2000
DOI: 10.1080/00268970009483360
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Theoretical and experimental study of quadrupolar echoes for half-integer spins in static solid-state NMR

Abstract: International audienceNumerical simulations of powder spectra produced by a two-pulse sequence applied to a quadrupolar nuclei system of half-integer spin number make it possible to propose simple experimental instructions to record static echo spectra with minimum lineshape distortion. Calculations take into account quadrupolar (first and second orders), shielding, scalar and inhomogeneous dipolar interactions as well as the radiofrequency pulse specifications (strength, duration, phase). The suggested instru… Show more

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Cited by 67 publications
(47 citation statements)
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“…echo [100][101][102][103][104], which is located at t 2 = t 1 and whose amplitude is modulated neither in phase nor in amplitude, the MQ-MAS echo and anti-echo amplitudes are phase-modulated by exp[−t 2 ω F1 (I p)] with [105] …”
Section: Theorymentioning
confidence: 99%
“…echo [100][101][102][103][104], which is located at t 2 = t 1 and whose amplitude is modulated neither in phase nor in amplitude, the MQ-MAS echo and anti-echo amplitudes are phase-modulated by exp[−t 2 ω F1 (I p)] with [105] …”
Section: Theorymentioning
confidence: 99%
“…Pulses in the spin-echo sequence were optimized to reproduce the powder line shapes accurately. 28 The echo delays in QCPMG trains were set between 100 and 500 µs, and from 40 to 80 echoes were usually accumulated. In situations when the whole spectral range could not be excited in a single experiment (all compounds except K 2 SO 4 ), the spectra were obtained from several equally spaced offsets.…”
Section: Introductionmentioning
confidence: 99%
“…These measurements were performed using a Bruker 5 mm static horizontal solenoid design probe (at 9.4 T), and a home-built, balanced-circuit design 7.5 mm static horizontal solenoid probe (at 18.8 T). All static 93 Nb data were acquired with the solid echo θ -τ -θ -τ -(acquire) (θ ≈ π/4) experiment with an extended phase cycle to capture undistorted echoes with minimal influences from residual echo tails and finite pulse widths 28,29 . 'Non-selective' (solution) π/2 pulse widths of 8 -10 μs were calibrated on a saturated K[NbCl6]/CH3CN solution from which 'selective' (solid) θ pulses of 0.8 -1.0 μs were employed in the solid echo measurements.…”
Section: Solid State Nmrmentioning
confidence: 99%