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13 protocols using isr 2600plus

1

Comprehensive Material Characterization Protocol

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BPs concentrations were determined by inductively coupled plasma atomic emission spectroscopy (Agilent 8800, Tokyo, Japan), as described in our studies. SEM imaging was performed on a field-emission SEM (NOVA NANOSEM430, FEI, Eindhoven, Netherlands) at 5–10 kV after gold coating for 120 s (EM-SCD500, Leica, Wetzlar, Germany). TEM imaging was assessed using a high resolution JEOL JEM 2010 F TEM (Hitachi Scientific Instruments, Tokyo, Japan). The ultraviolet–visible–near infrared (UV–vis–NIR) absorption spectra were obtained on a UV–vis–NIR spectrometer with integrating sphere attachment (ISR-2600 Plus; Shimadzu UV-2600, Kyoto, Japan). The FTIR spectra were recorded with a Thermo-Nicolet Nexus 6700 FTIR spectrometer (Madison, WI).
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2

Shimadzu UV-Vis Spectrophotometry Protocol

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Absorption spectra were recorded using 1 cm quartz cuvettes with the Shimadzu UV-Vis spectrophotometer ISR-2600 Plus (Shimadzu, Japan).
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3

Optical Characterization of Turbid Phantoms

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Three different
homogeneous model samples, made of polytetrafluoroethylene (PTFE),
polyethylene (PE), and polystyrene (PS), exhibiting different optical
properties (μa, μS′) in the
NIR spectral region (see Figure 2a–c), were used as turbid media. A heterogeneous
phantom structured as a layered turbid matrix made of PE (50 mm ×
50 mm × 3 mm each layer) and paracetamol (cylindrical shape radius
= 2, 3, and 5 mm, thickness = 3 mm) was used for mimicking the presence
of an inclusion (paracetamol) at depth in the turbid matrix (PE) (see Figure 1a, bottom). The bilayer
phantom was an assembly in order to permit the variation of the overall
thickness (t = 12, 18, 21, and 24 mm) and the amount
of the inclusion (m = 125, 250, and 500 mg of paracetamol).
The optical properties of the phantom matrix were characterized using
a benchtop spectrophotometer equipped with an integrating sphere (ISR-2600Plus,
Shimadzu). Diffuse reflectance measurements were performed from 700
to 1100 nm with a spectral resolution of 0.2 nm. From the spectral
reflectance of the sample (R(λ)), the Kubelka–Munk
model22 (link) was applied for evaluating the
scattering and absorption properties of the turbid matrix (i.e., k/s
Kubelka–Munk function23 ).
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4

Quantification of ZnO Nanoparticles in Samples

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Firstly, calibration curves relating to ZnO NPs concentration in water (with absorbance value ~375 nm (due to the band-gap absorption for ZnO resulting from removed electrons from the valence band to the conduction band [33 (link),34 ,35 (link)]) were constructed, following a range of dilutions between 1:500 and 1:8000 that enabled reliable detection of the spectra’s region of interest. Results were plotted as absorbance vs. concentration (Figure S2). Then, absorbance scans of each sample (representative rectangles with 6 × 2 cm2) were collected between 190–1100 nm (resolution of 1 nm), with a UV-2600 UV-vis spectrophotometer by resorting to an integrating sphere (ISR-2600Plus) with a film holder for transmittance analysis (Shimadzu Corporation, Kyoto, Japan). The quantity of ZnO NPs loaded onto each functionalized NWF was estimated in an indirect manner. For each spectrum, absorbance peak height (values between 360–390 nm) was registered. The estimation of detected ZnO NPs presence (wt%) in these samples was then calculated taking into consideration detected ZnO NPs concentration (µg/mL) by means of the predetermined calibration curve, along with sample volume crossed by the laser that resulted from the determination of laser cross-section in transmission and sample thickness.
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5

