Microplastic pollution in Himalayan lakes: assessment, risks, and sustainable remediation strategies

• Sameeksha Rawat,
• S. M. Tauseef and
• Madhuben Sharma

Beilstein J. Nanotechnol. 2025, 16, 2144–2167, doi:10.3762/bjnano.16.148

• alpine ecosystems [46]. Tiwari et al. found that psychrophilic lipases and esterases found in marine environments degrade MPs in low-temperature experiments, lending credibility to their use in Himalayan habitats [42]. The ecological significance of cryophilic fungal species has been highlighted by

• the most prevalent mechanisms in nanomaterials to eliminate MPs, where metal oxides and carbon materials are particularly effective. Surface modification and environmental factors are crucial in controlling removal. 6.3 Tailoring nanomaterials for low-temperature, high-UV environments The Himalayan

• climates represent a promising direction for future trials. 7 Ecotoxicological impact and risk assessment MP pollution of high-altitude ecosystems is a new issue with significant ecological and health effects. Because of low temperature, high levels of UV irradiation, and slow biodegradation rates, MPs

Calibration of piezo actuators and systems by dynamic interferometry

• Knarik Khachatryan and
• Michael Reichling

Beilstein J. Nanotechnol. 2025, 16, 2086–2091, doi:10.3762/bjnano.16.143

• microscopy (NC-AFM) operation in an ultrahigh-vacuum (UHV) environment at low temperature and has been developed tremendously over the last three decades [7][8][9][10][11][12]. In frequency-modulated NC-AFM, the cantilever is kept at oscillation with constant amplitude, yielding an interferometric signal

Stereodiscrimination of guests in chiral organosilica aerogels studied by ESR spectroscopy

• Sebastian Polarz,
• Yasar Krysiak,
• Martin Wessig and
• Florian Kuhlmann

Beilstein J. Nanotechnol. 2025, 16, 2034–2054, doi:10.3762/bjnano.16.140

• spin probe covalently linked to the surface of the aerogels. Figure 13a shows ESR spectra of TEMPONHxSIL with x increasing from 0.01 to 0.15, recorded at 103 K. Because of the attachment to the surface and due to the low temperature, the spectra are characteristic for a slow tumbling dynamics and the

Low-temperature AFM with a microwave cavity optomechanical transducer

• Ermes Scarano,
• Elisabet K. Arvidsson,
• August K. Roos,
• Erik Holmgren,
• Riccardo Borgani,
• Mats O. Tholén and
• David B. Haviland

Beilstein J. Nanotechnol. 2025, 16, 1873–1882, doi:10.3762/bjnano.16.130

• force-sensor design is a significant improvement over piezoelectric force sensors commonly used in low-temperature AFM. We discuss the potential for further improvement of the sensor design to achieve optimal detection at the standard quantum limit. We demonstrate AFM operation with surface-tracking

• improving low-temperature AFM. AFM sensor and detection principle The advantages of cavity optomechanical detection for AFM sensors were already showcased by Liu et al. [8], who implemented a whispering gallery mode toroidal optical cavity coupled through its evanescent field to a doubly clamped beam with a

• = −Ωm, and the mechanical mode is measured on resonance Ω = Ωm where , detector noise is minimized when , where If the mechanical oscillator is cooled to a very low temperature, so that it is in its quantum ground state, a measurement at gives , the so-called standard quantum limit (SQL). In an actual

Further insights into the thermodynamics of linear carbon chains for temperatures ranging from 13 to 300 K

• Alexandre Rocha Paschoal,
• Thiago Alves de Moura,
• Juan S. Rodríguez-Hernández,
• Carlos William de Araujo Paschoal,
• Yoong Ahm Kim,
• Morinobu Endo and
• Paulo T. Araujo

Beilstein J. Nanotechnol. 2025, 16, 1818–1825, doi:10.3762/bjnano.16.125

• therefore, the extra data we bring in this paper provides a better low-temperature convergent behavior of ωLCC(N,T) and a better estimate for both and , when compared with reference [30]. Since γP depends on ΔωLCC(T), it is important to remind that, although the Debye model is understood to be valid even

