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198 protocols using tecnai g2 f20 s twin

1

Comprehensive Characterization of Materials

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The samples were characterized by
means of powder XRD analysis (Rigaku Ultima IV, Japan; Cu Kα
radiation, λ = 1.5418 Å), FESEM (Hitachi SU5000, Japan),
TEM and HRTEM with energy-dispersive X-ray spectroscopy (FEI Tecnai
G2 f20 s-twin, 200 kV), and XPS (Thermo Scientific ESCALAB 250Xi,
Al Kα X-ray monochromator).
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2

Microstructural Analysis of Heat-Treated Steels

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The heat-treated plates were obtained by wire cutting, ground to a roughness of 106 μm, 45 μm, 23 μm and 13 μm, and then polished, followed by soaking in aqueous solution of CuCl2 and hydrochloric acid for 10 s. The original structure of the steels were observed by a digital metallographic microscope (Zeiss 40MAT, Carl Zeiss AG, Oberkochen, Germany), at 50 times of magnification.
A thermal field emission scanning electron microscope (FEI-Quanta650, Thermo Fisher Scientific, Waltham, MA, USA) was used to observe the above samples at a magnification of over 1000 times. The SEM mode was secondary electronic imaging, with the working distance 10–15 mm, the magnification 5000 times, and the acceleration voltage 20 kV.
The microstructure was characterized by transmission electron microscope (TEM, Tecnai G2 F20 S-TWIN, Thermo Fisher Scientific, Hillsboro, OR, USA). The steel block samples were cut to 0.5 mm, then thinned by 13 μm sandpaper to 50 μm, then cut into a circle with a diameter of 3 mm. The Automatic Twin-Jet Electropolisher (MTP-1A, BUEHLER, Lake bluff, IL, USA) was used for double spray, with the current 40 mA, the voltage 20 V, the experimental temperature −20 °C, and the experimental solution 10% perchloric acid. The obtained samples were observed at an operating voltage of 200 kV.
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3

Comprehensive Material Characterization

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The samples were characterized by means of powder XRD analysis (Rigaku Ultima IV, Japan; Cu Kα radiation, λ = 1.5418 Å), Field-emission SEM (Hitachi SU5000, Japan), TEM and HRTEM with EDS (FEI Tecnai G2 f20 s-twin, 200 KV), XPS (Thermo SCIENTIFIC ESCALAB 250Xi, Al Ka X-ray monochromator), BET (Autosorb-IQ, USA).
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4

Visualizing Bacterial Flagella via TEM

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Different samples were examined by transmission electron microscopy (TEM; Tecnai G2 F20 S-TWIN, Thermo Fisher Scientific Inc., Waltham, MA, United States) for the appearance of flagella. Overnight cultures were diluted 1,000 (v:v) times with fresh TSB broth and statically cultured at 37°C for 7 h. The bacterial suspension was spotted onto a copper grid and air-dried. Then, the samples were stained using 3% phosphotungstic acid for 2 min and observed using the TEM.
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5

Physicochemical Characterization of Nanomaterials

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All nanomaterials were purchased from Sigma-Aldrich (MERCK, Darmstadt, Germany). For the preparation of experimental suspensions, sonicated nanomaterials were used without any further modification. Nanomaterials were prepared in the same manner as used in the microbiological studies (description below). The nanomaterials were investigated by transmission electron microscopy (Fei, Tecnai G2 F20 S Twin with energy dispersive X-ray spectroscopy, Thermo Fisher Scientific, Waltham, MA, USA). The crystalline structure and chemical composition of the samples was studied by X-ray diffraction. The XRD measurements were performed with a PRO X-ray diffractometer (X’Pert PRO Philips diffractometer, Co. Ka radiation, Almelo, Holland). The nanomaterials surface area was measured based on the N2 adsorption/desorption isotherms (Quantachrome Instruments, Quadrosorb SI, Boynton Beach, FL, USA). The specific surface area was calculated by the Brunauer-Emmett-Teller (BET) method.
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6

Characterizing CCD/RBD-HR Nanoparticles

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The 1H-NMR spectra of PEI 1.8 kDa, CD-1.8k, linker, and CCD were measured on a Bruker AM400 NMR spectrometer with D2O as the solvent. The surface chemical stages of CCD were explored by electron spectroscopy on an AXIS Supra (Kratos Analytical, UK). The FI-IR spectra of PEI 1.8 kDa, CD-1.8k, and CCD were obtained by an IRTracer-100 (Shimadzu, Japan). CCD was mixed with RBD-HR for 30 min at 25 °C in a certain proportion with ultrapure water as the soluble substance to obtain CCD/RBD-HR nanoparticles. The suspension of the CD-1.8k, CCDs, or CCD/RBD-HR nanoparticles was dropped on a copper grid and then dried in the air, and their morphologies were observed with transmission electron microscopy (TEM, Tecnai G2 F20 S-TWIN, Thermo Fisher, USA). The zeta potentials and average hydrodynamic diameters of RBD-HR, CCD, or CCD/RBD-HR nanoparticles were measured by a Zetasizer analyzer (Malvern Instruments Ltd., UK).
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7

