Approaching microwave photon sensitivity with Al Josephson junctions

• Andrey L. Pankratov,
• Anna V. Gordeeva,
• Leonid S. Revin,
• Dmitry A. Ladeynov,
• Anton A. Yablokov and
• Leonid S. Kuzmin

Beilstein J. Nanotechnol. 2022, 13, 582–589, doi:10.3762/bjnano.13.50

• samples in a single-shot regime and outline the junction parameter range where approaching single photon sensitivity is possible. Results and Discussion In this section, we describe our experimental setup, as well as the measurement results and comparison with theory. To study the dynamics of a SIS tunnel

• conclude that the optimal critical current range, allowing for improvement of both sensitivity and dark count time, is about hundreds of nanoamperes as predicted in [6]. Such junctions are currently being measured. (a) Scheme of the measurement electronics with thermal anchoring and various filtering

Revealing local structural properties of an atomically thin MoSe₂ surface using optical microscopy

• Lin Pan,
• Peng Miao,
• Anke Horneber,
• Alfred J. Meixner,
• Pierre-Michel Adam and
• Dai Zhang

Beilstein J. Nanotechnol. 2022, 13, 572–581, doi:10.3762/bjnano.13.49

• excitation power-dependent measurement, and the SHG signal shows a quadratic power dependence, shown in the inset of Figure 1e. The absorption spectrum of a CuPc film with a thickness of 10 nm on a glass substrate is shown in Supporting Information File 1, Figure S2. CuPc shows an intensive absorption region

Effects of substrate stiffness on the viscoelasticity and migration of prostate cancer cells examined by atomic force microscopy

• Xiaoqiong Tang,
• Yan Zhang,
• Jiangbing Mao,
• Yuhua Wang,
• Zhenghong Zhang,
• Zhengchao Wang and
• Hongqin Yang

Beilstein J. Nanotechnol. 2022, 13, 560–569, doi:10.3762/bjnano.13.47

• , Figure S3c,d. Cell surface roughness is a quantitative measurement of the variability of cellular surface topography and serves as an indicator to assess the state of the cell (i.e., the greater the roughness, the greater the undulation of the cell surface topography [27]). It can be involved in many

Stimuli-responsive polypeptide nanogels for trypsin inhibition

• Petr Šálek,
• Jana Dvořáková,
• Sviatoslav Hladysh,
• Diana Oleshchuk,
• Ewa Pavlova,
• Jan Kučka and
• Vladimír Proks

Beilstein J. Nanotechnol. 2022, 13, 538–548, doi:10.3762/bjnano.13.45

• [27]. The same trend was observed for the measurement of the pH-stimuli responsive behavior of DH of the PHEG-Tyr nanogel at 37 °C (Figure 2a). Interestingly, DLS measurements revealed a thermal transition of PHEG-Tyr nanogel with significantly smaller DH, that is, 30–40 nm at 37 °C. This observation

• side chains become more entangled inside the nanogel. The measurement of the stimuli-responsive properties of Nα-Lys-NG nanogel showed a different behavior compared to PHEG-Tyr nanogel (Figure 3a). An increase of DH from 200 to 240 nm measured at 25 °C was observed when the pH value was raised from 4

• to the measurement at 25 °C as a result of the contribution from hydrophobic interactions and hydrogen bonds. However, it is important to note that the measurement was also affected by the broad particle size distribution of Nα-Lys-NG nanogel documented by the error bars in Figure 3a. PDI values

Influence of thickness and morphology of MoS₂ on the performance of counter electrodes in dye-sensitized solar cells

• Lam Thuy Thi Mai,
• Hai Viet Le,
• Ngan Kim Thi Nguyen,
• Van La Tran Pham,
• Thu Anh Thi Nguyen,
• Nguyen Thanh Le Huynh and
• Hoang Thai Nguyen

Beilstein J. Nanotechnol. 2022, 13, 528–537, doi:10.3762/bjnano.13.44

• including 1.25:7.5 (solution 1.25), 2.5:15 (solution 2.5), and 5:30 (solution 5.0). The CV measurement was performed under a dynamic potential between −1.0 V and 1.0 V for ten cycles at a scan rate of 100 mV·s−1 in a nitrogen atmosphere. Fabrication of DSSCs DSSCs with an active area of 0.25 cm2 were

