E ﬀ ect of Ag Nanoparticle Size on Ion Formation in Nanoparticle Assisted LDI MS

: Metal nanoparticles (NPs) were reported as an e ﬃ cient matrix for detection of small molecules using laser desorption / ionization mass spectrometry. Their pronounced e ﬃ ciency is mostly in desorption enhancement, while, in some cases, NPs can facilitate charge transfer to a molecule, which has been reported for alkali metals and silver. In this work, we present the study of the inﬂuence of Ag NP size on the laser desorption / ionization mass spectra of a model analyte, the molecule of riboﬂavin. The NPs were produced by magnetron sputtering-based gas aggregation in a vacuum and mass-ﬁltered before the deposition on substrates. It was found that the utilization of smaller Ag NPs (below 15 nm in diameter) considerably enhanced the molecule desorption. In contrast, the laser irradiation of the samples with larger NPs led to the increased ablation of silver, resulting in [analyte + Ag] + adduct formation.


Introduction
Surface enhancement employing nanomaterials in detection and imaging is implemented in many applications, including mass spectrometry [1], fluorescence imaging [2], Raman scattering [3][4][5], and various sensing technologies [6]. Often, the nanomaterials are prepared as nanoparticles (NPs), as there is a number of efficient production methods [7] also allowing the tailoring of the NP properties [8]. In particular, metal NPs are widely used in laser desorption/ionization mass spectrometry (LDI MS) [9]. Irradiating the samples with short laser pulses creates a plume of species (neutrals, ions, and molecules in excited states). Ionized species can be extracted and analyzed. For a few reasons, an additional component is required (the so-called matrix) that enhances the desorption and facilitates the charging of the molecules of interest [10]. Metal NPs can be such a matrix; two methods in the literature are the so-called surface-assisted LDI MS (SALDI MS) [11] and nanoparticle-assisted LDI MS (nano-PALDI MS) [12]. Two effects are typically highlighted when NPs are used as a matrix in LDI MS: local heating [13] (resulting in desorption enhancement) and high surface reactivity (which can lead to improved selectivity [14] and, thus, the increased sensitivity of the method [15]). Moreover, the matrix should provide conditions for efficient ionization [16]. Commonly, a protonation of an analyte is expected. However, a NP can also be a source of ions, which can form adducts with the molecules of interest [17].
An empirical approach was employed in the majority of studies, where nanomaterials were used as a matrix for LDI MS [18][19][20]. Although the reported high sensitivity and selectivity are remarkable, only a few works have studied the fundamental aspects of the processes leading to the enhancement. In particular, the physics of laser-nanoparticle interaction in the presence of biological tissue has been studied relatively poorly, and this is easy to explain: the system is very complex. Though a nanoparticle matrix is considered to become "hot" under a laser impulse, leading to the more frequent fragmentation of an analyte, it also allows ionizing molecules that are not typically ionized using other matrix types [21,22]. The cationization of analytes was investigated, mostly focusing on alkali metals, as those form single charged ions [23,24]. In particular, a competition between different cationization agents on the riboflavin molecule was investigated [25]. In many cases [26][27][28], the charge transfer process was studied in metal salts or nanostructured surfaces. The conclusions of that research are not directly transferrable to NP-based matrices.
Silver is known as an element that efficiently forms adducts with different analytes [17]. This is related to the close proximity of the localized surface plasmon resonance (LSPR) wavelengths of Ag NPs to the typical laser wavelengths used in LDI MS devices and, thus, to an efficient energy transfer from the laser to the NPs [29]. For example, in our previous work, we showed that gas-aggregated Ag NPs have an adsorption maximum at 367 nm, while one of the commonly used laser wavelengths in MALDI devices is 355 nm [30]. We reported that use of large Ag NPs (32 ± 6 nm in diameter) led to a formation of adducts between small molecules and silver atoms. However, there were no studies on the NP size and its impact on ion formation and MALDI efficiency. Moreover, the application of small-size Ag NPs (below 10 nm) is intensively exploited for the detection of small molecules [30,31] and mass spectrometry imaging [32,33], demonstrating the enhancement of a signal [M + H] + ion in the most cases, where M denotes the molecule of interest. Even though a formation of [M + Ag] + ions was observed for certain molecules, the underlying physical processes were not investigated. The current study addresses two issues regarding the effect of NP size: i) the ion formation of a small-molecular-weight analyte; ii) the material release from NPs and adduct formation with the analyte molecule.

