Solid-state
NMR spectra @ 21.1 Tesla
(Click on a picture to enlarge)
Magic
angle adjustment in MAS probes is commonly performed by observing ST spinning
sidebands in 79Br MAS NMR spectra of KBr at low spinning speeds. The magic
angle is set correctly when the sidebands have the highest intensity.
A Hall effect magnetic flux sensor can be used for the same purpose [1],
for example in low-gamma MAS probes incapable of 79Br NMR. We have recently
tested this approach at the 900 NMR Facility: The figure shows the normalized
intensity of the 79Br ST spinning sidebands in KBr versus the Hall voltage
measured. This Hall sensor will be used for magic angle setup in a 2.5
mm boron-free MAS probe which is currently under construction.
For
more information see
[1] S. Mamone, A. Dorsch, O.G. Johannessen, M.V. Naik, P.K. Madhu, M.H. Levitt, "A Hall effect angle detector for solid-state NMR," Journal of Magetic Resonace 190 (2008) 135-141. http://dx.doi.org/10.1016/j.jmr.2007.07.012
A
standard QCPMG NMR pulse sequence consists
of a 90 pulse followed by a train of 180 pulses (more).
Ideally, the resulting spikelet envelope should outline the static lineshape
(middle spectrum, 90-180). If the first pulse deviates from 90 due to incorrect
calibration, the QCPMG spikelet pattern does not change significantly, the
only effect is somewhat lower overall intensity (Figure
A).
While the miscalibrated 90 pulse alone has little impact on the QCPMG lineshape,
of course it is often used to calculate the 180 pulse. As can be seen both,
experimentally and using SIMPSON calculations, the miscalibrated 180 pulse
leads to significantly distorted spikelet patterns (Figure
B). The 180 pulse misset by as little as 20-30 degrees could produce considerable
oscillations in spikelet intensity across the envelope. This illustrates that
the QCPMG NMR experiments are much more sensitive to proper setup of the 180
degree pulse than the Hahn-echo experiments.
QCPMG spectra shown were calculated by Eric Ye (900 Facility) using
the SIMPSON software for a central transition of a spin 3/2 nucleus resonating
at 295 MHz, CQ=10 MHz, etaQ=0.7, CS anisotropy -200 ppm, coincidental EFG
and CSA tensors.
For more information see
Renée Siegel, Thomas T. Nakashima and Roderick E. Wasylishen, "Signal-to-Noise Enhancement of NMR Spectra of Solids Using Multiple-Pulse Spin-Echo Experiments", Conc. Magn. Reson. 26A (2005) 62-77. http://dx.doi.org/10.1002/cmr.a.20038
A
WURST-QCPMG NMR technique has recently been introduced by Luke O'Dell
and Rob Schurko (Windsor)
to achieve uniform excitation of quadrupolar nuclei across very wide bandwidth.
Using this approach wideline spectra of stationary samples can now be acquired
with no need or just minimal transmitter frequency adjustment. The spectrum
shown was acquired in about 1 hour by co-adding 10 individual pieces. Experiments
were performed by Luke O'Dell, who also kindly provided the WURST-QCPMG pulse
sequence for the 900 MHz NMR instrument. This pulse program is now available
to our users. For more information about WURST-QCPMG:
L.A. O'Dell and R.W. Schurko, "QCPMG Using Adiabatic Pulses for Faster Acquisition of Ultra-Wideline NMR Spectra," Chem. Phys. Lett. 464 (2008) 97-102. http://dx.doi.org/10.1016/j.cplett.2008.08.095
May, 2009
Recently
developed Polarization Inversion Spin Exchange at the Magic Angle (PISEMA)
technique finds applications in correlation experiments and is used for accurate
measurements of chemical shift and heteronuclear dipolar interactions (see
Annual Reports on NMR Spectroscopy, 2004, volume 52, p.1-52). This
1H-15N PISEMA experiment with 5N-labeled N-acetyl valine was performed on
the 900 MHz instrument using the Facility's flat-coil E-free probe (M. Monette,
Bruker).
December, 2008
Two new NMR probes have been recently added to a growing array of tools at the
900 Facility. The previously announced 4 mm CP/MAS 1H/13C/15N probe has passed
its first tests in mapping 13C-15N REDOR distances, as in this experiment
with Glycine performed by Eric Ye (the 900 Facility).November, 2008

