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Cryo transfer holder

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The Cryo-transfer holder is a specialized accessory designed for use with electron microscopes. Its core function is to securely transport and transfer temperature-sensitive specimens from a cryogenic environment to the microscope's vacuum chamber while maintaining the specimen's low temperature.

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5 protocols using cryo transfer holder

1

Cryo-TEM Analysis of Kaatialaite Crystals

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Kaatialaite from Jáchymov forms white aggregates of needle-shaped crystals with micrometric size. The mineral is a good candidate for transmission-electron-microscopy analysis as the section of the needles is below 1 µm (Fig. 1). For transmission-electron-microscopy analysis, the mineral was gently crushed in acetone and deposited on an Au grid with a thin film of holey amorphous carbon. In order to preserve the hydrated structure of the mineral under vacuum, the grid was plunged into liquid nitro­gen and transferred to an FEI Tecnai 02 transmission electron microscope (TEM) (with an acceleration voltage of 200 kV, LaB6) using a Gatan cryo-transfer holder. The precession electron diffraction (PEDT) method was used to collect 3D ED data sets (Kolb et al., 2007 ▸ ; Mugnaioli et al., 2009 ▸ ; Vincent & Midgley, 1994 ▸ ). Several data sets were recorded at 100 K on different crystals with a Nanomegas Digistar precession device and an Olympus Veleta side-mounted CCD camera with an Octane 14 bit dynamic range energy-dispersive analyser silicon drift detector from EDAX (Fig. 1). The precession angle was set to 1° with a tilt step of 1°. To reduce the electron dose, a condenser aperture of 10 µm and a low illumination setting (spot size 7 or 8) were used.
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2

Cryogenic TEM of Samples

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Each sample was placed on a 400 mesh copper grid and transferred to a Gatan cryo transfer holder containing liquid N2. The samples were then investigated by cryogenic transmission electron microscopy (cryo-TEM) at 120 kV (Hitachi HT7800, Tokyo, Japan).
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3

Cryo-EM Sample Vitrification Protocol

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Sample vitrification was performed with a Leica EMGP plunger (Leica Microsystems). Briefly, 3 ul of purified sandwich sample was applied to a glow-discharged Quantifoil grid (R1.2/1.3, Electron Microscopy Sciences). The grid was quickly plunged into liquid propane after 3.5 s blotting time at 95% humidity. Specimen was then transferred onto a Gatan cryo-transfer holder (Gatan) and examined under a JEM2100F electron microscope (JEOL USA) with operation voltage at 200 kV. The images were recorded at electron dose <20 e/A2 and collected on a Gatan OneView CCD detector at pixel size of 2.8 Å at specimen space.
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4

Characterization of CpG-A-loaded SNAs

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To assess CpG-A incorporation into SNAs, agarose gel electrophoresis was performed using 1% agarose (Sigma) with SYBR Safe DNA gel stain in 0.5× tris/borate/EDTA (TBE) (ThermoFisher Scientific) under 120 V for 1 h. To assess dual-CpG loading, fluorophore-labeled oligonucleotides (fluorescein-CpG-A and Cy5-CpG-B) were used, and agarose gel electrophoresis was performed using 0.5% agarose in 1× TBE without further staining. Dynamic light scattering (DLS) and zeta potential measurements were performed using a Malvern Zetasizer Nano with ~10 nM samples by particle. CryoTEM was performed with a Hitachi HT7700 TEM with a Gatan cryo-transfer holder, and imaging was performed under a 120 kV accelerating voltage. CryoTEM samples were prepared by loading 4 μL of sample (100 μM CpG SNA stock solution or 1.33 μM liposome solution) onto 300-mesh copper TEM grids with lacey carbon films (Electron Microscopy Sciences) using a FEI Vitrobot Mark IV with its chamber equilibrated at 4 °C and 100% humidity. The samples were blotted for 5 s and plunged into liquid ethane before they were transferred and stored in liquid nitrogen. FRET measurements were performed using a Synergy plate reader (Biotek) with 10 nM samples by oligonucleotides. FRET efficiency (E) was calculated as
E=1FDAFD
where FDA and FD are the donor fluorescence intensities with and without an acceptor, respectively.
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5

Lorentz TEM for Magnetic Nanostructures

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We carried out the magnetic contrast observation by using the Lorentz TEM (JEOL-2100F). In Lorentz TEM mode, the objective lens was turned off and an objective mini-lens under the specimen was employed to induce the normal magnetic field to the thin nanostripe. The observed magnetic contrast can be understood qualitatively in terms of the Lorentz force acting on the moving electrons as they travel through in the magnetic foil. The high-resolution lateral magnetization distribution map was obtained by TIE analyses of the Lorentz TEM images. The details of the Lorentz TEM and the TIE analyses are given in the Supplementary Note 1. The magnetization distribution maps used in the main text and Supplementary Information are all original ones without subtracting the artificial magnetic contrasts. Thin-plate thickness was measured using Electron Energy Loss Spectroscopy (EELS). A double-tilt liquid-nitrogen cooling holder (Gatan, Cryo-Transfer Holder) was used to detect the phase transition below the Curie transition temperature Tc. This enables the specimen temperature to be reduced to 100 K with the measured temperature displayed on the cooling holder controller. The magnetic field applied normal to the thin plate was induced by the magnetic objective lens of the TEM.
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