Characterization of ion track-etched conical nanopores in thermal and PECVD SiO₂ using small angle X-ray scattering

• Shankar Dutt,
• Rudradeep Chakraborty,
• Christian Notthoff,
• Pablo Mota-Santiago,
• Christina Trautmann and
• Patrick Kluth

Beilstein J. Nanotechnol. 2025, 16, 899–909, doi:10.3762/bjnano.16.68

• corresponding one-dimensional intensity profiles (right) are shown as a function of the magnitude of the scattering vector . Two-dimensional small-angle X-ray scattering (SAXS) patterns of conical nanopores in thermal (a) and PECVD (b) SiO2 produced from irradiation of thin film samples with 1.6 GeV Au ions and

Synchrotron X-ray photoelectron spectroscopy study of sodium adsorption on vertically arranged MoS₂ layers coated with pyrolytic carbon

• Alexander V. Okotrub,
• Anastasiya D. Fedorenko,
• Anna A. Makarova,
• Veronica S. Sulyaeva,
• Yuliya V. Fedoseeva and
• Lyubov G. Bulusheva

Beilstein J. Nanotechnol. 2025, 16, 847–859, doi:10.3762/bjnano.16.64

• remain poorly understood with respect to sodium-ion storage behavior. Comprehensive studies in this direction are needed. In this work, a thin MoS2 film with vertically aligned layers was coated by a thin film of pyrolytic carbon (PyC) with predominantly horizontal orientation of graphitic domains. The

Facile one-step radio frequency magnetron sputtering of Ni/NiO on stainless steel for an efficient electrode for hydrogen evolution reaction

• Ha Huu Do,
• Khac Binh Nguyen,
• Phuong N. Nguyen and
• Hoai Phuong Pham

Beilstein J. Nanotechnol. 2025, 16, 837–846, doi:10.3762/bjnano.16.63

• and metal oxide phases, offering a potential for HER. These outcomes indicated the successful Ni/NiO thin film fabrication on SS substrates. The uniformity of the electrocatalyst material is a vital factor that has a direct effect on electrode performance. Scanning electron microscopy (SEM) was

• carried out to analyze the morphology of the Ni/NiO thin film on the SS substrate. The as-synthesized Ni/NiO film at 5 sccm of O2 flow rate showed uniform and continuous appearance on the entire surface of the SS substrate (Figure 2a,e). However, at high O2 flow rates, the surface of Ni/NiO/SS-10, Ni/NiO

Morphology and properties of pyrite nanoparticles obtained by pulsed laser ablation in liquid and thin films for photodetection

• Akshana Parameswaran Sreekala,
• Bindu Krishnan,
• Rene Fabian Cienfuegos Pelaes,
• David Avellaneda Avellaneda,
• Josué Amílcar Aguilar-Martínez and
• Sadasivan Shaji

Beilstein J. Nanotechnol. 2025, 16, 785–805, doi:10.3762/bjnano.16.60

• synthesized by PLAL. FeS2 NPs were successfully synthesized in five different solvents, along with a minor phase of iron sulfide (FeS). Additionally, by combining electrophoretic deposition and spin-coating techniques, thin film photodiodes of FeS2 were fabricated on an n-type Si substrate utilizing the

• detectivity in the order of 106–108 Jones is attained. The FeS2/n-Si photodetector works in self-powered mode also in addition to the photoconductive mode. The results show the effective fabrication of nanostructured ultraviolet–visible–near infrared thin film photodetectors using semiconductor nanocolloids

• results in obtainment of stable nanoparticles with highly active and pure surface in their colloidal form, electrophoretic deposition is an attractive technique for their thin film deposition. Electrophoretic deposition followed by spin-coating technique is applied for thin film fabrication using the

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

• structural improvement was observed at a deposition temperature of 850 °C. At this temperature, the XRD pattern confirms the epitaxial growth of the TaN thin film on the MgO substrate. This epitaxial growth is facilitated by the similar crystallographic structures of TaN and MgO (both cubic) and their

• mTorr as a function of the deposition temperature: (a) 650 °C, (b) 700 °C, (c) 750 °C, and (d) 850 °C. (a) SEM image of the cross section of a TaN thin film prepared with FIB. (b) TEM analysis of the lateral region of the TaN film deposited at T = 750 °C and pN2 = 90 mTorr. (c) TEM image at the

