Pulsed laser in liquid grafting of gold nanoparticle–carbon support composites

• Madeleine K. Wilsey,
• Teona Taseska,
• Qishen Lyu,
• Connor P. Cox and
• Astrid M. Müller

Beilstein J. Nanotechnol. 2025, 16, 349–361, doi:10.3762/bjnano.16.26

• . Results and Discussion Carbon fiber paper served as electrode support material because graphite is cost-effective, scalable, and the premier electrode support material for reduction reactions [21]. Gold nanoparticles were laser grafted from aqueous HAuCl4 solution. The use of an aqueous liquid requires

• pyrolytic graphite (HOPG); edge-plane HOPG is expensive, brittle, and not amenable to large electrode areas. In general, graphitic basal-plane carbon atoms are unreactive, unlike those in graphene, because of the π-stacking interactions of adjacent graphite sheets. We reported an environmentally friendly

• nanosecond pulses, graphite has an effective absorption coefficient of 5 µm−1 [26], resulting in an ablation threshold fluence of 0.7 J·cm−2 [27]; thus, our chosen fluence was well below this ablation threshold. The critical melting fluence of graphite has been reported to be 0.13 J·cm−2 [28], suggesting

Graphene oxide–chloroquine conjugate induces DNA damage in A549 lung cancer cells through autophagy modulation

• Braham Dutt Arya,
• Sandeep Mittal,
• Prachi Joshi,
• Alok Kumar Pandey,
• Jaime E. Ramirez-Vick,
• Govind Gupta and
• Surinder P. Singh

Beilstein J. Nanotechnol. 2025, 16, 316–332, doi:10.3762/bjnano.16.24

• autophagy and DNA damage in response to GO–Chl exposure in human lung epithelial carcinoma (A549) cells. Experimental Materials Graphite powder (Cat. No. 282863), chloroquine (Cat. No. C6628), paraformaldehyde (PFA; Cat. No. 24-0630), dimethyl sulfoxide (DMSO; Cat. No. D2650), propidium iodide (Cat. No

• from Thermo Scientific Nunc (Rochester, New York). Synthesis of graphene oxide Highly exfoliated GO nanosheets were chemically synthesized using slight modifications to the method documented by Dimiev et al. [26][27]. Briefly, 0.5 g of graphite powder was treated with a mixture of 0.5 g of NaNO3 and 40

• , until a dark brownish precipitate appeared, followed by addition of 1.5 mL of H2O2 (30%) and 100 mL of ice-cold ultrapure water to stop the oxidation reaction and eliminate unreacted KMnO4. The chemistry involved in the chemical exfoliation of graphite is shown in Figure 1. The purified graphitic sheets

Fabrication and evaluation of BerNPs regarding the growth and development of Streptococcus mutans

• Tuyen Huu Nguyen,
• Hong Thanh Pham,
• Kieu Kim Thanh Nguyen,
• Loan Hong Ngo,
• Anh Ngoc Tuan Mai,
• Thu Hoang Anh Lam,
• Ngan Thi Kim Phan,
• Dung Tien Pham,
• Duong Thuy Hoang,
• Thuc Dong Nguyen and
• Lien Thi Xuan Truong

Beilstein J. Nanotechnol. 2025, 16, 308–315, doi:10.3762/bjnano.16.23

• tubes were incubated at 37 °C. After 24 h, the samples were fixed onto a graphite substrate, and FE-SEM imaging was performed. Inhibition of biofilm formation The Crystal Violet Biofilm Assay was used to evaluate the biofilm formation of S. mutans [43]. BerNPs solution was diluted in TSB + 1% sucrose

Emerging strategies in the sustainable removal of antibiotics using semiconductor-based photocatalysts

• Yunus Ahmed,
• Keya Rani Dutta,
• Parul Akhtar,
• Md. Arif Hossen,
• Md. Jahangir Alam,
• Obaid A. Alharbi,
• Hamad AlMohamadi and
• Abdul Wahab Mohammad