Materials and Methods
The substrate choice was confined by conditions for the time-of-flight (TOF) MS. It was necessary to have relatively small-sized, thin, conductive-from-both-sides, and flexible substrates, which would not superinduce additional ions in the mass spectra. The substrates were made of 0.1 mm-thick polyethylene terephthalate (PET) sheets. Plastic sheets were cut into 12 × 12 mm pieces, cleaned in isopropanol, and dried in air. The 250 nm-thick Cu film was deposited on each side in a custom-made vacuum system equipped with a 2" water-cooled magnetron with a Cu target. The film thickness was measured using an AlphaStep D-500 profilometer from KLA Tencor. The sputtering was carried out using Ar under 4 Pa of pressure and an applied current of 150 mA (DC power, 43 W).
Riboflavin (C 17 H 20 N 4 O 6 ; molecular weight, 376.37 g/mol; p.a. grade) was used as a model molecule. The molecule contains a flavin group, representing importance for medical applications [34], and, as mentioned above, was used in similar studies. While a common approach to depositing an analyte onto the substrate is droplet crystallization, our preliminary tests showed that it results in the low reproducibility of MS in terms of both ion composition and absolute intensity. We relate this with the non-homogeneous analyte crystallization and coffee-ring effects [35]. Instead, a fine riboflavin powder was sprinkled over the substrate surface. We refer, by "fine powder", to microparticles that had a submillimeter diameter. By doing this, we were able to perform laser shots on the riboflavin surface, avoiding the necessity of dealing with crystallization issues. The substrates were placed into the vacuum chamber, where the NPs were deposited as described below, stabilizing the powder on the surface.
Silver NPs were produced using a commercial nanocluster source (NC200U from Oxford Applied Research) attached to the custom-built vacuum system, which, together with the source, was called MaSCA [36]. The particles were formed by the magnetron sputtering of a silver target (99.99% purity) and aggregation of the sputtered material in a vacuum. The NPs were collimated into a beam and mass-filtered prior to deposition using an electrostatic quadrupole mass selector, providing standard deviations of the particle diameters within 10% [37]. After the size selection, the NPs were deposited on the Cu/PET substrates in a soft-landing regime [38]. More details about the MaSCA and operation conditions can be found elsewhere [39]. For the current experiments, the NPs were filtered at voltages 200, 500, 700, 1100, and 1600 V. The chosen range of voltages defining the particle sizes (diameters) was based on the best sustainability for the deposition of mass-filtered NPs. The beam currents and deposition times were controlled in order to obtain the same surface coverage of NPs for every filtering voltage, (3 ± 1)·10 11 cm −2 .
The deposited NPs were studied by atomic force microscopy (AFM) using a Ntegra Aura system (from NT-MDT). Commercial Si cantilevers with a tip curvature radius ≤ 10 nm were employed. It was found that the copper films on the PET substrates had a nanogranular structure with relatively high roughness (root mean square, RMS = 11.5 nm), as can be seen in Figure 1. Such surface morphology made it difficult to distinguish the deposited nanometer-scale particles. Therefore, the NPs were also deposited in parallel on smooth Si substrates (RMS < 0.5 nm), which were used for the size analysis.
Appl. Nano 2020, 1, FOR PEER REVIEW 3 providing standard deviations of the particle diameters within 10% [37]. After the size selection, the NPs were deposited on the Cu/PET substrates in a soft-landing regime [38]. More details about the MaSCA and operation conditions can be found elsewhere [39]. For the current experiments, the NPs were filtered at voltages 200, 500, 700, 1100, and 1600 V. The chosen range of voltages defining the particle sizes (diameters) was based on the best sustainability for the deposition of mass-filtered NPs. The beam currents and deposition times were controlled in order to obtain the same surface coverage of NPs for every filtering voltage, (3 ± 1)•10 11 cm −2 .
