Measurements of dichroic bow-tie antenna arrays with integrated cold-electron bolometers using YBCO oscillators

• Leonid S. Revin,
• Dmitry A. Pimanov,
• Alexander V. Chiginev,
• Anton V. Blagodatkin,
• Viktor O. Zbrozhek,
• Andrey V. Samartsev,
• Anastasia N. Orlova,
• Dmitry V. Masterov,
• Alexey E. Parafin,
• Victoria Yu. Safonova,
• Anna V. Gordeeva,
• Andrey L. Pankratov,
• Leonid S. Kuzmin,
• Anatolie S. Sidorenko,
• Silvia Masi and
• Paolo de Bernardis

Beilstein J. Nanotechnol. 2024, 15, 26–36, doi:10.3762/bjnano.15.3

• than we had expected. Mainly because of the high resistance of the DC lines as well as the imperfection of the process of creating a barrier. Therefore, two more designs were created with an expansion of the DC lines in order to reduce the resistance. Also, adjustments were made to the oxidation

• process. In the future, it is planned to carry out a set of works to improve the barrier properties of aluminum oxide. The quality of the barrier largely depends on the roughness of aluminum. It can be critically large during electron beam deposition, which in turn affects the thickness of the barrier and

• the leakage resistance. We now test various ways to reduce the aluminum roughness. Also, the roughness strongly depends on the deposition rate. The oxidation process affects the barrier properties as well; perhaps with dynamic oxidation [26] (with constant pumping) one can try to achieve better

Elasticity, an often-overseen parameter in the development of nanoscale drug delivery systems

• Agnes-Valencia Weiss and
• Marc Schneider

Beilstein J. Nanotechnol. 2023, 14, 1149–1156, doi:10.3762/bjnano.14.95

• barriers besides cellular membranes need to be addressed. A few examples of these barriers are penetration in or permeation through mucus, skin penetration, overcoming the blood brain barrier, or extravasation from blood vessels. Another challenge is the accumulation of particulate drug delivery systems in

• particle elasticity to overcome the mucosal barrier Mucus covers a large area of our body and is an important barrier for many drugs as it covers common application routes such as the intestines, the lungs, nose, and vagina. Regarding the penetration through mucus, Lenzini et al. demonstrated in a study

A visible-light photodetector based on heterojunctions between CuO nanoparticles and ZnO nanorods

• Doan Nhat Giang,
• Nhat Minh Nguyen,
• Duc Anh Ngo,
• Thanh Trang Tran,
• Le Thai Duy,
• Cong Khanh Tran,
• Thi Thanh Van Tran,
• Phan Phuong Ha La and
• Vinh Quang Dang

Beilstein J. Nanotechnol. 2023, 14, 1018–1027, doi:10.3762/bjnano.14.84

• , a potential barrier forms because the CB and VB levels of CuO NPs (−4.96 and −3.26 eV vs absolute vacuum scale (AVS), respectively), are higher than those of ZnO NRs (−4.19 and −0.99 eV vs AVS) [62]. It is vital to prevent the recombination of the electron–hole pairs. The electrons are gathered by

Isolation of cubic Si₃P₄ in the form of nanocrystals

• Polina K. Nikiforova,
• Sergei S. Bubenov,
• Vadim B. Platonov,
• Andrey S. Kumskov,
• Nikolay N. Kononov,
• Tatyana A. Kuznetsova and
• Sergey G. Dorofeev

Beilstein J. Nanotechnol. 2023, 14, 971–979, doi:10.3762/bjnano.14.80

• . The rationale behind such functionalization is that fatty alcohols will form ether bonds with surface silicon atoms upon alcoholysis, and bulky alyphatic chains will provide a steric barrier and deter further surface reactions. In this example, the obtained sols showed no signs of particle

Antibody-conjugated nanoparticles for target-specific drug delivery of chemotherapeutics

• Mamta Kumari,
• Amitabha Acharya and
• Praveen Thaggikuppe Krishnamurthy

Beilstein J. Nanotechnol. 2023, 14, 912–926, doi:10.3762/bjnano.14.75

• -containing media, which confirmed protein corona formation. The protein corona establishes a barrier between the ligand and the target, significantly reducing the NP targeting efficiency as compared to bare NPs [79]. Salvati et al. developed transferrin (Tf)-modified fluorescent silica NPs to evaluate the