March, 2008

March, 2008

January, 2007

1H CSA recoupled spectra of citric acid. Experiments performed by Darren
Brouwer (SIMS NRC) with the 2.5 mm MAS probe. Journal
of Magnetic Resonance
185 (2007) 173-178
December,
2006

19F-13C CP MAS spectrum recorded for a hydrated Nafion film. In such
high-resolution spectra various C-F species can readily be identified. Experiments
performed by Shane Pawsey (the 900 Facility) with the 2.5 mm MAS probe.
October, 2006

August, 2006

Similar to MQMAS, satellite transition MAS of half-integer quadrupole nuclei
(STMAS) can be used to separate anisotropic from isotropic interactions.
Experiments performed by S. Steuernagel (Bruker) with the 2.5 mm MAS probe.
July,
2006
The
3Q-MAS spectrum of RbNO3 displaying the HR spectra of the three components
that make up the powder pattern. Experiment performed by V. Terskikh (the
900 Facility) with the 4 mm MAS probe.
Sensitivity
enhancement in MAS spectra of half-integer quadrupole nuclei, DFS (double
frequency sweep), RAPT (rotor assisted population transfer), compared
with a SP (single pulse) experiment. Performed by S. Steuernagel (Bruker)
with the 2.5 mm MAS probe.
July, 2006
127I
NMR of NaIO4 revisited at 21.1 T. Cq=42.3 MHz, CSA is negligible (the span
is <20 ppm). For more see: G.
Wu and S. Dong, SSNMR 20 (2001) 100-107
March,
2006
In
materials ultrahigh magnetic fields are beneficial when studying low-gamma
(and) quadrupolar nuclei. These 39K NMR spectra of KNO3 were recorded on our
900 instrument at the resonance frequency of 42 MHz (compare with 23 MHz at
11.7 T). Experiments performed by I. Moudrakovski (SIMS-NRC) with the wideline
static probe built by J. Bennett (NRC).
Journal of Physical Chemistry B 111 (2007) 491-495.
February,
2006
The
resolution in proton spectra of solids is improved by applying combined rotation
and multiple-pulse spectroscopy (CRAMPS). Experiments performed by
M. Monette (Bruker) with the 2.5 mm MAS probe.
January,
2006
1H/13C
HETCOR with Frequency-Switched Lee-Goldberg (FSLG) 1H homonuclear decoupling
for alpha-Hydroquinone. Experiments performed by D. Brouwer (NRC-SIMS) with
the 3.2 mm MAS probe.
December,
2005
Both
experiments were performed with the 3.2 mm MAS probe. With very short rf-pulses
available on the 900 very broad static lineshapes can be correclty recorded.
In
this case a solid-state 90-pulse for 55Mn was 0.6 us.
November,
2005
Quadrupolar
Carr-Purcell Meiboom-Gill (QCPMG) pulse sequence dramatically improves
signal-to-noise in solid-state NMR experiments of quadrupolar nuclei, here
for 87Rb (I=3/2).
October,
2005
13C
CP/MAS spectrum of caffeine. At 21.1 T note absence of the line splitting
due to the dipolar coupling with the quadrupolar 14N. At lower magnetic fields
such coupling results in very complicated spectra.
Crystal Growth and Design 8 (2007) 1406-1410.
September, 2005
11B MAS NMR spectra of sodium tetraborate (borax). Even at 14.1 T two non-equivalent
boron sites would partially overlap complicating interpretation and quantitative
analysis of the spectra.
13C
CP/MAS spectrum of tetracycline hydrochloride. Resonances from all 22
carbon atoms are well resolved.
September, 2005