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Uvisel

Manufactured by Horiba
Sourced in France

The UVISEL is a UV-Vis-NIR spectroscopic ellipsometer designed for thin film analysis. It measures the change in polarization of light upon reflection from a sample's surface, providing information about the sample's optical properties and layer structure.

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9 protocols using uvisel

1

Characterization of HfOx Thin Films

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The thickness of the film deposited on the Si substrate was measured using spectroscopic ellipsometry (UVISEL, Horiba, Kyoto, Japan). XPS (Theta Probe, Thermo Fisher Scientific Co., Waltham, MA, USA) was used to analyze the chemical bonding of the HfOx films and to ascertain the presence or absence of La in the HfOx films. The morphological properties of the deposited films were characterized by AFM (XE-100, Park Systems, Suwon, Korea). Furthermore, the crystalline phase and crystallite size and orientation were determined by GI-XRD (SmartLab, Rigaku, Tokyo, Japan) and TEM (Tecnai F20 G2, FEI, Hillsboro, OR, USA). For the cross-sectional TEM image, a sample was prepared using the focused ion beam system, and for the plan view TEM image, samples were prepared using the ion milling system.
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2

Electrochemical Characterization of SiC and Si Anodes

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The thickness of the films was measured by using ellipsometry (Horiba Uvisel). For electrochemical characterization, the SiC and Si electrodes were assembled into CR2016-type coin cells with Celgard 2400 as separator, 1 M LiPF6 dissolved in ethylene carbonate/dimethyl carbonate (v/v = 1 : 1) as electrolyte, and Li foil as counter electrode. Cyclic voltammetry was recorded at a scanning rate of 0.1 mV s−1 between 0 V and 3 V versus Li/Li+ (CHI 660E). Galvano-static cycling was carried out between 0.01 V and 3.0 V versus Li+/Li (Land CT2001A). To examine the film properties after electrochemical cycling, the anode electrodes were took out from the coin cells after 100 charge/discharge cycles and dried in an Ar ambient. The crystalline structures of the films were investigated by X-ray diffraction (XRD, Bruker D8 Advance). The morphologies of the films were characterized by scanning electron microscopy (SEM, Zeiss Ultra Plus). The elemental compositions of the films were evaluated by energy dispersive X-ray spectrometry (EDX). The chemical states of the films were measured by X-ray photoelectron spectroscopy (XPS, PHI Quantera II) and the XPS penetration depth is about 10 nm. The XPS spectra were calibrated according to ref. 37 (link). During the XPS measurements, the depth profiling was performed by Ar+ sputtering with an etching rate of about 3.5 nm min−1.
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3

Characterization of a-SiNxOy Thin Films

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The chemical compositions and atomic scale defect states were confirmed by the XPS (Thermo ESCALAB 250, ThermoFisher Scientific, Waltham, MA, USA) and the EPR (Bruker EMXplus, X-band, Bruker, Billerica, MA, USA) measurements. The TD-SSPL and PL excited (PLE) properties were measured by a Fluorolo-3 system (HORIBA Jobin Yvon, Paris, France) in a computer-controlled Delta 9023 oven (State College, PA, USA) under various temperatures, using a 75W Xe lamp (λexc = 250‒800 nm) and a He‒Cd laser (λexc = 325 nm) as light sources. The optical band gaps (Eopt) were obtained from transmittance measurements (Shimadzu UV-3600, Shimadzu Corp., Hadano, Kanagawa, Japan). The refractive indexes (n) were measured using a spectroscopic ellipsometer (Jobin Yvon UVISEL, HORIBA Jobin Yvon, Paris, France). Both the Eopt and n of a-SiNxOy samples are listed in Table 1. A FLS980 (Edinburgh Instrument Ltd., Edinburgh, UK) equipped with an EPL375 pulse diode laser (λexc = 375 nm, pulse width ~53 ps, repetition rate ~20 MHz), and a TCSPC (resolution time ~100 ps), were used to record the time-resolved PL.
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4