The deposited NPs were studied by atomic force microscopy (AFM) using a Ntegra Aura system (from NT-MDT). Commercial Si cantilevers with a tip curvature radius ≤ 10 nm were employed. It was found that the copper films on the PET substrates had a nanogranular structure with relatively high roughness (root mean square, RMS = 11.5 nm), as can be seen in Figure 1. Such surface morphology made it difficult to distinguish the deposited nanometer-scale particles. Therefore, the NPs were also deposited in parallel on smooth Si substrates (RMS < 0.5 nm), which were used for the size analysis. For the LDI MS, the prepared samples were placed on ITO-covered glass using double-sided carbon tape and positioned on an MTP Slide Adapter II from Bruker. Mass spectra were acquired in the positive reflector ion mode using pulsed extraction with an extraction voltage of 16.3 kV, an acceleration voltage of 19 kV, a reflector voltage of 21 kV, a lens voltage of 8.3 kV, and a delayed extraction time of 130 ns on an autoflex™ speed mass spectrometer (from Bruker Daltonics). The laser was a Nd:YAG laser generating the third harmonic with a 355 nm wavelength. It produced pulses of 3 ns with an up to 2 kHz repetition rate. A single spectrum was acquired as an accumulation of 500 shots with a random walk pattern. Mass spectra were calibrated on silver ions (from 100 to 970 Da). Further processing was performed using the mMass software.

Nanoparticle Characterization
An AFM image of a sample with NPs filtered at 200 V and deposited on the Si substrate is shown in Figure 2. The corresponding height histogram yields a mean value of 10.2 ± 1.0 nm. The height measurements were also carried for the particles deposited after filtering at 500, 700, 1100, and 1600 V (see Figures S1-S4 in Supplementary Materials). The particles filtered at adjacent For the LDI MS, the prepared samples were placed on ITO-covered glass using double-sided carbon tape and positioned on an MTP Slide Adapter II from Bruker. Mass spectra were acquired in the positive reflector ion mode using pulsed extraction with an extraction voltage of 16.3 kV, an acceleration voltage of 19 kV, a reflector voltage of 21 kV, a lens voltage of 8.3 kV, and a delayed extraction time of 130 ns on an autoflex™ speed mass spectrometer (from Bruker Daltonics). The laser was a Nd:YAG laser generating the third harmonic with a 355 nm wavelength. It produced pulses of 3 ns with an up to 2 kHz repetition rate. A single spectrum was acquired as an accumulation of 500 shots with a random walk pattern. Mass spectra were calibrated on silver ions (from 100 to 970 Da). Further processing was performed using the mMass software.

Nanoparticle Characterization
An AFM image of a sample with NPs filtered at 200 V and deposited on the Si substrate is shown in Figure 2. The corresponding height histogram yields a mean value of 10.2 ± 1.0 nm. The height measurements were also carried for the particles deposited after filtering at 500, 700, 1100, and 1600 V (see Figures S1-S4 in Supplementary Materials). The particles filtered at adjacent voltages-for example, 500 and 700 or 700 and 1100 V-have a slight overlap in sizes due to the standard deviations. However, small voltage steps allowing the fine tuning (increase) of NP size can be essential for judging the role of NP diameter. These data are summarized in Table 1. The obtained values are in good agreement with the results previously published for NP size selection in MaSCA [34]. It is worth mentioning that silver NPs soft-landed in MaSCA typically retain their almost spherical shape; they only slightly oblate [40]. Thus, the AFM measurements of the particle heights can be a good estimate for the mean diameter/size. The particles filtered at 200, 500, 700, 1100, and 1600 V will be further referred to as 10, 15, 17, 20, and 23 nm NPs.

Riboflavin Fragmentation
The riboflavin molecule consists of dimethyl isoalloxazine with an attached ribitol sugar. Figure 3 shows its molecular structure, highlighting possible bond cleavage spots. Two fragments with molecular weights of 242 (denoted as R1) and 135 g/mol (as R2) are observed in the mass spectra prepared with different matrices and under LDI mode, as the cleavage of the C-N bond comes up at lower laser fluence [41]. The cleavage of C-C bonds in ribitol sugar under higher laser fluence results in the appearance of charged fragments: adducts between the riboflavin molecule, its R1 part, cleaved parts of ribitol sugar (CH 2 , CH 2 COH 2 , etc.), and Ag atoms. The mass spectra of riboflavin covered with Ag NPs have ions grouped into three categories. The first one is the silver clusters Ag n + (n ≤ 9). The intensities of Ag + , Ag 2 + , and Ag 3 + ions are found to be stable (within 10% error) for each measured mass spectrum, resulting in a ratio of 1:  Table 2 summarizes the experimental ion patterns and attributed molecular components. The observed ions were taken from a few randomly selected mass spectra for samples covered with NPs of different sizes, while it should be noted that the increase in laser energy and NP size led to the appearance of higher ion variety.