• smaller when proteins were bound to NPs [81]. Xiao et al. functionalized Tf onto the surface of PEGylated polystyrene NPs to evaluate the effect of the protein corona on blood–brain barrier transcytosis, endocytosis, and intracellular trafficking. They demonstrated that Tf-NPs completely lost their

• or elimination of NP targeting capability by shielding or completely covering relevant functional groups. To block the adhesion of corona proteins on NP surfaces, various strategies have been established using surface barrier layers, such as polymer, protein, or biomimetic coatings, with the ultimate

Cross-sectional Kelvin probe force microscopy on III–V epitaxial multilayer stacks: challenges and perspectives

• Mattia da Lisca,
• José Alvarez,
• James P. Connolly,
• Nicolas Vaissiere,
• Karim Mekhazni,
• Jean Decobert and
• Jean-Paul Kleider

Beilstein J. Nanotechnol. 2023, 14, 725–737, doi:10.3762/bjnano.14.59

• defects is responsible for reducing the carrier lifetime, or by the lack of a true ohmic contact between the sample holder and the n-type InP substrate during the KPFM measurement. In the second case, a potential barrier would be present at the metal contact/n-InP substrate interface, which could reduce

Current-induced mechanical torque in chiral molecular rotors

• Richard Korytár and
• Ferdinand Evers

Beilstein J. Nanotechnol. 2023, 14, 711–721, doi:10.3762/bjnano.14.57

• potential barrier V(ϑ), we find that the mass current needs to overcome a threshold for the wire to rotate. The resulting time-averaged angular velocity is time-independent and directional for all supercritical currents. Finally, we consider a situation where the net torque exerted by the transmitted

• following specific conditions: (1) Equation 16 comes from the SA, demanding that the impact velocity is large enough (see Equation 13). (2) The time between collisions should be much smaller than T in order to silence the restoring torque: I−1 ≪ T. (3) The time required to overcome the potential barrier

• velocity must be corrected due to energy transfer, which yields a term of the second order in μ. Switching in the SA The condition for switching is that the energy gain of the path, Equation 6, must overcome the potential barrier. In the limit of large velocities, the kinetic term (due to angular momentum

Metal-organic framework-based nanomaterials as opto-electrochemical sensors for the detection of antibiotics and hormones: A review

• Akeem Adeyemi Oladipo,
• Saba Derakhshan Oskouei and
• Mustafa Gazi

Beilstein J. Nanotechnol. 2023, 14, 631–673, doi:10.3762/bjnano.14.52

• 100 nm are the main choice for the design of electrochemical sensors. These characteristics all combine to improve the electrochemical process. A sensing or working electrode that acts as a transducer, an electrolyte, a diffusion barrier, and a reference counter electrode are the common components of

Thermal transport in kinked nanowires through simulation

• Alexander N. Robillard,
• Graham W. Gibson and
• Ralf Meyer

Beilstein J. Nanotechnol. 2023, 14, 586–602, doi:10.3762/bjnano.14.49

• kinked systems specifically, the kinks further limit those paths through a form of phonon blocking [23]. Introducing a bend in the wire provides a barrier to direct ballistic transit, as there are fewer and fewer straight paths through the system as the bend angle increases. Theoretical insight on the

• effects of this barrier can be obtained through a simple analysis of the LoS. Park et al. [30] categorized systems into blocked LoS systems, where there are no direct paths for transit from one end to the other, and continuous (or unblocked) LoS systems, where there are direct lines through the system

Observation of multiple bulk bound states in the continuum modes in a photonic crystal cavity

• Rui Chen,
• Yi Zheng,
• Xingyu Huang,
• Qiaoling Lin,
• Chaochao Ye,
• Meng Xiong,
• Martijn Wubs,
• Yungui Ma,
• Minhao Pu and
• Sanshui Xiao

