Patent application number | Description | Published |
20120153953 | MAGNETIC RESONANCE APPARATUS WITH A BASIC FIELD MAGNET FORMED BY AT LEAST TWO SEPARATED MAGNETIC COILS - A magnetic resonance apparatus for examination in THE teeth and/or jaw region of a patient has at least one basic magnet to generate a constant basic magnetic field. The basic magnet is formed at least in part from at least one magnetic coil pair with at least two magnetic coils, and the at least one magnetic coil pair generates the basic magnetic field with a homogeneous magnetic field region between the at least two magnetic coils thereof. | 06-21-2012 |
20130069648 | METHOD AND MAGNETIC RESONANCE SCANNER FOR HYPERINTENSE DISPLAY OF AREAS IN THE VICINITY OF DIPOLE FIELDS - In a method and magnetic resonance apparatus for the hyperintense display of areas containing particles of magnetically active substances, in an examination region in a measurement volume of a magnetic resonance scanner, measurement data from the examination area are generated by a pulse sequence and recorded, the pulse sequence causing an echo time of less than one millisecond, so that a suppression of undesired signals is also caused. | 03-21-2013 |
20130076357 | METHOD AND MAGNETIC RESONANCE APPARATUS TO GENERATE A SERIES OF MR IMAGES TO MONITOR A POSITION OF AN INTERVENTIONAL DEVICE - In a magnetic resonance (MR) method and system to generate a series of MR images to monitor the position of an interventional device located in an examination region, radial scanning of k-space is combined with other scans, in particular for the k-space center. The measurement time until the entirety of k-space corresponding to the imaging region is scanned is thereby markedly shortened in total. The short echo times that are possible with this reduce susceptibility artifacts in the reconstructed image data and enable a depiction of tissue or substances with very short T2 values, for example plastics. Due to the rapidly repeated excitation and acquisition of measurement data and the reconstruction of image data, it is possible to monitor a position of the intervention device in the examination region. | 03-28-2013 |
20130082703 | METHOD TO GENERATE MAGNETIC RESONANCE MEASUREMENT DATA WITH IMAGE CONTRAST SELECTED AND PRODUCED BY PREPARATION PULSES - In a method and magnetic resonance apparatus to generate magnetic resonance measurement data, k-space corresponding to the examination region is subdivided into a first region and a second region. The first region includes the k-space center, and a ratio of preparation pulses radiated by the radio-frequency antenna of the magnetic resonance apparatus to RF excitation pulses radiated by the radio-frequency antenna is greater in the first region than in a second region of k-space corresponding to the examination region that is not covered by the first region of k-space. Preparation pulses in the entirety of k-space corresponding to the examination region are therefore not radiated uniformly often, but instead a reduced number of preparation pulses is applied in the second region in comparison to the first region. The total measurement time to generate magnetic resonance data, as well as a SAR exposure, are reduced. | 04-04-2013 |
20130082704 | METHOD AND MAGNETIC RESONANCE APPARATUS FOR NON-SELECTIVE EXCITATION OF NUCLEAR SPIN SIGNALS IN AN EXAMINATION SUBJECT - In a method for non-selective excitation of nuclear spin signals in an examination subject with a magnetic resonance system, RF excitation pulses are radiated to excite nuclear spin signals in the examination subject with simultaneous switching of gradients for spatial coding of the excited nuclear spin signals, wherein the RF excitation pulses are designed such that the base frequency of a radiated RF excitation pulse is adapted to the simultaneously switched gradient. By the dynamic adaptation of the radiated RF excitation pulses to the respective simultaneously switched gradients, artifacts due to insufficiently excited nuclear spins in an examination region to be examined (in particular even in examination regions that are arranged off-center) are avoided. | 04-04-2013 |
20130101198 | METHOD AND APPARATUS FOR CORRECTION OF ARTIFACTS IN MAGNETIC RESONANCE IMAGES - In a method and apparatus for the correction of artifacts in magnetic resonance images (MR) acquired with an MR pulse sequence in which gradients are switched simultaneously during the radiation of at least one non-selective excitation pulse, measurement data acquired with the pulse sequence in k-space are loaded into a processor, in which a perturbation matrix is determined on the basis of spatial and k-space point data of the acquired measurement data and the gradients used during the excitation. A corrected image is calculated from the acquired measurement data in k-space and the perturbation matrix, with the calculation of the corrected image including a matrix inversion of the perturbation matrix. The corrected image is then stored or displayed. | 04-25-2013 |