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

• Ultura DLD system (Kratos, UK), and the binding energies were calibrated to C 1s = 284.8 eV. The specific surface area and pore size were analyzed using low-temperature N2 adsorption–desorption measurements conducted with an ASAP 2460 (USA). The absorption spectrum of the sample was acquired through UV

• . (b) Low-temperature nitrogen adsorption–desorption isotherm of CC/NW-450 °C. The inset shows the corresponding pore size distribution curve. XPS spectra of CC/NW-450 °C and CC/HTNW. (a) Survey spectra and detailed XPS spectra of (b) C 1s, (c) O 1s, and (d) Ti 2p. (a) Photocatalytic degradation of

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

• , and HER/OER devices. These films exhibit unique morphologies and properties due to the controlled nanoparticle size and dispersion. Additionally, these nanocolloids enable facile, low-temperature, single-step film fabrication under standard laboratory conditions, making it an efficient and versatile

• volume [113]. A pellet of copper metal was utilized as a target for the production of CuO NPs in deionized water and the CuO NPs were then dropped on 3–5 Ω·cm p-type silicon substrate employing drop casting at low temperature to study its photodiode properties with a layer thickness of 400 nm. Packed

Automated collection and categorisation of STM images and STS spectra with and without machine learning

• Dylan Stewart Barker and
• Adam Sweetman

Beilstein J. Nanotechnol. 2025, 16, 1367–1379, doi:10.3762/bjnano.16.99

• number of STS measurements can be obtained over various molecules automatically with optimised tips and the quality of the spectra and image assessed automatically. Methods Experimental details We used a third-generation commercial low-temperature (LT) STM NC-AFM instrument (Scienta Omicron GmbH), which

Tendency in tip polarity changes in non-contact atomic force microscopy imaging on a fluorite surface

• Bob Kyeyune,
• Philipp Rahe and
• Michael Reichling

Beilstein J. Nanotechnol. 2025, 16, 944–950, doi:10.3762/bjnano.16.72

• stable configuration. Unlike in the RT data, where we observe both polarity-preserving and polarity-changing tip changes, at low temperature, so far no polarity-preserving tip changes were observed. This is a plausible result as tip stability is generally considered a merit of LT measurements. However

• , conclusions drawn from LT data are based on a much smaller number of measurements than those for RT data, and we anticipate that polarity-preserving tip changes at low temperature would be found as rare events in a sample of measurements with higher statistical significance. Conclusion In conclusion, we

• foremost tip atom may rearrange to minimize the tip surface energy in response to increasing tip–sample interaction forces. Here, we perform an experimental investigation of tip changes during NC-AFM imaging of a CaF2(111) surface with non-functionalized tips at both room temperature (RT) and low

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

• surface is a frequently used process of focused ion beam (FIB) systems. Here, we report on the deposition of platinum (Pt) with a new kind of cesium (Cs) FIB, in which the cesium ions are produced by a low-temperature ion source. Platinum was deposited at different acceleration voltages and ion beam

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

• /Si substrates in a two-zone quartz reactor. The substrate was placed in the high-temperature zone and annealed there at 423 K for 30 min in an argon flow of 250 sccm. Then, this zone was heated to 873 K. 200 mg of sulfur powder (99.9% purity) were placed in a quartz crucible in the low-temperature

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

• metal and X can be Si, Ge or Al) have gained attention because of their magneto-structural phase transition at low temperatures. As ternary alloys, these materials undergo a magnetic and structural transition from a low-temperature orthorhombic TiNiSi-type structure to a high-temperature hexagonal Ni2In

• the Al-based CCA is more gradual, possibly because of different multiple phases and microstructures. However, the low-temperature magnetization of the Al-based CCA (≈1 A·m2·kg−1) is much lower than that of the Ge-based CCA (≈5 A·m2·kg−1), indicating that antiferromagnetic correlations may become

