Probing internal continua and atomic ultrafast charge transfer within size-controlled nanoparticles by post-collision interaction in core-hole clock spectroscopy

• Johannes Lütgert,
• Erika Giangrisostomi,
• Nomi L. A. N. Sorgenfrei and
• Alexander Föhlisch

Beilstein J. Nanotechnol. 2026, 17, 505–514, doi:10.3762/bjnano.17.33

• a function of photon energy and particle size. Top panel: The X-ray absorption cross section (PFY, orange line) is shown in comparison to an integration of the resonant Auger spectra (CFS-PEY, light green line). Also, the deconvolution of the signal into the intensities of Auger (green) and Raman

Defects and defect-mediated engineering of two-dimensional materials: challenges and open questions

• Arkady V. Krasheninnikov,
• Matthias Batzill,
• Anouar-Akacha Delenda,
• Marija Drndić,
• Chris Ewels,
• Katharina J. Franke,
• Mahdi Ghorbani-Asl,
• Alexander Holleitner,
• Ado Jorio,
• Ute Kaiser,
• Daria Kieczka,
• Hannu-Pekka Komsa,
• Jani Kotakoski,
• Manuel Längle,
• David Lamprecht,
• Yun Liu,
• Steven G. Louie,
• Janina Maultzsch,
• Thomas Michely,
• Katherine Milton,
• Anna Niggas,
• Hanako Okuno,
• Joshua A. Robinson,
• Marika Schleberger,
• Bruno Schuler,
• Alexander Shluger,
• Kazu Suenaga,
• Kristian S. Thygesen,
• Richard A. Wilhelm,
• E. Harriet Åhlgren and
• Carla Bittencourt

Beilstein J. Nanotechnol. 2026, 17, 454–488, doi:10.3762/bjnano.17.31

• surface of WS2, resulting in rapid desorption from the surface at room temperature. The short residence time limits encounters with reactive defect sites, leading to a small effective reaction cross section for vacancy dimers and trimers; dissociation requires overcoming a finite barrier (see Figure 1

Eco-efficient materials for agricultural crops based on a mineral rich in MOR- and HEU-type zeolites

• Esperanza Yamile de la Nuez-Pantoja,
• Inocente Rodríguez-Iznaga,
• Gerardo Rodríguez-Fuentes,
• Vitalii Petranovskii,
• Ariel Martínez García,
• José Juan Calvino Gámez and
• Daniel Goma Jiménez

Beilstein J. Nanotechnol. 2026, 17, 381–395, doi:10.3762/bjnano.17.26

• content is much higher than in the natural zeolite from the Tasajeras deposit, composed mainly of HEU. There are differences at the structural level between the two types of zeolites, MOR and HEU. MOR has channels with a higher number of tetrahedra in the channel cross section and larger dimensions than

Comparative study on 3D morphologies of delignified, single tracheids and fibers of five wood species

• Helen Gorges,
• Felicitas von Usslar,
• Cordt Zollfrank,
• Silja Flenner,
• Imke Greving,
• Martin Müller,
• Clemens F. Schaber,
• Chuchu Li and
• Stanislav N. Gorb

Beilstein J. Nanotechnol. 2026, 17, 239–250, doi:10.3762/bjnano.17.16

• the pixel sizes were set based on the respective effective pixel size of the scan. Because the diameters differed strongly within and between several wood species, we measured two diameters of each tracheid and fiber, that is, the long and short axes of the lumen from cross section per sample and

Capabilities of the 3D-MLSI software tool in superconducting neuron design

• Irina E. Tarasova,
• Nikita S. Shuravin,
• Liubov N. Karelina,
• Fedor A. Razorenov,
• Evgeny N. Zhardetsky,
• Aleksandr S. Ionin,
• Mikhail M. Khapaev and
• Vitaly V. Bol’ginov

