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X ray diffractometer with cu kα radiation

Manufactured by Rigaku
Sourced in Japan

The X-ray diffractometer with Cu Kα radiation is a laboratory instrument used for the analysis of crystalline materials. It utilizes X-rays generated from a copper source to probe the atomic structure of samples, providing information about their crystal structure, chemical composition, and other physical properties.

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2 protocols using x ray diffractometer with cu kα radiation

1

Comprehensive Material Characterization Protocol

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The surface morphologies of the samples were characterized by scanning electron microscopy (SEM) (Carl Zeiss AG., Germany). The Brunauer–Emmett–Teller (BET) surface area and the total pore volume were measured from N2 isotherms using a surface area and porosimetry analyzer (Quantachrome Instruments, USA). Surface chemical composition of the samples was confirmed by X-ray photoelectron spectroscopy (XPS) (Thermo Fisher Scientific, USA). The Fourier transform infrared spectroscopy (FTIR) of the samples was measured on a spectrophotometer (Thermo Fisher Scientific, USA) using KBr pellets in the range of 400–4000 cm−1. The X-ray diffraction (XRD) patterns of the samples were examined by an X-ray diffractometer with Cu Kα radiation (Rigaku Corporation, Japan). The zeta potential was measured at a range of 1–5 using a zeta potential analyzer (Malvern Instruments Ltd., United Kingdom). The magnetization measurement of E-CMBC was performed using a vibrating sample magnetometer (VSM) (Lake Shore Cryotronics, Inc. USA).
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2

Physicochemical Characterization of MOF-based NPs

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The polydispersity index (PDI) and zeta potential of MOF@GSK-J1 and HA@MOF@GSK-J1 NPs were determined using a Zetasizer Nano ZS90 instrument (Malvern Instruments, Malvern, United Kingdom) at 25°C. The morphologies of MOF@GSK-J1 and HA@MOF@GSK-J1 NPs were imaged via transmission electron microscopy (TEM, Talos F200C, FEI, United States) with an acceleration voltage of 200 kV. The phase and crystal structures of MOF and MOF@HA NPs without GSK-J1 were examined by X-ray diffraction (XRD) patterns using a Rigaku X-ray diffractometer with Cu-Kα radiation (Rigaku, Japan). The FTIR spectra were recorded by Fourier transform-infrared spectroscopy (Perkin Elmer, United States).
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