Four self-made free surface electrospinning devices for high-throughput preparation of high-quality nanofibers

• Yue Fang and
• Lan Xu

Beilstein J. Nanotechnol. 2019, 10, 2261–2274, doi:10.3762/bjnano.10.218

• electric field vectors, and the largest resulting electric field intensity. Furthermore, the impact of the device design on the morphology and the yield of nanofibers was experimentally investigated. We found that the average diameter of the nanofibers prepared by the MFSE method was the largest. The size

• distribution of the nanofibers produced by the MBE device was the least uniform. In contrast, the size distributions of the nanofiber generated by the of MFSE and SSFSE devices were more uniform. These experimental data are in accordance with the results of the simulations and the theoretical analysis. Our

Design and facile synthesis of defect-rich C-MoS₂/rGO nanosheets for enhanced lithium–sulfur battery performance

• Chengxiang Tian,
• Juwei Wu,
• Zheng Ma,
• Bo Li,
• Pengcheng Li,
• Xiaotao Zu and
• Xia Xiang

Beilstein J. Nanotechnol. 2019, 10, 2251–2260, doi:10.3762/bjnano.10.217

• are almost completely removed during the hydrothermal synthesis and annealing process [41]. Full nitrogen sorption isotherms of the composites were measured to obtain the specific surface area and the pore size distribution. A type-IV isotherm with a type-H3 hysteresis loop in the relative pressure

• range of 0.45–1.0 P/P0 suggests the presence of a mesoporous structure, as displayed in Figure 5a. The specific surface area was calculated to be 131.72, 300.64, 539.16 m2·g−1 by using the Brunauer–Emmett–Teller (BET) method. The pore size distribution obtained from the Barrett–Joyner–Halenda (BJH

• carbon is reduced by hydrogen to cause further increase of carbon defects; and the crystallinity of the MoS2 nanosheets is further improved. This is consistent with the results of XRD and Raman. The pore size distribution of the composites exhibits a sharp peak at 3 nm and another broad peak at 40 nm

Nontoxic pyrite iron sulfide nanocrystals as second electron acceptor in PTB7:PC₇₁BM-based organic photovoltaic cells

• Olivia Amargós-Reyes,
• José-Luis Maldonado,
• Omar Martínez-Alvarez,
• María-Elena Nicho,
• José Santos-Cruz,
• Juan Nicasio-Collazo,
• Irving Caballero-Quintana and
• Concepción Arenas-Arrocena

Beilstein J. Nanotechnol. 2019, 10, 2238–2250, doi:10.3762/bjnano.10.216

• ) (Figure 2a and 2b). The size distribution of the NCs was determined with the Image J software (Figure 2c). The X-ray pattern of these NCs, reported in our previous work [48], showed peaks at 2θ = 28, 33, 37, 40.7, 47.5, 56, 61.5 and 64.5°, corresponding to the pyrite crystalline phase (pyrite JCPDS (Joint

• structure of PTB7 and PC71BM. a) and b) TEM images of the FeS2 NCs at the 50 and 100 nm scale and c) size distribution of the NCs. a) STM image of FeS2 deposited on HOPG substrate (thickness ≈20 nm) with 50 nm × 50 nm scan size and b) SEM image of FeS2 NCs (scale bar = 100 nm). a) Cyclic voltammograms of

Targeted therapeutic effect against the breast cancer cell line MCF-7 with a CuFe₂O₄/silica/cisplatin nanocomposite formulation

• B. Rabindran Jermy,
• Vijaya Ravinayagam,
• Widyan A. Alamoudi,
• Dana Almohazey,
• Hatim Dafalla,
• Lina Hussain Allehaibi,
• Abdulhadi Baykal,
• Muhammet S. Toprak and
• Thirunavukkarasu Somanathan

Beilstein J. Nanotechnol. 2019, 10, 2217–2228, doi:10.3762/bjnano.10.214

• improve the crystallinity. Such stabilization of the cubic phase of CuFe2O4 inside the pore channels of silica have been reported due to suppression of John–Teller distortion [16]. The surface area and pore size distribution of HYPS and CuFe2O4/HYPS were analyzed using BET theory and the nitrogen

• multifunctional theranostic applications, whereby the nanocomposite may be further engineered with biocompatible polymers, antioxidants and drugs. Powder XRD patterns of CuFe2O4/HYPS with different Cu concentrations (x = 0.08, 0.10, 0.12, 0.15 and 0.17). BET adsorption–desorption isotherm and pore size