• interface between MgO substrate and TaN thin film. (d) Transversal section showing the interplanar spacing of TaN. (e) Indexed electron diffraction pattern of the TaN thin film. AFM image of the TaN film deposited at pN2 = 90 mTorr and T = 850 °C. Atomic composition of TaN thin films as function of pN2

Retrieval of B1 phase from high-pressure B2 phase for CdO nanoparticles by electronic excitations in Cd_xZn_1−xO composite thin films

• Arkaprava Das,
• Marcin Zając and
• Carla Bittencourt

Beilstein J. Nanotechnol. 2025, 16, 551–560, doi:10.3762/bjnano.16.43

• mode. Table 1 summarizes the irradiation ion energies and fluences for each thin film, along with their corresponding labels. Results and Discussion Influence of Ag and O ion irradiation on crystallographic phase by X-ray diffraction and Raman spectroscopy Figure 1a shows the XRD patterns illustrating

• decrease in the intensity of the B2 phase is observed, which is attributed to enhanced electronic energy loss and the phenomenon of multiple ion impacts. The B1 phase is fully reestablished in this thin film, while the signature of the Zn2SiO4 phase is no longer detectable. This amorphization of the

• spectra for both pristine and irradiated thin films are shown. The spectra for the undoped ZnO thin film annealed at 900 °C (Z900) are included to facilitate a comparative analysis concerning the presence of the B2 phase. These measurements were conducted in backscattering geometry without accounting for

Electron beam-based direct writing of nanostructures using a palladium β-ketoesterate complex

• Chinmai Sai Jureddy,
• Krzysztof Maćkosz,
• Aleksandra Butrymowicz-Kubiak,
• Iwona B. Szymańska,
• Patrik Hoffmann and
• Ivo Utke

Beilstein J. Nanotechnol. 2025, 16, 530–539, doi:10.3762/bjnano.16.41

• of the thin focused electron beam (FEB) deposit containing Pd, C, and O without substrate interference (native silicon oxide and silicon), the SAMx Stratagem thin film correction software, based on the work by Pouchou and Pichoir [43] was employed. Stratagem needs k-ratios (i.e., the ratio of X-ray

• these k-ratios, Stratagem then recalculates the composition for a thin film (multi)layered structure. The native-oxide Si(100) substrate was accounted for by including a 1 nm thick SiO2 layer of density 2.65 g·cm−3 between the Si substrate and the deposit for the thin film correction. This way, the

• , calculated using the method of Kanaya and Okayama [46], is outlined with a yellow border. The prominent silicon peak indicates that thin film correction of EDX data is necessary for the accurate quantification of the thin Pd-containing FEB deposit. Using thickness values from AFM measurements and Stratagem

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

• electron beam evaporation [10] have been reported in the literature. RF sputtering is the predominant technique for thin film deposition because of its benefits regarding layer adhesion, uniformity, composition, and deposition rate compared to other methods [11]. In the deposition of molybdenum films, RF

• (111), (200), (220), or (311) orientations. The calculated TChkl values for each Mo thin film are summarized in Table 2. The texture coefficients of as-deposited and N2+-implanted Mo thin films demonstrate a strong orientation preference in the (111) direction. The TC111 values of these films are

• implantation may also be an influential factor regarding the preferred orientation. If the applied stress promotes the (111) orientation, this plane will be more pronounced in the resultant thin film [9]. Additionally, the texture coefficients increase with the thickness for both as-deposited and implanted Mo

Impact of adsorbate–substrate interaction on nanostructured thin films growth during low-pressure condensation

• Alina V. Dvornichenko,
• Vasyl O. Kharchenko and
• Dmitrii O. Kharchenko

Beilstein J. Nanotechnol. 2025, 16, 473–483, doi:10.3762/bjnano.16.36

• adsorbate matrix due to the percolating structure of the adsorbate. Summarizing, one can conclude that the effects of adsorbate–substrate interactions during nanostructured thin film growth at low-pressure deposition are profound and multifaceted. Understanding and controlling these interactions are

• essential for tailoring thin film properties to meet specific application requirements. Further research efforts focusing on elucidating the underlying mechanisms of adsorbate–substrate interactions and their impact on thin film growth dynamics will continue to drive advancements in materials science and

• morphology of surface of the thin film, (b) the mean adsorbate concentration on the substrate ⟨x⟩, and (c) the order parameter η (the inset represents the distribution of islands over sizes R*; the curve corresponds to the Lifshitz–Slyozov–Wagner distribution) during deposition at α = 0.04, ε = 4.0, and δ