Beilstein J. Nanotechnol. 2026, 17, 122–138, doi:10.3762/bjnano.17.8

• insets in Figure 3), the variable segment has the simplest (two-layer) cross section. The simulation was performed with mesh steps of 0.125…1 μm, using a reduced-size superconducting screen truncated at a distance of 10 μm from the structure edges (see next section for details). For clarity, the data is

• inductance dependence on the Δy variable part length for the test SQUID sample presented in Figure 2b. Orange triangles show experimental data, filled black dots correspond to calculations with non-planar cross section (lower inset), and empty black dots were calculated with planar cross section (upper inset

Internal 3D temperature mapping in biological systems using ratiometric light-sheet imaging and lipid-coated upconversion nanothermometers

• Dannareli Barron-Ortiz,
• Enric Pérez-Parets,
• Rubén D. Cadena-Nava,
• Emilio J. Gualda,
• Jacob Licea-Rodríguez,
• Juan Hernández-Cordero,
• Pablo Loza-Álvarez and
• Israel Rocha-Mendoza

Beilstein J. Nanotechnol. 2025, 16, 2306–2316, doi:10.3762/bjnano.16.159

• photonic UC of multiple NIR photons into visible luminescence [38]. As an example, in the NaYF4:Er3+/Yb3+ composite (such as that used in this work), the NaYF4 crystal matrix is co-doped with Yb3+ acting as the sensitizer to enhance the NIR absorption cross section, whereas the Er3+ ion acts as the emitter

Terahertz-range on-chip local oscillator based on Josephson junction arrays for superconducting quantum-limited receivers

• Fedor V. Khan,
• Lyudmila V. Filippenko,
• Andrey B. Ermakov,
• Mikhail Yu. Fominsky and
• Valery P. Koshelets

Beilstein J. Nanotechnol. 2025, 16, 2296–2305, doi:10.3762/bjnano.16.158

• technological layers near the JJ and the shunt in the cross-section shown by the dashed line in Figure 2 is shown in Figure 3. The details of the fabrication processes can be found in our previous works [19][20]. Measurement technique When the JJ array irradiates the SIS mixer, the probability of quasiparticle

• image of the junctions in the array. The length of each of the three sections of the array is 2 mm (the major part is not shown for visibility). The dashed red line shows the cross-section of the layers illustrated in Figure 3. Cross-section of the technological layers near the JJ and the shunt (see the

Chiral plasmonic nanostructures fabricated with circularly polarized light

• Tian Qiao and
• Ming Lee Tang

Beilstein J. Nanotechnol. 2025, 16, 2245–2264, doi:10.3762/bjnano.16.154

• vicinity of the Au nanostructures [56]. However, the drawback of the Au/PbO2 heterostructures is evident: PbO2 is an indirect-bandgap semiconductor and, therefore, does not significantly contribute to the total extinction cross section of the nanostructure compared to Ag and Au. It would be more beneficial

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

• improve fiber homogeneity, strategies such as fine-tuning the core–shell flow rate ratio and optimizing solution viscosities can be employed, enhancing coaxial jet stability and promoting more continuous cores [16]. The evaluation of the cross-section before and after core removal is a key technique for

• SEM imaging of the cross-section of the HA+NE2/PLA sample was performed before and after core removal to observe the core–shell structure. For core removal, a portion of the sample was washed multiple times with distilled water, followed by ethanol, and then dried at room temperature. Samples, both

• bars are 10 μm, and the magnification is 8000×. Confocal microscopy images of nanofibers containing fluorescein. The scale bar is 50 μm. SEM images of the cross-section of nanofibers obtained before (A) and after (B) core removal. The scale bars are 4 μm, and the magnification is 25000×. FTIR spectra

The cement of the tube-dwelling polychaete Sabellaria alveolata: a complex composite adhesive material

• Emilie Duthoo,
• Aurélie Lambert,
• Pierre Becker,
• Carla Pugliese,
• Jean-Marc Baele,
• Arnaud Delfairière,
• Matthew J. Harrington and
• Patrick Flammang