Appl. Nano 2020, 1 7 The attribution is based on the mass/charge ratio (m/z), possible chemical structure, and isotopic pattern (modeled in mMass based on the chemical formula). The difference between the experimental and theoretical values is related to the spectrometer resolution. The typical full width at half maximum (FWHM) of the detected peaks is found between 0.1 and 0.4 Da, depending on the counts for particular ion. The intensity of the given mass peaks depends on the laser fluence and NP sizes. These effects are discussed below.
Appl. Nano 2020, 1, FOR PEER REVIEW 5 experimental and theoretical values is related to the spectrometer resolution. The typical full width at half maximum (FWHM) of the detected peaks is found between 0.1 and 0.4 Da, depending on the counts for particular ion. The intensity of the given mass peaks depends on the laser fluence and NP sizes. These effects are discussed below.

Effect of Laser Fluence and NP Size on Mass Spectra of Riboflavin
The effect of laser fluence on the obtained mass spectra is shown in Figure 4. Note that laser fluence is calculated as a percentage of the total laser power (TLP), the only parameter provided by the TOF MS manufacturer. The lower fluence limit is determined by the threshold above which the number of generated ions start prevailing over the instrumental noise (40% of the TLP in our case) [42]. The upper fluence limit is related to the phenomenon of electrostatic repulsion in the ion cloud, causing m/z shifts, an increase in the FWHM, and signal distortion [43]. In our case, these effects become drastic when the fluence approaches 55% of the TLP.

Effect of Laser Fluence and NP Size on Mass Spectra of Riboflavin
The effect of laser fluence on the obtained mass spectra is shown in Figure 4. Note that laser fluence is calculated as a percentage of the total laser power (TLP), the only parameter provided by the TOF MS manufacturer. The lower fluence limit is determined by the threshold above which the number of generated ions start prevailing over the instrumental noise (40% of the TLP in our case) [42]. The upper fluence limit is related to the phenomenon of electrostatic repulsion in the ion cloud, causing m/z shifts, an increase in the FWHM, and signal distortion [43]. In our case, these effects become drastic when the fluence approaches 55% of the TLP.
At the lowest used laser fluence, the mass spectrum contains only protonated riboflavin, its protonated fragments, and [M + Ag] + ions of relatively low intensity. The absence of Ag n + clusters and their adducts means that the transferred energy is not sufficient to eject Ag atoms from the Appl. Nano 2020, 1 8 NPs. The abovementioned clusters, as well as silver ions, and adducts with riboflavin/fragments start appearing at higher fluences.
Appl. Nano 2020, 1, FOR PEER REVIEW 6 At the lowest used laser fluence, the mass spectrum contains only protonated riboflavin, its protonated fragments, and [M + Ag] + ions of relatively low intensity. The absence of Agn + clusters and their adducts means that the transferred energy is not sufficient to eject Ag atoms from the NPs. The abovementioned clusters, as well as silver ions, and adducts with riboflavin/fragments start appearing at higher fluences. Figure 5 shows the differences in the mass spectra for riboflavin covered with 10, 15, 17, and 23 nm Ag NPs (all the graphs have the same y-scale). In this case, the sample was irradiated with a fluence equivalent to 43% of the TLP. In the obtained spectra, one can see two main tendencies: (i) the intensity of protonated ions (for example, [R1 + H] + and [M + H] + ) changes insignificantly with an increase in the particle size, while (ii) the ion counts related to silver clusters and adducts increase drastically for the cases of larger NPs. Two effects can be attributed to the observed phenomena: an increased interaction cross-section for the NPs of larger diameter (and, as a result, higher laser energy absorption) [44], and enhanced optical extinction due to the LSPR of Ag NPs [38,45]. Thus, the laser power transferred to an NP causes heating and a strong local electromagnetic field; both effects can facilitate the ejection of atoms or even small clusters. According to the Mie theory, the absorption cross-section depends on the cube of the particle radius [46]. Thus, one can suppose that for the smallest NPs, the absorbed energy is lower than a threshold value required for the ejection, while with the particle size increase, an ejection of ions and small clusters becomes possible, as can be seen in Figure 5. Since the thermal and electromagnetic phenomena interact for a metal NP in a sophisticated manner, the abovementioned hypothesis requires further study going beyond the goals of the current paper.  Figure 5 shows the differences in the mass spectra for riboflavin covered with 10, 15, 17, and 23 nm Ag NPs (all the graphs have the same y-scale). In this case, the sample was irradiated with a fluence equivalent to 43% of the TLP. In the obtained spectra, one can see two main tendencies: (i) the intensity of protonated ions (for example, [R1 + H] + and [M + H] + ) changes insignificantly with an increase in the particle size, while (ii) the ion counts related to silver clusters and adducts increase drastically for the cases of larger NPs. Two effects can be attributed to the observed phenomena: an increased interaction cross-section for the NPs of larger diameter (and, as a result, higher laser energy absorption) [44], and enhanced optical extinction due to the LSPR of Ag NPs [38,45]. Thus, the laser power transferred to an NP causes heating and a strong local electromagnetic field; both effects can facilitate the ejection of atoms or even small clusters. According to the Mie theory, the absorption cross-section depends on the cube of the particle radius [46]. Thus, one can suppose that for the smallest NPs, the absorbed energy is lower than a threshold value required for the ejection, while with the particle size increase, an ejection of ions and small clusters becomes possible, as can be seen in Figure 5. Since the thermal and electromagnetic phenomena interact for a metal NP in a sophisticated manner, the abovementioned hypothesis requires further study going beyond the goals of the current paper.
