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14 protocols using pips 691

1

Characterization of Surface Hardness

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Surface hardness was characterized by Vickers-hardness and Nano-indentation hardness. The Vickers-hardness measurements were measured using a micro-hardness instrument (MVS 1000D1, Guangjing, Guangzhou, China) with a load of 0.98 N, dwell time of 15 s; The Nano-indentation measurements were carried out using a Nano-indentation instrument (G200, Keysight, Santa Rosa, CA, USA) with diamond Berkovich indenter, which selected the dynamic nano-indentation model with the maximum indentation depth of 2500 nm. Three measured data for each specimen were averaged to reduce errors caused by different positions. To reveal the microstructure, samples were etched with a 50 mL H2O, 25 mL HNO3 and 5 mL HF solution. The cross-sectional microstructure was observed by optical microscope (DMI 5000 M, LEICA, Weitzlal, Germany) and transmission electron microscope (TECNAI G2 S-TWIN F20, FEI, Hillsboro, OR, USA). Thin TEM foils were prepared via an ion-miller (PIPS-691, Gatan, Pleasanton, CA, USA) with a beam voltage of 3.5 kV and a milling angle of 4–8°. TEM images and the corresponding selected area electron diffraction (SAED) were obtained by TEM with an accelerating voltage of 200 kV.
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2

Atomic-scale Imaging of Perovskite Structures

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TEM and scanning transmission electron microscopy (STEM) specimens were prepared by mechanically polishing to approximately 20 μm, followed by argon-ion milling in a Gatan PIPS691. TEM and STEM studies were conducted using FEI Titan Cubed Thermis G2300, equipped with double spherical aberration (Cs) correctors. The atomic-scale high-angle annular dark-field (HAADF) images were recorded with a probe size in 9 mode, convergence semi-angle of 25.6 mrad, and collection semi-angle of 67–200 mrad. The A-site and B-site cation positions were determined simultaneously with picometer precision using the two-dimensional Gaussian fitting method. The relative displacement between a B-site cation and its four nearest neighboring A-site cations was calculated and the polarization vectors were extracted. The whole process was automatically completed using APPSA software.
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3

Characterization of Cryorolled Samples

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The microstructure of the cryorolled and annealed specimens were characterized using a transmission electron microscope (JEM-2100, JEOL) at an accelerating voltage of 200 kV. Thin slices were cut from the bulk sample and were mechanically polished. Finally, the specimens were dimpled followed by Ar-ion milling (PIPS-691, Gatan) with liquid N2 cooling facility for electron transparency.
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4

Microstructural Analysis of Al 7075 Alloy

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The composition of Al 7075 alloy was analyzed using an Inductively Coupled Plasma-Optical Emission Spectr (Prodigy 7). The median particles diameters were measured using a Malvern laser particle size analyzer (Mastersizer 2000). Samples for TEM studies were prepared by mechanically grinding the bulk material to a thickness of ~80 µm, then dimpling in the center to a thickness of approximately 15 µm. Further thinning to a thickness of electron transparency was carried out using an Ion Milling (Gatan PIPS 691) system at liquid nitrogen temperatures. The microstructure of the samples was characterized by transmission electron microscopy (JEOL2800, JEOL2500 and FEI CM20).
The number density of GP zones per unit area was estimated by counting the numbers of GP zones in at least ten STEM photographs of each zone using an image analysis tool, Image J®. The area for each photograph is approximately 160 nm × 160 nm.
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5

Structural and Transport Characterization

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The microstructural characterization has been conducted using TEM (FEI Tecnai G2 F20) as well as aberration-corrected STEM (FEI Titan G2 80–200), both operated at 200 kV. STEM HAADF images were taken using an annular detector with a collection range of 60–160 mrad. Cross-sectional samples for TEM characterization were prepared by a standard grinding and thinning and a final ion-milling (Gatan PIPS 691 precision ion polishing system). The X-ray diffraction was carried out with a Panalytical Empyrean high-resolution X-ray diffractometer using Cu- radiation (λ=1.5405 Å). To measure transport characteristics with temperature variation from 20 to 550 °C, we used a probe station equipped with a hot plate. The ac and dc measurements were performed by an HP 4294A Precision Impedance Analyser and Keithley 2,440 sourcemeter, respectively. For all transport measurements, we grounded the Nb:STO substrate and applied the voltage to the Pt electrodes.
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6

