Electron transport through nanoscale multilayer graphene and hexagonal boron nitride junctions

• Aleksandar Staykov and
• Takaya Fujisaki

Beilstein J. Nanotechnol. 2025, 16, 2132–2143, doi:10.3762/bjnano.16.147

• probability can be calculated using Green’s function of the semi-infinite electrode–conductor–electrode system. The transmission probability is a function of the applied bias between the electrodes, V, and the energy of the electrons within the conductor, E; it is given by Equation 3: GA and GR are the

Evaluating metal-organic precursors for focused ion beam-induced deposition through solid-layer decomposition analysis

• Benedykt R. Jany,
• Katarzyna Madajska,
• Aleksandra Butrymowicz-Kubiak,
• Franciszek Krok and
• Iwona B. Szymańska

Beilstein J. Nanotechnol. 2025, 16, 1942–1951, doi:10.3762/bjnano.16.135

• commercial FIBID systems commonly employ Ga+ ions, alternative ion species such as He+, Ne+, Ar+, or Xe+ can also be used [11][12][13][14]. The resulting FEBID/FIBID deposits are widely used for repairing photolithographic masks and printing or modifying integrated circuits. In addition, they are applied for

• significant beam-induced substrate defects (e.g., Ga atom implantation). Additionally, material growth is required to compete with the FIB milling process [4][9]. The use of ions instead of electrons, like in FEBID, offers several benefits, including enhanced film quality and adhesion, better control over the

• the FIB source) and reduced ion currents. It is also important to optimize beam energy for the deposition. Tripathi et al. [27] correlated ion beam parameters to the deposition characteristics using Ga FIB and various available precursors. Several tests of many different new precursors have to be done

Laser processing in liquids: insights into nanocolloid generation and thin film integration for energy, photonic, and sensing applications

• Akshana Parameswaran Sreekala,
• Pooja Raveendran Nair,
• Jithin Kundalam Kadavath,
• Bindu Krishnan,
• David Avellaneda Avellaneda,
• M. R. Anantharaman and
• Sadasivan Shaji

Beilstein J. Nanotechnol. 2025, 16, 1428–1498, doi:10.3762/bjnano.16.104

• pulsed laser ablation, and used the NPs to fabricate Cu–In composite NPs and Cu(In,Ga)Se2 (CIGS) thin film solar cells through EPD [134][135]. They used cathodic EPD, where the substrate serves as the cathode, to prevent potential oxidation of the metallic NPs and substrate that could occur on the anode

• side. This was achieved by adding a low concentration of trivalent cations such as In or Ga into the colloid. The authors then synthesized colloidal metallic NPs of Cu−In and Cu−Ga alloys using an ultrashort femtosecond laser (1040 nm wavelength, 600 fs pulse duration, 10 μJ pulse energy in the

Ferroptosis induction by engineered liposomes for enhanced tumor therapy

• Alireza Ghasempour,
• Mohammad Amin Tokallou,
• Mohammad Reza Naderi Allaf,
• Mohsen Moradi,
• Hamideh Dehghan,
• Mahsa Sedighi,
• Mohammad-Ali Shahbazi and
• Fahimeh Lavi Arab

Beilstein J. Nanotechnol. 2025, 16, 1325–1349, doi:10.3762/bjnano.16.97

Piezoelectricity of hexagonal boron nitrides improves bone tissue generation as tested on osteoblasts

• Sevin Adiguzel,
• Nilay Cicek,
• Zehra Cobandede,
• Feray B. Misirlioglu,
• Hulya Yilmaz and
• Mustafa Culha

Beilstein J. Nanotechnol. 2025, 16, 1068–1081, doi:10.3762/bjnano.16.78

• Sevin Adiguzel Nilay Cicek Zehra Cobandede Feray B. Misirlioglu Hulya Yilmaz Mustafa Culha Sabanci University Nanotechnology Research and Application Center (SUNUM), Istanbul, Turkey Chemistry and Biochemistry Department, College of Science and Mathematics, Augusta University, Augusta, GA, USA

Focused ion beam-induced platinum deposition with a low-temperature cesium ion source

• Thomas Henning Loeber,
• Bert Laegel,
• Meltem Sezen,
• Feray Bakan Misirlioglu,
• Edgar J. D. Vredenbregt and
• Yang Li

Beilstein J. Nanotechnol. 2025, 16, 910–920, doi:10.3762/bjnano.16.69

• currents. Deposition rate, material composition, and electrical resistivity were examined and compared with layers deposited at comparable settings with a standard gallium (Ga) FIB. The deposition rate is found to depend linearly on the current density. The rate is comparable for Cs+ and Ga+ under similar

