Ultrathin water layers on mannosylated gold nanoparticles

• Maiara A. Iriarte Alonso,
• Jorge H. Melillo,
• Silvina Cerveny,
• Yujin Tong and
• Alexander M. Bittner

Beilstein J. Nanotechnol. 2025, 16, 2183–2198, doi:10.3762/bjnano.16.151

• overnight sample incubation to reach 90 ± 5% RH, corresponding to very wet climate or air during precipitation. In addition, we refer to “hydrophilic conditions” in AFM for hydrophilic surfaces (APDMES silicon) scanned by a silicon tip. We found a vertical resolution (∆z) of 0.04 nm and a surface roughness

Molecular and mechanical insights into gecko seta adhesion: multiscale simulations combining molecular dynamics and the finite element method

• Yash Jain,
• Saeed Norouzi,
• Tobias Materzok,
• Stanislav N. Gorb and
• Florian Müller-Plathe

Beilstein J. Nanotechnol. 2025, 16, 2055–2076, doi:10.3762/bjnano.16.141

• , surface roughness, substrate deformability, and explicit long-range electrostatics for hydrophilic systems, which will necessitate thicker substrate models. The coupling between each molecular spatula and the FE seta was handled via a bridging domain (BD), described in section “Methods”. Methods

Beyond the shell: exploring polymer–lipid interfaces in core–shell nanofibers to carry hyaluronic acid and β-caryophyllene

• Aline Tavares da Silva Barreto,
• Francisco Alexandrino-Júnior,
• Bráulio Soares Arcanjo,
• Paulo Henrique de Souza Picciani and
• Kattya Gyselle de Holanda e Silva

Beilstein J. Nanotechnol. 2025, 16, 2015–2033, doi:10.3762/bjnano.16.139

• unimodal distribution with a polydispersity index (PDI) range of 0.218. Most of the formed nanoemulsions are small in size and well distributed (Figure 1). The most favorable processing conditions for obtaining uniform fibers – free of surface roughness and with fewer beads – were determined based on

Mechanical property measurements enabled by short-term Fourier-transform of atomic force microscopy thermal deflection analysis

• Thomas Mathias,
• Roland Bennewitz and
• Philip Egberts

Beilstein J. Nanotechnol. 2025, 16, 1952–1962, doi:10.3762/bjnano.16.136

• probe, local surface roughness will yield a much smaller contact radius than the overall probe shape, it is still significantly larger than predicted by the models in Figure 5. In summary, we have used longstanding analytical models to convert the measured variation in cantilever resonant frequency with

Electrical, photocatalytic, and sensory properties of graphene oxide and polyimide implanted with low- and medium-energy silver ions

• Josef Novák,
• Eva Štěpanovská,
• Petr Malinský,
• Vlastimil Mazánek,
• Jan Luxa,
• Ulrich Kentsch and
• Zdeněk Sofer

Beilstein J. Nanotechnol. 2025, 16, 1794–1811, doi:10.3762/bjnano.16.123

• sputtering and the increase in surface roughness during implantation may result in a shallower experimental profile than predicted. Differences can also arise from the finite depth resolution of RBS, which is influenced by energy straggling and multiple scattering effects, leading to a broadening of the

• in an overall decrease in surface roughness compared to the untreated material, regardless of the specific ion fluence. The minimum roughness was attained with an ion fluence of 3.75 × 1012 cm−2, measuring 64 nm. A comparable trend is evident when PI is implanted with 1.5 MeV Ag ions wherein a

• reduction in roughness is observable at any ion fluence relative to the reference condition. The lowest roughness in this instance was achieved with an ion fluence of 3.75 × 1012 cm−2. One possible explanation for the change in surface roughness measured by AFM may be surface sputtering. When there is

Photocatalytic degradation of ofloxacin in water assisted by TiO₂ nanowires on carbon cloth: contributions of H₂O₂ addition and substrate absorbability

• Iram Hussain,
• Lisha Zhang,
• Zhizhen Ye and
• Jin-Ming Wu

Beilstein J. Nanotechnol. 2025, 16, 1567–1579, doi:10.3762/bjnano.16.111

• ). Remarkably, the CC/NW-450 °C composite exhibits a contact angle of 0° (Supporting Information File 1, Figure S9c), showing complete wettability. This significant enhancement in hydrophilicity is attributed to the high surface roughness and porous hydrophilic nanowire architecture formed on the carbon cloth

The role of biochar in combating microplastic pollution: a bibliometric analysis in environmental contexts

• Tuan Minh Truong Dang,
• Thao Thu Thi Huynh,
• Guo-Ping Chang-Chien and
• Ha Manh Bui

