Reduced subthreshold swing in a vertical tunnel FET using a low-work-function live metal strip and a low-k material at the drain

• Kalai Selvi Kanagarajan and
• Dhanalakshmi Krishnan Sadhasivan

Beilstein J. Nanotechnol. 2024, 15, 713–718, doi:10.3762/bjnano.15.59

• previously published model, the proposed design uses a low-k material in the drain region to reduce Cgd. A metal strip with low work function placed at the source–channel interface causes an abrupt change in electron concentration, increasing the tunneling rate [14][15][16][17][18]. Molybdenum, used here as

• compared to the VTFET in [12] to demonstrate the effects of the low-work-function live strip and the low-k material. The device parameters used are listed in Table 1. Reference [12] used bandgap narrowing, Shockley–Read–Hall recombination, Lombardi's mobility model, and band-to-band (non-local) modeling

• Spacer) The proposed model VTFET with DLWLS + spacer is compared with the previously published work [12]. The Id vs Vgs curve of the model proposed here is better in terms of leakage current as illustrated in Figure 6. The off-current of the proposed model is 1.40 × 10−17 A/μm, while that of the model in

Elastic modulus of β-Ga₂O₃ nanowires measured by resonance and three-point bending techniques

• Annamarija Trausa,
• Sven Oras,
• Sergei Vlassov,
• Mikk Antsov,
• Tauno Tiirats,
• Andreas Kyritsakis,
• Boris Polyakov and
• Edgars Butanovs

Beilstein J. Nanotechnol. 2024, 15, 704–712, doi:10.3762/bjnano.15.58

• these different methods arise from multiple factors. For instance, different NW growth mechanisms and sensitive synthesis conditions, their structural and geometrical variations, beam theory model validity, and the resolution of microscopy techniques leading to inaccurate measurements of the NW

Enhancing higher-order modal response in multifrequency atomic force microscopy with a coupled cantilever system

• Wendong Sun,
• Jianqiang Qian,
• Yingzi Li,
• Yanan Chen,
• Zhipeng Dou,
• Rui Lin,
• Peng Cheng,
• Xiaodong Gao,
• Quan Yuan and
• Yifan Hu

Beilstein J. Nanotechnol. 2024, 15, 694–703, doi:10.3762/bjnano.15.57

• traditional rectangular cantilever is weaker in air, which affects the sensitivity of multifrequency AFM detection. To address this issue, we previously proposed a bridge/cantilever coupled system model to enhance the higher-order modal response of the cantilever. This model is simpler and less costly than

• performance of the coupled system with that of traditional cantilevers and quantify the enhancement in higher-order modal response. Also, the optimal conditions for the enhancement of macroscale cantilever modal response are explored. Additionally, we also supplement the characteristics of this model

• micromachining the cantilever, which is costly and complex. To develop a simpler method to enhance the higher-order modal response of cantilever, we previously proposed a model based on a bridge/cantilever coupled system [19]. The model divides the rectangular cantilever into two parts, namely, the left clamped

Laser synthesis of nanoparticles in organic solvents – products, reactions, and perspectives

• Theo Fromme,
• Sven Reichenberger,
• Katharine M. Tibbetts and
• Stephan Barcikowski

Beilstein J. Nanotechnol. 2024, 15, 638–663, doi:10.3762/bjnano.15.54

• as water and even aqueous solutes. Thus, this model formed the basis that enabled the derivation of yield functions for a variety of direct electron-mediated DNA damage pathways and indirect damage by •OH radicals resulting from laser and electron interactions with water [85]. In general, LSPC in

• colloidal Pt solution [138]. The chemical processes leading to the formation of polyynes are still not fully understood, but a few models have been proposed over the years. Tsuji et al. proposed a model for ns-LAL. They suggested a stepwise growth of hydrogen-capped polyynes by the addition of carbon

• result in higher carbon shell thicknesses for larger nanoparticles due to the decrease in surface-to-volume ratios of the nanoparticles [104][149]. Reichenberger et al. proposed a model formula (Equation 1) for the ablation in acetone to calculate the volume-specific nanoparticle surface area SNP and the

Stiffness calibration of qPlus sensors at low temperature through thermal noise measurements

• Laurent Nony,
• Sylvain Clair,
• Daniel Uehli,
• Aitziber Herrero,
• Jean-Marc Themlin,
• Andrea Campos,
• Franck Para,
• Alessandro Pioda and
• Christian Loppacher

