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The R4000 is a high-precision liquid chromatography system designed for analytical applications. It features a robust and reliable pumping system, a temperature-controlled column compartment, and a sensitive absorbance detector. The R4000 is capable of performing a variety of chromatographic separations and analyses, including reversed-phase, normal-phase, and ion-exchange chromatography.

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34 protocols using r4000

1

High-resolution Angle-resolved Photoemission Spectroscopy

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High-resolution angle-resolved photoemission measurements were carried out on our lab system equipped with a Scienta R4000 electron energy analyzer51 (link),52 (link). We use a helium discharge lamp as the light source that can provide a photon energy of hν = 21.218 eV (helium I). The energy resolution was set at ~ 20 meV for the Fermi-surface mapping (Fig. 1) and band-structure (Figs. 2a, c, 3 and 5) measurements and at 4 meV for the CDW gap measurements (Fig. 4). We also use an ultraviolet laser as the light source that can provide a photon energy of hν = 6.994 eV with a bandwidth of 0.26 meV. The energy resolution was set at ~2.5 meV for the measurements in Fig. 2f–i. The angular resolution is ~0.3°. The Fermi level is referenced by measuring on a clean polycrystalline gold that is electrically connected to the sample. The sample was cleaved in situ and measured in a vacuum with a base pressure better than 5 × 10−11 Torr.
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2

Algal Cyst Analysis by XPS

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The algal suspension supernatant in a 3% formalin solution was frozen at −20 °C and freeze-dried to remove formalin. The powder obtained after lyophilization was examined by X-ray photoelectron spectroscopy to identify chemical bonds. The XPS analyses were performed using a multi-chamber UHV system (PREVAC). The spectra were acquired using a Scienta SAX-100 X-ray source (Al Kα, 1486.6 eV, 0.8 eV band) equipped with an XM 650 X-ray monochromator (0.2 eV band) and a Scienta R4000 hemispherical electron analyzer. The transition energy of the analyzer was set to 200 eV for the measurement of spectra (500 meV step) and 50 eV for the regions (high-resolution spectra) with a 50 meV step. The pressure in the analytical chamber during the collection of the spectra did not exceed 2 × 10–8 mbar. Samples from site 1 and site 3 were compared, as these samples comprised many cyst cells characterized by a polysaccharide envelope and no infections with the parasitic fungus.
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3

ARPES Measurements of FeSe Thin Films

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ARPES measurements were carried out at beamline 5-4 of the Stanford Synchrotron Radiation Lightsource and beamline 10.0.1 of the Advanced Light Source using SCIENTA R4000 electron analyzers. The total energy resolution was set to 10 meV and the angular resolution was 0.3°. Single crystals were cleaved in situ at 10 K for each measurement. The FeSe films were transported to the beamline under vacuum and further annealed before measurements. All measurements were done in ultra high vacuum with a base pressure lower than 4 × 10−11 torr.
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4

ARPES Measurements in Ultrahigh Vacuum

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Experiments were performed at the University of British Columbia (UBC) in a ultrahigh vacuum chamber equipped with a SPECS Phoibos 150 analyzer with ΔE = 6 meV and Δk=0.01 A°1 optimum energy and momentum resolutions, respectively, at a base pressure of better than p = 7 × 10−11 torr. Photons with an energy of 21.2 eV were provided by a SPECS UVS 300 monochromatized gas discharge lamp. Our home-built six-axis cryogenic manipulator allows for measurements between 300 and 3.5 K. Additional datasets were taken at the UBC with a second ARPES setup equipped with a Scienta R4000 analyzer and a Scienta VUV5000 ultraviolet source with ΔE = 1.5 meV and Δk=0.01 A°1 optimum energy and momentum resolutions, respectively, for 21.2-eV photons. The samples were annealed at 600°C for about 2 hours at p = 1 × 10−9 torr and then at 500°C for about 10 hours at p = 5 × 10−10 torr immediately before the ARPES measurements.
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5