• conditions, but the deposit has lower Pt content for Cs+. The electrical resistivity of the deposit is found to be higher for Cs+ than for Ga+ and decreasing with increasing acceleration voltage. Keywords: cesium ion source; cold atom ion source; focused ion beam (FIB); FIB-induced deposition (FIBID

• time, and refresh time, precursor material and substrate have an influence on the effective deposition rate. Gallium (Ga+) and helium (He+) are the most often utilized ion species for FIBID [1][2][5]. Besides these standard FIB systems, new kinds of laser-cooled ion sources have been developed in the

Synthesis of a multicomponent cellulose-based adsorbent for tetracycline removal from aquaculture water

• Uyen Bao Tran,
• Ngoc Thanh Vo-Tran,
• Khai The Truong,
• Dat Anh Nguyen,
• Quang Nhat Tran,
• Huu-Quang Nguyen,
• Jaebeom Lee and
• Hai Son Truong-Lam

Beilstein J. Nanotechnol. 2025, 16, 728–739, doi:10.3762/bjnano.16.56

• , abundance of raw materials, and cost-effective synthesis, CMC is now widely used in food, textile, pharmaceutical, and wastewater treatment industries. This study aims to synthesize a cellulose-based multicomponent adsorbent material (PGC) using commercial sodium CMC, cross-linked with glutaraldehyde (GA

• concentration exceeds this threshold, TC adsorption efficiency declines. This is because higher PVA levels hinder dissolution and mixing, particularly as viscosity increases. Similarly, TC adsorption efficiency also declines as GA concentration increases. At high concentrations, GA can dissolve PVA

• , compromising the material’s stability. This interaction significantly influences the model (p-value < 0.05), particularly through the GA volume (X3). The interaction of the mole ratio between Ca2+ and Mg2+ (X4) with other factors also has a significant effect on the model, yielding an optimal value of

Nanoscale capacitance spectroscopy based on multifrequency electrostatic force microscopy

• Pascal N. Rohrbeck,
• Lukas D. Cavar,
• Franjo Weber,
• Peter G. Reichel,
• Mara Niebling and
• Stefan A. L. Weber

Beilstein J. Nanotechnol. 2025, 16, 637–651, doi:10.3762/bjnano.16.49

• , which is 25·1021 Ω, taking into account the electrical resistivity of silicon dioxide of [92] and a thickness of the SiO2 layer of 300 nm on an area of 9 μm2. The observed discrepancy may be attributed to the increased conductivity of the microcapacitors, which is a result of the incorporation of Ga

• Nanolab FIB apparatus with a dual Ga+ ion beam. Multifrequency heterodyne electrostatic force microscopy MFH-EFM was measured on an Oxford Instruments/Asylum Research MFP-3D Infinity AFM in a nitrogen glovebox (level of humidity below 0.3%, level of oxygen below 0.1%). The typical resonance frequency of

Synthetic-polymer-assisted antisense oligonucleotide delivery: targeted approaches for precision disease treatment

• Ana Cubillo Alvarez,
• Dylan Maguire and
• Ruairí P. Brannigan

Beilstein J. Nanotechnol. 2025, 16, 435–463, doi:10.3762/bjnano.16.34

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

The round-robin approach applied to nanoinformatics: consensus prediction of nanomaterials zeta potential

• Dimitra-Danai Varsou,
• Arkaprava Banerjee,
• Joyita Roy,
• Kunal Roy,
• Giannis Savvas,
• Haralambos Sarimveis,
• Ewelina Wyrzykowska,
• Mateusz Balicki,
• Tomasz Puzyn,
• Georgia Melagraki,
• Iseult Lynch and
• Antreas Afantitis

Beilstein J. Nanotechnol. 2024, 15, 1536–1553, doi:10.3762/bjnano.15.121

• Algorithm (GA) (using MAEtrain as the fitness function) were implemented for feature selection followed by the BSS method to select the best model based on the quality and prediction performance. Initially selected QSAR descriptors (obtained by the grid search algorithm). Ten descriptors (from a total of 72

• descriptors) were obtained after Stepwise Selection, GA, and BSS. These are Hamaker (self/water), amount of Ce, amount of Zr, rod (shape), coating, the total number of atoms, tot_metal_alpha, Metals_SumIP, X_ActivM, and Valence electron potential. Additionally, we performed a correlation analysis of the

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

• , respectively. (As we know, most elements of the periodic table are metals.) Among the metals undergoing polymorphic transformations are Fe, Co, V, W, Ti, Tl, Zr, Sr, Mn, Al, Ga, Sc, Ba, Li, Na, and K. Therefore, it is important to examine a comprehensive range of quantities, including thermodynamic parameters