• distribution of (a) HYPS and (b) 30 wt% CuFe2O4/HYPS. FTIR spectra of HYPS and 30 wt % CuFe2O4/HYPS. Transmission electron microscopy of (a, b) 30 wt % CuFe2O4/HYPS at different scale magnifications and (c, d) high-resolution TEM (HRTEM) images of CuFe2O4/HYPS. Vibrating sample magnetometer spectrum of 30 wt

Mannosylated brush copolymers based on poly(ethylene glycol) and poly(ε-caprolactone) as multivalent lectin-binding nanomaterials

• Stefania Ordanini,
• Wanda Celentano,
• Anna Bernardi and
• Francesco Cellesi

Beilstein J. Nanotechnol. 2019, 10, 2192–2206, doi:10.3762/bjnano.10.212

• size distribution by scattering intensity (%) was determined by the CONTIN algorithm, as provided by the Zetasizer software (Malvern, UK). Particle size distribution by volume (%) was calculated from the scattering intensity distributions by the Zetasizer software, by setting the refractive index of

• presence of the Man-H1 proton (1, lower) in the product demonstrate the formation of the mannosylated polymer (A4-PEG8-PCL2-Man2). TEM images of A4-PEG8-PCL2 10 mg/mL in water; size distribution is dominated by small nanoparticles (diameter ≤ 20 nm). DLS size distribution (vol %) of the glycopolymers PEG9

BergaCare SmartLipids: commercial lipophilic active concentrates for improved performance of dermal products

• Florence Olechowski,
• Rainer H. Müller and
• Sung Min Pyo

Beilstein J. Nanotechnol. 2019, 10, 2152–2162, doi:10.3762/bjnano.10.208

• intensity signal of the scattered laser light, which is used to calculate a so-called correlation function g(τ). The obtained mean diameter is the intensity-weighted so-called z-average (z-ave). The correlation function g(τ) can be converted to a size distribution by Fourier transformation. EU regulations

Improved adsorption and degradation performance by S-doping of (001)-TiO₂

• Xiao-Yu Sun,
• Xian Zhang,
• Xiao Sun,
• Ni-Xian Qian,
• Min Wang and
• Yong-Qing Ma

Beilstein J. Nanotechnol. 2019, 10, 2116–2127, doi:10.3762/bjnano.10.206

• Instruments, USA). The pore size distribution was calculated using the Barret–Joyner–Halenda (BJH) method. The photoluminescence (PL) was measured on a fluorescence spectrophotometer (F-4500, Hitachi, Japan). Electron spin resonance (ESR) signals of the reactive species spin trapped by 5,5-dimethyl-1

• sample 2-S2 (a) and the variation of the MB concentration C/C0 with time in the presence of 2-S0, 2-S0.5, 2-S1, 2-S2, 2-S3, 2-S4 and 2-S5 and commercial P25 TiO2 irradiated by a xenon lamp (b). Nitrogen adsorption–desorption isotherms of samples 2-S0, 2-S and 2-S5. The inset shows the pore size

• distribution calculated using the BJH method. The PL spectra of 2-S0, 2-S0.5, 2-S2, 2-S3 and 2-S5 using an excitation wavelength of λex = 300 nm. ESR spectra of radical adducts trapped by DMPO in 2-S0 (a, e), 2-S2 (b, f), 2-S3 (c, g), and 2-S2 (d, h) dispersions: (a, b, c, d) DMPO–•OH formed in aqueous

Microbubbles decorated with dendronized magnetic nanoparticles for biomedical imaging: effective stabilization via fluorous interactions

• Da Shi,
• Justine Wallyn,
• Dinh-Vu Nguyen,
• Francis Perton,
• Delphine Felder-Flesch,
• Sylvie Bégin-Colin,
• Mounir Maaloum and
• Marie Pierre Krafft

Beilstein J. Nanotechnol. 2019, 10, 2103–2115, doi:10.3762/bjnano.10.205

• their DPPC shell are provided in Table 2 and Figure 6. The addition of dendronized IONPs led to a significant change in the MB mean radius and the size distribution for all the dendronized IONPs investigated, confirming their presence in the MB shell. A mean radius as small as 1.0 ± 0.2 µm was obtained

Incorporation of doxorubicin in different polymer nanoparticles and their anticancer activity

• Sebastian Pieper,
• Hannah Onafuye,
• Dennis Mulac,
• Jindrich Cinatl Jr.,
• Mark N. Wass,
• Martin Michaelis and
• Klaus Langer