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

• -fibrous thin film; hence. it may not suit applications that highly depend on the properties of a nanofibrous structure, such as large surface area-to-volume ratio or high permeability of the material. Similarly, Kang et al. [110] fabricated chitosan-coated PVA nanofibers by coating the heat-treated PVA

A review of metal-organic frameworks and polymers in mixed matrix membranes for CO₂ capture

• Charlotte Skjold Qvist Christensen,
• Nicholas Hansen,
• Mahboubeh Motadayen,
• Nina Lock,
• Martin Lahn Henriksen and
• Jonathan Quinson

Beilstein J. Nanotechnol. 2025, 16, 155–186, doi:10.3762/bjnano.16.14

• of MOF-based MMMs in a general context have been published by Lin et al. [27] and Kitao and coworkers [28]. Focusing on gas separation in general, Daglar et al. [29] have summarized computational approaches to simulate gas transport in thin-film MOF membranes and MOF-based MMMs. With an emphasis on

Modeling and simulation of carbon-nanocomposite-based gas sensors

• Roopa Hegde,
• Punya Prabha V,
• Shipra Upadhyay and
• Krishna S B

Beilstein J. Nanotechnol. 2025, 16, 90–96, doi:10.3762/bjnano.16.9

• , its composites, and their application in electrochemical sensors have been discussed [6][7][8]. There are research contributions on pristine graphene and ammonia gas sensors for detection of very low ammonia content [9]. The thin-film sensor fabricated on polyethylenimine- (PEI) functionalized SWCNTs

Mechanistic insights into endosomal escape by sodium oleate-modified liposomes

• Ebrahim Sadaqa,
• Satrialdi,
• Fransiska Kurniawan and
• Diky Mudhakir

Beilstein J. Nanotechnol. 2024, 15, 1667–1685, doi:10.3762/bjnano.15.131

• elucidate the mechanistic role of sodium oleate in promoting endosomal escape and compared the performance of SO-Lipo with unmodified liposomes (Unmodified-Lipo) and Aurein 1.2-modified liposomes (AUR-Lipo). Liposomes were prepared using the thin-film hydration method, resulting in Unmodified-Lipo, SO-Lipo

• medium. This approach ensures the anchorage of the peptide to the liposome membrane surface. Synthesis of the liposomal formulations was conducted via a refined thin-film hydration technique, as inspired by existing protocols [34]. Initially, the lipids were dissolved in a chloroform and methanol

Effect of radiation-induced vacancy saturation on the first-order phase transformation in nanoparticles: insights from a model

• Aram Shirinyan and
• Yuriy Bilogorodskyy

Beilstein J. Nanotechnol. 2024, 15, 1453–1472, doi:10.3762/bjnano.15.117

• . However, in cases where the structure is rebuilt, the role of vacancies becomes less obvious. This suggests that other factors must be considered to better understand the transformations in HDCMs under irradiation. A recent study reported a phase transformation in a 25 nm thick nanocrystalline Au thin

• film through in situ ion irradiation, observed using atomic-resolution transmission electron microscopy [16]. The gold sample was irradiated with 2.8 MeV Au4+ ions at 200 °C with a fluence of approximately 1014 ions·cm−2 (equivalent to a dose of 10 dpa). A combination of surface- and radiation-induced

Ion-induced surface reactions and deposition from Pt(CO)₂Cl₂ and Pt(CO)₂Br₂

• Mohammed K. Abdel-Rahman,
• Patrick M. Eckhert,
• Atul Chaudhary,
• Johnathon M. Johnson,
• Jo-Chi Yu,
• Lisa McElwee-White and
• D. Howard Fairbrother

Beilstein J. Nanotechnol. 2024, 15, 1427–1439, doi:10.3762/bjnano.15.115

• elementary reaction steps is invariant, although the rates of CO desorption and subsequent physical sputtering were greatest for the heaviest (Ar+) ions. The ability of IBID to produce pure Pt films was confirmed by AES and XPS analysis of thin film deposits created by Ar+/Pt(CO)2Cl2, demonstrating the

• /tantalum oxide substrate (230 ± 5 K) was exposed to Pt(CO)2Cl2 or Pt(CO)2Br2 vapor (ca. 5.0 × 10−8 Torr) for approximately 30 min to produce 1–2 nm thin films of each precursor. Pt(CO)2Cl2(s) was heated to 80–85 °C, and Pt(CO)2Br2(s) was heated to 85–90 °C to ensure sufficient volatility for thin film