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

• deposits with greater Pt content than FEBID expressed by C/Pt ratios of 4:1 or lower [21][32][33]. FIBID is commonly conducted using Ga+ ion sources; however, ion implantation is observed with gallium contamination reported between 5% [34] and 30% [33] in the resulting deposits. Ion implantation can be

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

• step width of 0.02°. The phase identification was performed using the search/match algorithm connected to (ICDD PDF-2). Nitrogen adsorption–desorption isotherms (BET) at 77 K were recorded on a Micromeritics ASAP 2020 analyzer (Norcross, GA, USA). The samples were degassed at 200 °C for 4 h under

A low-kiloelectronvolt focused ion beam strategy for processing low-thermal-conductance materials with nanoampere currents

• Annalena Wolff,
• Nico Klingner,
• William Thompson,
• Yinghong Zhou,
• Jinying Lin and
• Yin Xiao

Beilstein J. Nanotechnol. 2024, 15, 1197–1207, doi:10.3762/bjnano.15.97

• , collagen’s fibrillar structure, visible by microscopy, is denatured by heat to give gelatin that lacks any fixed structure [22][23], making heat damage easily recognizable. Despite the focus on Ga ions impacting in skin (simulations) and collagen (experimental), the broader results presented here are true

• numerical heat transfer approach A 3D numerical heat transfer approach was used to include the effect of multiple ion impacts. A time-dependent heat equation was used to assess the effects of global and local heat damage for 5 keV Ga ions when using picoampere and nanoampere ion beam currents. The surface

• simulations and experimental data Cross sections were cut into collagen using 5 keV energy Ga ions to evaluate the results from the simulations and the proposed model. One cross section was cut with an acceleration voltage of 30 kV, beam current of 1 nA, 200 nm blur, and 20% overlap to assess the heat damage

Electron-induced ligand loss from iron tetracarbonyl methyl acrylate

• Hlib Lyshchuk,
• Atul Chaudhary,
• Thomas F. M. Luxford,
• Miloš Ranković,
• Jaroslav Kočišek,
• Juraj Fedor,
• Lisa McElwee-White and
• Pamir Nag

Beilstein J. Nanotechnol. 2024, 15, 797–807, doi:10.3762/bjnano.15.66

• This work has been supported by the Czech Science Foundation project 21-26601X, by the OP JAK project CZ.02.01.01/00/22_008/0004558 “AMULET” co-financed by EU, and by the EU H2020 program via the RADON project (GA 872494). LMW and AC thank the National Science Foundation for funding under grant CHE

Level set simulation of focused ion beam sputtering of a multilayer substrate

• Alexander V. Rumyantsev,
• Nikolai I. Borgardt,
• Roman L. Volkov and
• Yuri A. Chaplygin

Beilstein J. Nanotechnol. 2024, 15, 733–742, doi:10.3762/bjnano.15.61

• -dispersive X-ray microanalysis with a focus on the distribution of oxygen atoms in the redeposited layer, which was recognized in the elemental map acquired for silicon, oxygen and gallium by the presence of Ga atoms. Subsequent analysis of silicon and oxygen concentrations was performed only in the gallium

• of the cross section are depicted in (a), while the cross-sectional view of the fabricated structure can be seen in (b). Averaged sputtering yield shown together with the dependences of Yi(θ′) for Ga ions with an energy of 30 keV. Plan-view SEM (a, e) and cross-sectional STEM (b–d, f–h) images with

Exploring the relationships between physiochemical properties of nanoparticles and cell damage to combat cancer growth using simple periodic table-based descriptors

• Joyita Roy and
• Kunal Roy

Beilstein J. Nanotechnol. 2024, 15, 297–309, doi:10.3762/bjnano.15.27

• model. Model development Zeta potential QSPR model To develop the property-based QSPR model, the training set was utilized for model development. The training set of 13 compounds was processed through feature selection via stepwise regression and genetic algorithm (GA) [29]. After feature selection, the

• after feature selection through GA was further used for model development. The model development was performed with stepwise regression using the MINITAB software followed by the best subset selection method. Further, to enhance the quality of predictions for the test set, we have performed a chemical

Ion beam processing of DNA origami nanostructures

• Leo Sala,
• Agnes Zerolová,
• Violaine Vizcaino,
• Alain Mery,
• Alicja Domaracka,
• Hermann Rothard,
• Philippe Boduch,
• Dominik Pinkas and
• Jaroslav Kocišek

Beilstein J. Nanotechnol. 2024, 15, 207–214, doi:10.3762/bjnano.15.20

• detector was calibrated beforehand using a Faraday cup. Focused ion beam irradiation A Tescan Amber FIB-SEM was used to etch the sample surface. A Ga+ focused ion beam was used (E = 30 keV, I = 10 pA) to draw 10 μm trenches with a nominal depth of 100 nm using single line scan. This resulted in actual