Beilstein J. Nanotechnol. 2023, 14, 544–551, doi:10.3762/bjnano.14.45

• . Light blocking by region B could be easily observed for the lower-order modes whose indices are lower than (3,3). For higher-order modes, large mode profiles need a larger size in region B to build a higher potential barrier to confine the light. Due to C4 symmetry of the structure, all Mpq and Mqp

Carbon nanotube-cellulose ink for rapid solvent identification

• Tiago Amarante,
• Thiago H. R. Cunha,
• Claudio Laudares,
• Ana P. M. Barboza,
• Ana Carolina dos Santos,
• Cíntia L. Pereira,
• Vinicius Ornelas,
• Bernardo R. A. Neves,
• André S. Ferlauto and
• Rodrigo G. Lacerda

Beilstein J. Nanotechnol. 2023, 14, 535–543, doi:10.3762/bjnano.14.44

• constant of the solvent as shown in Figure 4b. This result suggests that, when the liquid soaks the composite, it swells the material, creating a liquid dielectric barrier between the conductive clusters. Thus, it changes the tunneling process proportionally to the dielectric constant of the liquid. Hence

Specific absorption rate of randomly oriented magnetic nanoparticles in a static magnetic field

• Ruslan A. Rytov and
• Nikolai A. Usov

Beilstein J. Nanotechnol. 2023, 14, 485–493, doi:10.3762/bjnano.14.39

• = 300 K. As Figure 3a shows, in the absence of a dc field, Hdc = 0, the unit magnetization vector of the particle fluctuates near the bottom of the potential well, αx ≈ 1, αz ≈ 0. However, according to Figure 3b, as the dc field increases to Hdc = 200 Oe, due to a change in particle energy barrier, the

• , Hac = 200 Oe. Obviously, at Hdc = 0, the potential wells of the nanoparticle located at θ = 0 and θ = π are separated by a high potential barrier, which is independent of the angle φ. However, if the perpendicular dc magnetic field increases to Hdc = 200 Oe, a saddle trajectory appears on the barrier

• at φ = π (see Figure 4c). As a result, the height of the energy barrier between the potential wells decreases significantly. This leads to an increase in the probability of magnetization reversal of nanoparticles of large diameters, D = 30–50 nm. At Hdc = 200 Oe, this gives an almost rectangular

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

Quercetin- and caffeic acid-functionalized chitosan-capped colloidal silver nanoparticles: one-pot synthesis, characterization, and anticancer and antibacterial activities

• Akif Hakan Kurt,
• Elif Berna Olutas,
• Fatma Avcioglu,
• Hamza Karakuş,
• Mehmet Ali Sungur,
• Cansu Kara Oztabag and
• Muhammet Yıldırım

Beilstein J. Nanotechnol. 2023, 14, 362–376, doi:10.3762/bjnano.14.31

• conventional treatments. This resistance is mostly due to the blood–brain barrier, which is the most important obstacle to drug distribution. Since nanoparticles can penetrate through the blood–brain barrier, they are a preferred medicine in brain and nervous system diseases. In glioblastoma multiforme

The steep road to nonviral nanomedicines: Frequent challenges and culprits in designing nanoparticles for gene therapy

• Yao Yao,
• Yeongun Ko,
• Grant Grasman,
• Jeffery E. Raymond and
• Joerg Lahann

Beilstein J. Nanotechnol. 2023, 14, 351–361, doi:10.3762/bjnano.14.30

• gathering significant attention as highlighted by the broad clinical acceptance of mRNA-based COVID-19 vaccines. A significant barrier to progress in this emerging area is the wild variability of approaches reported in published literature regarding nanoparticle characterizations. Here, we provide a brief

Polymer nanoparticles from low-energy nanoemulsions for biomedical applications

• Santiago Grijalvo and
• Carlos Rodriguez-Abreu

Beilstein J. Nanotechnol. 2023, 14, 339–350, doi:10.3762/bjnano.14.29

• , nanocarriers need to be engineered to add functionalities, both in their cores and at their surfaces. This includes therapeutic drugs and genes, targeting moieties, performance enhancers (e.g., for barrier penetration and to avoid opsonization), and imaging agents [2][3]. Core and matrix of the nanoparticles