• to enhanced surface anisotropy effects that arise from the smaller particle size. However, Ms (300 K, 9 T) and Ms (5 K, 9 T) of the Al-based CCA NPs are comparable, while a lower Hc is exhibited at low temperature (5 K) compared to Ge-based CCA NPs (Table 4). This decrease in Hc can be attributed to

Changes of structural, magnetic and spectroscopic properties of microencapsulated iron sucrose nanoparticles in saline

• Sabina Lewińska,
• Pavlo Aleshkevych,
• Roman Minikayev,
• Anna Bajorek,
• Mateusz Dulski,
• Krystian Prusik,
• Tomasz Wojciechowski and
• Anna Ślawska-Waniewska

Beilstein J. Nanotechnol. 2025, 16, 762–784, doi:10.3762/bjnano.16.59

• AC) performed on the undissolved sample revealed the presence of a low temperature blocking process ( ≈ 10 K), and confirmed its superparamagnetic state between 70– 250 K. X-ray photoelectron spectroscopy and Raman studies showed a varied composition of the undissolved sample in which organic

• magnetization of the curves slightly increases, then a low temperature maximum, at TMAX ≈ 10 K, appears in the ZFC curve, while the magnetization value of the FC curve begins to more rapidly increase. The observed maximum in the ZFC relation is sharp, and this is the only singularity visible in this curve in

• the microcapsule as a magnetic system, it is expected that the sucrose shell will prevent or significantly diminish interactions between nanoparticles, also probably modifies the surface state of the core. To understand the low-temperature magnetic state of the FS0 sample, the zero field cooled

Quantification of lead through rod-shaped silver-doped zinc oxide nanoparticles using an electrochemical approach

• Ravinder Lamba,
• Gaurav Bhanjana,
• Neeraj Dilbaghi,
• Vivek Gupta and
• Sandeep Kumar

Beilstein J. Nanotechnol. 2025, 16, 422–434, doi:10.3762/bjnano.16.33

• they were fabricated using a low-temperature co-precipitation method. The resulting Ag@ZnO NRs had good optical properties, nanorod morphologies, and high crystallinity with no impurities. Technological advancements are leading people to use lightweight electronics and affordable sensors

• experiments. Conclusion In conclusion, a low-temperature co-precipitation technique was utilized to yield highly crystalline nanorods of ZnO doped with Ag. A variety of techniques were employed to analyze the physical and chemical characteristics of as-synthesized Ag@ZnO NRs. The results demonstrate that the

Vortex lattices of layered HTSCs at different vortex–vortex interaction potentials

• Valerii P. Lenkov,
• Anastasia N. Maksimova,
• Anna N. Moroz and
• Vladimir A. Kashurnikov

Beilstein J. Nanotechnol. 2025, 16, 362–370, doi:10.3762/bjnano.16.27

• discovered. Indications were also obtained that the second peak on the magnetization curve (second magnetization peak) at low temperature (less than 0.55Tc) coincides with the transition between the regimes of the flow of the vortex lattice. The measurements were also performed in a magnetic field inclined

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

• blending of functional agents in the polymer solution, wet chemical methods, surface graft polymerization, and plasma treatment [160]. Low-temperature plasma offers advantages over other techniques in terms of lower energy consumption, faster processing, and minimal solvent use [161]. By appropriately

• , wet chemical procedures, low-temperature plasma treatment, and co-electrospinning with surface-active chemicals and polymers [160]. Among these methods, low-temperature plasma treatment is particularly popular because it can modify the surface properties of the nanofibers without affecting their bulk

Orientation-dependent photonic bandgaps in gold-dust weevil scales and their titania bioreplicates

• Norma Salvadores Farran,
• Limin Wang,
• Primoz Pirih and
• Bodo D. Wilts

Beilstein J. Nanotechnol. 2025, 16, 1–10, doi:10.3762/bjnano.16.1

• interesting for their use as templates. The work of Galusha and colleagues demonstrated a double-imprint templating process to create a positive titania replica of beetle scales with high refractive index. This showed the effectiveness of a sol–gel process at relatively low temperature (130 °C) in replicating

