The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.
The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.
Patent No.:
Date of Patent:
Aug. 23, 1988
Filed:
Apr. 17, 1987
Johannes H Den Boef, Eindhoven, NL;
Johannes M Van Eggermond, Bridgeport, CT (US);
Cornelis M Van Uijen, Eindhoven, NL;
U.S. Philips Corporation, New York, NY (US);
Abstract
The invention relates to a method and system for determining an image of a nuclear magnetization distribution in a body. In known methods, particularly in nuclear spin echo techniques, a resonance signal is generated which has high dynamics. In the method according to the invention dephasing is effected which is non-linear place-dependent or which is frequency-dependent within a spectroscopy distribution, as a result of which the generated resonance signal will have a much smaller amplitude. Since the non-linear dephasing applied within the distribution is known, a correction can be made for this after the determination of the measuring signals. The non-linear dephasing can be effected by means of excitation pulses and/or with subsequent nuclear spin echo pulses (also termed refocusing pulses) which have a frequency spectrum with a non-linear phase characteristic (possibly in the presence of a gradient magnetic field), or by means of a non-linear, place-dependent extra magnetic field, which can, for example, be applied during the preparation period. The non-linear extra magnetic field will preferably have higher order components, such as quadratic components. The reduction in signal dynamics to be achieved depends on the (frequency or) place-dependence of non-linear dephasing. If, for example, in an image of n.times.n pixels a non-linear, place-dependent extra magnetic field is used, which is dependent on two coordinates, then it is possible to achieve a maximum reduction in signal dynamics equal to .sqroot.n.times.n.