20130154641 | METHOD AND DEVICE TO GENERATE MAGNETIC RESONANCE IMAGE DATA OF AN EXAMINATION SUBJECT - In a method, magnetic resonance system and a reconstruction device for generation of magnetic resonance image data of an examination subject, raw magnetic resonance data are acquired in k-space, the raw magnetic resonance data including measurement values at multiple readout points that are arranged along multiple different trajectories in k-space. A displacement value is determined for each trajectory on the basis of the measurement values of a collection of multiple trajectories. Readout points of the raw magnetic resonance data are displaced by the displacement value, and image data are reconstructed from the displaced raw magnetic resonance data. | 06-20-2013 |
20130169273 | MAGNETIC RESONANCE SYSTEM, OPERATING METHOD AND CONTROL DEVICE TO GENERATE T2-WEIGHTED IMAGES USING A PULSE SEQUENCE WITH VERY SHORT ECHO TIMES - In a method to control a magnetic resonance system to generate magnetic resonance exposures of an examination subject, a first magnetic resonance radio-frequency pulse with a pulse length of at most 50 μs is initially emitted in a volume region of the examination subject. At least one second magnetic resonance radio-frequency pulse, whose phase is essentially rotated by 180° relative to the first magnetic resonance radio-frequency pulse, with a pulse length of at most 50 μs, is emitted in the same volume region of the examination subject in a predetermined time interval immediately after the first magnetic resonance radio-frequency pulse. An acquisition of raw data from the volume region of the examination subject then takes place. Furthermore, a control device for operating a magnetic resonance system as well as a magnetic resonance system with such a control device to implement such a method, are described. | 07-04-2013 |
20130265050 | METHOD AND MAGNETIC RESONANCE SYSTEM FOR FUNCTIONAL MR IMAGING OF A PREDETERMINED VOLUME SEGMENT OF THE BRAIN OF A LIVING EXAMINATION SUBJECT - In a method and a magnetic resonance (MR) system for functional MR imaging of a predetermined volume segment of THE brain of a living examination subject, an RF excitation pulse is radiated into the subject and at least one magnetic field gradient is activated, and MR data of the predetermined volume segment is acquired beginning at a predetermined echo time after the RF excitation pulse. The echo time is in a time period of 10 μs to 1000 μs. | 10-10-2013 |
20130267827 | METHOD AND MAGNETIC RESONANCE SYSTEM FOR FUNCTIONAL MR IMAGING OF A PREDETERMINED VOLUME SEGMENT OF THE BRAIN OF A LIVING EXAMINATION SUBJECT - In a method and a magnetic resonance (MR) system for functional MR imaging of a predetermined volume segment of the brain of a living examination subject, MR data of the predetermined volume segment are acquired, EEG data of the examination subject are acquired with the acquisition of the EEG data taking place simultaneously with the acquisition of the MR data, and the MR data automatically evaluated dependent on the acquired EEG data. | 10-10-2013 |
20130271139 | DETERMINATION OF A CONTROL SEQUENCE FOR A MAGNETIC RESONANCE IMAGING SYSTEM - In a method to determine a control sequence for a magnetic resonance imaging system in order to acquire echo signal-based raw magnetic resonance data in k-space along one or more trajectories on the basis of the control sequence, the control sequence is optimized so that, to control a gradient magnetic field for at least a predetermined portion of the control sequence, a change of an attribute of the gradient magnetic field is limited. The limitation takes place so that a momentary amplitude change rate of the gradient magnetic field falls below a predetermined amplitude change rate limit value, and/or so that a momentary direction change rate of the gradient magnetic field falls below a predetermined direction change rate limit value, and/or so that a momentary gradient change rate of the gradient magnetic field that is based on a combination of the momentary amplitude change rate and the momentary direction change rate falls below a predetermined gradient change rate limit value. | 10-17-2013 |