Beilstein J. Nanotechnol. 2025, 16, 1998–2014, doi:10.3762/bjnano.16.138

• applications in various fields. Structure of the tubes of Sabellaria alveolata. Picture of a reef fragment (Champeaux, Bay of Mont Saint-Michel) (A), with detailed views of the natural tubes (B, C). SEM image of an epoxy-embedded tube in cross section showing the arrangement of mineral particles (D

Laser ablation in liquids for shape-tailored synthesis of nanomaterials: status and challenges

• Natalie Tarasenka

Beilstein J. Nanotechnol. 2025, 16, 1963–1997, doi:10.3762/bjnano.16.137

• melting point to the boiling point Tb. These energies are calculated using the formulae (Equations 4–7): In the equations above, σλabs is the absorption cross section at the wavelength λ, Φ is the laser irradiance (W/m2), tp is the pulse duration, m is the mass, Cpsol and Cpliq are the heat capacity of

Beyond the bilayer: multilayered hygroscopic actuation in pine cone scales

• Kim Ulrich,
• Max David Mylo,
• Tom Masselter,
• Fabian Scheckenbach,
• Sophia Fischerbauer,
• Martin Nopens,
• Silja Flenner,
• Imke Greving,
• Linnea Hesse and
• Thomas Speck

Beilstein J. Nanotechnol. 2025, 16, 1695–1710, doi:10.3762/bjnano.16.119

• of the pine cone scale the most as the geometry was modeled on the basis of five sketches of corresponding CT cross sections from five distinguished locations with defined distance along the longitudinal scale axis. Starting with a cross section from the basal part of the bending zone, the following

• X- and Y-directions (spanning the cross section of each model), the mean value of the two measured values was used, while the Z-value (from the basal to the apical end of the models) was derived directly. The same coefficients were used in all simulations. A linear elastic material model was applied

• embedded in a brown tissue matrix. Therefore, the use of more complex geometries, such as a remodeled scale, is recommended for a more accurate study of the biological system in silico. Tissue sample extraction from a Pinus jeffreyi cone scale. (A) The position of the cross section along the longitudinal

Bioinspired polypropylene-based functionally graded materials and metamaterials modeling the mistletoe–host interface

• Lina M. Rojas González,
• Naeim Ghavidelnia,
• Christoph Eberl and
• Max D. Mylo

Beilstein J. Nanotechnol. 2025, 16, 1592–1606, doi:10.3762/bjnano.16.113

• the fact that, in the V-shaped specimens, there is no cross section in which only the strength-dominating PPGF is present. In contrast, such cross sections are present in the rectilinear specimens, resulting in strength values that correspond well to those of pure PPGF. For the production of the

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

• technique exhibit broader peaks compared to those deposited by laser ablation, where the peaks are narrower and sharper. SEM images of the surface and cross section of the films deposited by the doctor blade method, with varying ZnO layer thicknesses, reveal a noticeable difference in morphology. The films

Synthesis and antibacterial properties of nanosilver-modified cellulose triacetate membranes for seawater desalination

• Lei Wang,
• Shizhe Li,
• Kexin Xu,
• Wenjun Li,
• Ying Li and
• Gang Liu

Beilstein J. Nanotechnol. 2025, 16, 1380–1391, doi:10.3762/bjnano.16.100

• , highlighting the detailed arrangement of PDA and Ag nanoparticles on the membrane surface. Morphological changes in (g) surface (g) and (h) cross section of Ag@PCTA after desalination, with an enlarged view of the cross-sectional layer in the upper right corner. Water flux and salt rejection rate (NaCl) for

Wavelength-dependent correlation of LIPSS periodicity and laser penetration depth in stainless steel

• Nitin Chaudhary,
• Chavan Akash Naik,
• Shilpa Mangalassery,
• Jai Prakash Gautam and
• Sri Ram Gopal Naraharisetty