Quantifying Au Nanoparticles on TiO2

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For quantifying the loading amount of Au, Au NPs loaded on TiO2 were dissolved by using aqua regia, and the concentration was determined by inductively coupled plasma spectroscopy. The samples for TEM and HR-TEM observation were prepared by dropping a suspension of the samples in ethanol onto a copper grid with a carbon support film (grid-pitch 150 μm, Okenshoji Co., Ltd, #10-1006). The measurements were performed by using a JEOL JEM-2100F at an applied voltage of 200 kV. The Au particle size (dAu) was determined from the image analysis of ∼200 Au particles observed in TEM images. Diffuse reflectance UV-vis-NIR absorption spectra were measured by using a UV-2600 spectrometer (Shimadzu) with an integrating sphere unit (Shimadzu, ISR-2600Plus). BaSO4 was used as a reference for the reflectance (R). The Kubelka–Munk function [F(R) = (1 − R)2/2R] was used for expressing the relative absorption coefficient. The measurement was carried out by using sample powder without dilution. X-ray photoelectron spectra (XPS) were collected by using a Kratos Axis Nova X-ray photoelectron spectrometer at 15 kV and 10 mA using Al Kα as the X-ray source. For the energy reference, the peak of C 1s (284.6 eV) was used.
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6

Diffuse Reflectance Spectra Acquisition

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Diffuse reflectance spectra were acquired on a Shimadzu (Kyoto, Japan) UV-Visible UV-2600 spectrophotometer equipped with an integrated sphere (ISR-2600 Plus). All diffuse reflectance spectra were corrected for background using a BaSO4 standard in the regarded spectral range (200–1200 nm).
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7

UV-vis and Photoluminescence Characterization

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Steady-state absorbance and reflectance data were acquired using a UV-vis spectrophotometer (Shimadzu UV-2600) equipped with a two-detector integrating sphere module (Shimadzu ISR-2600Plus). Photoluminescence spectra were acquired using a modular spectrofluorometer (Horiba Fluorolog-3).
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8

Characterization of Au-CdS Nanocomposites

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The loading amounts
of Au and CdS were quantified by inductively coupled plasma spectroscopy
(ICPS-7500, Shimadzu). X-ray diffraction (XRD) analysis was carried
out with a Rigaku SmartLab X-ray diffractometer. Diffuse reflectance
UV–vis spectra of the samples were recorded on a UV-2600 spectrometer
(Shimadzu) with an integrating sphere unit (Shimadzu, ISR-2600Plus)
at room temperature. BaSO4 was used as a reference material
to evaluate the reflectance (R) of the samples. The reflectance was transformed to the Kubelka–Munk
function [F(R)] presenting the relative absorption coefficient by the equation F(R) = (1 – R)2/2R.43 (link) Transmission electron
microscopy (TEM) measurements were performed using a JEOL JEM-2100F
at an applied voltage of 200 kV. X-ray photoelectron (XP) spectroscopy
measurements were performed using a Kratos Axis Nova X-ray photoelectron
spectrometer with a monochromated Al Kα X-ray source (hν = 1486.6 eV) operated at 15 kV and 10 mA. The takeoff
angle was 90°, and multiplex spectra were obtained for Cd 3d
and Au 4f photopeaks.
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9

Optical Properties of AuNPs-HAp Suspensions

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The optical properties of the AuNPs-HAp suspensions were analyzed based on absorption spectra measured on a UV-Vis-NIR spectrophotometer (Shimadzu UV-3600i; Kyoto, Japan) with a double beam, in the range between 185 and 750 nm with a spectral resolution of 1 nm. For every dispersion, the adsorption was measured at least 3 times.
The optical properties of the textile samples were analyzed based on the total reflectance spectra measured on a UV-Vis-NIR spectrophotometer (Shimadzu UV-2600i; Kyoto, Japan) coupled with an integration sphere (Shimadzu ISR-2600Plus; Kyoto, Japan) in the range between 220 and 1400 nm, with a spectral resolution of 5 nm. The color difference (ΔE) was determined by the Shimadzu Colour Analysis complementary software - LabSolutions UV-vis version 1.12, using as a reference the respective textile treated under the same conditions, but without the AuNPs-HAp. For every sample, the reflectance was measured at least 3 times, in different spots of the sample.
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10

Spectrophotometric Analysis of Wire Coating

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The color of non-coated and BG-coated wire specimens was measured using a spectrophotometer (UV-2600, Shimadzu, Kyoto, Japan) with an integrated sphere (ISR-2600 Plus, Shimadzu). Diffuse reflectance measurements were performed in the range of 350-800 nm in 1-nm steps. Color was measured according to the Commission International de L'Eclairage (CIE) L * a * b * color system (n=5) 26) , which comprises a lightness scale, L * , and two opponent color axes, a * and b * . Redness and greenness are represented by the a * values, and yellowness and blueness are represented by the b * values.
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