Beilstein J. Nanotechnol. 2019, 10, 2062–2072, doi:10.3762/bjnano.10.201

• ]. Optimisation is possible [39][42] but was not subject of this study focused on the comparison of different nanoparticle systems prepared by simple methods. Polydispersity indices smaller than 0.1 indicated a monodisperse size distribution for all nanoparticle preparations. Monodispersity and particle diameters

• particle size, size distribution and zeta potential Average particle size and the polydispersity were measured by photon correlation spectroscopy (PCS) using a Malvern zetasizer nano (Malvern Instruments, Herrenberg, Germany). The resulting particle suspensions were diluted 1:100 with purified water and

Synthesis of highly active ETS-10-based titanosilicate for heterogeneously catalyzed transesterification of triglycerides

• Muhammad A. Zaheer,
• David Poppitz,
• Khavar Feyzullayeva,
• Marianne Wenzel,
• Jörg Matysik,
• Radomir Ljupkovic,
• Aleksandra Zarubica,
• Alexander A. Karavaev,
• Andreas Pöppl,
• Roger Gläser and
• Muslim Dvoyashkin

Beilstein J. Nanotechnol. 2019, 10, 2039–2061, doi:10.3762/bjnano.10.200

• min, but more pronounced for longer treatment times (Figure 8). Despite these defects, the particle size distribution probed by laser diffraction revealed minor changes suggesting that treatment neither leads to dissolution of smaller particles, nor to detectable fractioning of the larger ones (Figure

Gold-coated plant virus as computed tomography imaging contrast agent

• Alaa A. A. Aljabali,
• Mazhar S. Al Zoubi,
• Khalid M. Al-Batanyeh,
• Ali Al-Radaideh,
• Mohammad A. Obeid,
• Abeer Al Sharabi,
• Walhan Alshaer,
• Bayan AbuFares,
• Tasnim Al-Zanati,
• Murtaza M. Tambuwala,
• Naveed Akbar and
• David J. Evans

Beilstein J. Nanotechnol. 2019, 10, 1983–1993, doi:10.3762/bjnano.10.195

• particles are listed in Table 1. The values are in accordance with the size observed from the TEM images and further confirms the narrow size distribution of the three types of Au-CPMV particles. The particle size measured by DLS is influenced by the substances adsorbed on the NP surface and by the

• . The particle size distribution obtained from NTA analysis (Figure 2A) showed a peaks of 51 ± 2 nm, 71 ± 3 nm and 100 ± 5 nm, respectively, with over 90% of the particles being within the measured size thus confirming the narrow size distribution. CPMV (uncoated particles) have an average diameter of

• DLS measurements were carried out per sample after 2 min waiting time to allow the solutions to be at rest. The hydrodynamic radius (intensity particle size distribution was used for all measurements) was calculated by the instrument from the translational diffusion coefficient using the Stokes

Porous silver-coated pNIPAM-co-AAc hydrogel nanocapsules

• William W. Bryan,
• Riddhiman Medhi,
• Maria D. Marquez,
• Supparesk Rittikulsittichai,
• Michael Tran and
• T. Randall Lee

Beilstein J. Nanotechnol. 2019, 10, 1973–1982, doi:10.3762/bjnano.10.194

• deposited on clean silicon wafers and thoroughly dried at room temperature overnight before obtaining the SEM images. The images at low magnification were taken to demonstrate good dispersion. The image analysis for size distribution was carried out using ImageJ software. Bare pNIPAM-co-AAc hydrogel

Magnetic properties of biofunctionalized iron oxide nanoparticles as magnetic resonance imaging contrast agents

• Natalia E. Gervits,
• Andrey A. Gippius,
• Alexey V. Tkachev,
• Evgeniy I. Demikhov,
• Sergey S. Starchikov,
• Igor S. Lyubutin,
• Alexander L. Vasiliev,
• Vladimir P. Chekhonin,
• Maxim A. Abakumov,
• Alevtina S. Semkina and
• Alexander G. Mazhuga

Beilstein J. Nanotechnol. 2019, 10, 1964–1972, doi:10.3762/bjnano.10.193

• within the coherent X-ray scattering region, and the size can be slightly different from the values obtained by transmission electron microscopy (TEM). The TEM images of the nanoparticles are presented in Figure 2. The particle size distribution estimated from the high-resolution TEM (HRTEM) images is

