Patent ID: 12248044

DETAILED DESCRIPTION OF THE DISCLOSURE

FIG.1shows a schematic flow diagram of a method according to the disclosure for establishing permitted gradient intensities Geon physical gradient axes of a gradient unit of a magnetic resonance system1during a recording, with the magnetic resonance system1, of scan data MD from an examination object U situated in a scan volume of said magnetic resonance system1.

An examination protocol P, with which scan data is to be recorded, is loaded (block101). The examination protocol comprises an examination target which establishes which data is to be recorded from where, and can specify at least one pulse sequence to be used during the recording of the scan data MD.

A list L(K-G) of at least three rotation classes is loaded (block103), wherein associated with each rotation class K is a rotation range RB(K) lying between a minimum rotation angle R1 and a maximum rotation angle R2, wherein the rotation ranges RB(K) of the rotation classes K do not overlap, and all the rotation classes K with their rotation ranges RB(K) altogether cover the entire region lying between the minimum rotation angle R1 and the maximum rotation angle. Associated herein with each rotation class K is a permitted gradient intensity G for this rotation class K.

The minimum rotation angle R1 can be a rotation angle of 0°. This corresponds to a (strict) axial orientation along a physical gradient axis. The maximum rotation angle R2 can be a rotation angle of 45°. This corresponds to a maximum deviation from a physical gradient axis. With a selection of this type, an overall possible region of rotation angles is covered by the rotation classes.

Herein, in a simple case, the rotation ranges RB(K) of the rotation classes K can each cover equal-sized angular ranges of the region between the minimum rotation angle R1 and the maximum rotation angle R2. Thus, an equidistant coverage of the full region between the minimum rotation angle R1 and the maximum rotation angle R2 can be achieved.

Another distribution of the region between the minimum rotation angle R1 and the maximum rotation angle R2 into the rotation classes K is conceivable, for example, also with any desired steps in the coverage of the region between the minimum rotation angle R1 and the maximum rotation angle R2 through the rotation ranges RB(K) of the rotation classes K.

For example, the rotation class K, the rotation range RB(K) of which comprises the minimum rotation angle R1 can include exactly the minimum rotation angle R1 as the rotation range RB(K). Thus, a gradient intensity G associated with the rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R1 would be permitted precisely for fields of view with a strictly axial orientation along the physical gradient axis.

The rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R1 can, however, also be selected somewhat more generously and includes, for example, as the rotation range RB(K), a region from the minimum rotation angle R1 to an angle of a half, one, or three, not more than five degrees removed from the first rotation angle, etc. Similarly, the rotation range RB(K) of the rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R1 which covers, starting from the minimum rotation angle R1, approximately one, two or nine, not more than eleven percent of the region between the minimum rotation angle R1 and the maximum rotation angle R2 could be selected as the rotation range RB(K), etc.

Similarly, the rotation class K, the rotation range RB(K) of which comprises the maximum rotation angle R2, can include exactly the maximum rotation angle R2 as the rotation range RB(K). Thus, a gradient intensity G associated with the rotation class K, the rotation range RB(K) of which includes the maximum rotation angle R2, would be permitted precisely for fields of view with an orientation maximally rotated away from the physical gradient axis.

The rotation class K, the rotation range RB(K) of which includes the maximum rotation angle R2 can, however, also be selected somewhat more generously and includes, for example, as the rotation range RB(K), a region from the maximum rotation angle R2 to an angle of a half, one, three or a maximum of five degrees removed from the first rotation angle, etc. Similarly the rotation angle RB(K) of the rotation class K, the rotation range RB(K) of which includes the maximum rotation angle R2 which covers, starting from the minimum rotation angle R1, approximately one, two or nine, not more than eleven percent of the region between the minimum rotation angle R1 and the maximum rotation angle R2 can be selected as the rotation range RB(K), etc.

As the gradient intensity G, a maximum specified gradient intensity of the gradient unit can be associated with the rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R1. It is thus established that for this rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R1, the full maximum specified gradient intensity can be used.

As the gradient intensity G, a maximum specified gradient intensity of the gradient unit divided by the value of the square root of the number three can be associated with the rotation class K, the rotation range of which includes the maximum rotation angle. It is thus established that for this rotation class K, the rotation range RB(K) of which includes the minimum rotation angle R2, only a usable maximum gradient intensity determined by the convention KV can be used.