Beilstein J. Nanotechnol. 2025, 16, 1401–1416, doi:10.3762/bjnano.16.102

• of these two models are based on different mechanisms, as described in Figure 6. MP removal by BC filter columns is primarily facilitated by the fixation of particles through filtration effects, entanglement due to surface roughness and hydrophobic interactions [47]. The negatively charged surfaces

Functional bio-packaging enhanced with nanocellulose from rice straw and cinnamon essential oil Pickering emulsion for fruit preservation

• Tuyen B. Ly,
• Duong D. T. Nguyen,
• Hieu D. Nguyen,
• Yen T. H. Nguyen,
• Bup T. A. Bui,
• Kien A. Le and
• Phung K. Le

Beilstein J. Nanotechnol. 2025, 16, 1234–1245, doi:10.3762/bjnano.16.91

• in diameter and ≈1 μm in length. Pure BP films (Figure 3b) exhibited a relatively smooth surface with visible small pores, indicative of weak intermolecular interactions. The incorporation of NC into the PVA matrix significantly reduced surface roughness and void formation, suggesting enhanced

Influence of ion beam current on the structural, optical, and mechanical properties of TiO₂ coatings: ion beam-assisted vs conventional electron beam evaporation

• Agata Obstarczyk and
• Urszula Wawrzaszek

Beilstein J. Nanotechnol. 2025, 16, 1097–1112, doi:10.3762/bjnano.16.81

• high refractive index and thickness up to 400 nm are required. Although the density and the refractive index of crystalline TiO2 are higher than those of the amorphous phase, it is often preferred in optical devices due to its lower surface roughness and light scattering [65]. Nanoindentation

• scratches was reduced by half (Figure 8b). In contrast, when an ion beam gun current of 4 A was applied, the scratches almost disappeared, and the cross-sectional surface profile showed that they were only a few nanometers deep (Figure 8c). The surface roughness of the coating deposited without the ion gun

• ) without and with IBAD with ion beam gun currents of (b) Iibg = 3 A and (c) Iibg = 4 A after additional annealing at 800 °C. The dependence of (a) hardness and (b, c) surface roughness before and after abrasion tests on ion beam gun current for as-deposited and annealed thin films. (d) Hardness, packing

Single-layer graphene oxide film grown on α-Al₂O₃(0001) for use as an adsorbent

• Shiro Entani,
• Mitsunori Honda,
• Masaru Takizawa and
• Makoto Kohda

Beilstein J. Nanotechnol. 2025, 16, 1082–1087, doi:10.3762/bjnano.16.79

• intensity analysis and profiles of normal-incidence X-ray standing wave (NIXSW) spectroscopy [18]. In the SLGO film, the wrinkles disappeared and the surface roughness increased. The root mean square surface roughness (RMS) of the SLGO film is estimated to be less than 0.13 nm. The changes of the local

Ar⁺ implantation-induced tailoring of RF-sputtered ZnO films: structural, morphological, and optical properties

• Manu Bura,
• Divya Gupta,
• Arun Kumar and
• Sanjeev Aggarwal

Beilstein J. Nanotechnol. 2025, 16, 872–886, doi:10.3762/bjnano.16.66

• in grazing incidence angle X-ray diffraction patterns. Atomic force microscopy images show grain size reduction and a fall in the surface roughness value of films after implantation. The implantation-induced structural modifications are further correlated with the variation in diffuse reflectance

• foreign ions in the ZnO film lattice can create an impact on its surface roughness and particle size. Previous reports available discuss the implantation-induced optical longitudinal phonon symmetry in ZnO films using heavy ions with high energy and low implantation fluences [12][13][14][15]. Singh et al

High-temperature epitaxial growth of tantalum nitride thin films on MgO: structural evolution and potential for SQUID applications

• Michelle Cedillo Rosillo,
• Oscar Contreras López,
• Jesús Antonio Díaz,
• Agustín Conde Gallardo and
• Harvi A. Castillo Cuero

Beilstein J. Nanotechnol. 2025, 16, 690–699, doi:10.3762/bjnano.16.53

• makes this film an excellent candidate for superconducting applications, particularly in devices such as superconducting quantum interference devices (SQUIDs). Figure 7 presents an AFM image revealing the low surface roughness (2.2 nm) of even the film deposited at an elevated growth temperature of 850

• °C. This observation suggests that while deposition parameters significantly influence the structural and superconducting properties of the TaN thin films, they had only minimal impact on the surface roughness. Notably, the film roughness remains largely unaffected by variations in growth temperature

