2004
DOI: 10.1016/j.jmr.2004.05.016
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Accelerated acquisition of high resolution triple-resonance spectra using non-uniform sampling and maximum entropy reconstruction

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Cited by 223 publications
(215 citation statements)
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“…With very low α, or for many cases of radial sampling, the apparent noise would be larger due to the presence of artifacts. For general CRS, the signal and noise levels for ring j (σ j and η j , respectively) would be: [22] where σ 0 and η 0 are the signal level and the standard deviation of the noise distribution, respectively, for a single sampling point. The signal level σ of the spectrum is not dependent on the sampling pattern, due to the normalization by 1/N j :…”
Section: Sensitivity Considerationsmentioning
confidence: 99%
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“…With very low α, or for many cases of radial sampling, the apparent noise would be larger due to the presence of artifacts. For general CRS, the signal and noise levels for ring j (σ j and η j , respectively) would be: [22] where σ 0 and η 0 are the signal level and the standard deviation of the noise distribution, respectively, for a single sampling point. The signal level σ of the spectrum is not dependent on the sampling pattern, due to the normalization by 1/N j :…”
Section: Sensitivity Considerationsmentioning
confidence: 99%
“…With the recent push to discover faster methods for measuring multidimensional NMR spectra, significant attention has been focused on alternatives to the conventional Cartesian sampling of the time domain, such as the "radial" approaches, which measure points along radial spokes [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17], or the methods that measure a randomly-selected subset of the points from a Cartesian grid, often weighted according to the signal envelope [18][19][20][21][22]. These efforts have been motivated by the discovery that it is possible, in many cases, to use one of the new patterns coupled to a suitable processing method to obtain very high resolution spectral information, with very limited sampling of the time domain.…”
Section: Introductionmentioning
confidence: 99%
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“…Specifically, modifications to the pulse sequence for non-linear acquisition were made according to Vladislav Orekhov (Swedish NMR Centre, see Biopack manual). For the non-TOCSY experiments, 415 complex fids were acquired using a sampling scheme generated using the COAST software (Rovnyak et al 2004), corresponding to a maximum of 60 and 32 points in the 13 C and 15 N dimensions respectively, and a reduction in acquisition time of ~ 4.5 fold. For the C(CO)NH-TOCSY experiment 1000 complex fids were collected, using a sampling schedule generated from the non-uniform sampling scheduler from Mark Maciejewski (http://sbtools.uchc.edu/nmr/sample%5Fscheduler/) corresponding to a maximum of 100 points in 13 C and 32 points in 15 N, leading to a reduction in acquisition time of ~ 2-fold.…”
mentioning
confidence: 99%
“…Backbone resonance assignments were obtained at 45°C using the following three-dimensional experiments, employing conventional or nonuniform sampling in the 15 N and 13 C dimensions: HN(CA)CO, HNCO, HN(CO)CA, HNCA, CBCA-(CO)NH, and HNCACB (15). Nonuniform sampling datasets were processed using the multidimensional decomposition algorithm (16).…”
Section: Methodsmentioning
confidence: 99%