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215 protocols using empyrean diffractometer

1

X-ray Diffraction Analysis Protocol

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X-ray diffraction measurements were carried out with an Empyrean diffractometer (PANalytical, Almelo, The Netherlands) equipped with a X’Celerator X’Pert detector. A Cu anode was used as the X-ray source (K radiation: 40 kV and 40 mA), and a 1/4° divergence slit was used to collect the data in the 2θ range of 10–80°.
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2

Comprehensive Characterization Techniques

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TEM images were acquired using a FEI Tecnai F30 Transmission Electron Microscope, with a field emission gun operated at 200 kV. The XRD pattern was collected using a PANalytical Empyrean diffractometer, with a 1.8 KW copper X-ray tube. XPS was performed using a Physical Electronics 5400 ESCA photoelectron spectrometer. Gas products were analyzed by a gas chromatograph (SRI Multiple Gas Analyzer #5) equipped with molecular sieve 5 A and HayeSep D columns, with Ar as the carrier gas.
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3

Phase Purity Characterization of Transition Metal Thiocyanates

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Phase purity was assessed via powder diffraction measurements on a PANalytical Empyrean Diffractometer using Cu-Kα radiation (λ = 1.541 Å) in Bragg-Brentano geometry. Diffraction patterns were recorded over the range 2θ = 5-80° using a step size of 0.02° and a scan speed of 0.01° s -1 . Due to their sensitivity to moisture and air, the diffraction patterns of Mn(NCS)2 and Fe(NCS)2 were measured by encasing the samples between polyimide (Kapton) films. All diffraction patterns were analysed via Pawley 46 and Rietveld 47, 48 refinements using TOPAS Academic 6 structure refinement software. 49, 50
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4

Flux Growth and Characterization of Mn(Bi,Sb)4Te7

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Single crystals were grown using the flux method (43) . Powder X-ray diffraction was performed via a PANalytical Empyrean diffractometer (Cu Kα radiation) to determine the phase purity. The Sb doping levels of the Mn(Bi 1-x Sb x ) 4 Te 7 crystals refer to the actual concentrations, determined by wavelength dispersive spectroscopy.
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5

Polymer Crystallinity Analysis by WAXD

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The crystallinity of the different copolymers was analyzed by WAXD in an Empyrean Diffractometer (PANalytical, Almelo, Netherlands) using Ni-filtered Cu radiation generated at 40 mA and 40 kV.
The experimental data were collected between 0º and 60º at a scanning rate of 2º/min.
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6

Structural Characterization of (m-PdH2)CuCl4 via Synchrotron X-ray Diffraction

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Preliminary X-ray diffraction data were collected on a PANalytical EMPYREAN diffractometer using Cu K1 ( = 1.5406 Å) radiation in the range of 3 to 70°.
High-resolution synchrotron X-ray powder diffraction (SXRD) data of (m-PdH2)CuCl4 were collected at Beamline I11 Diamond Light Source, UK, using the Cryostream Plus (92 -300 K). The X-ray wavelength was chosen as 1.0008(1) Å. All SXRD data were analyzed by the Rietveld method, using the GSAS/EXPGUI package. 29, 30 Refinement strategies remained consistent at each temperature, with twelve background coefficients, four profile parameters, lattice parameters, atomic positional coordinates and isotropic atomic displacement parameters for all non-H atoms. Symmetry mode analysis, for both single crystal and powder crystallography, was carried out via the on-line tool ISODISTORT. 31
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7

Powder Diffraction Analysis of Seized Material

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The powder diffraction measurements of the seized material were performed using an Empyrean diffractometer (PANalytical, Malvern, UK) employing Cu anode (voltage: -40 kV; current: 25 mA) and 2θ range from 4.96° to 90.03° with the step size of 0.026°.
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8

In-situ XRD Structural Characterization

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The in-situ XRD measurements were carried out on a PANalytical Empyrean diffractometer using Cu-Kα radiation. This technique was used to determine in-situ structural changes during heating and cooling cycles performing in the 25–120 °C range. The diffraction data were acquired using a step size of 0.013° 2θ and the count time of 1 S per step.
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9

X-ray Diffraction of Nanomaterial Powders

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An X-ray diffraction analysis of nanomaterial powders was performed with a Panalytical Empyrean diffractometer (step size 0.02, time per step 1 s) at room temperature. For all analyses made, Cu Ka radiations with l = 1.541874 Å were used. Samples were scanned at a Bragg 2u angle between 10–80.
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10

XRPD and SAXS Analysis of Samples

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X-ray powder diffraction (XRPD) analysis was performed using an Empyrean diffractometer (PANalytical, 2012, Malvern, UK) in reflection–transmission mode. X-ray tubes equipped with Cu anodes were utilized as radiation sources (X-ray wavelength (1.5418 Å)). The PIXcel3D detector was used in linear (1D) scanning mode. The incident beam path consisted of W/Si, and a stepped X-ray mirror with an elliptical shape. Scans were made over a 2θ range of 10–90° with a total exposure time of 2 h. The SAXS measurements were performed by the same device at the SAXS/WAXS sample stage with capillary mode. The device was operated with a generator setting of 40 kV and 40 mA. The incident beam path consisted of W/Si, with a stepped X-ray mirror with an elliptical shape. The SAXS measurements were performed at −0.1–4 degrees 2θ with a step size of 0.005. The primary beam was measured with a Cu 0.2 mm beam attenuator and a PIXcel3D detector. The length of the scattering vector (or scattering vector) q is defined as q = (4πsinθ)/λ, where 2θ is the scattering angle and λ is the X-ray wavelength (1.5418 Å). Background scattering was evaluated by an air scattering measurement using an empty sample holder with foil. The Dv(R) calculations were performed using the indirect Fourier transform technique applied in the EasySAXS software (PANalytical, Malvern, United Kingdom, version 1.2).
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