• with DNA origami nanotriangles and then etched with FIB (Ga+, 30 keV, 10 pA). The height gradient scale is shown on the right; its range is chosen to reveal the surface features and the deposited DNA origami nanostructures. Everything below 0 nm appears black (i.e., the bottom of the trenches

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

• -beam bombardment, which initially introduces defects into the graphene structure and then knocks out carbon atoms, although the edges of the fabricated nanostructures remain rough after the process [11]. Other direct techniques, such as focused ion beam (FIB) milling with heavy Ga+ ions, are not

Curcumin-loaded albumin submicron particles with potential as a cancer therapy: an in vitro study

• Nittiya Suwannasom,
• Netsai Sriaksorn,
• Chutamas Thepmalee,
• Krissana Khoothiam,
• Ausanai Prapan,
• Hans Bäumler and
• Chonthida Thephinlap

Beilstein J. Nanotechnol. 2023, 14, 1127–1140, doi:10.3762/bjnano.14.93

• due to the preparation process, which involves cross-linking of amino acid residues in proteins by glutaraldehyde (GA). As shown in Figure 3B, HSA retained its secondary structure, while both HSA-MPs and CUR-HSA-MPs lost their peptide bonds and secondary structure. The lack of secondary structure of

• cancer [38][39]. The low percentage of CUR released from CUR-HSA-MPs could be attributed to CUR being covalently bound to the hydrophobic domains of albumin. Another important factor is the shell of GA molecules cross-linking the amino groups on the particles’ surface to form an effective polymeric

• ), manganese(II) chloride tetrahydrate (MnCl2·4H2O), and sodium borohydride (NaBH4) were supplied by Sigma-Aldrich Chemical Co. (St. Louis, MO, USA). Sodium carbonate anhydrous (Na2CO3) and glutaraldehyde (GA, 25% solution in water) were obtained from Merck KGaA (Darmstadt, Germany). Dimethyl sulfoxide (DMSO

Recognition mechanisms of hemoglobin particles by monocytes – CD163 may just be one

• Jonathan-Gabriel Nimz,
• Pichayut Rerkshanandana,
• Chiraphat Kloypan,
• Ulrich Kalus,
• Saranya Chaiwaree,
• Axel Pruß,
• Radostina Georgieva,
• Yu Xiong and
• Hans Bäumler

Beilstein J. Nanotechnol. 2023, 14, 1028–1040, doi:10.3762/bjnano.14.85

• with the particles for 5 min. After washing in 0.9% NaCl solution, particles were centrifuged (3000g, 3 min), and the supernatant was decanted. Particles were then resuspended in 0.9% NaCl. For crosslinking, 0.02% glutaraldehyde (GA) was added to the particle suspension, which was then incubated for 1

• uptake. Future research will have to show whether this mechanism might also be responsible for a part of the uptake of HBOCs in monocytes and macrophages. Conclusion With this study, the role of CD163 in the phagocytosis of hemins by monocytes could be confirmed also for our HbMPs, namely GA-polymerized

Plasmonic nanotechnology for photothermal applications – an evaluation

• A. R. Indhu,
• L. Keerthana and
• Gnanaprakash Dharmalingam

Beilstein J. Nanotechnol. 2023, 14, 380–419, doi:10.3762/bjnano.14.33

Observation of collective excitation of surface plasmon resonances in large Josephson junction arrays

• Roger Cattaneo,
• Mikhail A. Galin and
• Vladimir M. Krasnov

Beilstein J. Nanotechnol. 2022, 13, 1578–1588, doi:10.3762/bjnano.13.132

• using photolithography and reactive ion etching. The JJ sensor with variable thickness and a width of ≈100 nm is made by Ga+ focused ion beam etching. The JJ is made small in order to increase its resistance Rn to approx. 50 Ω, which is needed for a good impedance matching with the antenna. In order to

Hydroxyapatite–bioglass nanocomposites: Structural, mechanical, and biological aspects

• Olga Shikimaka,
• Mihaela Bivol,
• Bogdan A. Sava,
• Marius Dumitru,
• Christu Tardei,
• Beatrice G. Sbarcea,
• Daria Grabco,
• Constantin Pyrtsac,
• Daria Topal,
• Andrian Prisacaru,
• Vitalie Cobzac and
• Viorel Nacu

Beilstein J. Nanotechnol. 2022, 13, 1490–1504, doi:10.3762/bjnano.13.123

• addition of different dopants to the glass can enhance the osteogenesis (Mg, Sr, Fe, and Zr) or can yield particular properties such as angiogenesis (Cu and Co) and antimicrobial activity (Ag, Zn, Ce, Ga, and Cu). Also, dopants can change the glass solubility [13][15][16][17][18][19]. The presence of the