Optical Properties of PDMS Films

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The light transmittances of PDMS films and #1 glass coverslip were measured with an ultraviolet-visible-near-infrared (UV-Vis-NIR) spectrophotometer (Cary 5000, Varian, Palo Alto, CA, USA) in the wavelength range of 250–1500 nm. Five sets of PDMS sheets were measured. Each set consisted of 11 samples with thicknesses of 0.3 mm, 0.5 mm, 0.75 mm, 1.0 mm, 2.0 mm, 3.5 mm, 4.0 mm, 4.5 mm, 6.0 mm, 7.0 mm and 10.0 mm, respectively. The sheet size was kept constant as 2.0 cm × 2.0 cm. The #1 glass coverslips were commercially purchased (10212432C, LABSEE, Shanghai, China), they were 24 mm × 32 mm in size and 0.16 mm in thickness.
The refractive index of PDMS samples was characterized with a spectroscopic ellipsometer (UVISEL, HORIBA, Chilly-Mazarin, France). PDMS liquid was spin-coated (8000 rpm, 120 s) on a 4-inch silicon substrate to form a thin film with a thickness of 9.0 μm. After being solidified, the film was measured at five different positions for its refractive index in the wavelength range of 300–830 nm, and the average value was taken as the result.
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5

Temperature-Dependent Optical Properties of PCM

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Temperature-dependent ellipsometry measurements
were conducted
on a HORIBA JOBIN YVON UVISEL Spectroscopic Phase Modulated Ellipsometer
on samples of passivated PCM deposited on silicon substrates. All
measurements use an angle of incidence of 70° and produced results
with the default configuration II scheme (M = 0°
or 90°, A = ±45°), which was later
used for fitting. All samples were annealed at 250 °C for 10
min to ensure full crystallization before ellipsometry. We performed
ellipsometry at multiple temperatures between 40 and 180 °C with
20 °C steps using a custom-built heated stage with closed-loop
temperature control. Layer thicknesses of the deposited GST and passivation
layers were acquired through AFM measurements and fitting using known
optical values at room temperature. Temperature-dependent refractive
index data for the silicon substrate was interpolated from Vuye et
al. data points using third degree polynomial splines along the temperature
axis. Refractive indices were fitted to single Tauc-Lorentz dispersion
models at each tested temperature. The dispersions were then used
to extrapolate thermo-optic coefficients by performing first order
polynomial fits along the temperature axis.
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6

Measuring Gold Substrate Permittivity

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The permittivity of the gold substrate was measured by an ellipsometer (HORIBA UVISEL: 200–2000 nm).
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7

Ellipsometric Characterization of PETA-based Polymer

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The measurement was performed on the polymer film deposited on Si substrate by using a home-built rotating polarizer ellipsometer coupled with a FTIR. The optical constants are deduced from the ellipsometric parameters tanΨ and cos Δ assuming a simple system composed of a film deposited on a silicon substrate. The film thickness is first estimated from ellipsometric measurements in the visible spectral range by using a phase modulated ellipsometer (Horiba Jobin Yvon, UVISEL). Then, a wavelength by wavelength inversion42 (link) is used to determine the complex refractive index of the PETA-based polymer.
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8

Spectroscopic Mueller Matrix Analysis

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Two different instruments have been used for the measurement of the Mueller matrix. A home-built Mueller matrix polarimeter that incorporates four photoelastic modulators (4-PEM polarimeter) (53) was used to determine, in transmission mode, the full Mueller matrix of the samples in the spectroscopic range from 250 to 800 nm in steps of 2 nm (Figure 3 and Figures S8,S9, and S10). A phase-modulated ellipsometer (UVISEL, Horiba) that measures the first three columns of the Mueller matrix in the 270 to 800 nm spectral range was also used (Figure 4 and Figures S12 andS13). The light spot had a diameter of 1.5 mm, and measurements were done in the central area of the samples. The obtained measurements were, in good approximation, not depolarizing, and they were analyzed according to eq 2.
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9

Spectroscopic Characterization of Hydrogels

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The transmittance of the hydrated hydrogel samples was determined with a UV-Vis spectrophotometer (Multiskan GO, Thermo Scientific). The wavelength interval of 400 to 700 nm was scanned with 1 nm intervals.
Ellipsometric functions tan Ψ and cos ∆ were measured in the spectral range from 300 -850 nm using a phase modulated spectroscopic ellipsometer (UVISEL, Horiba Jobin-Yvon), at 70 o incidence angle. The thickness and refractive index of the films/hydrogels were determined through suitable modelling using the DeltaPsi2 software package from Jobin-Yvon with a Cauchy dispersion function.
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