Siemens Aktiengesellschaft

Siemens Healthcare Gmbh

Other

Siemens Healthineers Ag

Siemens Corporation

Dentsply Sirona Inc.

Sirona Dental Systems Gmbh

Matthias Gebhardt

Markus Vester

Gerhard Brinker

Wolfgang Bielmeier

Mario Zeller

David Grodzki

Stephan Biber

Dominik Paul

Stefan Popescu

Swen Campagna

Juergen Nistler

Gudrun Ruyters

Carsten Prinz

Bernd Erbe

Wolfgang Renz

Andreas Greiser

Franz Schmitt

Nikolaus Demharter

Andreas Krug

Helmut Lenz

Adrian Mark Thomas

Volker Schnetter

Eva Eberlein

Elfar Adalsteinsson

Carmel Hayes

Edgar Müller

Johannes Ulrici

Franz Boemmel

Stephan Stöcker

Jörg Ulrich Fontius

Jörg Rothard

Michael Mallett

Jürgen Nistler

Johann Schuster

Thorsten Speckner

Winfried Arz

Ralf Kartäusch

Stephan Stoecker

Peter Speier

Ralph Oppelt

Lawrence Leroy Wald

Thomas Beck

Dieter Ritter

Hans-Peter Fautz

Peter Dietz

Josef Pfeuffer

Dirk Diehl

Rene Gumbrecht

Lars Lauer

Thomas Benner

Axel Vom Endt

Franz Hebrank

Holger Adolf

Roland Werner

Stefan Wundrak

Mathias Blasche

Volker Weissenberger

Sebastian Dennert

Dirk Schneiderbanger

Heinz Hentzelt

Florian Odoj

Tobias Wichmann

Joonsung Lee

Gabriele Eichfelder

Robert James McGregor

Norbert Gebhardt

Titus Lanz

Marco Geissner

Nicolas Groß-Weege

A magnetic resonance device for acquiring magnetic resonance data of an object, the magnetic resonance device including a main magnet operable to provide a main magnetic field along at least one surface of the main magnet, wherein the main magnet comprises: a first magnet segment; a second magnet segment; and a cavity to accommodate the second magnet segment, wherein the second magnet segment is arranged in the cavity of the main magnet, and wherein the second magnet segment is variably positioned and/or oriented relative to the first magnet segment to adjust a magnetic field contribution of the second magnet segment to the main magnetic field.

Dedicated magnetic resonance device

A magnetic resonance imaging device may include a field generator for generating at least one magnetic gradient field. The field generator may include a first magnet and a second magnet confining an imaging volume of the magnetic resonance imaging device in two spatial directions. The first magnet and the second magnet may be arranged asymmetrically with respect to the imaging volume. The magnetic resonance imaging device may be used to perform a method for acquiring an image of a diagnostically relevant body region of a patient.

Magnetic resonance imaging device with asymmetric field generation unit

A magnetic resonance imaging device having a field generation unit configured to provide a magnetic field in an imaging volume of the magnetic resonance imaging device. The field generation unit has at least one magnet. A surface of the field generation unit directed towards the imaging volume of the at least one magnet has a concave shape, wherein a direction of access to the imaging volume is oriented essentially perpendicular to a main direction of magnetic field lines in the imaging volume.

Magnetic resonance imaging device with a concave-shaped field generation unit

A magnetic resonance imaging system comprises a field generation unit and a supporting structure for providing structural support for the field generation unit, wherein the field generation unit comprises at least one magnet for generating a B0 magnetic field and an opening configured to provide access to an imaging volume positioned in the B0 magnetic field along at least one direction and wherein the at least one direction is angled with respect to a main direction of magnetic field lines of the B0 magnetic field in the imaging volume.

Magnetic resonance scanner and magnetic resonance imaging system

A magnetic resonance apparatus, for acquiring magnetic resonance data from a person who is asleep, includes a person support apparatus to provide a sleeping place; an acquisition arrangement including a radiofrequency coil arrangement for transmitting excitation pulses and for receiving magnetic resonance signals; and a controller, designed to operate the acquisition arrangement according to a magnetic resonance sequence for acquiring a magnetic resonance dataset from a region under examination of the person. The magnetic resonance apparatus includes a main magnetic field of strength less than 20 mT, in particular less than 10 mT, and the controller includes an acquisition unit for acquiring a magnetic resonance dataset via a prolonged magnetic resonance sequence having a total acquisition duration of more than one hour.

Magnetic resonance apparatus and method for operating a magnetic resonance apparatus, computer program and electronically readable data storage medium

In a magnetic resonance apparatus and a method for operation thereof, at least one electrical operating value of at least one predetermined component of the apparatus is captured and, as a function of the at least one operating value, at least one coil operating value of a transmitting coil arrangement of the magnetic resonance apparatus is controlled for the purpose of limiting a B1 value.

Magnetic resonance apparatus and operating method therefor with monitoring and control of RF energy-relevant operating value

An apparatus and a method for spatial encoding in magnetic resonance tomography using a radio frequency signal are provided. A first set of parameters from a first frequency and from a first amplitude, and from a second frequency and a second amplitude is determined by the magnetic resonance tomograph, and corresponding signals are generated by a radio frequency device and transmitted by an antenna apparatus. A first gradient above the Larmor frequency of the nuclear spins is generated by the Bloch-Siegert effect. The same thing ensues with a second set of parameters that differs from the first set of parameters at least in one frequency or amplitude and therefore generates a second, different gradient.

