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Topas 4

Manufactured by Bruker
Sourced in Germany, United States

TOPAS 4.2 is a software application developed by Bruker for the analysis of powder diffraction data. It provides advanced capabilities for structure determination, Rietveld refinement, and quantitative phase analysis. The software offers a user-friendly interface and a wide range of features to support researchers in the field of materials science and structural characterization.

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20 protocols using topas 4

1

Structural Characterization of Synthetic Materials

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Powder X-ray diffraction (XRD) patterns of the as-synthesized and heated samples were recorded on a D8 Advance powder diffractometer (Bruker, Karlsruhe, Germany) with Bragg–Brentano geometry using CuKα radiation in the range 2θ = 10°–70° using a step size of 0.02° and an accumulated time per step of 35 s. Phase identification was carried out using the PDF-4 database (ICDD, Release 2011). The unit cell parameters, crystallite size, and phase concentrations were determined using the Rietveld method [36 (link)] using Topas 4.2 software (Bruker, Karlsruhe, Germany). The fundamental parameter approach was used to account for the instrumental contribution.
Fourier transform infrared (FTIR) spectra of the powders were recorded on an Infralum FT-801 spectrometer (Simex, Novosibirsk, Russia) in the wavelength range 550–4000 cm−1. Pellets made up of a 4 mg sample and 540 mg of KBr were used for the FTIR study.
Simultaneous thermal analysis (STA) experiments were carried out using an STA 449 F1 Jupiter device (Netzsch, Selb, Germany) equipped with a QMS 403C Aeolos mass spectrometer. The measurements were performed under an argon–oxygen mixture (80:20) at a heating rate of 10 °C/min. The analyzed sample with a mass of 30 mg was placed in a corundum crucible.
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2

WAXD Analysis of Polyimide Membranes

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Wide angle X-ray diffraction (WAXD) analysis of initial polyimides and MMMs were obtained at room temperature using a D8 DISCOVER diffractometer (Bruker, Rheinstetten, Germany) at scattering angles varying from 5° to 60° with 0.05° step. Cu-Kα radiation (40 kV, 40 mA) was used. The volume fraction of crystalline regions (χ, %) was calculated according to the equation:
χ=0Icr(q)dq0[Icr(q)+Iam(q)]dq,
where Icr and Iam are intensities that arise from diffraction on the crystalline and amorphous regions, and q is the length of the scattering vector. Deconvolution of WAXD curves was performed before calculation of degree of polymer crystallinity in order to exclude additional crystallinity arising from ZrO2 nanostars.
The identification of crystalline phase in the ZrO2 was performed by comparing our data with the Joint Committee for Powder Diffraction Standards (JCPDS) files. The Bruker Topas 4.2 software was used for calculation of lattice parameters from WAXD data.
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3

Quantifying Crystalline Silica in Engineered and Natural Stones

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The forms of crystalline silica in the engineered and the natural stones were determined by an X-ray Diffraction (XRD) technique conducted using a Bruker D8 Advance Powder X-ray Diffractometer (Bruker AXS Inc., Madison, Wisconsin, USA) with a Cu-radiation source operating at 40 kV and 40A, scanning 2 theta from 278 to 338 K with sample rotation of 30 rotations/min.
The respirable dust sample was transferred from the filter onto silicon wafers in a fine dusting over the centre of the wafer. Data was processed using Bruker DIFFRAC.EVA software and Crystallography Open Database reference patterns for identifying mineral phases. Quantification was calculated using TOPAS 4.2 software (Bruker AXS Inc., Madison, Wisconsin, USA).
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4

X-ray Diffraction and Stable Isotope Analysis of Carbonate Samples

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Carbonate samples were powdered and homogenized. Mineralogical analyses were performed by X-ray diffraction on un-oriented samples scanned by a Bruker D8 Advance diffractometer (Cu Kα radiation in 3–75° 2θ range). Quantitative data were obtained with the Rietveld algorithm-based code, Topas-4, provided by Bruker. Following a displacement correction of the spectrum made on the main quartz peak, the d104 displacement of calcite was used to estimate the MgCO3 in mol% (ref. 38 ).
An aliquot of the powder prepared for X-ray diffraction was used for stable carbon and oxygen isotopic measurements using a GasBench II preparation line connected to a Thermo Scientific Delta V Advantage IRMS (Thermo Fisher Scientific). Carbon dioxide was produced by the reaction of the powdered sample with 103–105% concentrated phosphoric acid at 70 °C over 2 h. Reproducibility is better than ±0.15‰ for δ13C values. Stable isotopic compositions are reported in conventional delta (δ) units relative to Vienna Pee Dee Belemnite reference. Values are reported in Supplementary Table 1.
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5

