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4 mm mas probe

Manufactured by Bruker
Sourced in Germany

The 4 mm MAS probe is a critical component of Bruker's nuclear magnetic resonance (NMR) spectrometer systems. This probe is designed for magic-angle spinning (MAS) experiments, which are essential for the analysis of solid-state and semi-solid samples. The 4 mm probe enables high-resolution NMR measurements by rapidly spinning the sample at the magic angle (54.7 degrees) relative to the static magnetic field. This technique helps to improve the spectral resolution and enhance the sensitivity of the NMR analysis.

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10 protocols using 4 mm mas probe

1

Deuterium NMR of Lipid Bilayers

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2H quadrupole echo experiments29 (link) were performed at 61.46 MHz on a Bruker Avance 400 NMR spectrometer using a 4 mm MAS probe, spectral width of 100 KHz and with recycle delay, echo delay, acquisition time and 90° pulse lengths of 0.25 s, 100 μs, 2.6 ms and 3 μs respectively. The temperature was maintained at 310 K to keep the bilayers in their liquid-crystalline phase. During processing the first 10 points were removed in order to start Fourier-transformation at the beginning of the echo. Spectra were zero filled to 1 k points and 50 Hz exponential line-broadening was applied. Smoothed deuterium order parameter profiles were obtained from symmetrised and dePaked 2H-NMR powder spectra of POPG-d31 using published procedures30 (link)–32 (link).
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2

Structural Characterization of Graphene Oxide

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HR-TEM images of GO were collected on a Titan G2 60-300 spherical aberration–corrected TEM (FEI, USA) equipped with a high-brightness Schottky field emission gun and an image aberration corrector to provide a spatial resolution better than 0.8 Å in TEM mode. Solid-state NMR spectra were recorded using a Bruker AVANCE III 400 NMR spectrometer equipped with a 4-mm MAS probe (Bruker, Massachusetts, USA) and were operated at 400- and 100-MHz resonance frequency for 1H and 13C, respectively. All spectra were collected at 12.5 kHz and at ambient temperature. The 13C direct polarization NMR spectrum was collected with 4-μs excitation pulse, 1- or 5-s recycle delay, and 4096 scans. 1H NMR spectra were measured after a spin lock at a field strength of |γB1| = 50 kHz for durations up to 3.2 ms, probing T of different 1H NMR signals. The 1H and 13C chemical shift was referenced to hydroxyapatite peak at 0.18 ppm and carbonyl peak of freshly made crystalline glycine at 176.49 ppm.
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3

Solid-State Tin Oxide NMR Analysis

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The 119Sn MAS NMR spectra were recorded on a Bruker Advance III HD spectrometer equipped with a 4 mm MAS probe, operating at 186.5 MHz with the samples spinning at 12 kHz, high power proton decoupling, a 30 s recycle delay, and typically 2048 scans. SnO2 was used as a secondary reference at –604.3 ppm.
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4

Solid-state NMR of Riparin I

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High-resolution 13C solid-state spectra for both riparin I batches were recorded using the ramp CP/MAS sequence with proton decoupling during acquisition. The solid-state NMR experiments were performed at room temperature in a Bruker Avance II spectrometer (Bruker, Karisruhe, Germany) operating at 300.13 MHz for protons and equipped with a 4-mm MAS probe. The operating frequency for carbon was 75.46 MHz. Adamantane was used as an external reference for the 13C spectra and to set the Harmann–Hahn matching condition in the cross-polarization experiments. The spinning rate was 10 kHz. All spectra were recorded at ambient temperature and chemical shifts were externally referenced to tetramethylsilane.
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5

Solid-state NMR Analysis of Hydrated UMONT

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The UMONT material was heated to 393
K to remove the nanoconfined water and then rehydrated in a saturated
environment containing 17O labeled water. All solid-state
NMR experiments were performed on a Bruker AVANCE 500 solid-state
NMR spectrometer equipped with an 11.74 T magnet and a Bruker 4 mm
MAS probe. The resonance frequency was 67.8 MHz for 17O.
Room temperature 17O magic angle spinning (MAS) NMR experiment
was performed by employing a single 30° pulse sequence with a
recycle delay time of 0.1 s and 15 kHz of spinning speed. The data
were averaged over 20,548 scans and processed with 100 Hz of exponential
line broadening. Static 17O NMR data were collected by
using a Hahn Echo pulse sequence with a solid 90° pulse length
of 1.37 μs. The interpulse delay time was varied from 14 to
24 μs, and 22 μs was optimal for echo formation and signal
intensity. The recycle delay time was also varied from 0.05 to 1 s,
but there was no significant difference of the signal intensities
between the qualities of 0.1 and 1 s. The final parameters used for
data acquisition were 0.1 s of recycle delay time and 22 μs
of interpulse delay time. Static 17O NMR data were collected
in the temperature range of 293–193 K and temperatures were
calibrated by 207Pb NMR spectra.60 (link) The chemical shift was referenced to tap water (0 ppm) for the 17O NMR.
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6