The integration of the measured signal obtained from the full isotopic pattern of a single molecule provides a value proportional to the number of generated ions. Based on the relative simplicity of our system (monomolecular sample and size-selected NPs), we can collect mass spectra of similar intensity from different samples and, thus, analyze the changes in ion counts through the absolute values of areas for the isotopic patterns. After initial data filtering (the removal of artifacts and mass spectra with low total ion counts), it is possible to compare the most prominent attributed structures depending on both the laser fluence and silver NP size. The results of the data evaluation are presented in Figure 6. The first important conclusion is that the absolute intensity of protonated riboflavin is independent (within errors) of the Ag NP size, while it increases with the laser fluence. We observe a slight decrease in [M + H] + ion counts only for the highest laser fluences, which can be related to the significant increase in Ag ion intensity and consequent suppression effects [47]. The signal of Ag + shows the same tendency to increase with particle size for all laser fluences, although the intensity values are higher for the higher fluences, which is well understood; higher power transfer leads to a higher level of material ablation. An important finding is that the NPs should be above a certain "threshold size" (around 15 nm in our case) to promote the materials' release, which is already discussed above (see Figure 5). This "threshold size" is also evident for the formation of [M + Ag] + ions. Within the errors of the experiments, the intensity of this signal does not considerably depend on either NP size or laser fluence.
Appl. Nano 2020, 1, FOR PEER REVIEW 7 Figure 5. The effect of NP size on mass spectra of riboflavin for laser fluence equivalent to 43% of total laser power.
The integration of the measured signal obtained from the full isotopic pattern of a single molecule provides a value proportional to the number of generated ions. Based on the relative simplicity of our system (monomolecular sample and size-selected NPs), we can collect mass spectra of similar intensity from different samples and, thus, analyze the changes in ion counts through the absolute values of areas for the isotopic patterns. After initial data filtering (the removal of artifacts and mass spectra with low total ion counts), it is possible to compare the most prominent attributed structures depending on both the laser fluence and silver NP size. The results of the data evaluation are presented in Figure 6. The first important conclusion is that the absolute intensity of protonated riboflavin is independent (within errors) of the Ag NP size, while it increases with the laser fluence. We observe a slight decrease in [M + H] + ion counts only for the highest laser fluences, which can be related to the significant increase in Ag ion intensity and consequent suppression effects [47]. The signal of Ag + shows the same tendency to increase with particle size for all laser fluences, although the intensity values are higher for the higher fluences, which is well understood; higher power transfer leads to a higher level of material ablation. An important finding is that the NPs should be above a certain "threshold size" (around 15 nm in our case) to promote the materials' release, which is already discussed above (see Figure 5). This "threshold size" is also evident for the formation of [M + Ag] + ions. Within the errors of the experiments, the intensity of this signal does not considerably depend on either NP size or laser fluence. Appl. Nano 2020, 1, FOR PEER REVIEW 8 Figure 6. Comparison of absolute ion intensity for the selected ions as a function of Ag NP size for 43% and 48% of total laser power (TLP). Data points corresponding to the given NP sizes are intentionally slightly shifted on the x-axis for better visualization. Figure 7 shows the ratio between the intensities for [M + Ag] + and Ag + ions for different laser fluences and NP sizes. It can be seen that for the lowest laser fluence and smallest NPs, the energy transfer is not enough to cause any considerable release of [M + Ag] + ions. For the higher fluences, the observed tendencies are the same concerning the particle size. The release of the silver ions is higher for the higher values of the laser fluence, and it has the same trend for the larger NPs. As for the ablated silver ions, it is evident that the utilization of NPs as a matrix would require the proper optimization of the material quantity (NP surface coverage) together with the laser fluence. For the Figure 6. Comparison of