• low-energy methods (also called thermodynamic methods [5]) overcome this energy barrier by producing low interfacial tensions, changes in the surfactant layer curvature, or gradients of chemical potential between the phases. Herein, we focus on nanoemulsification by low-energy methods. The two main

• showed that the PLGA nanoparticles functionalized with 8D3 antibody were able to cross the blood–brain barrier (BBB) as demonstrated by the analgesic effect of encapsulated loperamide on mice. PLGA nanoparticles prepared using Polysorbate 80 with the same formulation discussed above (diameter ca. 27 nm

Overview of mechanism and consequences of endothelial leakiness caused by metal and polymeric nanoparticles

• Magdalena Lasak and
• Karol Ciepluch

Beilstein J. Nanotechnol. 2023, 14, 329–338, doi:10.3762/bjnano.14.28

• : endothelial leakiness; metal nanoparticles; NanoEL; nanotoxicity; vascular permeability; Review Introduction The vascular barrier is a highly selective boundary between blood and tissues. Its proper functioning is essential to maintaining homeostasis of the whole organism. Formed from mesodermal endothelial

• extracellular signals and regulate the function of the vascular barrier [3]. The endothelium is also covered by a negatively charged layer of glycocalyx, which has a protective function and is involved in the transport of molecules across the endothelium [11][12]. The degree of endothelial permeability depends

• (CNS), where endothelial cells form the tightest and the most selective blood–brain barrier (BBB) that provides protection against the penetration of harmful substances and pathogens. Other types of connections include adherens junctions, maintained primarily by transmembrane VE-cadherin, and gap

Bismuth-based nanostructured photocatalysts for the remediation of antibiotics and organic dyes

• Akeem Adeyemi Oladipo and
• Faisal Suleiman Mustafa

Beilstein J. Nanotechnol. 2023, 14, 291–321, doi:10.3762/bjnano.14.26

• semiconductor and a noble metal with an appropriate work function. A unidirectional charge transfer is enabled by the Schottky potential barrier, increasing charge density and separation [72]. Shen et al. [166] created a Schottky junction by synthesising NiSe2 nanosheets on top of BiVO4 nanosheets using a

• , the Schottky potential barrier, and efficiently separated photoinduced charge carriers. Table 8 provides a summary of the research on heterojunction photocatalysts for the degradation of antibiotics. Bismuth nanocomposites: A nanocomposite is a multiphase material (typically a solid) with one to three

Recent progress in cancer cell membrane-based nanoparticles for biomedical applications

• Qixiong Lin,
• Yueyou Peng,
• Yanyan Wen,
• Xiaoqiong Li,
• Donglian Du,
• Weibin Dai,
• Wei Tian and
• Yanfeng Meng

Beilstein J. Nanotechnol. 2023, 14, 262–279, doi:10.3762/bjnano.14.24

• , cancer cell membranes also show excellent performance in nontumor diseases such as immune system diseases [25] and cardiovascular diseases [26] because of their rich surface functions that yield immunomodulation [22] and biological barrier penetration [27]. Here, we review recent advances and original

• exhibit unique homotypic targeting to tumor tissues, as well as excellent antiphagocytosis, immunomodulation, and biological barrier penetration abilities. Second, the application of cancer cell-based NPs in different types of diseases are discussed (i.e., malignant neoplasms, hematological malignancies

• cells have also been found to have the ability to penetrate the blood‒brain barrier (BBB) in some special cases [26][27]. As a highly specialized structure, the BBB maintains homeostasis of the central nervous system [48]. The targeted delivery of drugs to the brain is challenging because of the limited

Nanotechnology – a robust tool for fighting the challenges of drug resistance in non-small cell lung cancer

• Filip Gorachinov,
• Fatima Mraiche,
• Diala Alhaj Moustafa,
• Ola Hishari,
• Yomna Ismail,
• Jensa Joseph,
• Maja Simonoska Crcarevska,
• Marija Glavas Dodov,
• Nikola Geskovski and
• Katerina Goracinova

Beilstein J. Nanotechnol. 2023, 14, 240–261, doi:10.3762/bjnano.14.23

• barriers by the use of different groups of particles carrying various functional modalities. Tasciotti et al. proposed a multistage delivery system composed of stage-1 mesoporous silica particles with improved deposition in the vascular endothelium, optimized for crossing the endothelial barrier through