• surface roughness. Comparison of Ta 4f XPS peaks determined for different samples. (a) pN2 = 60 mTorr, (b) pN2 = 70 mTorr, (c) pN2 = 90 mTorr, T = 700 °C, and (d) pN2 = 90 mTorr, T = 750 °C. Ta 4f XPS spectra of samples deposited at (a) pN2 = 60 mTorr, T = 800 °C and (b) pN2 = 60 mTorr, T = 850 °C. XRD

Colloidal few layered graphene–tannic acid preserves the biocompatibility of periodontal ligament cells

• Teissir Ben Ammar,
• Naji Kharouf,
• Dominique Vautier,
• Housseinou Ba,
• Nivedita Sudheer,
• Philippe Lavalle and
• Vincent Ball

Beilstein J. Nanotechnol. 2025, 16, 664–677, doi:10.3762/bjnano.16.51

• . The cellular response on different graphene surfaces was previously studied, and it was demonstrated that substrate characteristics such as surface roughness, surface chemistry, and electronic properties can influence cell response [38]. The implications of these results are particularly significant

N₂⁺-implantation-induced tailoring of structural, morphological, optical, and electrical characteristics of sputtered molybdenum thin films

• Usha Rani,
• Kafi Devi,
• Divya Gupta and
• Sanjeev Aggarwal

Beilstein J. Nanotechnol. 2025, 16, 495–509, doi:10.3762/bjnano.16.38

• particles are found to be small [43]. As the thickness of Mo thin films increases, smaller particles coalesce, which increases the surface roughness. The increase in roughness and particle size of implanted films results from structural modifications caused by N2+ implantation. AFM analysis reveals that N2

• thin films. Lattice constants and texture coefficients of as-deposited and implanted Mo thin films. Values of RMS surface roughness and particle size of as-deposited and implanted Mo thin films. The electrical parameters of as-deposited and implanted Mo thin films. Funding Usha Rani is thankful to

ReactorAFM/STM – dynamic reactions on surfaces at elevated temperature and atmospheric pressure

• Tycho Roorda,
• Hamed Achour,
• Matthijs A. van Spronsen,
• Marta E. Cañas-Ventura,
• Sander B. Roobol,
• Willem Onderwaater,
• Mirthe Bergman,
• Peter van der Tuijn,
• Gertjan van Baarle,
• Johan W. Bakker,
• Joost W. M. Frenken and
• Irene M. N. Groot

Beilstein J. Nanotechnol. 2025, 16, 397–406, doi:10.3762/bjnano.16.30

• the same color contrast as in Figure 5c). By observing the root-mean-squared (RMS) surface roughness (Rq) under UHV conditions of 0.17 nm in topography and 50 pA in the current signal, we determine that the surface is rather smooth and flat. In contrast, under oxidation conditions, the surface

• roughness in topography is increased to 0.63 nm because of the more challenging scanning conditions. However, the current signal surface roughness increases by an order of magnitude to 760 pA with respect to Figure 5c. This significant increase in surface roughness, which can be observed as the appearance

• voltage of −1 V applied to the sample. RMS surface roughness and RMS current for each image are, correspondingly, (a) 0.17 nm, (b) 50 pA, (c) 0.63 nm, and (d) 760 pA. AFM images of cobalt nanoparticles on a thick (50 nm) Al2O3 film taken (a) before reaction, at RT and high vacuum, (b) at 430 K and 2 bar

Tailoring of physical properties of RF-sputtered ZnTe films: role of substrate temperature

• Kafi Devi,
• Usha Rani,
• Arun Kumar,
• Divya Gupta and
• Sanjeev Aggarwal

Beilstein J. Nanotechnol. 2025, 16, 333–348, doi:10.3762/bjnano.16.25

• ). The Rq value only gives information about the vertical fluctuation in height on a surface. To get more insight into possible surface growth mechanisms and variations in surface roughness, both vertically and laterally power spectral density (PSD) analyses were carried out. In PSD analysis, the surface

• frequency range is proportional to the surface roughness. Therefore, PSD curves corresponding to higher roughness should lie at higher ordinates compared to PSD curves for lower roughness. In our case, it was found that the films fabricated at 300 and 600 °C had the lowest and highest roughness

Enhancing mechanical properties of chitosan/PVA electrospun nanofibers: a comprehensive review

• Nur Areisman Mohd Salleh,
• Amalina Muhammad Afifi,
• Fathiah Mohamed Zuki and
• Hanna Sofia SalehHudin

Beilstein J. Nanotechnol. 2025, 16, 286–307, doi:10.3762/bjnano.16.22

• , and an increase in surface roughness, which reduced the water contact angle, without altering the bulk properties of the material. Similar observations of improved mechanical strength of plasma-treated chitosan/PVA/hydroxyapatite were reported using DBD plasma air, which is considered more cost