Beilstein J. Nanotechnol. 2024, 15, 580–602, doi:10.3762/bjnano.15.50

• files support our framework. They contain important results from the literature and are organized to help the reader to follow our developments. Supporting Information File 1 reminds the most salient results of the Euler–Bernoulli model and how it sustains the point-mass SHO equivalence. Supporting

• qPlus sensor. The discussion is restricted to probes with a rectangular cross section (length l, thickness t, width w are such that l ≫ t and l ≫ w) treated in the Euler–Bernoulli model of the embedded beam, extensively detailed, for example, in [35] (cf. also Supporting Information File 1). The

• surrounding the probe [38], if described in the model, plays no role. Following Burnham’s classification [40], we essentially focus on two categories of non-destructive calibration methods, referred to as “geometric” and “thermal” methods. Geometric methods Geometric methods permit to calculate the stiffness

Radiofrequency enhances drug release from responsive nanoflowers for hepatocellular carcinoma therapy

• Yanyan Wen,
• Ningning Song,
• Yueyou Peng,
• Weiwei Wu,
• Qixiong Lin,
• Minjie Cui,
• Rongrong Li,
• Qiufeng Yu,
• Sixue Wu,
• Yongkang Liang,
• Wei Tian and
• Yanfeng Meng

Beilstein J. Nanotechnol. 2024, 15, 569–579, doi:10.3762/bjnano.15.49

• release from CUR-Fe@MnO2 NFs in the simulated TME. Drug release kinetics model fitting was also performed. The Higuchi, Ritger–Peppas, zero-order, and first-order methods were used to fit the experimental data, and R2 and release constants were calculated, as shown in Table 1. Among them, the Higuchi

• model has the highest degree of fitting with the release of NFs in different simulated environments within 72 h, which indicates conformity with the Fick diffusion mechanism. Meanwhile, we found that RF heating does not affect the release kinetics model. Ritger–Peppas is a semiempirical model, and n is

• an indicator of the drug release mechanism, where n ≤ 0.45 represents the Fick diffusion. The n values calculated in this study are all less than 0.45, indicating that the CUR release from NFs is in accordance with the Fick diffusion. Similarly, the Higuchi model has the highest degree of fitting

Directed growth of quinacridone chains on the vicinal Ag(35 1 1) surface

• Niklas Humberg,
• Lukas Grönwoldt and
• Moritz Sokolowski

Beilstein J. Nanotechnol. 2024, 15, 556–568, doi:10.3762/bjnano.15.48

• found a hole mobility of 0.1 cm2·V−1·s−1 and a photocurrent of about 1 mA·cm−2. These observations were both attributed to a close packing of the molecules due to strong intermolecular H-bonds. The empirical formula of QA is C20H12N2O2, and a structural formula and a hard-sphere model of QA are

• chains across the steps, we propose the following model: We note that, because of the specific orientation and size of the molecules, the distance between the ends of the chains and the step edge can vary by one Ag(100) lattice constant (aAg(100) = 2.89 Å [31]). This is illustrated by the two models in

• orientation will be labeled E from now on. It does not occur on the nominally flat Ag(100) surface. This indicates that, on large terraces, the orientation E is less favorable than A–D, but it is stabilized by the step edges of the vicinal surface. A model of a chain with orientation E is illustrated in

On the additive artificial intelligence-based discovery of nanoparticle neurodegenerative disease drug delivery systems

• Shan He,
• Julen Segura Abarrategi,
• Harbil Bediaga,
• Sonia Arrasate and
• Humberto González-Díaz

Beilstein J. Nanotechnol. 2024, 15, 535–555, doi:10.3762/bjnano.15.47

• list NDD or NP labels. Consequently, the resulting model cannot predict multioutput properties and/or labels such as different organisms or cell lines [25][26][27][28][29][30][31][32][33][34][35][36][37]. Sizochenko et al. reported a new methodology for NP safety estimation in different organisms [38

• theory (PT) + machine learning (ML) algorithm [40]. In recent investigations, the IFPTML model has shown to be a powerful tool in molecular sciences and NDD research for the analysis of big datasets that include both structural and non-structural parameters. Application examples are drug screening