absolute ion intensity for the selected ions as a function of Ag NP size for 43% and 48% of total laser power (TLP). Data points corresponding to the given NP sizes are intentionally slightly shifted on the x-axis for better visualization. Figure 7 shows the ratio between the intensities for [M + Ag] + and Ag + ions for different laser fluences and NP sizes. It can be seen that for the lowest laser fluence and smallest NPs, the energy transfer is not enough to cause any considerable release of [M + Ag] + ions. For the higher fluences, the observed tendencies are the same concerning the particle size. The release of the silver ions is higher for the higher values of the laser fluence, and it has the same trend for the larger NPs. As for the ablated silver ions, it is evident that the utilization of NPs as a matrix would require the proper optimization of the material quantity (NP surface coverage) together with the laser fluence. For the proper measurement, the intensity of the silver ions should not significantly exceed the [M + Ag] + intensity. For example, for the TLP of 43%, the silver ion counts do not exceed those of the riboflavin/silver ions (see Figure 6). Meanwhile, for the TLP of 52%, the quantity of silver ions released from 17 nm NPs is equal to that of [M + Ag] + . Figure 6. Comparison of absolute ion intensity for the selected ions as a function of Ag NP size for 43% and 48% of total laser power (TLP). Data points corresponding to the given NP sizes are intentionally slightly shifted on the x-axis for better visualization. Figure 7 shows the ratio between the intensities for [M + Ag] + and Ag + ions for different laser fluences and NP sizes. It can be seen that for the lowest laser fluence and smallest NPs, the energy transfer is not enough to cause any considerable release of [M + Ag] + ions. For the higher fluences, the observed tendencies are the same concerning the particle size. The release of the silver ions is higher for the higher values of the laser fluence, and it has the same trend for the larger NPs. As for the ablated silver ions, it is evident that the utilization of NPs as a matrix would require the proper optimization of the material quantity (NP surface coverage) together with the laser fluence. For the proper measurement, the intensity of the silver ions should not significantly exceed the [M + Ag] + intensity. For example, for the TLP of 43%, the silver ion counts do not exceed those of the riboflavin/silver ions (see Figure 6). Meanwhile, for the TLP of 52%, the quantity of silver ions released from 17 nm NPs is equal to that of [M + Ag] + .

Conclusions
Size-selected Ag NPs were prepared using the gas aggregation of magnetron-sputtered Ag and deposited on the substrates with the model analyte, riboflavin, in order to study the efficiency of NPs as a matrix for enhancing nano-PALDI MS. It has been shown that the release of Ag atoms, clusters, and ions from the NP surface and the formation of Ag adducts with the analyte molecule strongly depend on the NP size and laser fluence. Our study revealed that the silver release under the laser irradiation is insignificant for small NPs. However, it considerably increases for the particles with sizes ≥ 15 nm: silver ions and small charged silver clusters become the dominant species in the spectra. It is suggested that the particle heating and formation of a strong electromagnetic field (due to LSPR) upon interaction with laser light could be the main factors affecting the materials' release. The presence of metal ions in the plume triggers the formation of adducts with riboflavin and its fragments. In order to use the adduct ions for molecular detection, a proper amount of NP material in the matrix (requiring the adjustment of the NP size and surface coverage) should be used. One can also conclude that the use of matrices with large silver NPs could allow the investigation of other cationization agents.
Supplementary Materials: The following are available online at http://www.mdpi.com/2673-3501/1/1/2/s1. Figure S1: (a) AFM image and (b) height distribution of deposited Ag NPs filtered at 500 V; Figure S2 Funding: V.P. acknowledges the financial support from the Czech Science Foundation through the project GACR 19-20927Y and financial support from the Standard Trainership Erasmus+ program for staff mobility. F.D. was supported from the European Regional Development Fund-Project "Mechanisms and dynamics of macromolecular complexes: from single molecules to cells" (No. CZ.02.1.01/0.0/0.0/15_003/0000441). J.K. was supported from TAČR GAMA-2 TP01010019. V.S. acknowledges the financial support from the Czech Science Foundation through the project GACR 19-20168S.