Design and characterization of polymeric microneedles containing extracts of Brazilian green propolis

• Camila Felix Vecchi,
• Rafaela Said dos Santos,
• Jéssica Bassi da Silva and
• Marcos Luciano Bruschi

Beilstein J. Nanotechnol. 2022, 13, 503–516, doi:10.3762/bjnano.13.42

• corroborates the results that MNs containing more EE were better formed macroscopically. As for GE, none of the variables significantly interfered in the height measurement (p > 0.05), which was confirmed by the difficult formation of MNs containing GE. It can also be confirmed by the response surface graphs

• ; however, greater height values were observed for smaller amounts of P407. Regarding the measurement of the base width, the amounts of both extracts presented significant negative interference in the final value (p < 0.05) (Supporting Information File 1, Table S2 and Figure S5). For GE, positive

• important factors by selecting the performed experiments [41]. The response surfaces for analysis of height and base width measurements are shown in Figure 5. The equations obtained for the height and base measurement responses, as well as the values for the correlation coefficient (r), from the statistical

Zinc oxide nanostructures for fluorescence and Raman signal enhancement: a review

• Ioana Marica,
• Fran Nekvapil,
• Maria Ștefan,
• Cosmin Farcău and
• Alexandra Falamaș

Beilstein J. Nanotechnol. 2022, 13, 472–490, doi:10.3762/bjnano.13.40

• fluorescence based on ZnO nanoscaled films is different from the metal enhancement. The use of ZnO nanosubstrates for enhanced biomedical detection has received great attention due to their optical properties and other great advantages. Early detection of disease markers and the measurement of specific protein

Tubular glassy carbon microneedles with fullerene-like tips for biomedical applications

• Sharali Malik and
• George E. Kostakis

Beilstein J. Nanotechnol. 2022, 13, 455–461, doi:10.3762/bjnano.13.38

• local crystalline structure [17]. This is in good agreement with Raman spectrum data for glassy carbon [17][18] and confirms that the carbon microneedles fabricated here are glassy in nature. Figure 5 shows the XRD measurement of the glassy carbon tubules. The single sharp peak is indicative of

The role of sulfonate groups and hydrogen bonding in the proton conductivity of two coordination networks

• Ali Javed,
• Felix Steinke,
• Stephan Wöhlbrandt,
• Hana Bunzen,
• Norbert Stock and
• Michael Tiemann

Beilstein J. Nanotechnol. 2022, 13, 437–443, doi:10.3762/bjnano.13.36

• the frequency range from 1 Hz to 4.61 MHz at an applied voltage of 0.1 V. Temperature and humidity were controlled by an Espec SH-242 climate chamber. Prior to each measurement, samples were allowed to equilibrate for 24 h. Crystal structures of [Mg(H2O)2(H3L)]·H2O) (left) and [Pb2(HL)]·H2O) (right

A non-enzymatic electrochemical hydrogen peroxide sensor based on copper oxide nanostructures

• Irena Mihailova,
• Vjaceslavs Gerbreders,
• Marina Krasovska,
• Eriks Sledevskis,
• Valdis Mizers,
• Andrejs Bulanovs and
• Andrejs Ogurcovs

Beilstein J. Nanotechnol. 2022, 13, 424–436, doi:10.3762/bjnano.13.35

• pharmaceuticals [16][17][18], environmental protection [19], and industrial areas (especially food production) [20][21][22][23][24][25]. Measurement techniques including fluorescence [26][27], luminescence [28], spectrometry [29][30], and electrochemistry [31][32][33] are widely used for H2O2 determination

• response and, as a consequence, the selectivity of the sensor. This type of sensor is characterized by good reproducibility of measurement, low production cost, fast response, high sensitivity and selectivity, and chemical and mechanical stability in aggressive environments [40][41][42][43][44][45][46

• mechanical stability, and can, thus, be easily damaged during production, storage, and measurement. These disadvantages can be avoided by using an in situ growth process of CuO nanostructures directly on a copper substrate, in the presence of certain surfactants or additives. This method makes it possible to

A chemiresistive sensor array based on polyaniline nanocomposites and machine learning classification