• , protein targeting, the prediction of coated-NP drug release systems [41][42][43][44][45][46][47][48][49], multitarget networks of neuroprotective compounds for a theoretical study of new asymmetric 1,2-rasagiline carbamates [50], a TOPS-MODE model of multiplexing neuroprotective effects of drugs, an

Cholesterol nanoarchaeosomes for alendronate targeted delivery as an anti-endothelial dysfunction agent

• Horacio Emanuel Jerez,
• Yamila Roxana Simioni,
• Kajal Ghosal,
• Maria Jose Morilla and
• Eder Lilia Romero

Beilstein J. Nanotechnol. 2024, 15, 517–534, doi:10.3762/bjnano.15.46

• -8 levels by, respectively, 75% and 65% in the mild and by, respectively, 60% and 40% in the pronounced inflammation model. This is the first report showing that the endocytosis of nanoARC-Chol(ALN) by HUVECs magnifies the anti-inflammatory activity of ALN even under conditions of intense irritation

• /II. We observed here that nanoARC(ALN) was much less cytotoxic for THP-1 macrophages than for J774A1 cells, probably, because the expression of SRA1 in THP-1 macrophages (and subsequent internalization) is reported to be lower than in J774A1 macrophages [43]. Co-cultures Mild inflammation model The

• IL-8 levels in either compartment (Figure 9). nanoARC-Chol(ALN) caused a slight decrease in reactive oxygen species (ROSs) in macrophages (Figure 10A). Pronounced inflammation model The previous crosstalk induced mild levels of IL-6 and IL-8 on the apical side with HUVECs (Supporting Information File

Electron-induced deposition using Fe(CO)₄MA and Fe(CO)₅ – effect of MA ligand and process conditions

• Hannah Boeckers,
• Atul Chaudhary,
• Petra Martinović,
• Amy V. Walker,
• Lisa McElwee-White and
• Petra Swiderek

Beilstein J. Nanotechnol. 2024, 15, 500–516, doi:10.3762/bjnano.15.45

• cryo-EBID, we focus on scenario A as model for the evaluation of the resulting deposits. However, this ideal situation is, again, very likely not exactly fulfilled so that only trends can be derived from the analysis. Based on the assumption of a homogeneous overlayer, the attenuation of the TaNNN

Photocatalytic degradation of methylene blue under visible light by cobalt ferrite nanoparticles/graphene quantum dots

• Vo Chau Ngoc Anh,
• Le Thi Thanh Nhi,
• Le Thi Kim Dung,
• Dang Thi Ngoc Hoa,
• Nguyen Truong Son,
• Nguyen Thi Thao Uyen,
• Nguyen Ngoc Uyen Thu,
• Le Van Thanh Son,
• Le Trung Hieu,
• Tran Ngoc Tuyen and
• Dinh Quang Khieu

Beilstein J. Nanotechnol. 2024, 15, 475–489, doi:10.3762/bjnano.15.43

• /GQDs nanoparticles. Magnetic properties, morphology, structure, and fluorescence of the nanocomposites were studied, and the photocatalytic degradation of methylene blue as a dye model and the mechanism of methylene degradation were also addressed. Experimental Materials Cobalt(II) nitrate hexahydrate

• first-order kinetic model is widely employed to assess the kinetic data of photocatalytic degradation. This model is as follows: where Ct and C0 are the MB concentration at the beginning and at the time t, respectively; k1 is the first-order kinetic rate constant. The slope of the linear plot of vs t

Superconducting spin valve effect in Co/Pb/Co heterostructures with insulating interlayers

• Andrey A. Kamashev,
• Nadir N. Garif’yanov,
• Aidar A. Validov,
• Vladislav Kataev,
• Alexander S. Osin,
• Yakov V. Fominov and
• Ilgiz A. Garifullin

Beilstein J. Nanotechnol. 2024, 15, 457–464, doi:10.3762/bjnano.15.41

• applications in modern superconducting spintronics [18][19][20][21][22]. In 1997, Beasley and coworkers proposed a theoretical F1/F2/S model of the SSV structure [1]. Another F1/S/F2 model was developed a little later in 1999 by Tagirov [2] and Buzdin and coworkers [3]. In these structures, F1 and F2 are

• the same time, the quantitative agreement between theory and experiment is not good, as expected. The same is true in the case of the dependence plotted in the inset to Figure 4. The theoretical model predicts a sharp decline in Tc at a dPb value close to 40 nm, but the measurements suggest a