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

• carbides. For a given Hf target (regarding purity and surface roughness), the ablation products depend critically on the surrounding liquid, input pulse duration, input pulse energy, and the number of pulses incident on the sample. Figure 7 illustrates the EDX data for the particles synthesised in DW

Facile synthesis of size-tunable L-carnosine-capped silver nanoparticles and their role in metal ion sensing and catalytic degradation of p-nitrophenol

• Akash Kumar,
• Ridhima Chadha,
• Abhishek Das,
• Nandita Maiti and
• Rayavarapu Raja Gopal

Beilstein J. Nanotechnol. 2024, 15, 1576–1592, doi:10.3762/bjnano.15.124

• > ʟ-car-AgNP5. Therefore, the results show maximum SERS enhancement for AgNP4. This is probably because of the greater surface roughness of the nanoparticles, leading to maximum electromagnetic enhancement in AgNP4. The SERS spectra of the ʟ-car-AgNPs are almost similar and show Raman bands at 1623 cm

A biomimetic approach towards a universal slippery liquid infused surface coating

• Ryan A. Faase,
• Madeleine H. Hummel,
• AnneMarie V. Hasbrook,
• Andrew P. Carpenter and
• Joe E. Baio

Beilstein J. Nanotechnol. 2024, 15, 1376–1389, doi:10.3762/bjnano.15.111

• composition of the layer was determined by XPS. Surface roughness was evaluated using AFM to confirm successful formation of a porous structure. Finally, ordering of specific chemical groups within our PDA SLIPS layer was explored via SFG spectroscopy. Initially, each functionalization step was assessed

• square roughness (Rq), a useful metric for comparing surface roughness. The final layer with FDT should increase the surface roughness as only a monolayer is expected to bond. The final value layer of the coating that contains FDT showed Rq values of 70.5 ± 23.5 nm for COC, 46.9 ± 26 nm for Si, and 47.8

Hymenoptera and biomimetic surfaces: insights and innovations

• Vinicius Marques Lopez,
• Carlo Polidori and
• Rhainer Guillermo Ferreira

Beilstein J. Nanotechnol. 2024, 15, 1333–1352, doi:10.3762/bjnano.15.107

• and durability. For instance, low-friction coatings inspired by Hymenoptera cuticles can be applied to materials to reduce wear and tear, thereby enhancing performance, and extending the lifespan of the material. Surface roughness can have beneficial effects on the overall aerodynamic characteristics

Mn-doped ZnO nanopowders prepared by sol–gel and microwave-assisted sol–gel methods and their photocatalytic properties

• Cristina Maria Vlăduț,
• Crina Anastasescu,
• Silviu Preda,
• Oana Catalina Mocioiu,
• Simona Petrescu,
• Jeanina Pandele-Cusu,
• Dana Culita,
• Veronica Bratan,
• Ioan Balint and
• Maria Zaharescu

Beilstein J. Nanotechnol. 2024, 15, 1283–1296, doi:10.3762/bjnano.15.104

• previous studies, the authors demonstrated that Mn-doped ZnO films exhibit superior optical and piezoelectric properties compared to undoped ZnO, with a more compact microstructure and reduced surface roughness [41]. Building on this foundation, the current article aims to focus on the methods of

Direct electron beam writing of silver using a β-diketonate precursor: first insights

• Katja Höflich,
• Krzysztof Maćkosz,
• Chinmai S. Jureddy,
• Aleksei Tsarapkin and
• Ivo Utke

Beilstein J. Nanotechnol. 2024, 15, 1117–1124, doi:10.3762/bjnano.15.90

• expense of a reduced shape fidelity [9]. This is also true for the recently established direct electron beam writing of silver, which demonstrated high purities of up to 74 atom % [27] but with large surface roughness and low vertical growth rates [28][29][30]. For silver, only few solid metalorganic

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

• environments represented by implant–tissue interfaces [18] through the tuning of different parameters (i.e., surface roughness and potential as well as hydrophobicity). Cells and biomolecules can selectively adhere to or be repelled from artificial implanted surfaces, triggering several metabolic pathways of

Atomistic insights into the morphological dynamics of gold and platinum nanoparticles: MD simulations in vacuum and aqueous media

• Evangelos Voyiatzis,
• Eugenia Valsami-Jones and
• Antreas Afantitis

Beilstein J. Nanotechnol. 2024, 15, 995–1009, doi:10.3762/bjnano.15.81

• measure of surface roughness, as well as a proxy to NP reactivity, is the surface area-to-volume ratio [83]. Its variation with the NP diameter for Au (blue line) and Pt (orange line) NPs at 100 K is shown in Figure 8. In general, it is expected to be inversely proportional to where N is the number of