Apparatus and method for spatial encoding using a radio frequency signal in magnetic resonance tomography

A method for correcting a B0 inhomogeneity in a magnetic resonance scan with a magnetic resonance tomograph is provided. The magnetic resonance tomograph includes a controller, a radio frequency unit, and a transmitting antenna. In the method, the controller determines a transmission signal that is suitable for correcting an effect of an inhomogeneity of a static B0 magnetic field in an examination volume by the Bloch-Siegert effect. The transmission signal is emitted into the examination volume.

Method and device for correcting a B0 inhomogeneity by a radio frequency signal

A method for monitoring a temporal change in a magnetic field in a magnetic resonance device, as well as an evaluation unit, a magnetic resonance device, and a computer program product for performing the method are provided. The method provides that a position-dependent magnetic field distribution that is produced by the plurality of gradient coils is provided with a plurality of monitoring points. In addition, time-dependent gradient values of the plurality of gradient coils are ascertained. Based on position-dependent magnetic field distribution and the time-dependent gradient values, the temporal change in the magnetic field is ascertained. The temporal change in the magnetic field is monitored by comparing the temporal change in the magnetic field with at least one limit value.

Monitoring of a temporal change in a magnetic field in a magnetic resonance device

In a method and magnetic resonance (MR) apparatus for avoidance of artifacts in the acquisition of MR data, first and second undersampled datasets are recorded, the measurement data of each dataset being selected such that artifacts in the first dataset exhibit a phase other than in the second dataset, and the measurement data in the first and second datasets, even when combined, correspond to undersampled dataset. The recorded, undersampled datasets are supplemented with the use of a supplementary kernel of a parallel acquisition method to form supplemented datasets from which a combined, artifact-free dataset is produced. Measurement time is thereby reduced overall compared with customary PAT averaging and compared with recording without the use of a parallel acquisition method.

Method and magnetic resonance apparatus for avoidance of artifacts in the acquisition of magnetic resonance measurement data

A circuit arrangement for an MRT system and a method for operating an MRT system are disclosed. The circuit arrangement includes a gradient amplifier having a switch-mode output stage, a regulator device, and a modulator connected therebetween in the circuit. To ensure patient safety, a control path is integrated into a drive path of the circuit arrangement or the MRT system provided for driving a gradient coil, the gradient coil being connected to an output of the switch-mode output stage. The control path includes a limiter stage connected downstream of the regulator device, the modulator, the switch-mode output stage and its supply voltage. The limiter stage is connected in the circuit between the regulator device and an input of the modulator, to limit a control signal output by the regulator device and limit the voltage for the gradient coil provided by the switch-mode output stage at its output.

Circuit arrangement for an MRT system, MRT system and method for operating an MRT system

In a method and an apparatus for magnetic resonance tomography, an eddy current field is compensated by taking into account its progression over time and its dependence on a sensed value, by having a sensor determine the sensed value and, on the basis of the sensed value, a current strength for a conductor in order to generate an opposing field to reduce the eddy current field is determined, and supplied to the conductor.

Method and apparatus for eddy current field compensation in magnetic resonance tomography

In a magnetic resonance (MR) apparatus and an operating method therefor, a sequence with which the MR data are to be recorded is created in or provided to a control computer of the MR apparatus. A maximum RF output and a maximum gradient performance of the scanner magnetic resonance apparatus during the performance of the sequence are determined by simulating or analyzing the performance of the sequence in the control computer, and it is verified whether the maximum RF output and/or the maximum gradient performance violate predetermined limit values. Execution of the sequence to record the MR data is performed only if the verification showed that the limit values are not violated.

Method and magnetic resonance apparatus wherein limit values are observed when recording magnetic resonance data

A method for operating a magnetic resonance apparatus by a safety unit, taking into account persons fitted with an implant, a safety unit, a safety system, a magnetic resonance apparatus, and a computer program product are provided. The magnetic resonance apparatus includes a first part and a second part. The first part is operated separately from the second part and includes the safety unit. During an examination of a person fitted with an implant, the safety unit checks that the magnetic resonance apparatus, in a restricted operating mode, is complying with implant-conformant limit values.

Operation of a magnetic resonance apparatus taking into account persons fitted with implants

A controller of a magnetic resonance system outputs a low frequency base signal to a conversion device. While outputting the base signal to the conversion device, the controller outputs an oscillator control signal to an oscillator. The oscillator outputs a frequency signal corresponding to the oscillator control signal to the conversion device. The conversion device converts the frequency signal into a high frequency transmit pulse with the aid of the base signal and outputs the transmit pulse to a magnetic resonance transmit antenna. The magnetic resonance transmit antenna applies a high frequency field corresponding to a transmit pulse to an examination volume of the magnetic resonance system. The controller varies the oscillator control signal output to the oscillator while outputting the base signal to the modulator. The transmit pulse) has a larger bandwidth than the base signal.

Magnetic resonance system having variable frequency transmit pulses

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Erlangen, Germany

Matthias Gebhardt