Solid-State NMR Analysis of Surgical Masks

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Initial characterization of the surgical masks occurred through solid‐state NMR spectroscopy. Data have been acquired using a 9.4 T Avance III Bruker spectrometer using a 4 mm MAS probe. 1H spectra were collected with a single‐pulse sequence adopting a π/2 pulse of 2.5 ms and averaging over 128 scans under MAS condition (10 kHz). 13C spectra were acquired with 1H‐13C CPMAS sequence under the same MAS condition. The 1H π/2 pulse was 2.5 ms, the delay time 5–200 s depending on the sample, as previously determined with 1H experiments, the contact time 2.5 ms, and the signals were averaged over 4–8k scans. High‐power 1H decoupling (HPDEC) 13C spectra have been collected averaging over 1k scans with a delay time of 50 s and pulse of 4 ms.
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7

Characterization of Synthesized Zeolites

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The scanning electron microscopy (SEM) images and energy-dispersive X-ray spectroscopy (EDS) of the synthesized zeolites were obtained using Auriga 60 CrossBeam (FIB/FE-SEM) microscopes, operating at an acceleration voltage of 1.5–3 keV and a current of 10 μA.
The X-ray powder diffraction (XRD) patterns were collected at room temperature on a Philips X'Pert Panalytical powder diffractometer using Cu Kα radiation (λ = 1.5418 Å). The data were collected in a stepwise fashion of 2θ ranging from 5.0° to 40.0° with a step size of 0.02° and 2 s per step.
The micropore volume and surface area of the zeolite samples were measured using N2 adsorption isotherms at 77 K with a Micromeritics ASAP 2020 device. Before the adsorption measurements, each sample was degassed at a temperature of 350°C for 6 h. The specific surface area (SBET) and microporous volume (Vmicro) were calculated using the BET and t-plot methods, respectively.
29Si and 27Al magic angle spinning nuclear magnetic resonance (MAS NMR) spectra were recorded on a Bruker AVIII-500 solid-state NMR spectrometer and a Bruker 4 mm MAS probe. The spectral operating frequencies were 500.1 MHz, 130.3 MHz, and 99.3 MHz for 1H, 27Al, and 29Si nuclei, respectively.
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8

Deuterium NMR of Phospholipid Bilayers

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2H quadrupole echo experiments47 (link) for samples containing POPG-d31 were performed at 61.46 MHz on a Bruker Avance 400 NMR spectrometer using a 4 mm MAS probe, spectral width of 100 KHz and with recycle delay, echo delay, acquisition time and 90° pulse lengths of 0.25 s, 100 μs, 2.6 ms and 3 μs respectively. The temperature was maintained at 310 K to keep the bilayers in their liquid-crystalline phase. During processing the first 10 points were removed in order to start Fourier-transformation at the beginning of the echo. Spectra were zero filled to 1 k points and 50 Hz exponential line-broadening was applied. Smoothed deuterium order parameter profiles were obtained from symmetrised and dePaked 2H-NMR powder spectra of POPG-d31 using published procedures48 49 50 (link).
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9

NMR Metabolomics of Larval Brains

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Third instar larvae were dissected in a drop of ice-cold phosphate buffer (pH 7.4 made in D2O) under the microscope in order to collect their brains and in a maintained cool environment to limit metabolic degradation. Ten to 15 brains and a drop of PBS were transferred into a 4 mm HR-MAS rotors. A total of 15 glioma samples, 9 UAS-control samples and 8 Gal4-control samples were prepared. Once ready, each sample was analyzed on a Bruker 750 MHz Avance III HD spectrometer (Bruker BioSpin, Germany) equipped with a Bruker 4 mm MAS probe. The sample was kept at 3°C with a rotor spinning frequency of 4 kHz. HR-MAS NMR data was acquired using a spin echo (echo time of 2 rotor periods) with water suppression. Each FID was acquired in 40k points for 1024 scans and an acquisition time of 53 minutes.
2D 1 H-1 H Total through Bond correlation SpectroscopY (TOBSY) experiments were also performed on several samples for assigning the observed peaks.
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10

Solid-State NMR Analysis of Kneading Complexes

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High-resolution solid-state 13 C spectra of the kneading complexes (KN I, KN II), the co-precipitated samples (CP I and CP II) and the physical mixtures (PM I, PM II) were recorded using the ramp cross polarization/magic angle spinning (CP-MAS) sequence with proton decoupling during acquisition (Harris, 1994) . All ssNMR experiments were performed at room temperature in a Bruker Avance II spectrometer equipped with a 4 mm MAS probe, operating at 300.13 MHz for protons. The operating frequency for carbons was 75.46 MHz. Glycine was used as external reference for the 13 C spectra and to set up the Hartmann-Hahn matching condition in the cross-polarization experiments. All the spectra were recorded with 1600 scans, a contact time of 1.5 ms during CP and a recycling time of 5 s. The spinning rate for all the samples was 10 kHz. 1 H spin-lattice relaxation times in the laboratory frame ( 1 H T 1 ) were measured for the samples under static conditions with an inversionrecovery pulse sequence (-t-/2) with recovery times t between 10 s and 32 s. The recycling delay in these experiments was 10 s.
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