20130275086 | METHOD AND MAGNETIC RESONANCE APPARATUS TO IDENTIFY A NOISE VOLUME FOR A MAGNETIC RESONANCE EXAMINATION - In a method and magnetic resonance apparatus to determine and/or adjust a noise volume for a magnetic resonance examination, a selection of a magnetic resonance sequence for the magnetic resonance examination of a subject to be examined hereby is made and an automatic calculation of an expected noise volume for the magnetic resonance examination is made in a volume determination unit using protocol parameters of the selected magnetic resonance sequence. Information about the expected volume is provided to an operator via a user interface. | 10-17-2013 |
20140021950 | Dynamic Adjustment of Gradient Rise Times for MR HF Pulse Sequences - In a method for image data acquisition using a magnetic resonance system, in order to excite nuclear spin signals, a sequence of high-frequency pulses is irradiated into an examination subject while gradients are simultaneously switched for position encoding of the excited nuclear spin signals. The rise times of the gradients used during the sequence are adjusted dynamically with each high-frequency pulse irradiation. | 01-23-2014 |
20140077810 | MAGNETIC RESONANCE SYSTEM AND METHOD TO ACQUIRE AT LEAST TWO MEASUREMENT DATA SETS FROM AN EXAMINATION SUBJECT - In a magnetic resonance data acquisition of at least two measurement data sets of an examination subject, each of the at least two measurement data sets is acquired in at least three partial measurements. Each partial measurement covers a partial region of k-space corresponding to the examination subject to be examined, and the partial measurements are executed in series in an order such that two successive partial measurements are associated with different data sets of the at least two measurement data sets, and such that two successive partial measurements respectively do not measure the same partial region. A reduced movement sensitivity is achieved by the acquisition of the interleaved partial measurements associated with different measurement data sets. Unwanted refocusings (and therefore echo signals of residual magnetization) are also avoided by avoiding successive partial measurements that measure the same partial region. | 03-20-2014 |
20140084923 | MAGNETIC RESONANCE METHOD, APPARATUS AND RADIOFREQUENCY COIL FOR ACQUIRING MAGNETIC RESONANCE DATA OF AT LEAST ONE TOOTH - In a magnetic resonance method and apparatus for the acquisition of measurement data of at least one tooth of an examination subject, a pulse sequence is employed that has an echo time TE of less than 0.5 milliseconds, and spatial coding of the acquired measurement data takes place in only two spatial directions. Projection image data are reconstructed from the acquired measurement data. A coil for a magnetic resonance tomography system, which coil is dedicated to dental imaging, has at least one coil element, and each coil element of the coil has an individual acquisition volume that encompasses at least one tooth. | 03-27-2014 |
20140084924 | MAGNETIC RESONANCE METHOD AND APPARATUS FOR CORRECTION OF MAGNETIC RESONANCE DATA - In a method and apparatus to acquire correction data in connection with pulse sequences to acquire measurement data whose echo times—the duration between excitation and measurement data acquisition of the pulse sequences—are less than 500 microseconds, the pulse sequences acquire measurement data by repetition of a pulse sequence scheme, wherein different gradients for spatial coding are switched in each repetition, and correction data are acquired every n repetitions in a time window in which no gradients are switched, wherein n is a predetermined natural number. The method and apparatus enable correction of measurement data with which solid substances can be depicted without the hardware being used needing to be adapted and without external sensors being necessary. | 03-27-2014 |
20140086468 | METHOD AND APPARATUS FOR CORRECTION OF ARTIFACTS IN MAGNETIC RESONANCE IMAGES - In a method for the calculation of individual elements of a matrix to correct artifacts in magnetic resonance images that are reconstructed from measurement data acquired using an MR pulse sequence, in which gradients are switched simultaneously during the radiation of at least one non-selective excitation pulse, at least one excitation profile of an excitation pulse used to acquire measurement data is loaded into a process, the profile depending on the measured location x and the measured k-space point k and the gradient strength applied in the measurement. From each loaded excitation profile, an element of a transposed, inverted disturbance matrix is calculated which corresponds to the location x and the measured k-space point k. Instead of a Fourier back-transformation, matrix inversion is used for the image reconstruction of a corrected image. | 03-27-2014 |