• smoother dependence of the critical temperature, possibly extending to lower temperatures. The model also suggests an asymmetric peak in ΔTc(dPb), whereas a more symmetric peak is observed in Figure 3 (at the same time, the left side of the peak is steeper than the right one both in theory and in

Sidewall angle tuning in focused electron beam-induced processing

• Sangeetha Hari,
• Willem F. van Dorp,
• Johannes J. L. Mulders,
• Piet H. F. Trompenaars,
• Pieter Kruit and
• Cornelis W. Hagen

Beilstein J. Nanotechnol. 2024, 15, 447–456, doi:10.3762/bjnano.15.40

• , which was not indicated by a simple model based on etching. An analytical model was developed to include continued etching once the deposit has been removed at the exposed pixel. At this stage the secondary electrons from the substrate then cause the adsorbed water molecules to become effective in

• explained, based on a simple model of the physics involved. Then experimental results are presented, which are quite surprising and call for an extension of the simple model. A more advanced model simulating the FEBIE-assisted sidewall modification is proposed. The simulation results are shown to be in good

• Gaussian sidewalls. Also shown, as a negative Gaussian function, is the etching profile resulting from a point exposure. Note that this is just a two-dimensional model, that is, it represents the cross section of the line and it has zero length in the perpendicular direction. When FEBIE is applied to the

Heat-induced morphological changes in silver nanowires deposited on a patterned silicon substrate

• Elyad Damerchi,
• Sven Oras,
• Edgars Butanovs,
• Allar Liivlaid,
• Mikk Antsov,
• Boris Polyakov,
• Annamarija Trausa,
• Veronika Zadin,
• Andreas Kyritsakis,
• Loïc Vidal,
• Karine Mougin,
• Siim Pikker and
• Sergei Vlassov

Beilstein J. Nanotechnol. 2024, 15, 435–446, doi:10.3762/bjnano.15.39

• ) experiments were performed to study the effect of heat treatment on the inner structure of NWs. Two transmission electron microscopes (Tecnai GF20, FEI and JEOL microscope, model ARM-200F) were used at a 200 kV acceleration voltage. Simulations The extent and distribution of mechanical stresses induced by

• stresses in the middle of the suspended part (up to 1 × 109 N/m2). In this simplified idealistic model, the contact between a NW and Si is absolutely rigid, preventing any slippage or plastic deformation at the interface. Moreover, FEM simulations do not include possible rearrangement of atoms that can

• occur in the real system as a mechanism of stress mitigation. The model is completely elastic, and the simulated processes are fully reversible. Therefore, the results of FEM simulations should only be treated as a simplified qualitative illustration of the thermomechanical processes that may occur in

Classification and application of metal-based nanoantioxidants in medicine and healthcare

• Nguyen Nhat Nam,
• Nguyen Khoi Song Tran,
• Tan Tai Nguyen,
• Nguyen Ngoc Trai,
• Nguyen Phuong Thuy,
• Hoang Dang Khoa Do,
• Nhu Hoa Thi Tran and
• Kieu The Loan Trinh

Beilstein J. Nanotechnol. 2024, 15, 396–415, doi:10.3762/bjnano.15.36

• and increased the survival rate of cells under high H2O2 concentration. In vivo results of another experiment demonstrated the ROS scavenging ability of Au@Cu2O heterostructures in a zebrafish model, which is an organism with morphological and physiological functions similar to those of humans [48

• between cerium(IV) and cerium(III). SOD activity immobilized through cross-linking on a Zr framework (SOD-ZrMOF) demonstrates effective scavenging of ROS and inhibition of oxidative stress. A prolonged investigation using an animal model of acute myocardial infarction revealed that SOD-ZrMOF has the

Insect attachment on waxy plant surfaces: the effect of pad contamination by different waxes

• Elena V. Gorb and
• Stanislav N. Gorb

Beilstein J. Nanotechnol. 2024, 15, 385–395, doi:10.3762/bjnano.15.35

• wax coverage were collected near Jagotyn (Kyiv District, Ukraine; 50° 15′ 25″ N, 31° 46′ 54″ E) and used fresh in the force tests. Insect The leaf beetle C. fastuosa served as a model insect species in this study because it has been used in previous relevant experimental studies on insect attachment

