2008
DOI: 10.1063/1.2975206
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Z -matrix formalism for quantitative noise assessment of covariance nuclear magnetic resonance spectra

Abstract: Due to the limited sensitivity of many nuclear magnetic resonance ͑NMR͒ applications, careful consideration must be given to the effect of NMR data processing on spectral noise. This work presents analytical relationships as well as simulated and experimental results characterizing the propagation of noise by unsymmetric covariance NMR processing, which concatenates two NMR spectra along a common dimension, resulting in a new spectrum showing spin correlations as cross peaks that are not directly measured in e… Show more

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Cited by 21 publications
(14 citation statements)
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“…However, for nonlinear spectral estimates, such as covariance spectroscopy, the signal‐to‐noise ratio is no longer a reliable indicator of the sensitivity 67. 68 The assessment of sensitivity for NUS‐Cov is currently under investigation. Furthermore, the level of artifacts can be decreased by optimizing the NUS schedule.…”
Section: Resultsmentioning
confidence: 99%
“…However, for nonlinear spectral estimates, such as covariance spectroscopy, the signal‐to‐noise ratio is no longer a reliable indicator of the sensitivity 67. 68 The assessment of sensitivity for NUS‐Cov is currently under investigation. Furthermore, the level of artifacts can be decreased by optimizing the NUS schedule.…”
Section: Resultsmentioning
confidence: 99%
“…An important property of unsymmetric covariance NMR is that the sensitivity of the covariance spectrum is limited only by the sensitivity of the experiments it combines 16. For example, unsymmetric covariance of an 13 C- 1 H HMBC17 with a 13 C- 1 H HSQC spectrum establishes carbon-carbon correlations with the enhanced sensitivity characteristic of an inverse detected 13 C- 1 H heteronuclear spectra rather than that of a direct detected 13 C- 13 C correlation spectrum 4…”
Section: Introductionmentioning
confidence: 99%
“…Invocation of the command [C C_axes] = covar(A, B, ‘axes1’, A_axes, ‘axes2’, B_axes, ‘power’, λ) performs the covariance transformation [A*B] λ (using the GIC notation described previously [12]) and, depending on the size of the resulting covariance spectrum, either stores that spectrum as a MATLAB array C (with the information required to write C out as an NMRPipe format file tabulated in C_axes ) or stores in C the name of a temporary file storing the covariance result as its singular value decomposition. Invocation of the command [C C_axes] = covar(A, B, ‘axes1’, A_axes, ‘axes2’, B_axes, ‘power’, λ, ‘Z’, 1 ) produces a Z-matrix [16] instead of an unscaled covariance spectrum. Invocation of covar with only a single spectrum provided performs symmetric covariance processing, either direct or indirect, depending on which dimension(s) are identified as donor dimensions.…”
Section: Resultsmentioning
confidence: 99%
“…Here we present a Covariance NMR Toolbox – compatible with both the MATLAB and the freely available OCTAVE computing environments – that implements all of the major covariance techniques, including direct covariance [8], indirect covariance [9], GIC [12] and the Z-matrix transform [xvi]. The Covariance NMR Toolbox, which is available via the MATLAB Central File Exchange (http://www.mathworks.com/matlabcentral/fileexchange/) or by request from the authors, reads and writes data in the well-documented and spectrometer independent NMRPipe [xvii] format and uses a small number of easy to use and extensible scripts to manipulate frequency domain data.…”
Section: Introductionmentioning
confidence: 99%