20140091794 | MAGNETIC RESONANCE APPARATUS AND OPERATING METHOD - In a method to operate a magnetic resonance apparatus with a magnetic resonance sequence—in particular a PETRA sequence—in which k-space is radially scanned for an image acquisition in a first region of k-space that does not include the center of k-space, and in which an excitation pulse is radiated as the full strength of at least two phase coding gradients is reached, and in which k-space is scanned in a Cartesian manner—in particular by single point imaging—in a second region of k-space remaining without the first region, the gradient strength corresponding to a shortest total acquisition time is determined automatically from predetermined sequence parameters and/or sequence parameters defined by a user. The sequence parameters parameterize the magnetic resonance sequence and describe the number of acquisitions for the regions of k-space and the repetition time, and the gradient strength is indicated to a user as a recommendation and/or is set automatically in the implementation of the magnetic resonance sequence. | 04-03-2014 |
20140091795 | MAGNETIC RESONANCE METHOD AND APPARATUS FOR AUTOMATIC CALCULATION OF A MAXIMUM PULSE-LENGTH OF AN EXCITATION PULSE - In a method and magnetic resonance apparatus for automatic calculation of a maximum pulse length of a non-selective excitation pulse for a magnetic resonance data acquisition pulse sequence in which gradients are switched during the radiation of at least one non-selective excitation pulse, a first parameter, which indicates the field of view (FOV) desired in the measurement for which the pulse length of the excitation pulse should be maximized, is loaded into a processor, and a second parameter, which indicates the maximum gradient strength (G | 04-03-2014 |
20140091796 | METHOD AND MAGNETIC RESONANCE APPARATUS TO GENERATE AN ARTIFACT-FREE MAGNETIC RESONANCE IMAGE DATA SET - In a method and magnetic resonance (MR) system for the creation of an artifact-free image data set of an imaging area located in a measurement volume of the MR system, measurement data are acquired from which an image data is to be reconstructed, with gradients for spatially coding of the measurement data are ramped continuously over time to a strength desired for the acquisition of the measurement data, without abrupt changes in the gradient strength. The actual gradients present in the measurement volume are measured by a field mapping device in the measurement volume of the MR system. The trajectories along which k-space is scanned during the acquisition of the measurement data are calculated on the basis of the measured actual gradients. An artifact-free image data set is reconstructed from the acquired measurement data under consideration of the calculated trajectories, and is displayed and/or stored. | 04-03-2014 |
20140097840 | METHOD AND MAGNETIC RESONANCE APPARATUS FOR IMAGE ACQUISITION - A method and magnetic resonance apparatus for image acquisition using a magnetic resonance sequence (in particular a PETRA sequence) in which k-space corresponding to the imaging area is scanned, with a first region of k-space, which does not include the center of k-space, being scanned radially along a number of spokes emanating from the center of k-space, and with at least two phase coding gradients being completely ramped up before administration of the excitation pulse, and a second central region of k-space, which remains without the first region, is scanned in a Cartesian manner (in particular via single point imaging). For the purpose of a contrast increase a pre-pulse—in particular an inversion pulse to establish a T1 contrast—is provided before a predetermined number of individual measurements. The number of spokes to be measured is selected such that a measurement point located (in a Cartesian manner) nearest to the center of k-space is measured at a predetermined point in time after a pre-pulse, which point in time is optimal with regard to the signal-to-noise ratio and/or the contrast. | 04-10-2014 |
