontinuous topology, imaged by scaling the spatial resolution down to the 300 nm scale, reveals highly interconnected graphene sheets, with only a slight compressive strain and presence of rotational misoriented bilayers. The very low defect density and the absence of frayed borders and edges optimize the 2D properties of this topologically bicontinuous and connected 3D structure. The presence of wrinkled and bent regions, where the distorted sp3-like bonds increase and the Dirac cone is perturbed with a tiny gap opening, does not invalidate the potentialities of these 3D NPG samples. The interconnected graphene sheets retain the structural, vibrational, electronic, and transport responses of the ideal 2D graphene, with a positive cost-benefit ratio to overcome the limitation of integrating graphene in 3D devices.
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ASSOCIATED CONTENT
S Supporting Information *
The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acsomega.7b00706. NPG synthesis preparation protocols and procedures; a wide-energy XPS spectrum with focus on the potential contamination; and TEM analysis of the moiré pattern, Raman fitting curves, and HIM, Raman, and C 1s XPS spectroscopy at the nanoscale on an NPG sample with smaller pore sizes (PDF)
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MATERIALS AND METHODS The NPG sample was synthesized by following the procedure described in detail in the Supporting Information: Ni30Mn70 ingots were used to generate nanoporous Ni and then loaded in a quartz tube for producing graphene by CVD into the template. The as-grown NPG, which inherited the spongy structure of the substrate, was then exfoliated by chemically removing the Ni substrate. HIM images were collected with the Zeiss Orion Nanofab helium ion microscope (Peabody, USA) located in the CARF Laboratories of the Queensland University of Technology (Brisbane, Australia), with a beam acceleration of 25 kV and a working distance of 14 mm. The secondary electron signal was collected with an Everhart−Thornley detector with 500 V collector bias. Micro-Raman spectra were acquired in the same facility by using a WITec alpha300R microscope (WITec GmbH, Ulm, Germany) equipped with a diode-pumped Nd:YAG laser, operating at 532 nm, focused through a 50× Zeiss objective (0.7NA) to obtain a spot size of about 250 nm. The Raman maps were collected in pixels of 300 × 300 nm2, and the laser power was kept at 1.0 mW to avoid beam damage. TEM images and diffraction patterns were taken with a JEOL JEM-2100F system equipped with two aberration correctors for the image- and probe-forming lens systems. High-resolution TEM observations were conducted at an accelerating voltage of 120.0 and 200.0 kV, both Cs correctors were optimized for image observations, and the point-to-point resolutions of TEM
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AUTHOR INFORMATION
Corresponding Author
*E-mail:
[email protected] (M.G.B.). ORCID
Carlo Mariani: 0000-0002-7979-1700 Mingwei Chen: 0000-0003-0145-3872 Maria Grazia Betti: 0000-0002-6244-0306 Notes
The authors declare no competing financial interest.
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ACKNOWLEDGMENTS We acknowledge Francesco Mauri for discussions and for critical reading of the manuscript and Enrico Casadio Tarabusi for useful discussions. This work was supported by Ateneo funds of Sapienza Università di Roma, FATA project of Regione Lazio, and partly sponsored by JST-PRESTO “Creation of Innovative Core Technology for Manufacture and Use of Energy Carriers from Renewable Energy”, JSPS KAKENHI grant number JP15H05473. The authors acknowledge the financial support of the Queensland Government (DSITI) through the Q-CAS project, “Graphene-based thin film Supercapacitors”. Dr. Llew Rintoul and Dr. Peter Hines are kindly acknowledged for the Raman microscopy and HIM 3696
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measurements, respectively, obtained at the Central Analytical Research Facility operated by the Institute for Future Environments (QUT). Access to CARF is supported by generous funding from the Science and Engineering Faculty (QUT). I.D.B. acknowledges the hospitality of the Science and Engineering Faculty and the Endeavour Fellowship funding and J. Lipton-Duffin for useful discussions. The Synchrotron SOLEIL is supported by the Centre National de la Recherche Scientifique (CNRS) and the Commissariat à l’Energie Atomique et aux Energies Alternatives (CEA), France.
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DOI: 10.1021/acsomega.7b00706 ACS Omega 2017, 2, 3691−3697