• production observed at m/z 29 for two different ion fluxes. The inset shows the linearization of the kinetic decay profiles with the corresponding fits for a first-order decay process. Evolution of the C 1s, Cl 2p, and Pt 4f XP regions for a thin film (≈2 nm) of Pt(CO)2Cl2 on a cooled (230 ± 5 K) tantalum

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

• steady-state fluorescence measurements. In the second part of the study, CDs were dripped onto silicon substrates, and a CDs thin film was formed by evaporation. A diode structure was obtained by evaporating gold with the shadow mask technique on the CDs film, and the current–voltage characteristics of

• , the quantum yield of the CDs was calculated as 0.03. Schottky diode fabrication The usability of these newly synthesized CDs in an application area was also discussed. For this purpose, a metal (Au)–semiconductor (CDs) junction-based thin film device was produced. SEM images were taken to determine

• bandgap value of the CDs layer was 5.25 eV (Figure 6b). The current–voltage (I–V) characteristics of the Si/CDs/Au-based Schottky diode were investigated. I–V measurements of the CDs-based thin film device were carried out using a semiconductor parameter analyzer between −2.5 V and +2.5 V at room

The role of a tantalum interlayer in enhancing the properties of Fe₃O₄ thin films

• Hai Dang Ngo,
• Vo Doan Thanh Truong,
• Van Qui Le,
• Hoai Phuong Pham and
• Thi Kim Hang Pham

Beilstein J. Nanotechnol. 2024, 15, 1253–1259, doi:10.3762/bjnano.15.101

• ) peak at 43.07° (red line). This indicates the epitaxial growth of the Fe3O4 thin film on MgO(100). To our surprise, the Fe3O4 thin film deposited on the multilayer structure shows the two peaks Fe3O4(311) and Fe3O4(400) at 35.68° and 43.36°, respectively (blue line). This implies that the tantalum

• the Fe3O4 thin films causes a shift in the peak observed in sample 3 [32]. Our results reveal that the growth orientation of the Fe3O4 thin film depends on the lattice mismatch between the Fe3O4 thin film and the substrate or buffer layer. When the Fe3O4 thin film is deposited on the amorphous SiO2

• substrate, the lattice mismatch between the amorphous substrate and the crystalline film is large. In this case, the growth orientation of Fe3O4 thin film is determined by the direction having the least internal energy, which is [111]. The energetically favored [111] direction also has the highest

Photocatalytic methane oxidation over a TiO₂/SiNWs p–n junction catalyst at room temperature

• Qui Thanh Hoai Ta,
• Luan Minh Nguyen,
• Ngoc Hoi Nguyen,
• Phan Khanh Thinh Nguyen and
• Dai Hai Nguyen

Beilstein J. Nanotechnol. 2024, 15, 1132–1141, doi:10.3762/bjnano.15.92

• min. The etched p-Si NWs substrate was eventually washed with DI water and dried under N2 flow, as shown in Figure 9. Second, the as-prepared SiNWs sample was transferred to the chamber of an ALD system (R200 Advanced Picosun, 2013) for TiO2 thin film deposition. The TiO2 thin film deposition was

• (HAL-320). First, the reactor containing the photocatalytic thin film samples was evacuated using a vacuum pump for 10 min and filled with a mixture of CH4/air (4.5/0.5 pressure ratio). The pressure ratio of the gas mixture was varied to study gas composition-dependent efficiency. The total pressure of

• spectrometer (DRS-UV, Shimazu UV-2450). The chemical structure of the catalyst surface was analyzed using a Raman spectrometer (excitation of 532 nm, ANDOR Monora 500i). The surface wettability of the thin film sample was measured using a static contact angle system (Biosin Scientific), as shown in Supporting

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

• cluster by enhanced diffusion. Finally, the second halo region (H2) depicts similar particle sizes around below 20 nm sitting on top of larger bright areas of 50–250 nm. The composition of the different halo regions was studied by EDX. Because of the rich morphology observed in the deposit, no thin-film

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

• temperature because the higher number of phonons increases the efficiency of thermal transport [75]. NDs show also exceptional mechanical strength and low chemical reactivity, making them sound candidates for thin film coatings [76]. These properties are counterbalanced by a low electrical conductivity due to

• deposition (PVD), and in situ formation through laser treatments. CVD offers several advantageous features such as a high degree of control over the deposition process. CVD involves the deposition of a thin film of material onto a substrate through homogeneous or heterogeneous reactions [79]. Homogeneous

