摘要:
Described are methods and apparatus, referred to as “temperature-lock,” which can control and stabilize the sample temperature in an NMR spectrometer, in some instances with a precision and an accuracy of below about 0.1 K. In conventional setups, sample heating caused by experiments with high-power radio frequency pulses is not readily detected and is corrected by a cumbersome manual procedure. In contrast, the temperature-lock disclosed herein automatically maintains the sample at the same reference temperature over the course of different NMR experiments. The temperature-lock can work by continuous or non-continuous measurement of the resonance frequency of a suitable temperature-lock nucleus and simultaneous adaptation of a temperature control signal to stabilize the sample at a reference temperature value. Inter-scan periods with variable length can be used to maintain the sample at thermal equilibrium over the full length of an experiment.
摘要:
Described are methods and apparatus, referred to as “temperature-lock,” which can control and stabilize the sample temperature in an NMR spectrometer, in some instances with a precision and an accuracy of below about 0.1 K. In conventional setups, sample heating caused by experiments with high-power radio frequency pulses is not readily detected and is corrected by a cumbersome manual procedure. In contrast, the temperature-lock disclosed herein automatically maintains the sample at the same reference temperature over the course of different NMR experiments. The temperature- lock can work by continuous or non-continuous measurement of the resonance frequency of a suitable temperature-lock nucleus and simultaneous adaptation of a temperature control signal to stabilize the sample at a reference temperature value. Inter-scan periods with variable length can be used to maintain the sample at thermal equilibrium over the full length of an experiment.
摘要:
A method of projection spectroscopy for N-dimensional NMR experiments with the following steps. Data recording through; a) selection of N-dimensional NMR experiments out of a group of N-dimensional experiments, selection of the dimensionalities (Di) of the projections and unconstrained selection of j sets of projection angles, with j≧2; b) recording of discrete sets of j projections from the N-dimensional NMR experiments at the selected projection angles; c) peak picking and creating a peak list for each of the j projection spectra is characterized by d) automated identification of peaks in the projection spectra that arise from the same resonance in the N-dimensional spectrum (N≧3) using vector algebra to exploit geometrical properties of projections in the N-dimensional space, and computation of a N-dimensional peak list using vector algebra to exploit geometrical properties of projections in the N-dimensional space. A reliable method of automated projection spectroscopy without restrictions on projection angles and dimensionality is thereby realized.
摘要:
A method of projection spectroscopy for N-dimensional NMR experiments with the following steps. Data recording comprising: a) selection of N-dimensional NMR experiments out of a group of N-dimensional experiments, selection of the dimensionalities (Di) of the projections and unconstrained selection of j sets of projection angles, with j≧2; b) recording of discrete sets of j projections from the N-dimensional NMR experiments at the selected projection angles; c) peak picking and creating a peak list for each of the j projection spectra is characterized by d) automated identification of peaks in the projection spectra that arise from the same resonance in the N-dimensional spectrum (N≧3) using vector algebra to exploit geometrical properties of projections in the N-dimensional space, and computation of a N-dimensional peak list using vector algebra to exploit geometrical properties of projections in the N-dimensional space. A reliable method of automated projection spectroscopy without restrictions on projection angles and dimensionality is thereby realized.