For a rotation class K, the rotation range RB(K) of which includes neither the minimum rotation angle R1 nor the maximum rotation angle R2, as the permitted gradient intensity G, a gradient intensity can be assigned which lies between the maximum specified gradient intensity of the gradient unit and the maximum specified gradient intensity of the gradient unit divided by the value of the square root of the number three. For example, a gradient intensity associated with a rotation class K, the rotation range RB(K) of which includes neither the minimum rotation angle R1 nor the maximum rotation angle R2, can be determined according to a spacing of the rotation range RB(K) from the minimum rotation angle R1 and/or from the maximum rotation angle R2, from the maximum specified gradient intensity and/or from the scaled gradient intensity determined from the usable maximum gradient intensity by the convention KV.

Associated with each of the rotation classes K are gradient intensities G that are determined such that they lead to an overloading on a physical gradient axis for no rotation R that is included in the rotation range RB(K). A determination of such gradient intensities G associated with the rotation classes K can take place, similarly to the convention KV, on the basis of geometric considerations. Alternatively, the gradients G associated with the rotation classes K can be somewhat less strictly determined in that, at the most, for a low percentage of not more than 1% of the rotations included in the rotation range of the rotation class, for example, an overloading can occur on a physical gradient axis. Thus the probability of an overloading is at least very low and a still better utilization of the gradient intensities can take place.

The list L(K-G) loaded can comprise, for example, at least six rotation classes K. The more rotation classes K that are included in the list L(K-G), the higher is the flexibility achievable through the use of the list L(K-G) in the optimization of the utilization of the gradient intensity. However, as the number of rotation classes increases, the complexity of the determination of the maximum permitted gradient intensities Ge and the adaptation to be performed of the parameters of the pulse sequence used according to the determined maximum permitted gradient intensity Gealso increases.

A field of view FOV of the examination object U, from which scan data MD is to be recorded, is established (block105). Therein, the orientation of the field of view FOV relative to the physical gradient axes is simultaneously established.

The establishing of the field of view FOV can be undertaken by a user N who, for example, positions a desired field of view in a previously recorded scout view of the examination object and for example orients it along structures in the examination object that are desired to be represented, and so establishes it as the field of view FOV to be used. A user can herein be notified that a user-established orientation of the field of view FOV relative to the physical gradient axes influences a scan duration required for the recording of the scan data MD. It can be offered to the user optionally, for example, to leave the orientation of the field of view FOV fixed along the physical gradient axes in order to achieve a shorter scan duration.

It is also conceivable that the field of view FOV of the examination object U is established dependent upon the loaded examination protocol P. For instance, an orientation of the field of view FOV can already be established by way of the loaded examination protocol P, but also a position of a field of view FOV can be specified, for example, as central in a scan volume of the magnetic resonance system1.

For example, for examination protocols P for which, for the underlying clinical objective, no specific orientation of the field of view FOV is required, a strictly axial orientation of the field of view FOV to the physical gradient axes can be established by way of the examination protocol P. This is, for example, often the case for recordings of scan data in an abdominal region of a patient as the examination object U, since then in any event a great deal of anatomy is examined with different orientations. In this way, it is ensured that a required scan duration is kept as short as possible without impairing the quality of the recorded scan data MD. For example, recordings of scan data in an abdominal region of a patient as the examination object U are often time-critical and benefit from shortened scan durations, especially if a patient must hold his breath for the recording.

A rotation that describes a relative position of logical gradient axes established by way of the orientation of the field of view to the physical gradient axes of the gradient unit is determined (block107). Techniques and mathematical operations used for this purpose are known.

Maximum permitted gradient intensities Ge for the loaded protocol are established dependent upon the rotation as determined and using the loaded list of rotation classes (block109).

To achieve this, it can be determined in which of the rotation classes K of the list L(K-G) the determined rotation R lies, and the gradient intensity G associated with this rotation class K as the maximum permitted gradient intensity Geis automatically established.

Using the examination protocol P, and with the established maximum permitted gradient intensities Ge, scan data MD is recorded from the field of view FOV of the examination object U (block111). The recorded scan data MD can be stored or further processed. For example, image data can be reconstructed from the recorded scan data MD, and optionally displayed via a suitable device (e.g. the user interface as discussed with respect toFIG.2).

The method described can also be applied separately for all physical gradient axes.

By way of the use of rotation classes K with associated gradient intensities which prevents an overloading of the gradient unit and simultaneously permits a better utilization of the gradient intensities available by way of the gradient unit, a scan duration of recordings of scan data can be shortened.