• Jiri Kroutil,
• Alexandr Laposa,
• Ali Ahmad,
• Jan Voves,
• Vojtech Povolny,
• Ladislav Klimsa,
• Marina Davydova and
• Miroslav Husak

Beilstein J. Nanotechnol. 2022, 13, 411–423, doi:10.3762/bjnano.13.34

• (Figure 5). The characterization system consists of mass flow controllers (Bronkhorst High-Tech) for setting the required gas concentration, a source-meter (Keithley, Model 2400) for resistance measurement of active layers, an air-tight chamber with electrical feedthroughs for the sensor array, a relay

Effect of sample treatment on the elastic modulus of locust cuticle obtained by nanoindentation

• Chuchu Li,
• Stanislav N. Gorb and
• Hamed Rajabi

Beilstein J. Nanotechnol. 2022, 13, 404–410, doi:10.3762/bjnano.13.33

• sandpaper with a grain diameter of 0.3 µm (ITW Test & Measurement GmbH, Esslingen, Germany). We performed the indentations normal to the cross section of the tibiae. This resulted in the measurement of the elastic moduli of the tibial cuticle in the longitudinal direction (along the axis of tibia) (Figure 1

• ). The specimens were indented using a SA2 Nanoindenter (MTS Nano Instruments, Oak Ridge, TN, USA) equipped with a Berkovich diamond tip. The elastic modulus of the specimens was measured using the continuous stiffness measurement (CSM) technique. CSM is a well-established technique for obtaining the

• have smaller surface areas with respect to their total volume. It must be clarified whether the desiccation discussed here happens during the nanoindentation measurement instead of during the freezing process. Water content of locust tibial cuticle According to previous reports, the water content of

Selected properties of Al_xZn_yO thin films prepared by reactive pulsed magnetron sputtering using a two-element Zn/Al target

• Witold Posadowski,
• Artur Wiatrowski,
• Jarosław Domaradzki and
• Michał Mazur

Beilstein J. Nanotechnol. 2022, 13, 344–354, doi:10.3762/bjnano.13.29

• -needle distance of 1.00 mm. The measurement was carried out such that the line connecting the four needles was perpendicular to the longest dimension (350 mm) of the glass stripe. The optical properties were evaluated on the basis of the transmission spectra. The characteristics were acquired using an

• measurement performed on the back side of the glass substrate (Figure 4, RY(back)). The surface resistance measured at the place corresponding to the target center was seven to eight orders lower than on the front side. The lowest resistance, about 103 Ω/sq, was measured directly near the target axis

• less than 10% aluminium [26][27][28][29] taking into account Al, Zn, and O. In this work, the material composition was measured using EDS, in which the measurement of X-ray intensities of light elements, such as oxygen, can be difficult and often subject to systematic errors. Therefore, in the case of

Controllable two- and three-state magnetization switching in single-layer epitaxial Pd_1−xFe_x films and an epitaxial Pd_0.92Fe_0.08/Ag/Pd_0.96Fe_0.04 heterostructure

• Igor V. Yanilkin,
• Amir I. Gumarov,
• Gulnaz F. Gizzatullina,
• Roman V. Yusupov and
• Lenar R. Tagirov

Beilstein J. Nanotechnol. 2022, 13, 334–343, doi:10.3762/bjnano.13.28

• throughout the core part of the sample supplied with the potential terminals. The magnetic hysteresis loops for the Pd0.92Fe0.08(20 nm)/Ag(20 nm)/Pd0.96Fe0.04(20 nm) heterostructure were obtained via vibrational sample magnetometry since the AMR measurement for this system is useless due to a short cut by

• Figure 1. Let us consider in more detail the dependence of ρxy on the magnetic field applied at φH = 6° (Figure 3a). The measurement started from the saturation in the positive direction of the field (not shown). This direction is close to the hard axis; therefore, on the field value decrease, at its

Interfacial nanoarchitectonics for ZIF-8 membranes with enhanced gas separation

• Season S. Chen,
• Zhen-Jie Yang,
• Chia-Hao Chang,
• Hoong-Uei Koh,
• Sameerah I. Al-Saeedi,
• Kuo-Lun Tung and
• Kevin C.-W. Wu