Beilstein J. Nanotechnol. 2025, 16, 1302–1315, doi:10.3762/bjnano.16.95

• our comprehension of laser–material interactions and hold potential implications for surface engineering and material science applications. Keywords: cross section of LIPSS; high spatial frequency LIPSS (HSFL); laser-induced periodic surface structures (LIPSS); low spatial frequency LIPSS (LSFL

• -resolution images of cross section and surface morphologies of the sample were obtained using a FESEM (Zeiss, Ultra 55). EDS was used to determine the elemental distribution on the bare and laser-treated surfaces. The periodicity in various locations on the FESEM images was determined using ImageJ software

Mechanical stability of individual bacterial cells under different osmotic pressure conditions: a nanoindentation study of Pseudomonas aeruginosa

• Lizeth García-Torres,
• Idania De Alba Montero,
• Eleazar Samuel Kolosovas-Machuca,
• Facundo Ruiz,
• Sumati Bhatia,
• Jose Luis Cuellar Camacho and
• Jaime Ruiz-García

Beilstein J. Nanotechnol. 2025, 16, 1171–1183, doi:10.3762/bjnano.16.86

• obtain the spectrum of the cantilever. A Lorentzian fit was then performed to the obtained peak and finally the cantilever constant was calculated. To take into account any potential change in the dimensions of PA at different osmolarities, the cross section tool from the NanoScope software was used to

• estimation of the size of PA by AFM was made using the cross-section tool along both axes to obtain its length, width, and height, as shown in Figure 2A and 2B. With a resolution of 48 points or pixels per line, FV can also provide accurate morphological measurements for bacteria, as shown in the 3D

• location of single nanoindentations can be easily discerned. B) Cross-section profiles taken from both main axes of the bacteria shown in A) with dashed lines for length (blue) and width (red). C) 3D reconstruction of the image shown in A) shows how FV can also accurately represent the topography of the

Crystalline and amorphous structure selectivity of ignoble high-entropy alloy nanoparticles during laser ablation in organic liquids is set by pulse duration

• Robert Stuckert,
• Felix Pohl,
• Oleg Prymak,
• Ulrich Schürmann,
• Christoph Rehbock,
• Lorenz Kienle and
• Stephan Barcikowski

Beilstein J. Nanotechnol. 2025, 16, 1141–1159, doi:10.3762/bjnano.16.84

• are in good agreement with the near-equimolar composition of the bulk target (Cr21Mn18Fe21Co18Ni22), determined by both XRF and SEM-EDX measurements, quantifying not only the surface compositions of the corresponding targets but also bulk compositions determined from a target cross-section (Supporting

• analytical techniques, we can prove that carbon incorporation into HEA NPs via ns-LAL is observable as seen in Figure 6. We prepared a cross-section sample of an amorphous HEA NP from ns-LAL synthesis via focused ion beam (FIB) preparation and compared EELS signals originating from both the core and shell

• structure of the particle. Figure 6a highlights the elemental distribution of Cr, Mn, Fe, Co, Ni, O, and C throughout the cross section of the HEA NP. Here, evenly distributed metal atoms can be observed, surrounded by a carbon shell. However, note that carbon signals additionally originate from the

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

• coatings, there are no significant differences between the surface morphology for films deposited without and with ion gun. SEM images showed smooth surfaces composed of very small grains with columnar-like character. Post-process annealing caused a significant change of the surface and cross-section

• morphology. After thermal modification, the surface morphology of the prepared coatings without additional ion bombardment showed very large grains with an average size of approximately 100 nm, which formed agglomerates with visible voids between them (Figure 3 A). Additionally, the cross-section image

• the cross-section morphology of the titanium dioxide coating deposited with Iibg = 3 A (Figure 3b), changing its fibrous structure to a coarse-grained one. The width of these elongated grains ranged from 60 to 120 nm. Contrary to this, the cross-section image (Figure 3c) of the TiO2 coating deposited

Time-resolved probing of laser-induced nanostructuring processes in liquids

• Maximilian Spellauge,
• David Redka,
• Mianzhen Mo,
• Changyong Song,
• Heinz Paul Huber and
• Anton Plech

