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8 protocols using x pert pro diffractometer

1

Nanoparticle Characterization Using Advanced Techniques

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Powder diffraction data were
obtained using a PANalytical X’Pert Pro diffractometer equipped
with an Anton Paar TCU 1000 N temperature control unit using Ni-filtered
Cu Kα radiation (V = 40 kV, I = 30 mA). Transmission electron microscopy (TEM) images were performed
with a Philips CM-20 SuperTwin transmission electron microscope operating
at 160 kV. A drop of the suspension was put on a copper microscope
grid covered with carbon. Before the measurement, the sample was dried
and purified in an H2/O2 plasma cleaner for
1 min. The hydrodynamic size of nanoparticles was determined by dynamic
light scattering (DLS) using Malvern ZetaSizer at room temperature
in a quartz cuvette using hexane as a dispersant. Measurements were
made using histograms representing the number of particles per their
average size. The emission spectra and luminescence decay profiles
were measured using an FLS1000 fluorescence spectrometer from Edinburgh
Instruments equipped with a 450 W Xenon lamp and 808 nm line laser
as excitation sources and an R928P side window photomultiplier tube
from Hamamatsu as a detector. The temperature of the sample was controlled
using a THMS 600 heating–cooling stage from Linkam.
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2

Structural and Optical Characterization

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Powder diffraction studies were carried out on PANalytical X’Pert Pro diffractometer equipped with an Anton Paar TCU 1000 N Temperature Control Unit and using Ni-filtered Cu radiation (V = 40 kV, I = 30 mA).
Transmission electron microscope images were obtained using a TEM Philips CM-20 SuperTwin operating at 160 kV with an optical resolution of 0.25 nm.
The emission spectra were measured using the 266 nm excitation line from a laser diode (LD) and a Silver-Nova Super Range TEC Spectrometer form Stellarnet (1 nm spectral resolution). The temperature of the sample was controlled using a heating stage from Linkam (0.1 °C temperature stability and 0.1 °C set point resolution).
Luminescence decay profiles were recorded using FLS980 Fluorescence Spectrometer from Edinburgh Instruments with μFlash lamp as an excitation source and the signal was detected using a R928P side window photomultiplier tube from Hamamatsu.
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3

Characterization of Nanomaterials by XRD, TEM, and Emission Spectroscopy

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Powder diffraction studies were carried out on PANalytical X'Pert Pro diffractometer equipped with Anton Paar TCU 1000 N Temperature Control Unit using Ni-filtered Cu Kα radiation (V = 40 kV, I = 30 mA).
Transmission electron microscopy images were obtained using the Tecnai G2 20 S/TEM Microscope from FEI Company. The microscope was equipped with a thermionic LaB6 emitter and EDS detector for elemental analysis. The study was conducted in the TEM mode at maximum voltage of 200 kV. Micrographs were taken at various magnifications, including high resolution images with lattice fringes.
The emission spectra were measured using the 266 nm excitation line from a laser diode (LD) and a Silver-Nova Super Range TEC Spectrometer form Stellarnet (1 nm spectral resolution) as a detector.
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4

In situ Heating Powder XRD of Cs3LiCl4 · 4H2O

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Cs3LiCl4 · 4H2O was studied in an in situ heating powder XRD experiment in the range between 300 and 670 K. A PANalytical X’Pert Pro diffractometer equipped with an Anton Paar HTK-1200N furnace was used in Bragg-Brentano geometry in θ/2θ mode with Cu-Kα1,2 radiation, and an X’Celerator multi-strip detector. Diffraction patterns were collected every 10 K with a scan step width of 0.0167 °2θ and 90.17 s of total counting time per step. The used ramp rate between set points was 10 K/min with 10 min dwell time at the set points before starting the measurement. The total data collection per scan was approx. 0.5 h.
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5