On the mechanism of piezoresistance in nanocrystalline graphite

• Sandeep Kumar,
• Simone Dehm and
• Ralph Krupke

Beilstein J. Nanotechnol. 2024, 15, 376–384, doi:10.3762/bjnano.15.34

• strain within the grains remains constant even though the externally applied strain increased to ca. 0.4%. In an attempt to model piezoresistance in NCG, we have used the tunneling + destruction model for composite materials [24]: The model with five free parameters was fitted to the data as shown in

• Figure 2c, and the fit parameters are given in Table 1. The model was initially given for a matrix in which conducting particles are dispersed in a polymer matrix and are separated by tunnel junctions. In this model, the conductivity in the film is determined by the number of conductive paths, N, and the

• tunneling distance, d. The model has been used to explain the piezoresistance for several composite materials [29][30]. Zhao et al. [24] used the model to explain the piezoresistance in nanographene films, although the material is comparable to ours and not a composite material in the original sense. NCG

Investigating ripple pattern formation and damage profiles in Si and Ge induced by 100 keV Ar⁺ ion beam: a comparative study

• Indra Sulania,
• Harpreet Sondhi,
• Tanuj Kumar,
• Sunil Ojha,
• G R Umapathy,
• Ambuj Mishra,
• Ambuj Tripathi,
• Richa Krishna,
• Devesh Kumar Avasthi and
• Yogendra Kumar Mishra

Beilstein J. Nanotechnol. 2024, 15, 367–375, doi:10.3762/bjnano.15.33

• processes (i.e., thermal diffusion and ion-induced diffusion) [32]. This approach is based on the linear cascade model and Gaussian approximation of energy distribution as developed by Sigmund [26] to describe ion–atom collisions inside the target. Rutherford backscattering spectrometry (RBS) studies in the

Modulated critical currents of spin-transfer torque-induced resistance changes in NiCu/Cu multilayered nanowires

• Mengqi Fu,
• Roman Hartmann,
• Julian Braun,
• Sergej Andreev,
• Torsten Pietsch and
• Elke Scheer

Beilstein J. Nanotechnol. 2024, 15, 360–366, doi:10.3762/bjnano.15.32

• oscillatory manner by the magnetic field in the nanowire-based devices. We present a toy model to qualitatively explain these observations. Keywords: AAO template; critical current; multilayered magnetic nanowires; spin-transfer torque; three-dimensional devices; Introduction Spin-transfer torque (STT) has

• the applied magnetic field [28][33]. To our knowledge, this oscillatory behavior of the critical currents in multilayer nanowire arrays is rarely reported. To phenomenologically interpret the nonmonotonous changes of the critical currents, we propose a model system consisting of five adjacent layers

• (one fixed layer, two free layers, and two spacer layers) as shown in Figure 4. With this model we qualitatively explain how one period of the Ic+ modulation is formed. As shown in Figure 4, the NiCu layers are labelled as layer 1 to layer 3 from top to bottom. As discussed above, layer 1 is the fixed

Controllable physicochemical properties of WO_x thin films grown under glancing angle

• Rupam Mandal,
• Aparajita Mandal,
• Alapan Dutta,
• Rengasamy Sivakumar,
• Sanjeev Kumar Srivastava and
• Tapobrata Som

Beilstein J. Nanotechnol. 2024, 15, 350–359, doi:10.3762/bjnano.15.31

• heterostructures were performed by preparing Ag electrodes (1 mm diameter) on top of the WOx films and p-Si substrates. The I–V data were acquired by applying DC voltage sweeps (−1 V→0 V→+1 V) using a Keithley source meter (Model 2400, Tektronix, USA) in a sandwiched configuration. During the measurements, the

Nanomedicines against Chagas disease: a critical review

• Maria Jose Morilla,
• Kajal Ghosal and
• Eder Lilia Romero

Beilstein J. Nanotechnol. 2024, 15, 333–349, doi:10.3762/bjnano.15.30

• than in the laboratory and showed a comparable in vitro activity to free BNZ [33]. Formulated as oral tablets containing a reduced dose of BNZ/cyclodextrin (50% loading of BNZ (% BNZ/total mass)) and administered to a murine model, BNZ/cyclodextrin did not overcome the efficacy of free BNZ during the