• shown in Figure 3. Roughly 70% of the particles are of 5–8 nm in diameter (half maximum of the size distribution) and all of them exhibit an equiaxed morphology. The analysis of the electron diffraction pattern along with the fast Fourier transform (FFT) patterns (see insets in Figure 2a and Figure 2b

• of 2.0, which is characteristic of magnetite Fe3O4. The distribution function in Hhf values is used for a number of reasons, such as the size distribution of the nanoparticles, the different nature of the interparticle interaction, lattice defects and surface effects [21]. According to Table 1 and

Synthesis and potent cytotoxic activity of a novel diosgenin derivative and its phytosomes against lung cancer cells

• Liang Xu,
• Dekang Xu,
• Ziying Li,
• Yu Gao and
• Haijun Chen

Beilstein J. Nanotechnol. 2019, 10, 1933–1942, doi:10.3762/bjnano.10.189

• size distribution of phytosomes seems a little broad. We used the thin-film hydration method followed by sonication to prepare the phytosomes in this study. The mean size and size distribution are significantly influenced by the sonication conditions. Further optimization of the formulation and the

Facile synthesis of carbon nanotube-supported NiO//Fe₂O₃ for all-solid-state supercapacitors

• Shengming Zhang,
• Xuhui Wang,
• Yan Li,
• Xuemei Mu,
• Yaxiong Zhang,
• Jingwei Du,
• Guo Liu,
• Xiaohui Hua,
• Yingzhuo Sheng,
• Erqing Xie and
• Zhenxing Zhang

Beilstein J. Nanotechnol. 2019, 10, 1923–1932, doi:10.3762/bjnano.10.188

• –Halenda (BJH) pore size distribution of CC-CNT@Fe2O3 are shown in Supporting Information File 1, Figure S4. It is a type-IV isotherm, indicating the mesoporous texture of the sample (Figure S4a, Supporting Information File 1). The BET surface area was found to be 24.9 m2·g−1, much larger than that of pure

• carbon cloth (0.2 m2·g−1). The pore size distribution (Figure S4b, Supporting Information File 1) shows that most pores have a size of 40–50 nm. The high surface area, and the mesopores can help the ion diffusion between electrode and electrolyte. The morphologies of CNT@Fe2O3 were further examined by

• CC-CNT substrate by the same method as Fe2O3. As shown in Figure 5a, NiO is homogeneously coated on CC-CNT forming porous structures. N2 adsorption–desorption isotherm and BJH pore size distribution of CC-CNT@NiO are shown in Supporting Information File 1, Figure S7. It is a type-IV isotherm

Preservation of rutin nanosuspensions without the use of preservatives

• Pascal L. Stahr and
• Cornelia M. Keck

Beilstein J. Nanotechnol. 2019, 10, 1902–1913, doi:10.3762/bjnano.10.185

• potential, antioxidant capacity and the microbial quality were determined and monitored over this period of time (Figure 1). Results and Discussion Production and characterization of nanosuspensions High-pressure homogenization yielded rutin nanosuspensions with a relatively broad size distribution, i.e

• the Poloxamer-stabilized formulations, which possessed a narrower size distribution, i.e., no agglomerates at the day of production (c.f. Table 2), were found to be more stable than the Plantacare-stabilized formulations with a broader size distribution due to a slight agglomeration of the

Toxicity and safety study of silver and gold nanoparticles functionalized with cysteine and glutathione

• Barbara Pem,
• Igor M. Pongrac,
• Lea Ulm,
• Ivan Pavičić,
• Valerije Vrček,
• Darija Domazet Jurašin,
• Marija Ljubojević,
• Adela Krivohlavek and
• Ivana Vinković Vrček

Beilstein J. Nanotechnol. 2019, 10, 1802–1817, doi:10.3762/bjnano.10.175

• NP stability, as the NPs are generally considered electrostatically stabilized when the absolute values of the zeta potential exceed 30 mV [70]. The size distribution of all NPs was bimodal and the AgNPs were generally smaller than the AuNPs (Table 1). TEM experiments showed a spherical shape for all

• . The obtained NPs were carefully characterized by means of size distribution and surface charge employing dynamic light scattering (DLS) and electrophoretic light scattering (ELS) methods. The visualization of the NPs was performed using TEM. The most stable AuNPs and AgNPs with similar physico

• (Malvern Instruments, Malvern, UK) with a green laser (532 nm), set at an angle of 173°. The size distribution of the NPs is expressed as the hydrodynamic diameter (dH) obtained from the size-volume distribution function and given as an average of 10 measurements. The surface charge was determined by

