๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Relaxation of AB Spin Systems in Stimulated-Echo Spectroscopy

โœ Scribed by Klaus Straubinger; Fritz Schick; Otto Lutz


Publisher
Elsevier Science
Year
1995
Tongue
English
Weight
233 KB
Volume
109
Category
Article
ISSN
1064-1866

No coin nor oath required. For personal study only.

โœฆ Synopsis


The behavior of the strongly coupled AB spin system during as analytical functions, incorporating all parameters as varithe STEAM (stimulated echo acquisition mode) sequence was calables. It is possible to evaluate how changing parameters culated analytically. Relaxation during the TM interval, in which (chemical-shift difference, coupling constant, sequence timlongitudinal magnetization and zero-quantum coherences (ZQCs) ing, etc.) affects spectra and signal intensities. occur, was accounted for by following the course of the different density-matrix terms. The result allows one to determine sequence THEORY timings to provide high signal intensities or signals resulting from certain coherences. Theoretically calculated spectra can be gener-Basics and Software ated, using an analytical function. Series of proton spectra were recorded from a 0.1 m aqueous solution of citrate on a 1.5 T whole-

The time evolution of strongly coupled spin systems can body imager at 22ะŠC. Spectra series with constant echo time TE be calculated by density-operator theory (10,11). The mawere used to evaluate the longitudinal relaxation time T 1 as well trix form of the spin operators (12, 13) was used, because as the zero-quantum relaxation time T ZQ by fitting the theoretically it was found to be better adapted for treatment by computer predicted curve to the experimental data. The evaluated proton algebra than the AB-system product-operator formalism relaxation times T 1 and T ZQ in citrate differ strongly: T 1 ร… 770 (14). The resulting density matrix was converted to the ms, T ZQ ร… 1300 ms.


๐Ÿ“œ SIMILAR VOLUMES


Measurement of Spin-Lattice Relaxation T
โœ Max S. Lin ๐Ÿ“‚ Article ๐Ÿ“… 1984 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 489 KB ๐Ÿ‘ 1 views

Calculation of tissue TI in double spin-echo imaging (90"-T-I 80"-2T-1 SO0) using two repetition times (6, and b2) has entailed an approximation that ignores the two 180" pulses. The theoretical consequence of the simplification is to overestimate TI with a fractional error that increases with incre

The Nonlinear Stimulated Echo in the Pre
โœ I. Ardelean; R. Kimmich; S. Stapf; D.E. Demco ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 161 KB

The classical treatment is opposed by the macroscopic gradients at high magnetic fields (โ„ข7 T) produces multiple nonlinquantum-theoretical approach trying to describe short-as ear stimulated echoes (NOSE) at times n t 1 after the third pulse, well as long-range dipolar interactions on a purely quant

Selective Storage of Magnetization in St
โœ M.L. Kilfoil; P.T. Callaghan ๐Ÿ“‚ Article ๐Ÿ“… 2001 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 309 KB

We have investigated the use of a "split-sinc" RF pulse to selectively store magnetization from a selected region of a sample, for later recall in imaging or spectroscopy experiments. The pulse sequence is based on an original suggestion by Post et al. (West German Patent No. P3209263.6, 13 March 19

Modified stimulated echo sequence for el
โœ H. Lahrech; A. Briguet; D. Graveron-Demilly; E. Hiltbrand; P. R. Moran ๐Ÿ“‚ Article ๐Ÿ“… 1987 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 297 KB

Simple modification of the basic stimulated echo sequence (MSTE), including bipolar gradient modulation, permits one to generate relative motion phase modulations between the two STE magnetization components. It is shown how this self-referencing process can provide flow enhancement without combinat