The largest database of trusted experimental protocols

67 protocols using diffractometer

1

X-Ray Powder Diffraction Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols

Example 10

X-ray powder diffraction patterns of FIGS. 1 and 4 were obtained with a Rigaku diffractometer using Cu Kα (30.0 kV, 15.0 mA) radiation. The analysis was performed with the goniometer running in continuous-scan mode of 3° per min with a step size of 0.03° over a range of 2 to 400. Samples were prepared on quartz specimen holders as a thin layer of powdered material. The instrument was calibrated with a silicon standard.

+ Open protocol
+ Expand
2

Structural Characterization of TiO2 Nanocrystals

Check if the same lab product or an alternative is used in the 5 most similar protocols
Transmission electron microscope (TEM) images and selected area electron diffraction (SAED) patterns of the TiO2 nanocrystals were obtained using a JEOL 2010F transmission electron microscope operated at 200 kV. Raman spectra were collected using a Raman spectrometer (LabRAM HR spectrometer, Horiba) with a 532.05-nm Ar-ion laser. XRD patterns were recorded over the range 20–80° on a Rigaku diffractometer equipped with a Cu Kα radiation source operated at 40 kV and 120 mA.
+ Open protocol
+ Expand
3

Characterization of Nanostructure Materials

Check if the same lab product or an alternative is used in the 5 most similar protocols
A Hitachi S-7400 system was used for the FE-SEM study; it was operated at 15 kV and at a 13° tilt-view. A JEOL JEM-ARM-200F system operated at 200 KV was used in the HR-TEM study. Samples of the NW structures were prepared by coating with Platinum using a dual-beam focused ion beam (FIB, Quanta 3D FEG) technique with a beam current of 65 nA and a resolution of 7 nm at 30 KV. Single-crystal X-ray diffraction (XRD) measurements were performed using a Rigaku diffractometer equipped with a Cu-Kα radiation source. PL spectroscopy was carried out using a 325 nm line of a He-Cd laser as an excitation source at room temerature. CL measurements were taken at the applied accelerating voltage (Va) and beam current (Ib) 10 KV and 1000 pA, respectively. For measuring photocurrent of the fabricated devices, we utilized a solar simulator (McScience Lab 100) as a light source. This light source generated white light with a maximum power density of 100 mW/cm2. A monochromator (Oriel Cornerstone 130) was used to provide the monochromatic light incident on the channel.
+ Open protocol
+ Expand
4

Powder X-ray Diffraction Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
Powder X-ray diffraction (PXRD) data were collected on a Rigaku diffractometer using Cu Ka radiation (λ = 1.5418 Å). The sealed samples were scanned for every 0.01° increment over the Bragg angle range of 10 − 80°.
+ Open protocol
+ Expand
5

Characterization of Functionalized Halloysite Nanotubes

Check if the same lab product or an alternative is used in the 5 most similar protocols
The IR spectra of the produced materials were captured using a Bruker Tensor II FTIR spectrometer, ranging from 400 to 4000 cm−1, to identify the functional groups within the f-HNTs. To ascertain the crystallinity and phase of both pure and f-HNTs, X-ray diffraction patterns were carefully analyzed using a Rigaku diffractometer, which operated with an incident wavelength of Cu Kα (λ = 1.542 Å). To assess the morphology and microstructures of both unmodified and f-HNTs, scanning electron microscopy (SEM, MIRA3 TESCAN) was employed at an operating voltage of 10 kV. In addition, energy-dispersive X-ray spectroscopy (EDX), integrated with SEM, was utilized for the elemental analysis of the nanomaterials. Furthermore, a Shimadzu AA 670 flame atomic absorption spectrophotometer was used specifically to measure the chromium(vi) ions.
+ Open protocol
+ Expand
6

Comprehensive Characterization of Samples

Check if the same lab product or an alternative is used in the 5 most similar protocols
The crystal structures of the samples were analyzed by a Rigaku diffractometer using Cu Kα radiations, and the X-ray tube was operated at 40 kV and 40 mA. The Fourier Transform-IR (FT-IR) spectroscopy measurements were performed on a Nicolet 6700 spectrometer using the KBr pellet support. The scanning electron microscope (SEM) image was obtained on a JSM-6610 system. The transmission electron microscope (TEM), high-resolution transmission electron microscope (HRTEM), and the selected area electron diffraction (SAED) images were taken at a JEM2100 electron microscope. X-ray photoelectron spectroscopy (XPS) and valence band X-ray photoelectron spectroscopy (VBXPS) were performed using a PHI 5000 Versa Probe X-ray photoelectron spectrometer with monochromatized Al Kα X-ray radiation. The binding energies of all elements were calibrated by the C 1s peak at 284.6 eV. UV-vis diffuse reflection spectroscopy (DRS) was carried out on a Shimadzu UV-2600 spectrometer, and BaSO4 was used as the reference at room temperature. The photoluminescence (PL) spectra of the samples were collected by an Agilent MY15170004 spectrometer with an excitation wavelength of 350 nm. Electron spin resonance (ESR) spectra were obtained from a Bruker model EMXplus spectrometer.
+ Open protocol
+ Expand
7

Characterization of Luliconazole Formulations

Check if the same lab product or an alternative is used in the 5 most similar protocols
The XRD analysis of pure luliconazole, polymer, and the physical mixture was performed at room temperature, and the patterns were obtained by using a Rigaku diffractometer. The patterns of diffraction were obtained by Ni-filtered Cu Kα radiation, where λ = 1.498° A, under 20 mA current, and 40 kV voltage operation [18 (link)]. The samples were screened across the 10° to 90° 2θ range, with experimental parameters set as a scan step size of 0.02° for 2 s with a scan speed of 0.01°/S.
+ Open protocol
+ Expand
8

Powder X-ray Diffraction Analysis of Amorphous Solid Dispersions

Check if the same lab product or an alternative is used in the 5 most similar protocols
Powder X-ray diffraction analyses for the pure drug and prepared ASDs were performed at room temperature, and the patterns were obtained using a Rigaku diffractometer. The diffraction patterns were obtained via Ni-filtered CuKa radiation (λ = 1.5418 Å), under a 20 mA, 40 kV voltage operation. The samples were screened in the 10- to 90-degree 2θ range, with the experimental parameters set to a scan step size of 0.020 for 2 s, with a scan speed of 0.010/s [46 (link)].
+ Open protocol
+ Expand
9

Structural Analysis of Silver Nanoparticles

Check if the same lab product or an alternative is used in the 5 most similar protocols
The physical and chemical nature of AgNPs were elucidated by XRD (X‐ray diffraction) analysis using the Rigaku diffractometer. The samples were analysed by powder diffraction using finely ground powder of AgNPs.
+ Open protocol
+ Expand
10

Powder X-Ray Diffraction Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
The PXRD analysis was performed on a Rigaku diffractometer with Cu Kα (λ = 1.5406 Å)radiation and operated at 40 kV and 40 mA with a scanning step of ≈5 min−1.
+ Open protocol
+ Expand

About PubCompare

Our mission is to provide scientists with the largest repository of trustworthy protocols and intelligent analytical tools, thereby offering them extensive information to design robust protocols aimed at minimizing the risk of failures.

We believe that the most crucial aspect is to grant scientists access to a wide range of reliable sources and new useful tools that surpass human capabilities.

However, we trust in allowing scientists to determine how to construct their own protocols based on this information, as they are the experts in their field.

Ready to get started?

Sign up for free.
Registration takes 20 seconds.
Available from any computer
No download required

Sign up now

Revolutionizing how scientists
search and build protocols!