Microstructural Analysis of Ceramic Pellets

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Microstructure
analyses were performed on thermally etched (1150 °C in air for
15 min) cross sections using a scanning electron microscope (SEM;
Thermo Fisher Quanta 650 ESEM, Massachusetts, USA) with a thermionic
electron source.
Samples for scanning transmission electron
microscopy (STEM) were prepared by cutting a 3 mm disk from the ceramic
pellet, mechanical thinning to ∼100 μm, dimpling to ∼20
μm in the disc center (Dimple grinder, Gatan Inc., Warrendale),
and finally, ion milling to perforation using 3.8 keV Ar ions at an
angle of 8° from both sides (PIPS 691, Gatan Inc., Pleasanton,
USA). After perforation, the energy was gradually lowered, finally
to 500 eV for 5 min to minimize the thickness of the amorphous surface
layer. STEM analyses were performed using a probe-corrected atomic-resolution
microscope (JEOL ARM200 CF, Jeol Ltd., Tokyo, Japan) operated at 200
kV and equipped with a high-angle annular dark-field (HAADF) detector
with inner and outer semiangles of 68 and 180 mrad, respectively.
EELS spectra were acquired using a Gatan DualEELS Quantum ER spectrometer.
Samples for STEM analyses were coated with 2 nm of amorphous carbon
(PECS 682, Gatan Inc., Pleasanton, USA) to prevent charging under
the electron beam.
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7

Characterizing Nanoparticle Distribution in Metals

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The microstructure, distribution, and dispersion of nanoparticles in metals were studied by SEM, FIB imaging, EBSD, and TEM. To clean the surface and reveal the nanoparticles in the metal matrix, the mechanically grinded and polished as-cast samples were further polished by low-angle ion milling (model PIPS 691, Gatan). SEM images were acquired at 0° and 52° with Zeiss Supra 40VP and FEI Nova 600, respectively. The composition of the material was characterized by energy-dispersive x-ray spectroscopy. The volume fraction of nanoparticles was estimated on the basis of the atomic fraction of the major element in the base metal and nanoparticles. Taking advantage of the channeling contrast of different grains induced from the ion beam, FIB imaging was used to reveal the grain structure. Grain size and orientation were studied with EBSD (FEI Quanta 3D) at 30 kV with a current of 12 nA and FIB with a CDEM (channel detection electron multiplier) detector. The interfaces between the matrix and the nanoparticles were studied with an FEI Titan TEM at 300 kV. The thin-film TEM samples were machined with FIB.
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8

Microstructural Characterization by EBSD and TEM

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Electron backscattered diffraction (EBSD) mapping using a step size of 1 μm was performed on a FEI Nova 400 SEM equipped with a HKL Channel 5 system. The precipitates were examined by transmission electron microscopy (TEM) on a FEI-F20 TEM. Thin foils for TEM observation were prepared by mechanical grinding and subsequent ion beam thinning (Gatan PIPS 691).
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9

Microstructural Analysis of Zn-Li Alloy

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As-extruded Zn-0.8Li alloys were cut into 1 mm thickness disk followed by grounding and polishing with 0.25 µm diamond slurry. Polished samples were etched with 4% HNO3/alcohol solution for 5-10 s and pictured by a scanning electron microscopy (Hitachi S-4800, Japan). An X-ray diffractometer (XRD, Rigaku DMAX 2400, Japan) was used to examine the intermetallic phases with scanning range from 10° to 90° at a scan rate of 2° min−1 and step of 0.02°. Polished samples were further processed into 60 µm thickness, followed by punching into 3 mm diameter disks, and ion-beam milling using Gatan PIPS 691 with 10 KeV at −25 °C to −30 °C. Samples were plasma cleaned by Gatan SOLARUS 950 before visualized under a high-resolution high-angle annular dark-field mode (HAADF) at 300 kV using a scanning transmission electron microscopy (FEI Titan G2 60–300 ChemiSTEM).
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10

Grain Growth in Magnesium Alloy via Chill-Casting

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High purity Mg (>99.9%) ingot was melted at 720 o C for 1 h, and then directly solidified by a chill-casting method. The cooling rate was below 0.5 mm/s to achieve the bar of 50 mm in diameter with a large grain size (~ 5 mm). The grain orientation was confirmed by electron back scattered diffraction equipped with a HKL-EBSD system. The specimens were prepared by traditional mechanical grinding and polishing from 500 to 10 μm in thickness, then ion-beam milling using Gatan PIPS 691 with 4 keV. The atomic structures of specimens were identified by high revolution transmission electron microscopy (HRTEM, FEI TITAN ETEM G2: an ultra-high point resolution of 0.1 nm with a Gatan Model-994 CCD digital camera and an electron energy loss spectrometer (EELS), operated 12 ACS Paragon Plus Environment at a voltage of 300 kV. The CO 2 gas around the thin specimen was performed at a pressure range of 0.5 ~ 1.2 mbar during the entire experiments, and the range of e-beam dose is between 5×10 3 and 1×10 7 e/nm 2 •s. Video and image recording were started only until the range of pressure of dioxide-gas was reached.
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