20140103928 | METHOD AND MAGNETIC RESONANCE DEVICE FOR IMAGE ACQUISITION - In a method and magnetic resonance apparatus for acquiring image data using a sequence in which k-space corresponding to the imaging area is scanned in a first region of k-space, which does not include the center of k-space, radially along spokes emanating from the center of k-space, with at least two phase coding gradients being completely ramped up before the excitation pulse, and in a second central region of k-space, which remains without the first region, in a Cartesian manner. For contrast increase, a pre-pulse is provided before a predetermined number of individual measurements. A portion of the measurement points of the second region of k-space, which portion is situated nearest the center of k-space, is scanned as central measurement points after the first administration of the pre-pulse immediately following a zero crossing of the contrast-relevant magnetization of one of at least two materials in the image. | 04-17-2014 |
20140111200 | METHOD AND APPARATUS FOR OPTIMIZATION OF A PULSE SEQUENCE FOR A MAGNETIC RESONANCE SYSTEM - A method and a pulse sequence optimization device to optimize a pulse sequence for a magnetic resonance system, wherein the pulse sequence includes at least one refocusing pulse, one slice selection gradient pulse, and one gradient spoiler pulse. The pulse duration of the refocusing pulse is shortened, and the pulse duration of the slice selection gradient pulse is adapted to the shortened pulse duration of the refocusing pulse. The amplitude of the slice selection gradient pulse is increased so that the same slice thickness is selected as before the shortening of the pulse duration of the refocusing pulse. The pulse shape of the gradient spoiler pulse is adapted without changing a total spoiler moment, and an optimally shortened pulse duration of the refocusing pulse is achieved when, with the adaptation of the pulse shape of the gradient spoiler pulse, the maximum amplitude of the gradient spoiler pulse equals the amplitude of the slice selection gradient pulse, and an edge steepness of the gradient spoiler pulse is minimized. | 04-24-2014 |
20140117985 | METHOD AND MAGNETIC RESONANCE APPARATUS TO GENERATE RAW DATA SETS FROM DOUBLE ECHO DATA ACQUISITIONS - In a method and magnetic resonance apparatus to create two raw data sets from double echo exposures of an imaging area located in a measurement volume of the magnetic resonance system, two echo signals are acquired in the form of raw data sets at different times, and k-space corresponding to the imaging area is either scanned completely only for the first raw data set and incompletely for the second raw data set, or is scanned completely only for the second raw data set and incompletely for the first raw data set. The completion of the incomplete raw data set takes place using a model that is based on the completely scanned raw data set. | 05-01-2014 |
20140117986 | METHOD AND MAGNETIC RESONANCE SYSTEM TO GENERATE RAW DATA SETS IN A DOUBLE ECHO ACQUISITION SEQUENCE - In a method, a magnetic resonance apparatus and non-transitory, a computer-readable storage medium, two raw data sets are created using at least one double-echo acquisition of an imaging area located in a measurement volume of the magnetic resonance apparatus. In the acquisition and storage of two echo signals in the form of raw data sets at different times, a second echo signal is not acquired after each and every radiated RF excitation pulses. | 05-01-2014 |
20140159721 | Magnetic Resonance Coil Apparatus - A magnetic resonance coil apparatus includes a receiving region for receiving a subregion of a patient to be examined, a housing shell unit enclosing the receiving region, and an antenna unit for picking up magnetic resonance signals. The magnetic resonance coil apparatus includes a camera unit with at least one light field camera element. | 06-12-2014 |
20140232396 | OPTIMIZATION OF A PULSE SEQUENCE FOR A MAGNETIC RESONANCE SYSTEM - In a method and a pulse sequence optimization device to determine a pulse sequence for a magnetic resonance system, a pulse sequence is selected for optimization that includes a number of radio-frequency pulses and a number of gradient pulses chronologically coordinated therewith. An automatic analysis of the pulse sequence takes place to identify fixed point/time periods in the pulse sequence that are to be left unmodified, and modifiable time intervals in the pulse sequence that may be optimized. An automatic optimization of gradient pulses in the modifiable time intervals takes place according to a predetermined optimization criterion, while keeping the length of modifiable time intervals constant. | 08-21-2014 |