• increased 10-fold (from 0.4 mg/mL for bulk BNZ to 3.99 mg/mL for BNZ-NC) [49]. After oral administration of BNZ-NC to an acute murine model infected with the Nicaragua strain of T. cruzi at 300 mg/kg total dose (TD) (30 days treatment) and 375 mg/kg TD (15 days treatment), which was about half of the 750 mg

• /kg free BNZ TD administered at 50 mg/kg/day over 15 days, both BNZ-NC and free BNZ showed 100% survival at 50 days post-infection (dpi) [50]. In a model of immunosuppressed chronic phase, 750 mg/kg BNZ-NC TD showed the same efficacy as 1500 mg/kg free BNZ. Immunosuppressed mice treated with BNZ-NC

Comparative electron microscopy particle sizing of TiO₂ pigments: sample preparation and measurement

• Ralf Theissmann,
• Christopher Drury,
• Markus Rohe,
• Thomas Koch,
• Jochen Winkler and
• Petr Pikal

Beilstein J. Nanotechnol. 2024, 15, 317–332, doi:10.3762/bjnano.15.29

• . The complete EM particle size distributions were used to calculate the SSA values for the five samples using three distinct models, namely one based on particle ECD, another on MinFeret values, and the third on the Cauchy model. These results are summarised in Table 5. Comparing the calculated SSA

• , and M3 completely rely on particle edge detection by the human eye, which is the most accurate detection method assuming good laboratory practice. Methods M1, P1, and P6 rely on automated particle detection, the former using a model-free sizing algorithm and the latter two using a sizing algorithm

Investigating structural and electronic properties of neutral zinc clusters: a G₀W₀ and G₀W₀Г₀⁽¹⁾ benchmark

• Sunila Bakhsh,
• Muhammad Khalid,
• Sameen Aslam,
• Muhammad Sohail,
• Muhammad Aamir Iqbal,
• Mujtaba Ikram and
• Kareem Morsy

Beilstein J. Nanotechnol. 2024, 15, 310–316, doi:10.3762/bjnano.15.28

• cluster size, the curve slightly flattens (up to n = 6). There is a sharp increase in the curve for n = 7, 9, and 10. These high binding energies display the higher stability of these particular clusters, which is consistent with the shell model and spectroscopic observations. Wang et al. [7] also

• correction is closer to the experimental value of 9.0 ± 0.2 eV. IPs from a model Hamiltonian presented by Tarento [34] suggested a value of 8.61 eV, and our IP is the closest to the reported experimental result. Furthermore, the correction for a cluster size of n = 2–7 was used to compare our IPs from G0W0

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

• lack such information. To further clarify the influence of the zeta potential on cell damage, a QSPR model was developed with 132 MeOx NMs to understand the possible mechanisms of cell damage. The results showed that zeta potential, along with seven other descriptors, had the potential to influence

• potential dataset; for the cell damage dataset, 111 compounds were present in the training set, and the remaining 21 compounds were in the test set. The training set compounds were used for feature selection and model development; the test set was utilized for assessing the predictivity of the developed

• 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

Determining by Raman spectroscopy the average thickness and N-layer-specific surface coverages of MoS₂ thin films with domains much smaller than the laser spot size

• Felipe Wasem Klein,
• Jean-Roch Huntzinger,
• Vincent Astié,
• Damien Voiry,
• Romain Parret,
• Houssine Makhlouf,
• Sandrine Juillaguet,
• Jean-Manuel Decams,
• Sylvie Contreras,
• Périne Landois,
• Ahmed-Azmi Zahab,
• Jean-Louis Sauvajol and
• Matthieu Paillet

Beilstein J. Nanotechnol. 2024, 15, 279–296, doi:10.3762/bjnano.15.26

• . For comparison with other setups or references, the polarization ratio of our setup and the relative values measured on Si(100) with native oxide and 90 nm SiO2 are given in Supporting Information File 1. As noted by several authors and predicted by the optical interference model, the normalized

• with the model of Li and coworkers [31] (black solid line in Figure S3d–f). (Note that in this latter work the experimental data on which the model has been adjusted were recorded using a numerical aperture N.A. ≈ 0.45). MoS2 flakes prepared by CVD In this part, we analyze the pertinence of the

• substrate surface is completely covered by MoS2 and increases continuously, representing about 50% of the thickest samples ( ≈ 2.8). In order to verify our approach, we implemented a 2D growth toy model (see Supporting Information File 1 for details). The model results are shown in Figure 9b as full lines