Beilstein J. Nanotechnol. 2022, 13, 313–324, doi:10.3762/bjnano.13.26

• measurements of N2 and CO2, the membrane was swept by the target gas for at least 10 min to remove other gaseous species from the measurement system. Then, the side of the ZIF-8 selective layer was fed with pressurized target gas to provide a driving force for the gas to permeate through the membrane. The

• area. The ideal separation factor α of gas species i with respect to gas species j was defined by the following equation: where Pi and Pj are the permeances of gas component i and j, respectively. The permeation flow volume of the target gas was recorded every 30 min during the measurement until the

Coordination-assembled myricetin nanoarchitectonics for sustainably scavenging free radicals

• Xiaoyan Ma,
• Haoning Gong,
• Kenji Ogino,
• Xuehai Yan and
• Ruirui Xing

Beilstein J. Nanotechnol. 2022, 13, 284–291, doi:10.3762/bjnano.13.23

• concentration of Myr: 0.5 mg·mL−1). Measurement of ROS scavenging. (a) UV–vis absorption spectra of ABTS solution incubated with different concentrations of MZG nanoparticles for 5 min (a sample picture is shown in the inset, equivalent concentration of Myr: 0.25, 0.5, 1, and 2 µg·mL−1). (b) The scavenging rate

Investigation of a memory effect in a Au/(Ti–Cu)Ox-gradient thin film/TiAlV structure

• Damian Wojcieszak,
• Jarosław Domaradzki,
• Michał Mazur,
• Tomasz Kotwica and
• Danuta Kaczmarek

Beilstein J. Nanotechnol. 2022, 13, 265–273, doi:10.3762/bjnano.13.21

• energies of the spectra were referred to the Fermi level (EF) determined from a cleaned reference Au sample. Measurement results were analyzed with the aid of CasaXPS software. In the case of XPS and UPS measurements, the results were averaged over a certain surface area, that is, the beam diameter was

• is the occurrence of the forming process, which occurs when the structure under test is first stimulated by an electric current (or voltage) in a cyclic I–V measurement. Conclusion The paper presents the results of investigations of the memory effect observed in a thin-film structure with a U-shape

Photothermal ablation of murine melanomas by Fe₃O₄ nanoparticle clusters

• Xue Wang,
• Lili Xuan and
• Ying Pan

Beilstein J. Nanotechnol. 2022, 13, 255–264, doi:10.3762/bjnano.13.20

• quadratic fit of the correlation function. The particle size distribution was measured using the inbuilt DTS (nano) software. Samples were equilibrated for 1 min before measurement. All measurements were performed in triplicates. Hyperthermia effect of Fe3O4 nanoparticle clusters in solution The Fe3O4

Effects of drug concentration and PLGA addition on the properties of electrospun ampicillin trihydrate-loaded PLA nanofibers

• Tuğba Eren Böncü and
• Nurten Ozdemir

Beilstein J. Nanotechnol. 2022, 13, 245–254, doi:10.3762/bjnano.13.19

• a scanning electron microscope (QUANTA 400F Field Emission SEM, Holland). The average diameters of the resulting nanofibers were calculated by the measurement of 100 single nanofibers from SEM images using the ImageJ analysis software (National Institutes of Health, USA). Mechanical properties The

Relationship between corrosion and nanoscale friction on a metallic glass

• Haoran Ma and
• Roland Bennewitz

Beilstein J. Nanotechnol. 2022, 13, 236–244, doi:10.3762/bjnano.13.18

• corrosion on nanoscale friction. The evolution of friction upon repeated scanning cycles on the corroded surfaces reveals a bilayer surface oxide film, of which the outer layer is removed by the scanning tip. The measurement of friction and adhesion allows one to compare the physicochemical processes of

Impact of device design on the electronic and optoelectronic properties of integrated Ru-terpyridine complexes

• Max Mennicken,
• Sophia Katharina Peter,
• Corinna Kaulen,
• Ulrich Simon and
• Silvia Karthäuser

Beilstein J. Nanotechnol. 2022, 13, 219–229, doi:10.3762/bjnano.13.16

• gaps almost unaffected. Thus, only a part of the orbitals relevant for a continuous conductive path from one electrode to the other is shifted into the respective voltage window defined by the measurement conditions. This kind of voltage divider, determined by the few-Ru(MPTP)2–AuNP device geometry, in