Beilstein J. Nanotechnol. 2025, 16, 264–285, doi:10.3762/bjnano.16.21

• level of reduction and the specific production techniques employed. GO is a type of insulating material that is made from graphene by oxidizing graphite. The reduction process eliminates functional groups in GO that contain oxygen, restoring π-conjugated structures and electrical conductivity. rGO has a

Radiosensitizing properties of dual-functionalized carbon nanostructures loaded with temozolomide

• Radmila Milenkovska,
• Nikola Geskovski,
• Dushko Shalabalija,
• Ljubica Mihailova,
• Petre Makreski,
• Dushko Lukarski,
• Igor Stojkovski,
• Maja Simonoska Crcarevska and
• Kristina Mladenovska

Beilstein J. Nanotechnol. 2025, 16, 229–251, doi:10.3762/bjnano.16.18

• significantly higher extent of functionalization with single-stranded DNA [64]. It was also shown that gamma radiation with low doses, 25 and 50 kGy, improved the graphite arrangement of MWCNTs; higher doses, 100 and 150 kGy, led to major structural deteriorations, while very high doses above 200 kGy distorted

• . In the diffractograms of non-irradiated and gamma ray-irradiated CNs (Figure 7), two peaks important for the graphite arrangement of MWCNTs [66] were recorded at 2θ angles of 26° and 43°. For the irradiated MWCNTs-COOH, a rise of the intensity of the 26° peak was observed pointing to an increase of

Fabrication of hafnium-based nanoparticles and nanostructures using picosecond laser ablation

• Abhishek Das,
• Mangababu Akkanaboina,
• Jagannath Rathod,
• R. Sai Prasad Goud,
• Kanaka Ravi Kumar,
• Raghu C. Reddy,
• Ratheesh Ravendran,
• Katia Vutova,
• S. V. S. Nageswara Rao and
• Venugopal Rao Soma

Beilstein J. Nanotechnol. 2024, 15, 1639–1653, doi:10.3762/bjnano.15.129

• liquids were used [34][35][36]. The d-spacing of the carbon shells was determined from the zoomed images in Figure 5. It was estimated to be ≈0.34 nm, confirming the outer shell to be made of graphite [37][38][39]. A similar analysis was conducted on the nanofibre-like structures formed when Hf was

• [11][31] did not discuss the formation of graphite shells around HfC NPs. The formation of polycrystalline HfC core–shell NPs with graphite shells similar to [36] in toluene and anisole can be explained by the possible reaction of carbon from decomposed surrounding liquid with Hf4+ ions in the plasma

• ][41][43]. The decomposed surrounding liquid has a carbon-rich environment. As the polycrystals grow, they also act as a nucleus for carbon atoms to self-assemble [27][50], forming graphite layers and, eventually, core–shell NPs of different sizes. This formation of graphite layers might prevent the

Electrochemical nanostructured CuBTC/FeBTC MOF composite sensor for enrofloxacin detection

• Thi Kim Ngan Nguyen,
• Tien Dat Doan,
• Huy Hieu Luu,
• Hoang Anh Nguyen,
• Thi Thu Ha Vu,
• Quang Hai Tran,
• Ha Tran Nguyen,
• Thanh Binh Dang,
• Thi Hai Yen Pham and
• Mai Ha Hoang

Beilstein J. Nanotechnol. 2024, 15, 1522–1535, doi:10.3762/bjnano.15.120

• the electrode blend, SEM and EDX mapping were used to investigate the distribution of CuBTC and FeBTC on the electrode surface (Figure 4). Figure 4a clearly shows the scattering of bright CuBTC and FeBTC particles on the graphite flakes. Figure 4b confirms the homogenous distribution of Fe, Cu, and O

• purchased from Thermo Fisher Scientific. Graphite powder and paraffin oil were supplied by Thermo Scientific Acros. Trimesic acid (H3BTC, 98%), CuCl2·2H2O (≥99%), FeCl3·6H2O (98%), N,N-dimethylformamide (DMF, 98%) and C2H5OH (96%), H3PO4 (85%), KOH (≥85.0%), KH2PO4 (≥99.5%), K2HPO4 (≥98.0%), KCl (>99.5