Beyond biomimicry – next generation applications of bioinspired adhesives from microfluidics to composites

• Dan Sameoto

Beilstein J. Nanotechnol. 2024, 15, 965–976, doi:10.3762/bjnano.15.79

• ]. Vacuum jamming forces a series of particles, fibers, or sheets together to act as a semi-solid under vacuum. For instance, granular jamming can employ something as simple as coffee grounds in a rubber balloon to function as a shape-morphing actuator. Layer jamming, where different stacks of paper or thin

• film sheets combine under vacuum, offers more resilience and strength. However, vacuum jamming can present problems due to leaks, power consumption, noise from pumps, and the ultimate strength of the parts being limited by coefficients of friction and applied vacuum pressure. My interest in stiffness

Effect of repeating hydrothermal growth processes and rapid thermal annealing on CuO thin film properties

• Monika Ozga,
• Eunika Zielony,
• Aleksandra Wierzbicka,
• Anna Wolska,
• Marcin Klepka,
• Marek Godlewski,
• Bogdan J. Kowalski and
• Bartłomiej S. Witkowski

Beilstein J. Nanotechnol. 2024, 15, 743–754, doi:10.3762/bjnano.15.62

• . Despite the existence of numerous methods for thin film growth based on various physical and chemical phenomena, it remains acknowledged that these techniques do not yield ideal outcomes in terms of applications in any area [16]. Therefore, comprehending the potential and limitations of these different

• . Conversely, direct thin film growth through the hydrothermal approach is outlined in [44][45]. In a different study [46], CuO films were grown on glass substrates coated with CuHNO4 through 4, 8, and 12 h long hydrothermal treatments of copper hydroxide nitrate suspension at 200 °C. Another example is the

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

• -thermal plasma exfoliation process starting from micrometer-sized TiN powder. The resulting product exhibited a plate-like thin film morphology with an enlarged d-spacing of the (200) crystallographic planes and a relaxation of the Raman vibrational modes. While the cubic structure and chemical

AFM-IR investigation of thin PECVD SiO_x films on a polypropylene substrate in the surface-sensitive mode

• Hendrik Müller,
• Hartmut Stadler,
• Teresa de los Arcos,
• Adrian Keller and
• Guido Grundmeier

Beilstein J. Nanotechnol. 2024, 15, 603–611, doi:10.3762/bjnano.15.51

• crystal microbalance (QCM) during deposition. Samples were prepared with a SiOx thickness of 5 nm and 50 nm. The PECVD process is described elsewhere [16]. Surface and thin film analysis The infrared spectroscopic studies were performed using an Anasys NanoIR 3s system from Bruker Nano GmbH, Germany

• exemplify the enormous improvements in thin film sensitivity that can be achieved by this mode in comparison to the established contact mode measurements. While the measurements in contact mode were dominated by the signal of the polypropylene substrate, we were able to record clear and well-defined signals

• of the SiOx thin films in surface-sensitive mode. This way, we were able to record AFM-IR spectra of a 5 nm thin PECVD SiOx layer grown on the polypropylene substrate. AFM-IR enabled for the first time the analysis of PECVD SiOx thin film inhomogeneities during the initial layer growth. Overall, this

Potential of a deep eutectic solvent in silver nanoparticle fabrication for antibiotic residue detection

• Le Hong Tho,
• Bui Xuan Khuyen,
• Ngoc Xuan Dat Mai and
• Nhu Hoa Thi Tran

Beilstein J. Nanotechnol. 2024, 15, 426–434, doi:10.3762/bjnano.15.38

• located at 390 nm, which is suitable for SERS applications with 532 nm laser excitation. Besides, the shape of the UV–vis spectrum is in accordance with Mie scattering theory calculations, as reported in [39], proving the existence of Ag NPs in the solution. Moreover, the XRD pattern of the thin film

• thin film (Figure 3B). The uniform distribution of silver shows the uniformity of Ag NPs-DES thin film on the glass substrate, which is crucial for the applicability of this material. NFT detection The most fundamental component of a SERS-based biosensor is its SERS substrate. It directly affects the

• SERS performance of the biosensor [6]. Herein, the Ag NPs-DES thin film with the superiorly uniform Ag NPs-DES coating can be used as a SERS substrate for the analysis of antibiotics. First, residue tracing of nitrofurantoin (NFT) has been conducted in the range from 10−3 M down to 10−8 M (Figure 4A