Lipid nanostructures for antioxidant delivery: a comparative preformulation study

• Elisabetta Esposito,
• Maddalena Sguizzato,
• Markus Drechsler,
• Paolo Mariani,
• Federica Carducci,
• Claudio Nastruzzi,
• Giuseppe Valacchi and
• Rita Cortesi

Beilstein J. Nanotechnol. 2019, 10, 1789–1801, doi:10.3762/bjnano.10.174

• e/nm2 at 200 kV. The images were digitally recorded by a CCD camera (Ultrascan 1000, Gatan) using an image processing system (GMS 1.9 software, Gatan). In addition, the size distribution of the nanoparticles was performed by measuring 1000 nanoparticles for each cryo-TEM image by the digital

• absent (Table 4). In addition, the extent of agglomeration was lower for NLC, probably due to the presence of the liquid lipid. Effect of lipid composition on nanoparticle size distribution The SLN and NLC dimensions, measured by PCS and expressed by the Z-average, Dz, are reported in Figure 1 and Table

Synthesis of nickel/gallium nanoalloys using a dual-source approach in 1-alkyl-3-methylimidazole ionic liquids

• Ilka Simon,
• Julius Hornung,
• Juri Barthel,
• Jörg Thomas,
• Maik Finze,
• Roland A. Fischer and
• Christoph Janiak

Beilstein J. Nanotechnol. 2019, 10, 1754–1767, doi:10.3762/bjnano.10.171

• at 230 °C, a black powder was obtained after 10 min. The TEM measurements show spherical and non-aggregated nanoparticles with a narrow size distribution of 3.0 ± 0.5 nm (Figure 1). To validate the intermetallic 1:1 NiGa phase of the obtained nanoparticles, powder X-ray diffraction pattern (P-XRD) or

• size distribution of 2.5 ± 0.5 nm ([BMIm][BF4], Supporting Information File 1, Figure S2 and Figure S3) and 5 ± 1 nm (PC, Supporting Information File 1, Figure S4). EDX quantification over different spots on the TEM grid also shows equimolar ratios of nickel to gallium (Supporting Information File 1

• the microwave reactor. Subsequently, the TEM images show spherical and crystalline nanoparticles with a small size distribution of 5 ± 1 nm (Figure 3). Through the increased decomposition time the particles were grown slightly larger. The metal composition quantification by EDX spectra from three

TiO₂/GO-coated functional separator to suppress polysulfide migration in lithium–sulfur batteries

• Ning Liu,
• Lu Wang,
• Taizhe Tan,
• Yan Zhao and
• Yongguang Zhang

Beilstein J. Nanotechnol. 2019, 10, 1726–1736, doi:10.3762/bjnano.10.168

• composite. The BET specific surface area of the TiO2/GO composite was determined to be 155.2 m2 g−1. Through the Barrett–Joyner–Halenda (BJH) analysis, the pore size distribution of TiO2/GO shows that the majority of the pores are around 2.9 and 7.4 nm. The rich porosity not only provides abundant pore

• mV. Schematic illustration of a Li/S battery with a TiO2/GO-coated functional separator. (a) XRD patterns of the as-spun and as-dealloyed Ti10Al90 alloy foils. (b) Raman spectra of TiO2, GO and the TiO2/GO composite. (c) TGA curve and (d) N2 adsorption–desorption isotherms and pore size distribution

Doxorubicin-loaded human serum albumin nanoparticles overcome transporter-mediated drug resistance in drug-adapted cancer cells

• Hannah Onafuye,
• Sebastian Pieper,
• Dennis Mulac,
• Jindrich Cinatl Jr.,
• Mark N. Wass,
• Klaus Langer and
• Martin Michaelis

Beilstein J. Nanotechnol. 2019, 10, 1707–1715, doi:10.3762/bjnano.10.166

• 460 and 500 nm and polydispersity indices in the range of 0.153 and 0.213, indicating a narrow but not monodisperse size distribution (Table 1). The spherical shape and narrow size distribution of HSA nanoparticles was confirmed by scanning electron microscopy (SEM) as depicted for nanoparticles

• amount detected in the collected supernatants. Determination of particle size distribution The average particle size and the polydispersity were measured by photon correlation spectroscopy (PCS) using a Malvern zetasizer nano instrument (Malvern Instruments, Herrenberg, Germany). The resulting particle