Beilstein J. Nanotechnol. 2025, 16, 968–1002, doi:10.3762/bjnano.16.74

• formation via direct and near-field forces [24][25][26][27]. Furthermore, the application of TTM is hampered by the relatively high uncertainty of material parameters such as the temperature- or field-dependent interaction cross section or the non-linear heat capacities [28][29][30][31]. Heat flow and phase

• to liquid) should lead to restructuring. In a simple model, the laser energy is converted into heat that will be localized in the absorbing part within the laser penetration depth. Absorption is linear as expressed by the (known) absorption cross section. In the model by Takami et al. [46], which is

• heat capacity is temperature-dependent in simple metals [28] (and the scattering cross section decreases with temperature), the cooling of the electron gas tends to slow down with increasing excitation density [107]. A well-known case is gold with exceptionally weak electron–phonon coupling, such that

Shape, membrane morphology, and morphodynamic response of metabolically active human mitochondria revealed by scanning ion conductance microscopy

• Eric Lieberwirth,
• Anja Schaeper,
• Regina Lange,
• Ingo Barke,
• Simone Baltrusch and
• Sylvia Speller

Beilstein J. Nanotechnol. 2025, 16, 951–967, doi:10.3762/bjnano.16.73

• drops sharply due to reduction of ion cross section. This decrease triggers the feedback system to stop the approach at a predefined setpoint current, effectively determining the z-position of the sample at that location. By scanning the sample pixel-by-pixel in hopping mode, a three-dimensional

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

• of the ion beam is specified as ranging from 10 to 159 nm, changing with acceleration voltage (5, 8, 16, and 30 kV) and ion beam current. The actual thickness of each layer was measured with a standard cross section using the Ga+ FIB. All scanning electron microscopy (SEM) images were taken with the

• . All deposition parameters are shown in Table 1. To calculate the resistivity of the deposits, the NanoLab 650 dual beam system was used to determine the length and the cross section of each deposited layer. The TEM lamellas were prepared with a JEOL JIB 4601F FIB-SEM MultiBeam system. The sample

• using the two upper contacts, while the resulting voltage was measured between the two lower contacts to evaluate the resistivity R in the same way as in [11]. After these measurements were done, the area A of the cross section was determined with a FIB cut and SEM image (see Figure 8b). The length l

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

• on the surface of the MoS2 film annealed in a hydrogen atmosphere (Figure 1c). An attempt to measure the cross section of this film did not yield a contrast image because of the charging effect. Therefore, to estimate the thickness of the studied film, we used a thicker MoS2 film synthesized with a

• molybdenum layer sputtered for 90 s. Part of the film surface was covered with a protective Pt layer and a lamella was cut using a focused ion beam (FIB) system (see the Experimental section for details). Figure 1d shows the SEM image of the cross section of the lamella. The bright round spots on the film

• then dried under ambient conditions. Morphology of sample surfaces was examined by SEM with a CIQTEK SEM5000 (CIQTEK Ltd., Hefei, Anhui, PRC) microscope at an accelerating voltage of 15 kV. The cross section of MoS2 film was prepared using a gallium-ion column FIB system and a two-stage protective cap

Synthesis and magnetic transitions of rare-earth-free Fe–Mn–Ni–Si-based compositionally complex alloys at bulk and nanoscale

• Shabbir Tahir,
• Tatiana Smoliarova,
• Carlos Doñate-Buendía,
• Michael Farle,
• Natalia Shkodich and
• Bilal Gökce

Beilstein J. Nanotechnol. 2025, 16, 823–836, doi:10.3762/bjnano.16.62

• -evaluated from both the surface and cross-section, confirming that the composition remains consistent throughout the surface and bulk of the CCA within the limits of experimental error (Figure S1 and Table S1, Supporting Information File 1). Figure 2b provides an overview of the alloy’s crystallographic

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

• 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