Characterization of Luminescent Materials

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Powder diffraction studies were carried out using a PANalytical X'Pert Pro diffractometer equipped with an Anton Paar TCU 1000 N temperature control unit using Ni-filtered Cu Kα radiation (V = 40 kV, I = 30 mA). Transmission electron microscopy images were obtained using an FEI Tecnai G2 20 X-TWIN microscope equipped with a CCD FEI Eagle 2K camera with a HAADF detector and electron gun with a LaB6 cathode. The pattern present on the left side of the TEM images is a microscope artifact.
An FLS1000 spectrometer from Edinburgh Instruments equipped with a R928P side window photomultiplier tube and a Hamamatsu detector was used to carry out measurements of photoluminescence decay curves and excitation spectra utilizing a micro-flash lamp and a halogen lamp, respectively. The emission spectra were measured using a Silver-Nova Super Range TEC spectrometer from Stellarnet of 1 nm spectral resolution and 808 nm excitation lines from a laser diode. The excitation pulse duration was modulated using a simple electronic PWM system. The temperature dependencies of both emission spectra and luminescence decay profiles were measured using a THMS 600 heating–cooling stage from Linkam (0.1 °C temperature stability and 0.1 °C set point resolution) to control the temperature.
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6

X-ray Diffraction Analysis of Powders

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Powder
X-ray diffraction patterns were recorded using a Bruker D8 Twin diffractometer
(Billerica, Massachusetts) with Cu Kα radiation λ = 1.54
Å at room temperature scanning between 2θ = 0 and 50°.
Variable-temperature powder X-ray diffraction data were collected
using a Panalytical X’Pert Pro diffractometer (Cu Kα1,2, λ1 = 1.540598 Å, λ2 = 1.544426 Å) using a Bragg–Brentano geometry, equipped
with an Anton Paar XRK 900 high-temperature chamber.
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7

Thermal Analysis of Material Decomposition

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Simultaneous thermal analysis (STA) measurements in the temperature range 30–900°C were performed with a ∼50 mg sample in a corundum crucible on a NETZSCH STA 449 C Jupiter system coupled with a Aeolos quadrupole mass analyzer. The quartz capillary was kept at 250°C. The measured mass signals were 2 (H2), 12 (C), 14 (N), 15 (CH3), 16 (CH4, O), 17 (OH), 18 (H2O), 28 (N2, CO), 32 (O2) and 44 (CO2). All measurements were performed under a flowing argon atmosphere (20 ml min−1) and heating rates of 10 K min−1. Base line corrections of the TG curves were carried out by measuring the empty alumina crucible prior to each measurement. Temperature-dependent powder X-ray diffraction measurements (PXRD) were performed on a PANalytical X’Pert PRO diffractometer using a HTK1200 Anton-Paar high-temperature oven chamber mounted on the diffractometer. Prior to the measurement, the sample was finely ground and placed on a glass ceramic (Marcor) sample holder (depth 0.5 mm). The zero point was calibrated with a LaB6 standard and automatically adjusted during the measurements with a PC-controllable alignment stage. The samples were heated under atmospheric conditions at 10 K min−1 to the respective measurement temperature and kept for 5 min before measurement of each step to ensure temperature stability.
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8

Characterization of Nanostructured Materials

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Powder
diffraction studies were carried out
using a PANalytical X’Pert Pro diffractometer equipped with
an Anton Paar TCU 1000 N temperature control unit using Ni-filtered
Cu Ka radiation (V = 40 kV, I =
30 mA). Transmission electron microscopy (TEM) images were obtained
using a FEI Tecnai G2 20 X-TWIN microscope equipped with a CCD FEI
Eagle 2K camera with a high-angle annular dark field (HAADF) detector
and an electron gun with a LaB6 cathode. The FTIR spectra
were measured using a Bruker 66/s FTIR spectrometer. Raman spectra
were measured via a confocal microscope from Renishaw equipped with
a Si CCD camera for detection and 830 nm excitation line. The spectra
were taken in the range of 100–3200 cm–1 at
room temperature under a 100× objective. The spatial resolution
was lower than 1 μm.
The temperature-dependent emission
spectra were measured using 977 nm excitation lines using a OPOLLETE
355 LD OPO and NIRQuest-Ocean-Optics spectrometer. The temperature
of the sample was changed using a THMS 600 heating stage from Linkam
(0.1 °C temperature stability and 0.1 °C set point resolution).
The photoluminescence decay times and excitation spectra were obtained
using a FLS980 fluorescence spectrometer (Edinburgh Instruments) (1800
lines/mm grating blazed at 500 nm).
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