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Ge 111 monochromator

Manufactured by STOE

The Ge(111) monochromator is a device used to select a specific wavelength or energy from a polychromatic X-ray or neutron beam. It utilizes the diffraction properties of a germanium (111) crystal to filter and isolate the desired wavelength. The monochromator is a core component in various scientific and analytical applications that require a monochromatic beam of X-rays or neutrons.

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3 protocols using ge 111 monochromator

1

Comprehensive Materials Characterization Protocol

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All crystalline phases were characterized by powder X-ray diffraction, thermal, spectroscopic and elemental analyses.
X-ray powder patterns were recorded in transmission mode on a Stoe Stadi-P diffractometer equipped with a Ge(111) monochromator and a position-sensitive detector using Cu Kα1 radiation. The sample was rotated during the measurement.
Thermogravimetric analysis (TGA) was carried out using a TGA 92 system (SETERAM Instrumentation). Differential scanning calorimetric (DSC) measurements were performed with a DSC 131 systems (SETERAM Instrumentation) in the temperature window from room temperature up to 500°C.
Spectroscopically the samples were characterized by FTIR using a Shimadzu FTIR-8300 measuring in transmission mode; LDI-TOF-MS using a Voyager-DE STR (Applied Biosystems Inc.) using a nitro­gen laser with 337 nm and 10 ns; all liquid 1H NMR studies were carried out using an Avance 250 MHz NMR spectrometer (Bruker) at 300 K in d2-sulfuric acid.
Elemental analyses (EA, only C:H:N quantification) were performed on a vario MICRO cube from Elementar Analytical Systems GmbH.
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2

PXRD Characterization of DFQ Sample

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The DFQ sample was prepared between two polymer films. PXRD data were recorded at room temperature with Cu Kα1 radiation in transmission mode on a Stoe Stadi-P diffractometer equipped with a primary Ge(111) monochromator and a linear position-sensitive detector. The sample was rotated during the measurement. Data were collected in a 2θ range from 2.00 to 79.99° with a resolution of 0.01° per step, resulting in 7800 data points. The software WinXPow (Stoe & Cie, 2005 ▸ ) was used for data collection and reduction.
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3

Synchrotron X-ray Powder Diffraction Analysis

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Crystalline powders were filled into capillaries and measured at a powder diffractometer with synchrotron radiation at HASYLAB/DESY (Hamburg, Germany, beamline B2, λ = 49.9694 pm, Ge(111) double monochromator, Ge(111) analyzer, NaI scintillation counter). Structure refinements were performed using the Rietveld method, program GSAS. (32) Positional parameters and occupancies were refined freely. Isotropic displacement parameters were refined, too. Hightemperature X-ray powder diffraction data were collected by a powder diffractometer (STOE Stadi P, position-sensitive detector) with Cu Kα 1 radiation (Ge(111) monochromator, λ = 1.54060 Ã…, quartz capillary, Debyeâ€"Scherrer geometry). Further information on the data collection and crystal structure may be obtained from ref 33.
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