MR tomography method and MR tomography apparatus for performing the method

Claim 2

An MR tomography method for producing images of a plurality of slices of an object comprising: supplying a steady, uniform magnetic field in a first direction in an object imaging zone, supplying a sequence of first r-f pulses spaced apart in time for selectively and successively exciting each of said slices of said plurality by a respective first r-f pulse, thereafter supplying a sequence of second r-f pulses spaced apart in time by which the nuclear magnetization in the respective slices is rotated through 180° in the same sequence as occurred in response to said first pulses, supplying a switchable magnetic gradient field in which the gradient is perpendicular to said first direction, said magnetic gradient field being switched on and off during intervals occurring before the first and between each two of said second r-f pulses, and thereafter switching said magnetic gradient field on during a detection interval and detecting spin echo signals from each of said slices, said magnetic gradient field having amplitude and duration characteristics such that, with respect to each said slice, the time integral of said magnetic gradient field between first and second r-f pulses for said slice is substantially equal to the subsequent time integral of said magnetic gradient field between said second r-f pulse and the appearance of the spin echo signal corresponding to that slice.

Claim 3

An MR tomography method as claimed in claim 1 wherein: the time spacing between ones of said first and second r-f pulses that excite the same ones of said slices is substantially the same for each of said slices.

Claim 4

An MR tomography method as claimed in claim 1 or 2 wherein: the time integral of said magnetic gradient field between any two of sid second r-f pulses is equal to substantially one-half the integral of said gradient field between the corresponding two echo signals.

Claim 5

An MR tomography method as claimed in claim 1 or 2 wherein: the time integral of said magnetic gradient field before the first pulse of said second sequence being at least n-1 times larger than the time integral of said gradient field between two subsequent ones of said second r-f pulses in a sequence, n being the number of excited slices.

Claim 6

An MR tomography method as claimed in claim 1 or 2 wherein: between the occurrence of the last one of said first r-f pulses in a sequence and the first one of said second r-f pulses in a sequence, a further magnetic gradient field is supplied, said further magnetic gradient field having a gradient which is perpendicular to that of said switchable magnetic gradient field and an amplitude and/or duration which varies from one cycle to another.

Claim 7

An MR tomography method as claimed in claim 1 or 2 wherein: said first r-f pulses rotate the nuclear magnetization in the respective excited slice through an angle of less than 90°.

Claim 8

An MR tomography apparatus comprising: a magnet for generating a uniform steady magnetic field; an r-f coil system for generating an r-f magnetic field which extends perpendicular to said steady magnetic field; a plurality of gradient coil systems for generating magnetic fields which extend in the direction of said steady magnetic field and which have gradients which extend in different directions; an r-f generator for supplying said r-f coil system with r-f pulses having a presettable carrier frequency; generators for supplying energizing signals to said gradient coil systems; and control unit means for controlling said r-f generator and said generators for said gradient coil systems, said control unit means providing control signals to said r-f generator for supplying a sequence of first r-f pulses of different frequency spaced apart in time, and thereafter supplying a sequence of second r-f pulses spaced apart in time and having frequencies which vary from pulse to pulse in the same manner as said first r-f pulses and said control unit means further providing control signals to at least one of said gradient coil system generators for switching said one gradient coil generator on and off during intervals occurring before the first and between each two of said second r-f pulses and thereafter switching sid magnetic gradient field on during a detection interval to permit detection of spin echo signals relating to slices of a subject under investigation, said magnetic gradient field having amplitude and duration characteristics such that, with respect to each said slice, the time integral of said magnetic gradient field between first and second r-f pulses for said slice is substantially equal to the subsequent time integral of said magnetic gradient field between said second r-f pulse and the appearance of the spin echo signal corresponding to that slice.

Claim 9

An MR tomography apparatus comprising: a magnet for generating a uniform steady magnetic field; an r-f coil system for generating an r-f magnetic field which extends perpendicular to said steady magnetic field; a plurality of gradient coil systems for generating magnetic fields which extend in the direction of said steady magnetic field and which have gradients which extend in different directions; an r-f generator for supplying said r-f coil system with r-f pulses having a presettable carrier frequency; generators for supplying energizing signals to said gradient coil systems; and control unit means for controlling said r-f generator and said generators for said gradient coil systems, said control unit means providing control signals to said r-f generator for supplying a sequence of first r-f pulses of different frequency spaced apart in time, and thereafter supplying a sequence of second r-f pulses spaced apart in time and having frequencies which vary from pulse to pulse in the same manner as said first r-f pulses and said control unit means further providing control signals to at least one of said gradient coil system generators for switching said one gradient coil generator on and off during intervals occurring before the first and between each two of said second r-f pulses and thereafter switching sid magnetic gradient field on during a detection interval to permit detection of spin echo signals relating to slices of a subject under investigation, said magnetic gradient field having amplitude and duration characteristics such that, with respect to each said slice, the time integral of said magnetic gradient field between first and second r-f pulses for said slice is substantially equal to the subsequent time integral of said magnetic gradient field between said second r-f pulse and the appearance of the spin echo signal corresponding to that slice.