• -test was used for comparing two groups. Three and more groups were compared by ANOVA followed by the Student–Newman–Keuls test. P-values lower than 0.05 were considered to be significant. SEM confirmed the spherical shape and narrow size distribution of doxorubicin-loaded HSA (100%) nanoparticles

Upcycling of polyurethane waste by mechanochemistry: synthesis of N-doped porous carbon materials for supercapacitor applications

• Christina Schneidermann,
• Pascal Otto,
• Desirée Leistenschneider,
• Sven Grätz,
• Claudia Eßbach and
• Lars Borchardt

Beilstein J. Nanotechnol. 2019, 10, 1618–1627, doi:10.3762/bjnano.10.157

• (measured at −196 °C) and (B, D) cumulative pore size distribution (PSD) using QSDFT with cylindrical/slit-shaped pores of the samples (A, B): PUPC-800-1 (cyan), PUPC-800-2 (blue), PUPC-800-3 (green), and PU-BM-800 (black) and the samples (C, D): PUUPC-1-800 (green), PUUPC-2-800 (blue), PUUPC-3-800 (grey

High-temperature resistive gas sensors based on ZnO/SiC nanocomposites

• Vadim B. Platonov,
• Marina N. Rumyantseva,
• Alexander S. Frolov,
• Alexey D. Yapryntsev and
• Alexander M. Gaskov

Beilstein J. Nanotechnol. 2019, 10, 1537–1547, doi:10.3762/bjnano.10.151

• controllers (Bronkhorst). Synthesis scheme of nanocrystalline ZnO, SiC and ZnO/SiC nanocomposite materials. SEM micrographs of polymer nanofibers containing polycarbosilane (a) and zinc acetate (b). SEM micrographs of annealed SiC (c) and ZnO (d). (e) SEM micrograph of ZnO/SiC_45 nanocomposite. (f) Pore size

• distribution of annealed ZnO and SiC. X-ray diffraction patterns of (a) ZnO nanofibers and nanocrystalline SiC and (b) ZnO/SiC nanocomposites. The vertical solid and dotted lines correspond to ICDD 36-1451 (ZnO, wurtzite) and ICDD 29-1129 (SiC-3C polytype) references, respectively. FTIR spectra of ZnO

Development of a new hybrid approach combining AFM and SEM for the nanoparticle dimensional metrology

• Loïc Crouzier,
• Alexandra Delvallée,
• Sébastien Ducourtieux,
• Laurent Devoille,
• Guillaume Noircler,
• Christian Ulysse,
• Olivier Taché,
• Elodie Barruet,
• Christophe Tromas and
• Nicolas Feltin

Beilstein J. Nanotechnol. 2019, 10, 1523–1536, doi:10.3762/bjnano.10.150

• equality between their height and their lateral diameters. However, discrepancies between AFM and SEM measurements have been observed, showing significant deviation from sphericity as a function of the nanoparticle size. Keywords: AFM; hybrid metrology; nanoparticles; SEM; size distribution; uncertainty

• , binarizing the image to discriminate objects from the substrate, identifying each imaged nano-object, evaluating roughness and building the size distribution histogram by only counting isolated nanoparticles. NP agglomeration may induce errors in the measurements and should be avoided [1][11]. The program is

• of interest was identified and imaged by AFM (Figure 4a) and SEM (Figure 4b). From these measurements, the size distribution histograms of both techniques were created and are given in Figure 4c–f. The modal values of HAFM, DSEM, DFmin and DFmax measured on these 136 NPs have been found to be 24.8 nm

Synthesis of P- and N-doped carbon catalysts for the oxygen reduction reaction via controlled phosphoric acid treatment of folic acid

• Rieko Kobayashi,
• Takafumi Ishii,
• Yasuo Imashiro and
• Jun-ichi Ozaki

Beilstein J. Nanotechnol. 2019, 10, 1497–1510, doi:10.3762/bjnano.10.148

• from X-ray photoelectron spectra of P-series precursors (Table 1, for the naming scheme of the samples see section “Experimental”). The N2 adsorption isotherms together with the micropore size distribution curves are given in Figure S1 (Supporting Information File 1). The BET specific surface area

• Information File 1) with the micropore size distribution calculated by the MP-method. The BET-SSAs of these two carbon series exhibited different behaviors (Table 3), e.g., those of HH-series carbon materials were almost constant (ca. 30 m2·g−1) even though the corresponding precursors showed different BET