• of (Cu)(Fe)BTC@CPE Modified electrodes were prepared using a standardized procedure. CuBTC and FeBTC were carefully mixed to obtain a mixture called (Cu)(Fe)BTC. Then, paraffin oil, graphite powder, and (Cu)(Fe)BTC powder were combined in various weight ratios (as specified in Table 2) and thoroughly

Green synthesis of carbon dot structures from Rheum Ribes and Schottky diode fabrication

• Muhammed Taha Durmus and
• Ebru Bozkurt

Beilstein J. Nanotechnol. 2024, 15, 1369–1375, doi:10.3762/bjnano.15.110

• graphite lattice, while the G band is attributed to the vibrations of sp2-bonded carbon atoms in a 2D hexagonal lattice. The degree of defects in the CDs can be calculated from the relative intensity ratio (ID/IG) of two peaks of D band and G band. ID/IG was calculated to be approximately 0.69, indicating

Interaction of graphene oxide with tannic acid: computational modeling and toxicity mitigation in C. elegans

• Romana Petry,
• James M. de Almeida,
• Francine Côa,
• Felipe Crasto de Lima,
• Diego Stéfani T. Martinez and
• Adalberto Fazzio

Beilstein J. Nanotechnol. 2024, 15, 1297–1311, doi:10.3762/bjnano.15.105

• in surface engineering of graphene-based nanomaterials. Methods Materials GO was synthesized via chemical exfoliation of graphite by modified Hummers method [69] according to [70]. Graphite (5.0 g) and NaNO3 (3.75 mg) are added to a reaction flask in a bath of ice and covered with concentrated H2SO4

• (15 mL, 30% w/w) is added to complete the oxidation of graphite and the reduction of residual KMnO4; the mixture is left under stirring overnight. At the end, the material is precipitated by centrifugation and washed with H2SO4 (3.0%) and H2O2 (0.5%) to remove residues of oxidants and inorganic

Interface properties of nanostructured carbon-coated biological implants: an overview

• Mattia Bartoli,
• Francesca Cardano,
• Erik Piatti,
• Stefania Lettieri,
• Andrea Fin and
• Alberto Tagliaferro

Beilstein J. Nanotechnol. 2024, 15, 1041–1053, doi:10.3762/bjnano.15.85

• oxygen functionalities (hydroxy, epoxy, carbonyl, and carboxylic groups) arranged according to the Lerf–Klinowski model [45]. GO is generally produced through chemical oxidation and exfoliation of graphite flakes with different protocols to tune the oxygen content [46][47]. The defective structure of GO

• in 1991 [56]. CNTs can be described as single or multiple cylindrical graphite sheets rolled up in a tubular structure forming single-walled CNTs (SWCNTs) or multiwalled CNTs (MWCNTs). SWCNTs are characterized by diameters from 0.3 nm [57] to 1 nm [58], while the diameters of MWCNTs can reach 100 nm

Laser synthesis of nanoparticles in organic solvents – products, reactions, and perspectives

• Theo Fromme,
• Sven Reichenberger,
• Katharine M. Tibbetts and
• Stephan Barcikowski

Beilstein J. Nanotechnol. 2024, 15, 638–663, doi:10.3762/bjnano.15.54

• and the hydroxyl group forms the initial Au–H adduct needed for the catalytic reaction. Other alcohols, such as methanol or propanol, did not lead to carbyne formation during the experiments [139]. Condorelli et al. were able to synthesize carbon-encapsulated Pt nanoparticles by RLAL of graphite in a

• structures and graphitization during the LAL process are favored, resulting in a quick formation of graphite and, thus, no available fragments for the polyyne formation [101][144][145][146]. Considering these factors, the polyyne yield should be highly influenced by the applied fluence and undergo a maximum

• produce graphite structures. The carbon shell is a surface modification and, as such, affects the nanoparticles’ catalyst properties either positively [37][155] or negatively [149]. A low number of graphene layers on the surface of the nanoparticles was found to enhance the catalytic activity during

Exfoliation of titanium nitride using a non-thermal plasma process

• Priscila Jussiane Zambiazi,
• Dolores Ribeiro Ricci Lazar,
• Larissa Otubo,
• Rodrigo Fernando Brambilla de Souza,
• Almir Oliveira Neto and
• Cecilia Chaves Guedes-Silva

