Abstract A two-dimensional nuclear magnetic resonance spectrometry which comprises the following steps to facilitate phase correction: (a) taking the Fourier transform of the set S(t 1 , t 2 ) of the free induction decay signals with respect to t 2 to generate the transformed data sets of S c (t 1 , F 1 ) or S s (t 1 , F 2 ), the signals being stored in the memory corresponding to the values of t 1 ; (b) obtaining data S c (t 1000 , F 2 ) and S s (t 1000 , F 2 ) whose phases have been shifted by phase angle θ 2 , from the initial data S c (t 1000 , F 2 ) and S s (t 1000 , F 2 ) contained in two Fourier components S c (t 1 , F 2 ) and S s (t 1 , F 2 ) derived by the Fourier transformation made in the step (a), in such a way that the peak contained in the initial data S c (t 1000 , F 2 ) and S s (t 1000 , F 2 ) takes an absorption or dispersion waveform to make phase correction; (c) shifting the phases of the data in the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) derived in the step (b) by phase angle θ 1 to make phase correction with respect to t 1 ; and (d) taking the Fourier transform of the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) with respect to t 1 .
A method of two-dimensional nuclear magnetic resonance spectrometry comprising the steps of: (a) applying a radio-frequency pulse train to a sample containing gyromagnetic resonators, the pulse train consisting of a plurality of radio-frequency pulses; (b) detecting the free induction decay after the end of the application of the radio-frequency pulse train and storing it in a memory; (c) repeating the steps (a) and (b) with different values of evolution period t 1 that is defined as the pulse separation between certain two pulses of the radio-frequency pulse train to generate the data set S(t 1 , t 2 ) of the free induction decay signals, the initial value of t 1 being identified as t 1000 ; (d) taking the Fourier transform of the set S(t 1 , t 2 ) of the free induction decay signals with respect to t 2 to generate the transformed data set S c (t 1 , F 2 ) or S s (t 1 , F 2 ); (e) obtaining phase angle θ 2 for phase shifting interferograms defined by t 1 values corresponding to selected F 2 values in the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) so that each peak in the interferograms corresponding to peaks in the spectrums S c (t 1000 , F 2 ) and S s (t 1000 , F 2 ) takes an absorption or dispersion waveform; (f) shifting the phases of all the data in data sets S c (t 1 , F 2 ) or S 2 (t 1 , F 2 ) derived in the step (d) by phase angles θ 2 to make phase correction; and (g) shifting the phases of all the data in data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) derived in the step (f) by phase angles θ 1 to make phase correction with respect to t 1 , and then taking the Fourier transform of the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) with respect to t 1 .
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A method of two-dimensional nuclear magnetic resonance spectrometry comprising the steps of: (a) applying a radio-frequency pulse train to a sample containing gyromagnetic resonators, the pulse train consisting of a plurality of radio-frequency pulses; (b) detecting the free induction decay after the end of the application of the radio-frequency pulse train and storing it in a memory; (c) repeating the steps (a) and (b) with different values of evolution period t 1 that is defined as the pulse separation between certain two pulses of the radio-frequency pulse train to generate the data set S(t 1 , t 2 ) of the free induction decay signals, the initial value of t 1 being identified as t 1000 ; (d) taking the Fourier transform of the set S(t 1 , t 2 ) of the free induction decay signals with respect to t 2 to generate the transformed data set S c (t 1 , F 2 ) or S s (t 1 , F 2 ); (e) obtaining phase angle θ 2 for phase shifting interferograms defined by t 1 values corresponding to selected F 2 values in the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) so that each peak in the interferograms corresponding to peaks in the spectrums S c (t 1000 , F 2 ) and S s (t 1000 , F 2 ) takes an absorption or dispersion waveform; (f) shifting the phases of all the data in data sets S c (t 1 , F 2 ) or S 2 (t 1 , F 2 ) derived in the step (d) by phase angles θ 2 to make phase correction; and (g) shifting the phases of all the data in data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) derived in the step (f) by phase angles θ 1 to make phase correction with respect to t 1 , and then taking the Fourier transform of the data sets S c (t 1 , F 2 ) or S s (t 1 , F 2 ) with respect to t 1 .