Heterogeneous reactions in a HFCVD reactor: simulation using a 2D model

• Xochitl Aleyda Morán Martínez,
• José Alberto Luna López,
• Zaira Jocelyn Hernández Simón,
• Gabriel Omar Mendoza Conde,
• José Álvaro David Hernández de Luz and
• Godofredo García Salgado

Beilstein J. Nanotechnol. 2024, 15, 1627–1638, doi:10.3762/bjnano.15.128

• chemical vapor deposition reactor for the growth of polycrystalline SiO2 [23]. Most of these models describe CVD reactors at low pressure and low temperature, but there are not enough models regarding CVD systems at high temperature (>800 K) and high pressure (atmospheric pressure). In this investigation

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

• cubic (bcc) Fe lattice it is about 1.5–2.0 eV; the energy of interstitial formation ranges from 2 to 4 eV. It is accepted that interstitials are mobile at room (low) temperature because of significantly less migration energies of 0.01–0.50 eV, whereas vacancies are mobile at very high temperatures

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

• at low temperature and exposed to ion irradiation (Figure 2). Discussion MS and XPS data support the idea that, upon ion beam exposure, the initial process to occur is Pt–CO bond dissociation, evolving both CO ligands as the first volatile product. The volatilization of CO is readily identified in

Investigation of Hf/Ti bilayers for the development of transition-edge sensor microcalorimeters

• Victoria Y. Safonova,
• Anna V. Gordeeva,
• Anton V. Blagodatkin,
• Dmitry A. Pimanov,
• Anton A. Yablokov and
• Andrey L. Pankratov

Beilstein J. Nanotechnol. 2024, 15, 1353–1361, doi:10.3762/bjnano.15.108

• . Otherwise, the critical temperature of the structures would vary significantly, which we do not observe, as shown below. Cryogenic Measurement Results Low-temperature measurements of the chips with structures were performed in a Triton 200 dilution cryostat. The chips were placed in a 16-pin sample holder

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

• for any type of instrument and ion species, which includes gallium FIBs, plasma FIBs, helium ion microscopy FIBs, as well as low-temperature ion source and magneto-optical trap ion source FIBs. Results and Discussion SRIM simulations SRIM simulations were carried out to evaluate the interactions of 5

Bolometric IR photoresponse based on a 3D micro-nano integrated CNT architecture

• Yasameen Al-Mafrachi,
• Sandeep Yadav,
• Sascha Preu,
• Jörg J. Schneider and
• Oktay Yilmazoglu

Beilstein J. Nanotechnol. 2024, 15, 1030–1040, doi:10.3762/bjnano.15.84

• comparable to the responsivity of a vertically aligned MWCNT design obtained at very low temperature (84 K) and under vacuum conditions [25]. The responsivity of our miniaturized architecture in sample 2 was also competitive with larger bolometer architectures using suspended MWCNTs [23][24] and SWCNTs [22

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

• diameters of 2 and 8 nm are presented. A simple visual inspection confirms the formation of a multifaceted crystal surface at low temperature, while a smoother and uniform surface is seen at high temperature. The temperature dependence of the average coordination number as a function of the NP diameter is

Recent progress on field-effect transistor-based biosensors: device perspective

• Billel Smaani,
• Fares Nafa,
• Mohamed Salah Benlatrech,
• Ismahan Mahdi,
• Hamza Akroum,
• Mohamed walid Azizi,
• Khaled Harrar and
• Sayan Kanungo

Beilstein J. Nanotechnol. 2024, 15, 977–994, doi:10.3762/bjnano.15.80

• precisely etched to create separated nanocavity regions for enhancing the detection of biomolecule species. It has been reported that the SE SB FET-based biosensor structure offers a significant improvement in sensitivity at low-temperature values. Additionally, the SE SB FET-based biosensor provides