Beilstein J. Nanotechnol. 2024, 15, 631–637, doi:10.3762/bjnano.15.53

• flow. The arc was generated between a 316 L steel electrode and another electrode composed of graphite. The process lasted 60 min. Subsequently, the resultant material was collected, rinsed in a 1:1 mixture of water and isopropanol, and decanted for 24 h. Then, the liquid phase was filtered using a

Unveiling the nature of atomic defects in graphene on a metal surface

• Karl Rothe,
• Nicolas Néel and
• Jörg Kröger

Beilstein J. Nanotechnol. 2024, 15, 416–425, doi:10.3762/bjnano.15.37

• . Before presenting the AFM results, a comparison of the defect spectra in Figure 1d,e with previous results obtained for atomic-scale defects in graphene on other surfaces is noteworthy. Very pronounced electronic resonances localized at vacancy defects were reported for graphite surfaces [13], graphene

On the mechanism of piezoresistance in nanocrystalline graphite

• Sandeep Kumar,
• Simone Dehm and
• Ralph Krupke

Beilstein J. Nanotechnol. 2024, 15, 376–384, doi:10.3762/bjnano.15.34

• density of defects in the form of grain boundaries. It holds an advantage over graphene in easily achieving wafer-scale growth with controlled thickness. In this study, we explore the piezoresistivity in thin films of nanocrystalline graphite. Simultaneous measurements of sheet resistance and externally

• observed the plateau-like region as reported here, where the gauge factor is similar to the gauge factor at very low strain [24][33]. A plateau-like region has neither been observed in nanocrystalline graphite [33], amorphous carbon films [34], nor in metallic films [35]. The mechanism that leads to an

Controllable physicochemical properties of WO_x thin films grown under glancing angle

• Rupam Mandal,
• Aparajita Mandal,
• Alapan Dutta,
• Rengasamy Sivakumar,
• Sanjeev Kumar Srivastava and
• Tapobrata Som

Beilstein J. Nanotechnol. 2024, 15, 350–359, doi:10.3762/bjnano.15.31

• surface. The work function of the tip was estimated to be 4.94 eV by using highly oriented pyrolytic graphite as a reference, and the work functions of the films were estimated using Equation 2. Figure 4e depicts the variation in work function of NS-WOx films before and after annealing as a function of

Determining by Raman spectroscopy the average thickness and N-layer-specific surface coverages of MoS₂ thin films with domains much smaller than the laser spot size

• Felipe Wasem Klein,
• Jean-Roch Huntzinger,
• Vincent Astié,
• Damien Voiry,
• Romain Parret,
• Houssine Makhlouf,
• Sandrine Juillaguet,
• Jean-Manuel Decams,
• Sylvie Contreras,
• Périne Landois,
• Ahmed-Azmi Zahab,
• Jean-Louis Sauvajol and
• Matthieu Paillet

Beilstein J. Nanotechnol. 2024, 15, 279–296, doi:10.3762/bjnano.15.26

• ][8][9] because of a number of remarkable properties [10][11][12]. Particularly, it was found that the properties of layered TMDs drastically change when their thickness is reduced to a monolayer [13][14]. Layered TMD structures have a graphite-like structure with each graphene sheet replaced with an

Graphene removal by water-assisted focused electron-beam-induced etching – unveiling the dose and dwell time impact on the etch profile and topographical changes in SiO₂ substrates

• Aleksandra Szkudlarek,
• Jan M. Michalik,
• Inés Serrano-Esparza,
• Zdeněk Nováček,
• Veronika Novotná,
• Piotr Ozga,
• Czesław Kapusta and
• José María De Teresa

Beilstein J. Nanotechnol. 2024, 15, 190–198, doi:10.3762/bjnano.15.18

• graphene obtained with the standard Scotch© tape method [1] from highly oriented pyrolytic graphite (HOPG) to take advantage of the lack of residues on top of the graphene layer and the lowest possible amount of defects. Cleaved flakes were deposited onto doped Si with a 285 nm thick SiO2 layer. Optical

