Abstract: In a computer-implemented method for setting a field of view for a magnetic resonance scan, exclusion information describing a region of the original field of view that is unmapped owing to the distortion is ascertained on the basis of the distortion map for at least one first set of field-of-view parameters describing a rectangular or cuboidal original field of view, the exclusion information is used to determine a second set of field-of-view parameters to be used for the magnetic resonance scan, and the magnetic resonance scan is performed using the second set of field-of-view parameters.

Abstract: In a method and system for the generation of measurement data required k-space is read out in the readout direction in k-space rows such that at least a first k-space row of the k-space rows does not cover the k-space to be read out in the readout direction in full and at least a second k-space row of the k-space rows covers the k-space to be read out in locations in the readout direction at which the first k-space row does not cover the k-space to be read out. Measurement data that is missing in the k-space is completed in this way on the basis of recorded echo signals stored as measurement data.

Abstract: A computer-implemented method for determining a subset of coil elements for capturing a magnetic resonance tomography recording, comprises: providing a target volume in a scout view, and determining a plurality of subsets of coil elements from among the plurality of coil elements, wherein individual subsets are configured different from one another. The method further comprises: determining at least one quality criterion for each subset of coil elements, wherein the at least one quality criterion of a corresponding subset of coil elements relates to an image quality in the target volume, dependent upon the corresponding subset of coil elements; determining the subset of coil elements from the plurality of subsets, based on the corresponding at least one quality criterion; and providing an information item regarding which of the plurality of coil elements are included by the subset of coil elements.

Abstract: A computer-implemented method for determining correct operation of a receiving system of a magnetic resonance device using of a magnetic resonance measurement, by: acquiring a magnetic resonance image using the receiving system during the magnetic resonance measurement, determining a noise distribution of the acquired magnetic resonance image by means of a computing unit, and determining correct operation of the receiving system by means of the computing unit on the basis of the noise distribution. Also, a magnetic resonance device, having a computing unit which is designed to coordinate the computer-implemented method and execute the by means of the magnetic resonance device.

Abstract: A method is provided for the saturation-prepared recording of MR image data. The method includes establishment of at least two measurement slices in an examination volume of an examination object, wherein the examination volume has adjacent slices which each adjoin at least one of the at least two measurement slices; output of a saturation module including at least one saturation pulse for saturating a magnetization of the adjacent slices; output of an excitation pulse for exciting a magnetization of at least one of the at least two measurement slices; readout of an MR signal of the examination volume; reconstruction of the MR image data from the at least two measurement slices based on the MR signal; and provision of the MR image data. The disclosure further relates to a magnetic resonance system and a computer program product.

Abstract: In a computer-implemented method for setting a field of view for a magnetic resonance scan, exclusion information describing a region of the original field of view that is unmapped owing to the distortion is ascertained on the basis of the distortion map for at least one first set of field-of-view parameters describing a rectangular or cuboidal original field of view, the exclusion information is used to determine a second set of field-of-view parameters to be used for the magnetic resonance scan, and the magnetic resonance scan is performed using the second set of field-of-view parameters.

Abstract: High-quality magnetic resonance (MR) recordings are triggered with movements of an object, for example the heartbeat. In a method and apparatus for obtaining raw data reconstruction for an MR image, a spin-echo-based sequence is executed that includes applying a static magnetic field and applying a magnetization pulse train. A movement of the object to be imaged is detected and a target contrast for two tissue types of the object is prespecified. The repetition time of the pulse train is set in dependence on the movement of the object to be imaged, and the flip angle is set such that prespecified target contrast for the two tissue types is obtained at the set repetition time.

Abstract: In a method and system for the generation of measurement data required k-space is read out in the readout direction in k-space rows such that at least a first k-space row of the k-space rows does not cover the k-space to be read out in the readout direction in full and at least a second k-space row of the k-space rows covers the k-space to be read out in locations in the readout direction at which the first k-space row does not cover the k-space to be read out. Measurement data that is missing in the k-space is completed in this way on the basis of recorded echo signals stored as measurement data.

Abstract: A method is provided for the saturation-prepared recording of MR image data. The method includes establishment of at least two measurement slices in an examination volume of an examination object, wherein the examination volume has adjacent slices which each adjoin at least one of the at least two measurement slices; output of a saturation module including at least one saturation pulse for saturating a magnetization of the adjacent slices; output of an excitation pulse for exciting a magnetization of at least one of the at least two measurement slices; readout of an MR signal of the examination volume; reconstruction of the MR image data from the at least two measurement slices based on the MR signal; and provision of the MR image data. The disclosure further relates to a magnetic resonance system and a computer program product.

Abstract: In order to optimize magnetic resonance (MR) images in spin echo-based imaging, MR raw data are acquired by applying a static magnetic field, an excitation pulse, a refocusing pulse, and an RF pulse at the same time point as an echo elicited by the pulses with the result that the magnetization in the negative z-direction is deflected by a flip angle. The flip angle is selected such that, given a specified repetition time of the excitation pulse, a predetermined contrast is provided for two specified tissue types of the subject to be imaged. An MR image is reconstructed from the acquired MR raw data.