• demonstrated pH-dependent selective survivin-shRNA release in the acidic environment after endosomal escape and disassembly to single PAMAM nanoparticles showing continuous release of erlotinib and chloroquine. Chloroquine has a dual effect on the efficacy. It improves vascular barrier integrity and together

• targeting. Once in the lung microcirculation, the RBC-bound NPs are mechanically detached from the RBCs when the RBCs are squeezed through the tiny capillaries of the air–blood barrier and transferred to the endothelium by nonspecific interactions. When decorated with vascular endothelium-specific ligands

A novel approach to pulsed laser deposition of platinum catalyst on carbon particles for use in polymer electrolyte membrane fuel cells

• Bogusław Budner,
• Wojciech Tokarz,
• Sławomir Dyjak,
• Andrzej Czerwiński,
• Bartosz Bartosewicz and
• Bartłomiej Jankiewicz

Beilstein J. Nanotechnol. 2023, 14, 190–204, doi:10.3762/bjnano.14.19

• graphitized carbon material is a higher barrier to be overcome for the gases and the water generated in reactions occurring in the cell. Conclusion The fabrication of an efficient catalyst based on carbon particles with low Pt loading was successfully achieved by using the PLD method. The structural

A distributed active patch antenna model of a Josephson oscillator

• Vladimir M. Krasnov

Beilstein J. Nanotechnol. 2023, 14, 151–164, doi:10.3762/bjnano.14.16

• and dielectric losses in the junction barrier and surface resistance in electrodes. According to Equation 37, Rdis is defined via the effective quality factor, Qdis, which can be written as: where QQP, Qsurf and Qdiel are determined by QP, surface, and dielectric losses, respectively. QP and surface

• , Rsurf ≪ ωL*, and , we obtain Dielectric losses in the AlOx barrier of a JJ were estimated in [43]. At f ≃ 10 GHz, Qdiel ≈ 104. Although it should decrease at f = 400 GHz, we anticipate that it is still in the range of ca. 103. Therefore, dielectric losses are negligible, compared to QP and surface loses

Intermodal coupling spectroscopy of mechanical modes in microcantilevers

• Ioan Ignat,
• Bernhard Schuster,
• Jonas Hafner,
• MinHee Kwon,
• Daniel Platz and
• Ulrich Schmid

Beilstein J. Nanotechnol. 2023, 14, 123–132, doi:10.3762/bjnano.14.13

• that can even break this quantum barrier by redirecting noise from one quadrature to another [9][10][11]. Yet, there is even opportunity in revitalising the accessibility of standard AFM, as performing experiments at cryogenic temperatures and under ultra-high vacuum [12][13] requires years of

Cooper pair splitting controlled by a temperature gradient

• Dmitry S. Golubev and
• Andrei D. Zaikin

Beilstein J. Nanotechnol. 2023, 14, 61–67, doi:10.3762/bjnano.14.7

• investigated both theoretically [4][5][6][7][8][9][10] and experimentally [11][12][13][14][15][16][17][18] over the past decades. The process competing with CAR is the so-called elastic cotunneling (EC), where an electron is transferred from one normal metal to another across an effective barrier created by

• -transparency barriers at NS interfaces [20][21] and later extended to the case of arbitrary barrier transmissions [22][23][24][25]. Positively cross-correlated non-local shot noise was indeed observed in a number of experiments [26][27]. Real-time observation of Cooper pair splitting was also reported in a

Gap-directed chemical lift-off lithographic nanoarchitectonics for arbitrary sub-micrometer patterning

• Chang-Ming Wang,
• Hong-Sheng Chan,
• Chia-Li Liao,
• Che-Wei Chang and
• Wei-Ssu Liao

Beilstein J. Nanotechnol. 2023, 14, 34–44, doi:10.3762/bjnano.14.4

• obtained from micrometer-scale stamp features, thus greatly lowering the technical barrier in lithographic patterning. Diverse patterns, including lines, circles, triangles, squares, hexagons, and arrayed dots sized down to 5 nm can be obtained by implementing PDMS stamps with corresponding features and