Modification of graphene oxide and its effect on properties of natural rubber/graphene oxide nanocomposites

• Nghiem Thi Thuong,
• Le Dinh Quang,
• Vu Quoc Cuong,
• Cao Hong Ha,
• Nguyen Ba Lam and
• Seiichi Kawahara

Beilstein J. Nanotechnol. 2024, 15, 168–179, doi:10.3762/bjnano.15.16

• natural rubber latex (HANR, dry rubber content (DRC) 60%) supplied by Dau-Tieng rubber company. Sodium dodecyl sulfate (SDS, 97%) was bought from Nacalai Tesque, Japan. Graphite flake powder (>99% purity) was obtained from Yen-Bai province, Vietnam. The compounds KMnO4, NaNO3 (analytical grade), and TEPA

• (0.2%). Preparation of graphene oxide and silanization with VTES The graphene oxide used in this work was synthesized from graphite flakes using a modified version of Hummers’ method [31], similar to those reported in [24]. About 1 g of graphite powder was put into 23 mL of concentrated H2SO4, and 0.5

• , 200 g of DPNR (DRC 20%, SDS 0.2%), and with the same amount of TEPA/TBHPO as in the preparation of DPNR/GO-VTES. Characterizations X-ray diffraction patterns of graphite and GO were acquired by using a Panalytical X'Pert Pro X-ray diffractometer. The measurements were performed at room temperature

Dual-heterodyne Kelvin probe force microscopy

• Benjamin Grévin,
• Fatima Husainy,
• Dmitry Aldakov and
• Cyril Aumaître

Beilstein J. Nanotechnol. 2023, 14, 1068–1084, doi:10.3762/bjnano.14.88

• reference substrate, a bulk organic photovoltaic heterojunction thin film, and an optoelectronic interface obtained by depositing caesium lead bromide perovskite nanosheets on a graphite surface. The conclusion provides perspectives for future improvements and applications. Keywords: heterodyne

• optoelectronic interfaces formed between caesium lead bromide perovskite nanosheets and highly oriented pyrolytic graphite. Kelvin Probe Force Microscopy Background, Amplitude-Modulated Heterodyne KPFM Many KPFM modes rely on the detection of a modulated component of the electrostatic force proportional to the

• plane of the substrate. Results and Discussion Dual-heterodyne Kelvin probe force microscopy under electrical pumping: benchmarking Similar to the case of pp-KPFM [11], we tested this new implementation by performing DHe-KPFM measurements under electrical pumping on a highly oriented pyrolytic graphite

Experimental investigation of usage of POE lubricants with Al₂O₃, graphene or CNT nanoparticles in a refrigeration compressor

• Kayhan Dağıdır and
• Kemal Bilen

Beilstein J. Nanotechnol. 2023, 14, 1041–1058, doi:10.3762/bjnano.14.86

• hexagonal graphite peak for the carbon nanotubes (JCPDS No. 41-1487). These peak placements correspond nicely with previous studies in the literature. Lubricant In this study, nanoparticles were added to the compressor lubricant. The lubricant of the compressor in the test installation was an EMKARATE RL

Two-dimensional molecular networks at the solid/liquid interface and the role of alkyl chains in their building blocks

• Suyi Liu,
• Yasuo Norikane and
• Yoshihiro Kikkawa

Beilstein J. Nanotechnol. 2023, 14, 872–892, doi:10.3762/bjnano.14.72

• flat conducting substrates, such as metal surfaces and highly oriented pyrolytic graphite (HOPG), under ultrahigh vacuum (UHV) conditions, at solid/air or solid/liquid interfaces [23][24][25][26][27][28]. Although UHV-STM offers high-resolution imaging, it requires large, complex, and expensive

• ) as a reference can provide precise 2D structures, including intermolecular distances and molecular orientations. To study the adsorption of alkane on graphite, computational simulations such as molecular mechanics and DFT calculations with the local density approximation have been applied [48][49][53

• the entire system. Furthermore, the alkyl chains exhibit lateral interactions upon dense packing, and the dispersion interactions increased by −0.50 kcal/mol per CH2 unit [47]. Although alkyl chains basically follow the HOPG lattice, lattice mismatch between n-alkanes and graphite has been reported