Abstract: High-quality magnetic resonance (MR) recordings are triggered with movements of an object, for example the heartbeat. In a method and apparatus for obtaining raw data reconstruction for an MR image, a spin-echo-based sequence is executed that includes applying a static magnetic field and applying a magnetization pulse train. A movement of the object to be imaged is detected and a target contrast for two tissue types of the object is prespecified. The repetition time of the pulse train is set in dependence on the movement of the object to be imaged, and the flip angle is set such that prespecified target contrast for the two tissue types is obtained at the set repetition time.

Abstract: In order to optimize magnetic resonance (MR) images in spin echo-based imaging, MR raw data are acquired by applying a static magnetic field, an excitation pulse, a refocusing pulse, and an RF pulse at the same time point as an echo elicited by the pulses with the result that the magnetization in the negative z-direction is deflected by a flip angle. The flip angle is selected such that, given a specified repetition time of the excitation pulse, a predetermined contrast is provided for two specified tissue types of the subject to be imaged. An MR image is reconstructed from the acquired MR raw data.

Abstract: A magnetic resonance (MR) tomography apparatus has an array composed of a number n of single coils Ei to acquire reception signals Ii. The tomography apparatus is operated by a method that includes the following steps. For each single coil Ei, a processor determines, or is provided with, an individual reception sensitivity profile in positional space r B1i?(r). An examination subject introduced into the MR tomography apparatus is scanned to acquire reception signals Ii(k) in the frequency domain with the n reception coils Ei. Fourier-transformed signals IFi(r) are determined from the reception signals Ii(k). Complexly corrected signals ?Fi(r) are determined on the basis of the signals IFi(r) and the individual reception sensitivity profiles B1i?(r). A sum signal MR(r) is determined by complex addition of the corrected signals ?Fi(r). Image data of the examination subject are reconstructed on the basis of the sum signal MR(r).

Abstract: A method for controlling a magnetic resonance system outputs a pulse sequence including a first slice-selective excitation pulse that excites a first slice with a first magnetization. The pulse sequence includes a second slice-selective excitation pulse that excites a second slice with the first magnetization and a third slice-selective excitation pulse that excites the first slice with a second magnetization that cancels the first magnetization. The pulse sequence also includes and a fourth slice-selective excitation pulse that excites the second slice with a magnetization that cancels the first magnetization. The first slice and the second slice intersect.

Abstract: A magnetic resonance RF field is produced in a magnetic resonance imaging system that includes a main magnetic field apparatus and an object-bearing table movable relative to the main magnetic field apparatus and on which a local coil system is arranged. The local coil system includes a plurality of transmission elements. A current location of the object-bearing table relative to the main magnetic field apparatus is established. The transmission elements are automatically connected based on the current location of the object-bearing table.

Abstract: In a method and apparatus for acquiring magnetic resonance image data of an object by execution of a magnetic resonance data acquisition sequence that includes at least one adiabatic radio-frequency pulse, at least one parameter for the object under investigation is acquired that is specific to the object under investigation. At least one pulse parameter of the at least one adiabatic radio-frequency pulse is adjusted using the at least one parameter for the object under investigation. Magnetic resonance image data of the object under investigation are acquired by execution of the magnetic resonance sequence, using the at least one adiabatic radio-frequency pulse with the adjusted at least one pulse parameter.

Abstract: A method for operating a transmission device of a magnetic resonance device is provided. In order to actuate coil elements of a radiofrequency coil with different phases, phase differences in a reference plane are taken into consideration. In a first calibration measurement to be performed once for each transmission path, a first phase of a transmitted radiofrequency signal is measured by an internal measuring device installed permanently in the transmission device spaced apart from the reference plane. A second phase of the transmitted radiofrequency signal is measured by a second, external measuring device to be connected to the reference plane for the first calibration measurement. At least one phase of the first phase and the second phase is taken into consideration in the phase-accurate actuating of the coil elements and/or for correcting further measurements with the internal measuring device.

Abstract: In a magnetic resonance facility and operating method for acquiring image data of a patient in a manner defined by acquisition parameters, the acquisition of the image data is preceded by the performance of at least one alignment operation for adjusting operating parameters of the magnetic resonance facility that influence acquisition conditions for the current patient. At least one result data item describing the result of the alignment used for an at least partially automatic determination of at least one acquisition parameter not relating to the pulse shape of a radio-frequency pulse to be used during the acquisition.

Abstract: A method for the adjustment of at least one magnetic resonance image data set of a movable examination object and correspondingly designed magnetic resonance device is provided. Moreover, a method, a computer program product and a computer-readable storage medium for the adjustment by a magnetic resonance device of at least one magnetic resonance image data set of a movable examination object is provided. After capturing two different types of position data for determination of the position of the examination object using navigator measurements and with the help of external markers, recording parameters and/or reconstruction parameters for recording and/or reconstruction of the at least one magnetic resonance image data set are adjusted as a function of the first and/or the second position data.

Abstract: In a method to determine a B1 phase map for at least two excitation modes of a radio-frequency coil arrangement of a magnetic resonance apparatus, the radio-frequency coil arrangement having multiple independently controllable transmission channels, and the B1 phase map describing, with spatial resolution, the phase of radio-frequency field this is generated in a respective excitation mode relative to a common reference phase map, first magnetic resonance data describing the phase change of a basic magnetic field of the magnetic resonance apparatus between a first echo time and a second echo time are acquired, and are evaluated to determine a spatially resolved Larmor frequency value that describes the deviation from a nominal Larmor frequency of the magnetic resonance apparatus.