| Patent application number | Description | Published |
|---|
| 20080315113 | BEAM GUIDANCE MAGNET - A beam guidance magnet for deflecting a beam of electrically charged particles along a curved particle path is provided. The beam guidance magnet includes a coil system that does not include a ferromagnetic material affecting the beam guidance and has curved coils stretched out along the particle path, the coils being arranged in pairs in mirror symmetry to the beam guidance plane. The coil system includes two primary coils and two substantially flat secondary coils. The two primary coils include primary coil sides and primary coil end parts bent upward relative to the beam guidance plane. The two substantially flat secondary coils are disposed between the primary coil end parts. Supplementary coils are disposed in the field range of the respective curved secondary coil end parts. | 12-25-2008 |
| 20090090871 | Radiation treatment system with a beam control magnet - A radiation treatment system with a beam control magnet for deflecting a beam of electrically charged particles along a curved particle path. The beam control magnet is subdivided along a parting plane perpendicular to the direction of the particle path into a first region and a second region. The quadrupole moments of the beam control magnet have different signs in the first region and the second region. | 04-09-2009 |
| 20090321654 | BEAM GUIDING MAGNET FOR DEFLECTING A PARTICLE BEAM - A beam guiding magnet includes a first and second coil system, which are designed such that the dipole moments of the first and second coil systems point in opposite directions. Since the dipole moments of the first and second coil systems point in opposite directions, the two dipole moments at least partially compensate for one another. The resultant dipole moment of the beam guiding magnet may be reduced. The beam guiding magnet may take into account that the remote field of a beam guiding magnet can be lowered by a reduction in the dipole moment of the beam guiding magnet. The dipole moment decreases with the cube of the distance from the beam guiding magnet. A quadruple moment, which on attenuation of the dipole moment represents the next strongest field component, decreases with the fifth power of that distance. | 12-31-2009 |
| 20090322329 | MAGNETIC RESONANCE APPARATUS AND METHOD FOR DETERMINING A PULSE SEQUENCE TO FEED AN RF RADIATING COIL - In a magnetic resonance apparatus having an RF radiating coil and gradient coils, and in a method for operating such a magnetic resonance apparatus, a pulse sequence, composed of multiple time steps, is specified for operating the gradient coils to time-dependently select regions of a selected slice of a selected volume of a subject. A non-linear equation system is then solved to obtain feed parameters for individual channels of the transmit coil for each time step, with specification of a desired target magnetization, and dependent on the pulse sequence specified for the gradient coils. The non-linear equation system is based on discrete values for time and space variable and, in addition to equations resulting from the Bloch equation, which are non-linear in their feed parameters, includes at least one additional equation that describes boundary conditions for the examination of the subject. | 12-31-2009 |
| 20100327867 | METHOD TO DETERMINE PARAMETERS TO CONTROL THE GRADIENT COILS AND RADIO-FREQUENCY COILS OF A MAGNETIC RESONANCE DEVICE - In a method for examination subject-specific determination of parameters for activating gradient coils and radio-frequency of a coil array of a magnetic resonance device to generate a radio-frequency pulse with which nuclear spins in an examination region of an examination subject are moved out of a rest state by an arbitrary angle, a control unit activates phases and amplitudes of currents in the radio-frequency coils and respective currents in the gradient coils in a time-dependent manner in discrete steps to generate gradient fields. In a processor in communication with the control unit, parameters for the activation are automatically calculated dependent on measured sensitivity maps of the radio-frequency coils at the examination subject. The processor optimizes a non-linear equation system within the numerical calculation of the parameters involving a desired magnetization and a theoretical calculated real magnetization. The Jacobian matrix of the real magnetization is calculated in the determination of the parameters dependent on the direction of decline of the magnetization. The matrix elements of the Jacobian matrix consist of products of individual rotations that are determined from the optimized parameters. In the calculation of each matrix element, only factors in which the corresponding parameter is associated with the time step of the matrix element are determined. | 12-30-2010 |
