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25 protocols using lts420

1

Microscopic Imaging of Material Transformations

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Fluorescence images were acquired with a Leica-Microsystems DM2500 microscope. Optical microscope images were obtained with a Zeiss Axioplan 2 microscope, equipped with a MediaCybernetics Evolution VF digital camera. For images of the shape change this microscope was equipped with a Linkam LTS420 thermal stage under nitrogen atmosphere, using heating rates ranging from 3 to 10 °C min−1. The movie of the “kicking” glass bead was taken with a Leica WILD M10 microscope, equipped with an Evolution MP5.0 Leica DMC2900 digital camera with frame rate of 30 fps and a Linkam LTS420 thermal stage under nitrogen atmosphere.
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2

Hot Stage Microscopy of DAS-HA, DAS-HEA, and DAS-OA

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Hot stage microscopic
study on DAS-HA, DAS-HEA, and DAS-OA was performed using a Leica polarized
light microscope (Model, DM2700P) equipped with a Linkam hot stage
(Model, LTS 420 with LINK software). The test samples were individually
taken onto a hot stage microscopic glass slide by spreading the powder
sample properly on the microscopic slide. The prepared sample slide
is inserted into the Linkam hot stage accessory (LTS 420), and using
20× magnification with a 5.0 megapixel camera, the sample is
illuminated and focused. The resulting video then appears on a connected
computer. The sample is heated up to 300 °C with a 5 °C/min
ramp rate (LINK, version No. 1.2.20.8).
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3

Thermal Response of Microcapsules

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The melting of the core of the microcapsules depending
on the temperature has been investigated by an optical microscope
equipped with a hot stage. MC was placed on a light microscopy glass
slide on a temperature-controlled stage LTS-420 (Linkam, Surrey, U.K.)
and heated from rt to 50 °C and recooled to rt. Visual images
have been recorded with an Axio Imager (Carl Zeiss Microscopy GmbH,
Jena, Germany). Temperature-controlled microscopy was performed on
the neat microcapsules and the PDA-coated microcapsules.
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4

Quantifying Ice Crystal Growth Inhibition

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A 2 µL droplet of sample was sandwiched between two cover slides and placed in a stage attached to a Nikon ECLIPSE Ci-Pol Optical Microscope where the temperature is controlled by a Linkam LTS 420. A thin polycrystalline ice layer was created by rapidly freezing (20 °C min -1 ) to -40 °C. The temperature was then raised (10 °C min -1 ) to -7 °C and kept constant for 1 h. Images were taken every 5 min and analyzed using ImageJ and an in-house written Matlab script to obtain the equivalent radius for each ice crystal (details in the Supporting Information). The ice crystal growth rate constants, k dc , were obtained from the temporal increase in the number average radius cubed as described by LSW theory, [15a] according to 8 9
3 0
Finally, the inhibitory concentration c i was obtained from k d (c) as a function of VAM concentration fit to
where k d0 is the growth rate constant at zero inhibitor concentration. [15]
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5

Cryomicroscopic Visualization of Ice Crystals

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Optical cryomicroscope BX-51 (Olympus Corporation, Japan) was used to image the distribution of solution and ice crystals. A droplet (approx. 0.5 μl) of 50.4-mM sodium citrate buffer (mAb buffer without trehalose) was placed on an object plate and cooled in a temperature controlled cryostage LTS420 (Linkam Scientific Instruments, UK) using liquid nitrogen as a cooling medium. Samples were cooled to − 70°C at different rates between 0.5 and 5°C/min. Images were taken at − 70°C using a CCD camera after calibrating a ULWD 5×−50× objective (Olympus Corporation, Japan).
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6

Thermal and Optical Characterization of Polycrystalline Material

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The DSC curves on a PerkinElmer DSC 6000 instrument under a nitrogen atmosphere at a heating and cooling rate of 10 K min−1 was measured. The polycrystalline powder sample was placed in aluminum crucibles. It was performed temperature‐dependent SHG intensity on Ins 1 210 058, INSTEC Instruments using an unexpanded laser beam with low divergence (pulsed Nd: YAG at a wavelength of 1064 nm, 5 ns pulse duration, 1.6 MW peak power, 10 Hz repetition rate), and a Linkam LTS420 thermal stage was equipped to control the temperature. The laser was Vibrant 355 II, OPOTEK. The complex dielectric permittivity curves were measured on an automatic impedance Tonghui 2828 analyzer at the frequency of 1 MHz with the AC (Alternating Current) voltage of 1.0 V. For the dielectric measurements, the polycrystalline sample into powder and pressed it into a thin plate was first grounded. Then the conductive silver glue on both top and bottom plate surfaces as the electrodes of the sample sheet was deposited. Finally, silver conducting glue to stick the copper wire on it for connection with the six‐hole socket to form a capacitor was used.
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7

Electrical Characterization of VO2 Nanowires

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To directly compare the electronic MIT properties of the individual VO2 nanowires with their structural characteristics, which can only be examined using TEM due to the small diameters of the wires, we exploited the focused ion beam (FIB) technique to deposit metal (Pt) electrodes to fabricate individual nanowire devices directly on the customized grids. The electrical properties of the individual nanowire devices were measured by a semiconductor characterization system (Keithley 4200 SCS) on a temperature-controlled heating stage, whose resolution was within 0.1 °C (Linkam LTS420). Note that we performed the measurements with an upper current compliance of 200 μA to limit the Joule heating caused by excessive current.
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8

Hybrid Ionic Skin Sensing Protocol

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The real-time resistance signals of the samples under different strains, temperatures, or humidities were recorded by Tektronix multimeter (DMM 4050) and Keithley multichannel source meter (DAQ6510). During test, electrical connections were made by conductive copper tapes. The heating and cooling cycles were carried out on a temperature-controlled platform (LTS420, Linkam). Prior to test, the sample was sealed on a glass plate with 3 M VHB tape to reduce the influence of humidity on its conductivity. ECG signals were measured using a Heal Force ECG recorder (PC-80B). EMG signals were recorded using the two-channel EMG sensor (ED0136/EDK0056, SICHIRAY). For adhesion and sensing applications, the hybrid ionic skins were attached to several body parts of a volunteer who participated in the experiment approved by the Institutional Biomedical Research Ethics Committee of Shanghai Institutes for Biological Sciences (No. 3011-19-03). All human participants gave written and informed consent before related experiments.
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9

Thermal Characterization of Composites

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The POM observations were performed on the composites with a Leica microscope (DFC295, Leica Microsystems Corporation, Wetzlar, Germany) with a temperature controlled stage (LTS 420, Linkam Scientific Instruments, Tadworth, UK). The sample was first heating to 220 °C and maintained for 3 min, and then cooling down to 138 °C with the cooling rate of 50 °C/min maintained for 30 min. The crystal morphology of the sample can be observed at a constant temperature.
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10

Liquid Crystal Film Formation in Reservoir

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As a reservoir, we used a silicon wafer that has a circular hole with a 50 μm depth and 4 mm diameter. To reduce the meniscus of the water, we treated the O2 plasma to minimize the meniscus before we dropped the water into the reservoir, and we casted 8CB (Sigma-Aldrich) on the water filled in the reservoir. The LC film thickness is ∼1.5 μm that varies with an amount of LC materials. The temperature control to induce the phase transition of LCs was performed on a heating stage (LINKAM LTS420) using a temperature controller (LINKAM TMS94).
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