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Jem 2100f tem instrument

Manufactured by JEOL
Sourced in Japan

The JEM-2100F is a Transmission Electron Microscope (TEM) instrument manufactured by JEOL. The JEM-2100F is designed to provide high-resolution imaging and analytical capabilities for a wide range of materials and applications. The instrument features a Field Emission Gun (FEG) electron source, which enables the production of a high-intensity, coherent electron beam. The JEM-2100F can operate at accelerating voltages up to 200 kV, allowing for the examination of a variety of sample types and the acquisition of detailed structural and compositional information.

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5 protocols using jem 2100f tem instrument

1

Physicochemical Characterization of Catalysts

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The XRD patterns of the catalysts were obtained at room temperature on a PANalytical X'Pert Pro X-ray diffractometer at 40 kV and 40 mA over 20° to 80° 2θ range with Cu Kα radiation (λ = 0.15416 nm). N2 adsorption–desorption isotherms for the catalysts were recorded on a Beckman coulter SA 3100 type specific surface area and aperture measurement instrument at −196 °C. The size distribution of micropores was determined using the Horvarth–Kawazoe(H–K) equation. The surface areas of the catalysts were calculated by the Brunauer–Emmett–Teller (BET) method. Transmission Electron Microscopy (TEM) images were recorded on a JEOL JEM-2100F TEM instrument at an accelerating voltage of 200 kV. The morphology of the catalyst was analyzed via scanning electron microscopy (SEM 450, Nova nano, Japan). The elemental chemical states of the samples were analyzed via X-ray photoelectron spectroscopy (XPS) using a Thermo Scientific Escalab 250Xi X-ray spectrometer with binding energy corrected by C 1s (284.8 eV). The basicity of the catalyst was measured by temperature-programmed desorption of CO2 (CO2-TPD) techniques on an AutoChem II 2910 instrument (Micromeritics, USA). The reduction behavior of the catalysts was studied via hydrogen programmed temperature-reduction (H2-TPR) using a Micromeritics AutoChemII 2920 instrument equipped with a thermal conductivity detector (TCD).
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2

Characterization of Bi-Based Electrocatalysts

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The morphologies
of BOC and RB were observed using a Hitachi S-4800 SEM. The TEM observation
was carried out using a JEOL JEM-2100F TEM instrument. The XRD pattern
of BOC was obtained with a Bruker D8 Advance powder X-ray diffractometer
using Cu Kα radiation (wavelength λ = 0.15406 nm). The
valence state of Bi on the surfaces of the electrocatalysts was quantified
by an ESCALAB 250Xi XPS instrument. Ion chromatography (IC) was employed
to quantify the concentration of the formate product in the aqueous
solutions. The IC data was obtained using a Dionex ICS-5000+ ion chromatography instrument.
The FE for producing formate
can be determined by the equation where n is the number
of
moles of the formate product, which can be calculated according to
the IC data, F is Faraday’s constant, with
a value of 96 485 C mol–1, and Q is the total charge passed during electrolysis (here, Q = 10 C).
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3

Comprehensive Structural Analysis of HCs

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The morphology of the as-synthesized
HCs was observed using a VGA-3-SBH scanning electron microscope. The
specific surface area and pore structure of the HCs were characterized
using a Micromeritics ASAP 2020 analyzer. HR-TEM and SAED observations
were performed using a JEOL JEM-2100F TEM instrument. XRD patterns
were recorded using a PANalytical X’Pert instrument equipped
with Cu Kα radiation. Raman spectra were recorded using a Renishaw
Invia spectrometer with an Ar laser of 514.5 nm.
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4

Comprehensive Characterization of Nanomaterials

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The phase structures of the samples were characterized by an X-ray diffractometer (XRD) using a Rigaku D-Max 2200 XRD system with Cu Kα radiation at 40 kV and 26 mA (λ = 1.5405 Å). The high-resolution transmission electron microscopy (HR-TEM) images, elemental mapping, and energy-dispersive X-ray spectroscopy (EDX) data of the samples were recorded on a JEOL JEM 2100F TEM instrument with an acceleration voltage of 200 kV. The morphology and rough elemental composition were analyzed on an FEI Quanta scanning electron microscopy (SEM) instrument equipped with an energy-dispersive spectrometer (EDS). The Raman spectra were characterized by a Horiba Jobin Yvon HR800 Raman spectrometer. The excitation source was a 488 nm laser and the diameter of the laser spot was 1.0 μm. The photoluminescence (PL) emission spectra, photoluminescence excitation (PLE) spectra, and decay curves were measured by an FLS 980-combined time-resolved and steady-state fluorescence spectrometer (Edinburgh Instruments) equipped with Xe/nF/μF lamps. Temperature-dependent PL spectra and dynamics were measured on the same instrument within a temperature range of 77–500 K. The quantum yield (QY) was obtained with a Hamamatsu C9920-03G absolute QY measurement system.
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5

Comprehensive Characterization of Activated Carbon

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X-ray diffraction (XRD) analysis was carried out to study and confirm the structural characteristics of synthesized activated carbon. XRD analysis was carried out by using Shimadzu diffractometer equipment (XRD-6000). With the increased focus on carbonbased materials such as graphene, Raman spectroscopy has emerged as the major analysis technique to study the state of carbon in complex structures. An Enwave Optronics ProRaman-L spectrometer was used to record the Raman spectra presented in this study with a 532 nm laser for excitation. FTIR data were taken from analysis on FT-IR Nicolet 6700 by Thermos Scientific, Oklahama, OK, USA. Analysis of material surfaces by X-ray photoelectron spectroscopy (XPS) was carried out on a K-ALPHA (Thermo Fisher Scientific, Waltham, MA, USA) instrument. Thermal analysis was carried out using an NETZSCH STA 409 C/CD instrument in a helium atmosphere. Scanning electron microscopy images were obtained to study the morphology of prepared samples by Zeiss FESEM Ultra 60 (Oberkochen, Germany). High-resolution transmission electron microscopy (HRTEM) images were acquired at 200 kV using a JEOL model JEM 2100F TEM instrument (Tokyo, Japan).
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