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Genix

Manufactured by Xenocs
Sourced in Switzerland

The GeniX is a high-performance X-ray source developed by Xenocs. It is designed to provide a stable and intense X-ray beam for various analytical techniques. The core function of the GeniX is to generate X-rays that can be used for sample analysis and characterization. The technical specifications and capabilities of the GeniX are available upon request.

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6 protocols using genix

1

Aligned Amino Acid Nanostructure Characterization

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The amino acids were dissolved
in deionized water at a concentration of 2 mg/mL for individual amino
acids or 1 mg/mL each for dl-composites by heating to 90
°C. The assembled structures were drop-cast over a thin Kapton
film and left to dry in the presence of a magnetic field to produce
aligned structures. WAXS measurements were performed using an in-house
X-ray scattering system, with a GeniX (Xenocs) low-divergence Cu Kα
radiation source (wavelength of 1.54 Å) and a scatterless slits
setup.71 (link) Two-dimensional scattering data,
with a momentum transfer wave vector (q) range of
0.07–2.5 Å–1 at a sample-to-detector
distance of approximately 160 mm, were collected on a Pilatus 300
K detector (Dectris, Baden-Daettwil, Switzerland) and radially integrated
using Matlab (MathWorks, Natick, MA, USA)-based procedures (SAXSi).
Calibration was performed using silver behenate. The scattering data
of the empty Kapton film was collected as background and subtracted
from the sample measurement.
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2

WAXS Analysis of SHR-FLLF Peptide Solutions

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The SHR-FLLF peptide solutions at a concentration of 15 and 5 mg ml−1 were sealed in quartz capillaries with a 1.5 mm diameter. WAXS measurements were performed using an in-house X-ray scattering system, with a GeniX (Xenocs) low divergence Cu Kα radiation source (wavelength of 1.54 Å) and a scatterless slits setup48 . Two-dimensional scattering data, with a momentum transfer wave vector (q) range of 0.07−2.5 Å−1 at a sample-to-detector distance of about 160 mm, was collected on a Pilatus 300 K detector (Dectris, Baden-Daettwil, Switzerland) and radially integrated using Matlab (MathWorks, Natick, MA, USA)-based procedures (SAXSi). Calibration was performed using silver behenate. The scattering data of the water at pH 2 was collected as background and used to subtract the solvent and spurious scattering from the WAXS system itself, for example, Kapton vacuum windows and air gaps.
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3

X-ray Scattering Protocol with Detailed Instrumentation

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Measurements were performed using a lab-based X-ray scattering system, with a GeniX (Xenocs) low divergence Cu Kα radiation source (wavelength of λ=1.54 Å) and a scatterless slits setup17 (link). The full-width-half-maximum of the direct beam is 1 mm in diameter, and the measured divergence is 0.0372 degrees ( 2θ ). Samples were measured at distance of ds=117mm using Pilatus 300K detector (Dectris) having pixel size of 172×172μm2 (Ref.25 (link)). The detector, sample stage, and slits were motorized using stepper motors with a positioning accuracy of 1 μm and controlled by SPEC software. In all the measured images, only valid pixels are used. We removed the gaps between the separate detector’s modules in pre-processing. All 2D images presented below were cropped to show the scattering on a single module. The measured flux for the different beam sizes is presented in the supplementary materials Section 2.
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4

Small-Angle X-ray Scattering of Glycolipid Samples

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The aggregated
GlcCer samples at 30 mg/mL concentration were measured in 1.5 mm diameter
sealed quartz capillaries. WAXS/SAXS measurements were performed using
an in-house solution X-ray scattering system, with a GeniX (Xenocs)
low divergence Cu Kα radiation source (wavelength
of 1.54 Å) and a scatterless slits setup.70 (link) Two-dimensional scattering data with a wave vector amplitude
(Q) range of 0.06–2 Å–1 at a sample-to-detector distance of about 230 mm were collected
on a Pilatus 300 K detector (Dectris), and radially integrated using
MATLAB (MathWorks) based procedures (SAXSi). Background scattering
data were collected from buffer solution alone. The background-subtracted
scattering correlation peaks were fitted using a Gaussian with a linearly
sloped baseline. For each sample, time-resolved correlation peaks
position, intensity, and width were extracted.
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5

X-Ray Scattering Protocol for Lipid Samples

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Samples at 30 mg/ml lipid concentration were measured in 1.5 mm diameter sealed quartz capillaries. Measurements were performed using an in-house solution X-Ray scattering system, with a GeniX (Xenocs) low divergence Cu K α radiation source (wave length of 1.54 Å) and a scatter-less slits setup [19] . Two-dimensional scattering data with a q range of 0.06 -2 Å -1 at a sample-to-detector distance of about 230 mm were collected on a Pilatus 300K detector (Dectris), and radially integrated using MATLAB (MathWorks) based procedures (SAXSi). Background scattering data was collected from buffer solution alone. The background-subtracted scattering correlation peaks were fitted using a Gaussian with a linearly sloped baseline. For each sample, time-resolved correlation peaks position, intensity and width were extracted.
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6

Structural Analysis of NF Hydrogels

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The powder diffraction scattering data from NF hydrogels contained in quartz capillaries was integrated azimuthally and the intensity was plotted versus reciprocal distance q. The intensity, in arbitrary units, showed a broad peak with a maximum in the range of q = 0.1-0.2 nm À1 (see ref. 24 and 30). The peak location relates to the inter-filament spacing (d = 2p/q). Broadening of this peak is observed due to density fluctuations and the semi-flexible nature of the individual filaments. Baseline background of the form AÁq ÀB + C with B = 2-3 is subtracted (Fig. S2,ESI †), and the resultant peak is fitted with a Lorentzian function using Matlab routines. 13, 30 Preliminary experiments were performed at our home-lab using a Pilatus 300K detector and a Xenocs GeniX Low Divergence CuKa radiation source setup with scatterless slits. 31 Subsequent measurements were performed at synchrotron facilities: P12 beamline in DESY, Hamburg; SWING beamline in SOLEIL, Paris; and I911 SAXS beamline in MAX-lab, Lund with 10 keV.
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