• time evolution of the current measured for Ru(TP)2 nanowire devices shows very short pulses corresponding to the light switching event. The time constant of these spike-like features could not be resolved in our measurement apparatus. However, they appear also in empty nanogap devices and are

Piezoelectric nanogenerator for bio-mechanical strain measurement

• Zafar Javed,
• Lybah Rafiq,
• Muhammad Anwaar Nazeer,
• Saqib Siddiqui,
• Muhammad Babar Ramzan,
• Muhammad Qamar Khan and
• Muhammad Salman Naeem

Beilstein J. Nanotechnol. 2022, 13, 192–200, doi:10.3762/bjnano.13.14

• as well. Under high dynamic strain more output voltage is generated than under low dynamic strain. The maximum current density shown by the device is 172.5 nA/cm2. The developed piezoelectric nanofiber sensor was then integrated into a knitted fabric through stitching to be used for angle measurement

• . Keywords: electrospinning; human body angle measurement; nanofibers; piezoelectric; PVDF; Introduction Smart textiles are normally elevated to value-added textile products with improved properties and characteristics [1]. They exhibit properties of a textile with some added characteristics. Smart textiles

• (DMF) and acetone from Sigma-Aldrich were used as solvents without any further purification. A conductive tape was used to make electrodes. Knitted fabric was used for the integration of the nanofibrous mesh for human body angle measurement. Fabrication of the nanofibrous mesh and its characterization

Low-energy electron interaction and focused electron beam-induced deposition of molybdenum hexacarbonyl (Mo(CO)₆)

• Po-Yuan Shih,
• Maicol Cipriani,
• Christian Felix Hermanns,
• Jens Oster,
• Klaus Edinger,
• Armin Gölzhäuser and
• Oddur Ingólfsson

Beilstein J. Nanotechnol. 2022, 13, 182–191, doi:10.3762/bjnano.13.13

• with an integrated Oxford EDX detector. The elemental composition of Mo(CO)6 FEBID deposits obtained by EDX measurement is shown in Table 3. Figure 4 shows the corresponding EDX spectrum along with the SEM image of the deposit. Traces of the EDX signal are discernable from the Au and Si components of

• . Elemental composition of Mo(CO)6 FEBID deposits obtained by EDX measurement of a 1 μm2 pad deposited on a 100 nm thick polycrystalline gold substrate on a 4 inch silicon wafer. Funding This project has received funding from the European Union’s Horizon 2020 research and innovation programme under the Marie

Thermal oxidation process on Si(113)-(3 × 2) investigated using high-temperature scanning tunneling microscopy

• Hiroya Tanaka,
• Shinya Ohno,
• Kazushi Miki and
• Masatoshi Tanaka

Beilstein J. Nanotechnol. 2022, 13, 172–181, doi:10.3762/bjnano.13.12

• the literature. Initial oxidation processes were identified based on high-resolution STM images. Keywords: high-index Si surface; in situ measurement; oxidation; scanning tunneling microscopy (STM); Introduction High-index silicon surfaces have drawn considerable interest for their usefulness in

• was degassed over 12 h at 870 K and then cleaned by flashing to 1370 K for 10 s several times. The sample was observed at both room temperature (RT) and high temperatures. To reduce contamination effectively, we used a tip made of PtIr or Nb for the measurement at RT and a tip made of W for the

A photonic crystal material for the online detection of nonpolar hydrocarbon vapors

• Evgenii S. Bolshakov,
• Aleksander V. Ivanov,
• Andrei A. Kozlov,
• Anton S. Aksenov,
• Elena V. Isanbaeva,
• Sergei E. Kushnir,
• Aleksei D. Yapryntsev,
• Aleksander E. Baranchikov and
• Yury A. Zolotov

Beilstein J. Nanotechnol. 2022, 13, 127–136, doi:10.3762/bjnano.13.9

• overestimates the diameter in comparison with the data obtained from microphotographs. This may be related to the specificity of the dynamic light scattering (DLS) method (hydrodynamic diameter measurement). A mechanism of detecting hydrocarbons with a sensor based on a 3D PhC: (a, b) swelling of colloidal