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US4789832A Expired / Lapsed US ⏱️ 0.0 years remaining

Three-dimensional NMR spectroscopy

Assignee: Jeol Ltd
•
Filing: 1988-01-12
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Granted: 1988-12-06
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Expires: 2008-01-12
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Abstract

Abstract A three-dimensional NMR spectroscopy capable of obtaining a plurality of two-dimensional NMR spectra by a single series of measurements. In this spectroscopy, a pulse sequence consisting of three 90°-pulses and a 180°-pulse is utilized. The three 90°-pulses are produced at intervals. The interval between the second and the third 90°-pulses is set to τ m . The 180°-pulse is produced at the middle of the interval τ m . In a first embodiment of the invention, the interval t 1 between the first and the second 90°-pulses and the RF phases φ of the first and second 90°-pulses and of the 180°-pulse are taken as variables. The free induction decay signals produced after the lapse of a period of t 2 subsequent to the third 90°-pulse are collected to create data S (t 1 , t 2 , φ). In a second embodiment of the invention, the intervals t 1 and τ m are taken as variables, τ m being rewritten as t 3 . The free induction decay signals produced during the period t 2 are collected to create data S (t 1 , t 2 , t 3 ). The data of either kind is subjected to complex Fourier transformation with respect to t 1 and t 2 and then to cosine Fourier transformation with respect to φ or t 3 to obtain a three-dimensional NMR spectrum S (ω 1 , ω 2 , p) or S (ω 1 , ω 2 , J) made up of plural 2D NMR spectra.

Inventors

  • 👤 Kuniaki Nagayama

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-07 15:20
CPC Classifications
G; G01; G01R; G01R33/00; G01R33/20; G01R33/44; G01R33/46; G01R33/4633

Claims Analysis

Total Claims: 6
Claim 1
Independent Claim 261 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of T m that follows the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of T m ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and a second pulse train parameter X, obtaining the sum S (t 1 , t 2 , X) of the resulting free induction decay signals, and storing the data in the memory; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , X) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , X) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , X) with respect to X to obtain a spectrum S (ω 1 , ω 2 , Y).
Claim 2
Dependent Claim 261 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of T m that follows the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of T m ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and a second pulse train parameter X, obtaining the sum S (t 1 , t 2 , X) of the resulting free induction decay signals, and storing the data in the memory; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , X) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , X) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , X) with respect to X to obtain a spectrum S (ω 1 , ω 2 , Y).
Claim 3
Dependent Claim 269 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of τ m that follows the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of τ m ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and the RF phases φ of the first 90°-pulse, the second 90°-pulse, and the 180°-pulse, obtaining the sum S (t 1 , t 2 , φ) of the resulting free induction decay signals, and storing the data in the memory; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , φ) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , φ) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , φ) with respect to φ to obtain a spectrum S (ω 1 , ω 2 , p).
Claim 4
Dependent Claim 269 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of τ m that follows the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of τ m ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and the RF phases φ of the first 90°-pulse, the second 90°-pulse, and the 180°-pulse, obtaining the sum S (t 1 , t 2 , φ) of the resulting free induction decay signals, and storing the data in the memory; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , φ) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , φ) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , φ) with respect to φ to obtain a spectrum S (ω 1 , ω 2 , p).
Claim 5
Dependent Claim 265 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of t 3 after the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of t 3 ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and the length t 3 of the mixing period and obtaining the sum S (t 1 , t 2 , t 3 ) of the resulting free induction decay signals; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , t 3 ) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , t 3 ) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , t 3 ) with respect to t 3 to obtain a spectrum S (ω 1 , ω 2 , J).
Claim 6
Dependent Claim 265 words
A three-dimensional nuclear magnetic resonance spectroscopy comprising the steps of: (a) applying a first 90°-pulse to a sample containing gyromagnetic resonators after the lapse of a given preparation period; (b) applying a second 90°-pulse to the sample after the lapse of an evolution period of t 1 that follows the application of the first 90°-pulse; (c) applying a 180°-pulse to the sample at the middle of a mixing period of t 3 after the application of the second 90°-pulse and applying a third 90°-pulse to the sample after the mixing period of t 3 ; (d) detecting the free induction decay signal emanating from the resonators during a detection period of t 2 that follows the application of the third 90°-pulse and storing the obtained data in a memory; (e) carrying out the steps (a)-(d) while systematically varying the length t 1 of the evolution period and the length t 3 of the mixing period and obtaining the sum S (t 1 , t 2 , t 3 ) of the resulting free induction decay signals; (f) taking the complex Fourier transform of the data S (t 1 , t 2 , t 3 ) with respect to t 2 ; (g) taking the complex Fourier transform of the transformed data S (t 1 , ω 2 , t 3 ) with respect to t 1 ; and (h) taking the cosine Fourier transform of the transformed data S (ω 1 , ω 2 , t 3 ) with respect to t 3 to obtain a spectrum S (ω 1 , ω 2 , J).

References Cited (Backward Citations)

US4134058A Cited
US4510449A Cited
US4513247A Cited
US4520316A Cited
US4626783A Cited
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