Structural and Optical Characterization of Gr-CdS Nanocomposite

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The crystal structures and phases were analyzed using X-ray diffraction (XRD) (X’Pert PRO-Multipurpose Diffractor, PANalytical, The Netherlands) using Cu Kα radiation (λ = 0.15406 nm). The microstructure was observed by transmission electron microscopy (TEM) (Tecnai G2 F20 S-TWIN, Thermo Fisher Scientific, The Netherlands) at an accelerating voltage of 200 kV. Selected-area electron diffraction (SAED) analysis was also conducted using TEM to determine the interplanar distance and crystalline phase of the Gr–CdS nanocomposite. Raman spectroscopy (XploRA Plus, Horiba, Japan) with 532nm laser source was performed to further confirm the phase and structure. The elemental composition was obtained by energy-dispersive spectrometry (EDS) (S-4200, HITACHI, Japan). X-ray photoelectron spectroscopy (XPS) (K-Alpha, Thermo Fisher Scientific, UK) was employed to investigate the chemical state of the CdS NPs and Gr–CdS nanocomposite. The optical properties were examined by UV–vis–NIR spectroscopy (Cary 5000, Agilent, USA).
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8

Characterization of Laser-Induced Spalling in Metallic Glasses

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Cu50Zr50 MG samples with in-plane dimensions of 2 × 2 mm2 and thickness of approximately 50–100 μm were prepared for laser shock experiments using the single-roller melt spinning method. X-ray diffraction (Empyrean XRD, Malvern Panalytical Ltd) was performed to verify the amorphous state of the samples (Supplementary Fig. 6a and 9a). After laser shock tests, the MG samples were retrieved, and microscopy (Hitachi FE-SEM S4800) was used to characterize the plane where spalling occurred. Then, the void distribution underneath the spall plane was characterized using a focused ion beam (FIB) to mill a rectangular well in the sample (ZEISS Crossbeam 340). HRTEM and selected-area electron diffraction (SAED) characterizations were performed using Tecnai G2 F20 S-TWIN (FEI, US) at an accelerating voltage of 200 kV.
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9

Comprehensive Electrochemical and Spectroscopic Characterization

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All electrochemical measurements were performed on CHI760D electrochemical workstation (Shanghai Chenhua Instrument Co. Ltd., China). EIS was obtained from the impedance measurement unit (IM6e, ZAHNER elektrik, Germany). All electrochemical experiments were carried out in a conventional three-electrode cell with a modified GCE (diameter 4 mm) as the working electrode, a Pt wire electrode as the counter electrode and an Ag/AgCl electrode as the reference electrode. The UV-Vis absorption spectra of water colloid were recorded on Shimadzu UV3600 UV-Vis-NIR spectrophotometer (Lumerical Solutions, Inc.). XRD patterns of the prepared samples were acquired with a Rigaku D/MAX 2200 X-ray diffractometer (Tokyo, Japan) (Bragg equation 2d sin θ = , n = 1, λ = 0.154 nm). Transmission electron microscopy (TEM, JEOL JEM 1200EX working at 100 kV) and high-resolution TEM (HRTEM, FEI Tecnai G2 F20 S-Twin working at 200 kV) were utilized to characterize morphology and interfacial lattice details. Scanning electron microscope (SEM) images were obtained using a field emission SEM (Zeiss, Germany).
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10

Characterization of CdSe/ZnS Quantum Dots

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ZnS-coated CdSe QDs (CdSe/ZnS, Q21321MP) were purchased from Invitrogen Company. This core–shell material is coated with a polymer layer and it is terminated with COOH surface groups. The photoluminescence emission spectra of CdSe/ZnS were measured by a Fluorescence spectrophotometer (Cary Eclipse, Agilent, USA) with an excitation wavelength of 400 nm. UV–Visible-NIR absorption spectra were collected using a UV–Vis-NIR spectrophotometer (Cary 5000, Agilent, USA). The hydrodynamic size distribution of the CdSe/ZnS was obtained by a dynamic light scattering (DLS) machine (Zetasizer Nano ZS, Malvern, UK). The morphology of the CdSe/ZnS quantum dots was obtained with an FEI Tecnai G2 F20 S-TWIN transmission electron microscopy (TEM) operating at an accelerating voltage of 200 kV at room temperature.
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