Method and apparatus for magnetic resonance analysis of nuclear distribution

Claim 2

In a method for the determination of the spatial and of the spectral distribution of nuclear magnetization in a region under investigation, in which, in the presence of a homogeneous steady magnetic field, a number of sequences act on the region under investigation, each sequence comprising at least one magnetic high-frequency pulse for the excitation of nuclear magnetic resonance and subsequently a plurality of periods of a magnetic gradient field (Gx) with a gradient having a periodically varying polarity, after which echo signals generated in the course of this procedure in the region under investigation are converted into digital samples and these are subjected to discrete Fourier transformation, the improvement comprising the steps of recording samples which occur when the gradient field is varying in addition to recording samples which occur when the gradient field is constant, allocating the recorded samples to the spatial frequency range and transforming the samples into the spatial range by the Fourier transformation.

Claim 3

The method according to claim 1 further comprising the steps of allocating the samples to a spatial frequency grid with equally large intervals before the Fourier transformation.

Claim 4

The method according to claim 1 further comprising the step of applying in each sequence after the high-frequency pulse a magnetic gradient field (Gy), the gradient of which extends in a direction perpendicular to the direction of the periodic gradient field (Gx) and the amplitude and/or duration of which is varied from sequence to sequence.

Claim 6

In a method for determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, in which, in the presence of a homogeneous steady magnetic field, a number of sequences act on the region under investigation, each sequence comprising at last one magnetic high-frequency pulse for the excitation of nuclear magnetic resonance and subsequently a first gradient field reversed between a positive gradient and a negative gradient, after which the echo signals generated in the course of this procedure in the region under investigation are converted into digital samples and these are subjected to a discrete Fourier transformation, the improvement comprising the steps of generating a second magnetic gradient field, the gradient of which extends perpendicular to the gradient of the first gradient field, reversing the second gradient field synchronously with the first gradient field, the variation of the temporal integral over the gradient of the second gradient field being small in comparison with the temporal integral over the resultant gradient of both gradient fields, converting echo signals occurring during a positive gradient of the first magnetic gradient field into first digital samples and converting echo signals occurring during a negative gradient of the first magnetic gradient field into second digital samples and separately subjecting said first and second digital samples to a Fourier transformation.

Claim 7

In a method for determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, in which, in the presence of a homogeneous steady magnetic field, a number of sequences act on the region under investigation, each sequence comprising at last one magnetic high-frequency pulse for the excitation of nuclear magnetic resonance and subsequently a first gradient field reversed between a positive gradient and a negative gradient, after which the echo signals generated in the course of this procedure in the region under investigation are converted into digital samples and these are subjected to a discrete Fourier transformation, the improvement comprising the steps of generating a second magnetic gradient field, the gradient of which extends perpendicular to the gradient of the first gradient field, reversing the second gradient field synchronously with the first gradient field, the variation of the temporal integral over the gradient of the second gradient field being small in comparison with the temporal integral over the resultant gradient of both gradient fields, converting echo signals occurring during a positive gradient of the first magnetic gradient field into first digital samples and converting echo signals occurring during a negative gradient of the first magnetic gradient field into second digital samples and separately subjecting said first and second digital samples to a Fourier transformation.

Claim 8

The method according to claim 5, wherein during the reversal phase of the first magnetic gradient field the second gradient field is applied with polarity alternating from reversal phase to reversal phase, its gradient being small in comparison with the gradient of the first gradient field.

Claim 9

In an arrangement for carrying out a method for the determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, said arrangement having a magnet for the generation of a homogeneous steady magnetic field, a high-frequency coil for the generation of high-frequency excitation pulses, gradient coils for the generation of magnetic gradient fields with gradients extending in differing directions, a control arrangement for the control of the temporal progression of the fields generated by the gradient coils, an analog to digital converter arrangement for the generation of digital samples from echo signals, a memory for receiving the samples and a computer for carrying out a Fourier transformation with the samples, the improvement comprising the control arrangement (15) controlling at least one of the gradient coils (7) to generate a periodic magnetic field (Gx) with a temporal progression of non-quadrangular form, controlling the analog to digital converter arrangement (65, 66) to generate digital samples during the periods of time with a non-constant gradient from the echo signals (E1, E3 . . . ), store the digital samples in the memory and further comprising means (19) for converting the sequence of the digital samples into a sequence of values (F(kx, . . . )) which is equidistant in the spatial frequency range, which values are fed to the computer for the Fourier transformation from the spatial frequency range into the spatial range.

Claim 10

In an arrangement for carrying out a method for the determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, said arrangement having a magnet for the generation of a homogeneous steady magnetic field, a high-frequency coil for the generation of high-frequency excitation pulses, gradient coils for the generation of magnetic gradient fields with gradients extending in differing directions, a control arrangement for the control of the temporal progression of the fields generated by the gradient coils, an analog to digital converter arrangement for the generation of digital samples from echo signals, a memory for receiving the samples and a computer for carrying out a Fourier transformation with the samples, the improvement comprising the control arrangement (15) controlling at least one of the gradient coils (7) to generate a periodic magnetic field (Gx) with a temporal progression of non-quadrangular form, controlling the analog to digital converter arrangement (65, 66) to generate digital samples during the periods of time with a non-constant gradient from the echo signals (E1, E3 . . . ), store the digital samples in the memory and further comprising means (19) for converting the sequence of the digital samples into a sequence of values (F(kx, . . . )) which is equidistant in the spatial frequency range, which values are fed to the computer for the Fourier transformation from the spatial frequency range into the spatial range.

Claim 11

In an arrangement for carrying out a method for the determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, said arrangement having a magnet for the generation of a homogeneous steady magnetic field, a high-frequency coil for the generation of high-frequency excitation pulses, gradient coils for the generation of magnetic gradient fields with gradients extending in differing directions, a control arrangement for the control of the temporal progression of the fields generated by the gradient coils, an analog to digital converter arrangement for the generation of digital samples from echo signals, a memory for receiving the samples and a computer for carrying out a Fourier transformation with the samples, the improvement comprising the control arrangement (15) mutually synchronously periodic gradient fields are generated by two gradient coils (5, 7) and in that the computer for carrying out the Fourier transformation is dimensioned in such a manner that the digital samples of every second echo signal on the one hand and the digital samples of the remaining echo signals on the other hand are processed separately.

Claim 12

In an arrangement for carrying out a method for the determination of the spatial and of the spectral distribution of the nuclear magnetization in a region under investigation, said arrangement having a magnet for the generation of a homogeneous steady magnetic field, a high-frequency coil for the generation of high-frequency excitation pulses, gradient coils for the generation of magnetic gradient fields with gradients extending in differing directions, a control arrangement for the control of the temporal progression of the fields generated by the gradient coils, an analog to digital converter arrangement for the generation of digital samples from echo signals, a memory for receiving the samples and a computer for carrying out a Fourier transformation with the samples, the improvement comprising the control arrangement (15) mutually synchronously periodic gradient fields are generated by two gradient coils (5, 7) and in that the computer for carrying out the Fourier transformation is dimensioned in such a manner that the digital samples of every second echo signal on the one hand and the digital samples of the remaining echo signals on the other hand are processed separately.

Claim 13

Arrangement according to one of claims 7 or 8, wherein the control arrangement is designed in such a manner that the temporal interval between the high-frequency excitation pulse and the switched-on period of the periodic gradient field is variable by the value T/n, where n is an integer and T is the period of the gradient field.