Characterization of Bi-rich Antimonide Crystals

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High-quality single crystals were grown using a Bi rich melt in the ratios YbMnBi10 and EuMnBi10. The elements were heated to 1000 °C and cooled to 400 °C at 0.1 C/min, then subsequently centrifuged to remove excess Bi. The crystals exposed mirror-like portions of the surface after the cleave in ultra-high vacuum breaking z-periodicity. The structures of the compounds were solved by single crystal X-ray diffraction (Supplementary Table 3).
ARPES measurements were performed at the I05 beamline of Diamond Light Source, UK. Single crystal samples were cleaved in situ at a pressure lower than 2 × 10−10 mbar and measured at temperatures about 7 K. Measurements were performed using (s,p)-polarized synchrotron light from 18 to 100 eV and employing Scienta R4000 hemispherical electron energy analyzer with an angular resolution of 0.2–0.5° and an energy resolution of 3–20 meV39 (link).
Magneto-optical imaging of magnetic domains at the surface of the YbMnBi2 crystal was performed in a magneto-optical Kerr microscope adjusted for the Voigt effect at perpendicular light incidence at room temperature. White, linearly polarized light from a LED lamp was utilized.
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6

Angle-Resolved Photoemission Spectroscopy of Strongly Correlated Materials

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The angle and energy resolutions of the ARPES measurements (Scienta R4000) are set as 0.2o and ∼10 meV. The photon energy-dependent ARPES experiments were performed with photon energy varying from 70 eV to 115 eV. The kz was calculated by . The inner potential V0=12 eV. Unless otherwise stated, we used photon energy at 100 eV for normal ARPES measurements. The 2D and 3D carrier density can be calculated from the Luttinger area of the FSs. and . From the Ti3+ ratio, the carrier density can also be calculated by n2D=ratio × a−2 and n3D=ratio × a−3 with the lattice constant α=3.9 Å.
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7

Angle-Resolved Photoemission Spectroscopy of Cleaved Samples

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ARPES measurements (T = 10–160 K, hν = 45–85 eV) of in-situ cleaved single-crystal samples were performed using a Scienta R4000 hemispherical analyser at beamline 10.0.1 of the Advanced Light Source with an energy resolution between 8 and 35 meV, and an angular resolution of 0.35 .
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8

ARPES Study of Bi2O2Se Crystals

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The ARPES experiments were performed on the Bi2O2Se bulk crystals at beamline I05 of the Diamond Light Source. The data were recorded using a Scienta R4000 analyzer with the total convolved energy and angle resolutions of 20 meV and 0.2°, respectively. During the experiment, the sample was maintained in the UHV system under a pressure better than 1 × 10−10 torr, and the sample temperature was kept at 10 K. A fresh surface of Bi2O2Se single crystal for the ARPES measurement was obtained by cleaving the sample in situ along its natural (001) cleavage plane.
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9

ARPES Measurements of Thin Film Samples

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ARPES measurements were performed at beamline 10.0.1 of the Advanced Light Source (ALS) at Lawrence Berkeley National Laboratory. The measurement pressure was kept below 3 × 10−11 Torr at all times. The data was recorded using a Scienta R4000 analyser at variable sample temperatures. The total convolved energy and angle resolutions were 16 meV and 0.2°, respectively. The fresh surface for ARPES measurement was obtained by cleaving the thin film sample in situ as described in ref. 28 .
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10

ARPES Analysis of (Li0.8Fe0.2OH)FeSe

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ARPES measurement was conducted in an in-house ARPES system with a helium discharge lamp (21.2-eV photons), at the temperature of 11 K, using Scienta R4000 electron analyzers. The energy resolution was 8 meV, and the angular resolution was 0.3°. (Li0.8Fe0.2OH)FeSe samples were cleaved in situ under ultrahigh vacuum. During measurements, the spectroscopy qualities were carefully monitored to avoid the sample aging issue.
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