Abstract: An MR measuring assembly (3) with an MR device (2) is provided, which has a main magnet (4) generating a stray magnetic field and a platform (1), having a side border (5), on which the MR device (2) is placed. The border (5) marks an iso-contour surface of the stray field at a specified magnetic field strength. The platform (1) therefore forms a natural barrier that prevents people or objects being exposed to magnetic field strengths that are too high. To this end provision is additionally made, in accordance with the invention, for a step (15) for the marking of an iso-contour surface of a stray magnetic field of an MR device (2) at a specified magnetic field to be used.

Abstract: An MR measuring assembly (3) with an MR device (2) is provided, which has a main magnet (4) generating a stray magnetic field and a platform (1), having a side border (5), on which the MR device (2) is placed. The border (5) marks an iso-contour surface of the stray field at a specified magnetic field strength. The platform (1) therefore forms a natural barrier that prevents people or objects being exposed to magnetic field strengths that are too high. To this end provision is additionally made, in accordance with the invention, for a step (15) for the marking of an iso-contour surface of a stray magnetic field of an MR device (2) at a specified magnetic field to be used.

Abstract: A PET examination which acquires a data record of the body of a patient is carried out during at least one embodiment of a method for acquiring measured data. On the basis of the measured values of the data record, at least one region of interest in the body of the patient is determined, in which at least one examination of at least one embodiment of a method is carried out.

Abstract: In a method and apparatus for detection improvement of a weakly-sensitive atomic nucleus type in MR spectroscopy data acquisition using polarization transfer for a weakly-sensitive atomic nucleus type (A) with involvement of an MR-active, strongly-sensitive atomic nucleus type (X), all RF pulses are radiated sequentially, i.e. with defined time interval relative to one another, such that at no point in time of the sequence are different RF pulses radiated simultaneously or overlapping, and the sequence of the RF pulses causes a polarization transfer of the two involved atomic nucleus types (A), (X).

Abstract: In a method for dynamic frequency detection of the resonance frequency in magnetic resonance spectroscopy, by measuring navigator signals at the same point in time in each of a number of successive sequence passes, and by comparing the navigator signals, a frequency shift of the resonance frequency is determined on the basis of which the respective individual spectrum obtained from each sequence repetition is corrected with respect to the measured frequency shift.

Abstract: In a hybrid CSI procedure for a magnetic resonance device, for a predeterminable volume of interest of the hybrid CSI procedure, the magnetic resonance device automatically defines an increased volume that exceeds the volume of interest such that all magnetic resonance signal-emitting substances of interest contained in the volume of interest are excited in order to create the magnetic resonance signals to be evaluated spectroscopically, and a saturation volume directly adjoining the volume of interest is automatically defined and saturated before the excitation by the magnetic resonance device such that no unwanted magnetic resonance signals are created from outside the volume of interest.