X-ray Diffraction Characterization of Powders

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X-ray diffraction (XRD) spectra were acquired using a Bruker AXS D8 Advance X-ray powder diffractometer using Cu Kα radiation. The X-ray source was operated at 40 kV voltage and 30 mA current. Each point in the spectrum was acquired for 1 s. Crystal sizes were determined by fitting the main diffraction peak (~28°) with the Topas 4 (Bruker) software and using the Scherrer equation.
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6

Structural Analysis of Nanoparticles

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The X-ray diffraction pattern was measured from
2θ 15–70° with a Bruker AXS D8 Advance (Bruker,
Karlsruhe, Germany). The analysis of the diffraction spectrum was
done with the instrument software (Topas 4 software, Bruker, Karlsruhe,
Germany) using a Rietveld method to determine the nanoparticle phase
and crystalline size.
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7

Characterization of Nanorods via FESEM, HRTEM, and XRD

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Morphological observation of the nanorods was carried out using field emission scanning electron microscopy (FESEM, H-800, Hitachi Co.) with energy dispersive X-ray spectrometry (EDS), and using high resolution transmission electron microscopy (HRTEM, H-9500, Hitachi-Hitech Co.). The phases after sPFE were identified by X-ray diffraction (XRD, D2 PHASER, Bruker Co.) and Rietveld analysis using TOPAS 4 software (Bruker Co.).
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8

Rietveld Refinement of Bi2Te3

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PXRD patterns were collected with a Bruker D8 Advance diffractometer with Cu Kα radiation (λ: 1.5418 Å, 40 kV, 40 mA) using a Si single crystal as sample holder to minimize scattering. The powder samples were re‐dispersed in EtOH on the Si surface and investigated in a 2θ range from 10 to 90° with a step size of 0.01° 2θ (counting time 0.6 s). Rietveld refinement was done with the program package TOPAS 4.2 (Bruker) to determine lattice parameters and average crystallite sizes by using the Scherrer equation.[68] The background was modelled using Chebyshev polynomials. The structure model of Bi2Te3 (PDF 15–863) from the ICSD database was used. For each Rietveld refinement, the instrumental correction determined using a standard powder sample LaB6 from NIST (National Institute of Standards and Technology) as reference material (SRM 660b; a(LaB6)=4.15689 Å) was considered.
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9

X-Ray Diffraction Analysis Protocol

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X-ray diffraction patterns were recorded using a Bruker D8 diffractometer with Bragg–Brentano geometry equipped with an X-ray tube with Cu anode, and a Ni filter for the removal of the Kβ radiation. A VANTEC detector and a fixed divergence slit (0.3°) were used. The measurements were performed with a step size of 0.015° with a collection time of 1 s at 30 kV and 40 mA over the 2θ angular range between 10° and 120°. The phase quantifications are performed by Rietveld analysis using the program TOPAS 4.2 (Bruker AXS, Karlsruhe, Germany).33 (link) The instrumental intensity distribution for the X-ray data is determined empirically from a fundamental parameters set, using a reference scan of LaB6 (NIST 660a). The quality of the different refinement models discussed within the article are judged based on the quality of the overall fit, expressed by the parameter Rwp.34 (link)
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10

Microstructural Characterization of Tensile Specimens

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For the microstructural characterization, longitudinal cross-sections of the used tensile specimens were prepared by wire cutting. Prior to SEM (Vega II XLH, TESCAN, Brno, Czech), the specimen w etched with 3% alc. HNO3 and sputtered with gold. Hardness curves along the longitudinal axis were determined with the HV1 measurement method.
The EBSD samples were mechanically polished, using a 1-µm diamond lubricant for 10 min and finely polished with OP-S suspension and distilled water for 30 min. Measurements were conducted on a Helios G4 FEG-SEM (Thermo Fisher Scientific, Waltham, MA, USA) equipped with an EBSD Hikari Plus camera (Ametek EDAX, Berwyn, PA, USA). An acceleration voltage of 20 kV, a beam current of 6.4 nA and a step size of 0.03 µm were used to separate austenite and ferrite (martensite) of the fine grain structure in a small area of 20 × 20 µm2.
For X-Ray diffraction measurements, the samples were etched at about 100 µm with 80% phosphoric and 20% sulfuric acid. Measurements were carried out on an ETA 3003 diffractometer (XRD Eigenmann GmbH, Schnaittach-Hormersdorf, Germany) using Cr-k(alpha) radiation and a 0.5 mm primary X-ray beam. The phase analysis was performed over a range from 60–164° with a step size of 0.05° and a collecting time of 800 s and evaluated using the Rietveld method implemented in TOPAS 4.2 (Bruker-AXS, Billerica, MA, USA).
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