20140232397 | DETERMINATION OF A PULSE SEQUENCE FOR A MAGNETIC RESONANCE SYSTEM - In a method and a pulse sequence determination device to determine a pulse sequence for a magnetic resonance system, control protocol parameter values are initially acquired. A determination of k-space trajectory node points within k-space then takes place in a processor on the basis of the control protocol parameter values. The determination of the pulse sequence then takes place on the basis of the k-space trajectory node points. A method for operating a magnetic resonance system uses such a pulse sequence, and a magnetic resonance system embodies such a pulse sequence determination device. | 08-21-2014 |
20140375316 | METHOD AND APPARATUS TO GENERATE MAGNETIC RESONANCE IMAGE DATA OF AN EXAMINATION SUBJECT - In the magnetic resonance image data acquisition and apparatus, raw magnetic resonance data are acquired at multiple points along a trajectory in k-space from first and second magnetic resonance echo signals caused by a radio-frequency excitation pulse. The course of the trajectory in k-space is established by adjusting a magnetic field value of a gradient magnetic field. The gradient magnetic field has a field value of a first point in time of the trajectory curve and a subsequently modified and at a layer second point in time, the gradient magnetic field has the same field value as that said first point in time. The second point in time is before or during the acquisition of the raw magnetic resonance data of the first magnetic resonance echo signal. The shift value for the trajectory is determined and the trajectory is shifted according to this shift value, and an image is reconstructed from the shifted raw magnetic resonance data of the trajectory. | 12-25-2014 |
20150032406 | METHOD AND DEVICE FOR OPTIMIZATION OF A PULSE SEQUENCE FOR A MAGNETIC RESONANCE IMAGING SYSTEM - In a method for optimization of a pulse sequence for a magnetic resonance imaging apparatus, a plan gradient pulse train that is to be executed to chronologically match a radio-frequency pulse train to control an RF transmission system of the magnetic resonance imaging apparatus is adopted to control a gradient system of the magnetic resonance imaging apparatus. The determined plan gradient pulse train forms an optimization segment and for the optimization segment a plan gradient moment is determined. A real gradient pulse train that can actually be executed is determined for the optimization segment of the determined plan gradient pulse train and a real gradient moment is determined for the real gradient pulse train. An error gradient moment difference between the real gradient moment and the plan gradient moment is determined. The real gradient pulse train is modified so that the magnitude of the gradient moment difference between the plan gradient moment and the gradient moment of the modified real gradient pulse train is optimized. A pulse sequence optimization unit is designed to implement such a method and a magnetic resonance imaging system is operated using such a pulse sequence optimization unit. | 01-29-2015 |
20150042333 | MAGNETIC RESONANCE APPARATUS, AND METHOD AND CONTROL DEVICE THEREFOR - In a method to control a magnetic resonance apparatus, a control device, a magnetic resonance apparatus, and an electronically readable data storage medium, a reduction and/or limitation and/or monitoring of the noise volume of the magnetic resonance apparatus is enabled by a noise volume-reduced operating mode of the magnetic resonance apparatus being activated depending on at least one predeterminable event. | 02-12-2015 |
20150077109 | METHOD AND MAGNETIC RESONANCE APPARATUS TO OPTIMIZE A MAGNETIC RESONANCE DATA ACQUISITION SEQUENCE - In a method to optimize a magnetic resonance sequence of a magnetic resonance apparatus, the magnetic resonance sequence includes first imaging parameters that, during acquisition of magnetic resonance images by the magnetic resonance sequence, the first imaging parameters produce acoustic noise with a first acoustic noise volume level and magnetic resonance images with image noise at a first signal-to-image noise ratio. An automatic optimization of the imaging parameters is implemented such that during acquisition of magnetic resonance images by the magnetic resonance sequence, the optimized imaging parameters produce acoustic noise with a second acoustic noise volume level and magnetic resonance images with image noise at a second signal-to-image noise ratio. The second acoustic noise volume is reduced by at least 3 dB relative to the first acoustic noise volume and the second signal-to-image noise ratio is reduced by a maximum of 35 percent relative to the first signal-to-image noise ratio. | 03-19-2015 |