For example, for a magnetic resonance device with a maximum specified gradient intensity of GS=33 mT/m for which previously only examination protocols of a maximum usable gradient intensity of GN=17 mT/m were carried out, for example, when using a VIBE pulse sequence, the parameters echo time TE and repetition time TR of TE/TR=1.84 ms/4.4 ms at a gradient intensity of 17 mT/m on establishment of an orientation of the field of view and association with the corresponding rotation class with a gradient intensity of 30 mT/m for example can be reduced to TE/TR=1.36 ms/3.5 ms. It can therefore be achieved, for example, that a patient has to hold his breath a few seconds less for the recording of the scan data. A savings of, for example, just two seconds during breath holding can make the difference, in particular in sick patients, between a successful recording and a respiration-blurred recording that has to be repeated.

FIG.2shows schematically a magnetic resonance system1according to the disclosure. This comprises a magnet unit3for generating the main magnetic field, a gradient unit5(e.g. gradient coils) for generating the gradient fields, a high frequency (also known as a radio-frequency of RF) unit7for radiating in and receiving high frequency (also known as RF) signals and a control facility9configured for carrying out a method according to the disclosure.

InFIG.2, these subunits of the magnetic resonance system1are shown only roughly schematically. In particular, the RF unit7can consist of a plurality of subunits, for example, a plurality of coils such as the schematically shown coils7.1and7.2or more coils which can be configured either only to transmit RF signals or only to receive the triggered RF signals, or for both.

In order to examine an examination object U, for example, a patient or a phantom, the examination object can be introduced on a support L into the magnetic resonance system1, in the scanning volume thereof. The slice or the slab Sirepresents an exemplary target volume of the examination object from which echo signals are to be recorded and captured as scan data.

The control facility9(also referred to herein as a control computer, a controller, or controller circuitry) serves to control the magnetic resonance system1and can, for example, control the gradient unit5by means of a gradient control system5′ and the RF unit7by means of a RF transmitting/receiving control system7′. The RF unit7can herein comprise a plurality of channels on which signals can be transmitted or received.

The RF unit7is responsible, together with its RF transmitting/receiving control system7′ for the generation and radiating-in (transmission) of a RF alternating field for manipulation of the spins in a region to be manipulated (for example, in slices S to be scanned) of the examination object U. Herein, the center frequency of the RF alternating field, also designated the B1 field, is typically adjusted so that, as far as possible, it lies close to the resonance frequency of the spin to be manipulated. Deviations of the center frequency from the resonance frequency are referred to as off-resonance. In order to generate the B1 field, in the RF unit7, currents controlled by means of the RF transmitting/receiving control system7′ are applied to the RF coils.

Furthermore, the control facility9comprises a gradient establishing unit15, with which maximum permitted gradient intensities are established according to the disclosure dependent upon a rotation determined from an orientation of a field of view and making use of a list of rotation classes described herein. For instance, the gradient establishing unit15has access to at least one list of rotation classes. The control facility9is configured overall to carry out a method according to the disclosure.

A computing unit13included in the control facility9is configured to carry out all the computation operations necessary for the required scans and determinations. Intermediate results and results needed for this or determined herein can be stored in a storage unit S of the control facility9. The units mentioned are herein not necessarily to be understood as physically separate units, but represent merely a subdivision into units of purpose which, however, can also be realized, for example, in fewer, or even only in one single, physical unit.

By way of an input/output facility E/A (also referred to herein as a user interface or an input/output interface) of the magnetic resonance system1, for example, control commands can be passed by a user to the magnetic resonance system and/or results from the control facility9such as, for example, image data can be displayed.

A method described herein can also exist in the form of a computer program product which comprises a program and implements any of the methods described herein on a control facility9when said program is executed on the control facility9. An electronically readable data carrier26(e.g. a non-transitory computer-readable medium) with electronically readable control information stored thereon can also be provided, said control information comprising at least one computer program product as described above and being configured to carry out any of the methods described herein when the data carrier26is used in a control facility9of a magnetic resonance system1.

The various components described herein may be referred to as “units.” Such components may be implemented via any suitable combination of hardware and/or software components as applicable and/or known to achieve their intended respective functionality. This may include mechanical and/or electrical components, processors, processing circuitry, or other suitable hardware components, in addition to or instead of those discussed herein. Such components may be configured to operate independently, or configured to execute instructions or computer programs that are stored on a suitable computer-readable medium. Regardless of the particular implementation, such units, as applicable and relevant, may alternatively be referred to herein as “circuitry,” “controllers,” “processors,” or “processing circuitry,” or alternatively as noted herein.