In situ magnesiothermic reduction synthesis of a Ge@C composite for high-performance lithium-ion batterie anodes

• Ha Tran Huu,
• Ngoc Phi Nguyen,
• Vuong Hoang Ngo,
• Huy Hoang Luc,
• Minh Kha Le,
• Minh Thu Nguyen,
• My Loan Phung Le,
• Hye Rim Kim,
• In Young Kim,
• Sung Jin Kim,
• Van Man Tran and
• Vien Vo

Beilstein J. Nanotechnol. 2023, 14, 751–761, doi:10.3762/bjnano.14.62

• systems have become the most popular energy storage systems, with applications from mobile devices to EVs and grid-scale storage [8][9]. However, the low specific theoretical capacity of graphite limits the energy density of the commercial LIBs [10][11][12][13]. Germanium, as a lithium alloying material

• , is a possible alternative for graphite electrodes due to its high theoretical capacity of 1623 mAh·g−1 (four times higher than that of graphite) and good rate performance due to high electronic (2.1 S·m−1, 1 × 104 times higher than that of silicon) and ionic (6.51 × 10−12 cm2·s−1, 400 times higher

• Fd−3m, JCPDS card No. 04-0545). There is no observable signal related to the GeO2 precursor. The XRD pattern of the BC-800 carbon material exhibits a diffraction signal at 2θ = 26.3° attributed to the (002) plane of disordered graphite-like carbon. The peaks at 2θ = 28.1° and 44.0° correspond to the

Control of morphology and crystallinity of CNTs in flame synthesis with one-dimensional reaction zone

• Muhammad Hilmi Ibrahim,
• Norikhwan Hamzah,
• Mohd Zamri Mohd Yusop,
• Ni Luh Wulan Septiani and
• Mohd Fairus Mohd Yasin

Beilstein J. Nanotechnol. 2023, 14, 741–750, doi:10.3762/bjnano.14.61

• that the products of both syntheses are MWCNTs. In addition, the broad asymmetric feature in the G band is a property of MWCNTs, rather than of SWCNTs or graphite, which have a double peak or a narrow peak, respectively. The D band (ID) and G band (IG) intensities show an ID/IG ratio of less than 1.00

Cross-sectional Kelvin probe force microscopy on III–V epitaxial multilayer stacks: challenges and perspectives

• Mattia da Lisca,
• José Alvarez,
• James P. Connolly,
• Nicolas Vaissiere,
• Karim Mekhazni,
• Jean Decobert and
• Jean-Paul Kleider

Beilstein J. Nanotechnol. 2023, 14, 725–737, doi:10.3762/bjnano.14.59

• periodically in the course of the analysis using Equation 1 by measuring the VCPD value of a freshly exfoliated surface of highly ordered pyrolytic graphite (HOPG) with ϕsample being equal to 4.6 eV [19]. The successively measured ϕtip values showed only small variations with values ranging between 5.65 and

On the use of Raman spectroscopy to characterize mass-produced graphene nanoplatelets

• Keith R. Paton,
• Konstantinos Despotelis,
• Naresh Kumar,
• Piers Turner and
• Andrew J. Pollard

Beilstein J. Nanotechnol. 2023, 14, 509–521, doi:10.3762/bjnano.14.42

• separation of unexfoliated materials. In this work we assess these metrics when applied to non-ideal samples, where unexfoliated graphite has been deliberately added to the exfoliated material. We demonstrate that previously published metrics, when applied to averaged spectra, do not allow the presence of

• particular the absence of graphite or nanoscale graphite. It is important to recall that graphene has been defined as a “single layer of carbon atoms with each atom bound to three neighbours in a honeycomb structure” with materials with more than one layer defined as “few-layer graphene” or “graphene

• nanoplatelets” [6]. This assessment is generally based on examining the shape of the so-called 2D peak (ca. 2700 cm−1), which, for Bernal stacking, shows clear changes on going from single-layer through few-layer graphene to graphite [19]. Bulk graphite typically shows a signal comprising two components