Abstract: A method, a circuit arrangement and an X-ray system, in particular a CT system, are disclosed wherein, in order to correct the count rate drift of a detector for ionizing radiation having quantum-counting detector elements which include a combination of at least two counters with significantly different energy thresholds, and on the basis of previously determined functional dependencies of count rates on one another and using at least one of the counters per detector element as the reference, the count rates of the respective other counters with different energy thresholds are corrected.

Abstract: A method is disclosed for generating image data of an object under examination from X-ray projection data of the object under examination, wherein, before a reconstruction of the image data, the X-ray projection data are subjected to scattered radiation correction on the basis of scattered radiation measured values. Here, the scattered radiation measured values are initially subjected to an extra-focal radiation correction before being used for the scattered radiation correction. A projection data processing device is also disclosed for carrying out a method of this kind and an X-ray system, in particular computed tomography system, with a projection data processing device of this kind.

Abstract: In a method, with a current measurement, the history of the radiation exposure of the X-ray detector is taken into account with respect to the overall X-ray detector or subareas of the X-ray detector, in respect of a reduction in the measurement sensitivity produced as a result and a recovery of the reduction in the measurement sensitivity, and the determined measuring signal is corrected with a correction factor which is dependent on the history of the radiation exposure. Furthermore, an X-ray recording system includes a detector which includes a plurality of detector elements, which are read out in groups channel by channel and a read-out apparatus with computer-assisted device for correcting read-out detector data prior to a further processing of the detector data to form projective or tomographic images.

Abstract: A method and a CT system are disclosed for predicting specific cardiac cycle phases within the scope of a CT examination, wherein signal profiles of the heart are continuously recorded during the examination over a plurality of cardiac cycles, wherein times of successive cycle positions with the same characteristics are determined with the aid of the signal profiles and the successive cycle lengths of the cardiac cycles are determined with the aid of the determined times, wherein typical patterns in successive cycle lengths over a first number of past and successive cardiac cycles are sought after and a current or future cycle length is determined by recording cycle patterns in a second, smaller number of cycle lengths including their typical successive cycle length within the first number of current past cycle lengths, and predicting, using probabilistic methods, the cycle length that follows the last determined cycle pattern on the basis of the cycle patterns currently determined during the CT examination.

Abstract: A method is disclosed for transmitting measurement data from a transmitter system to a receiver system by way of a transmission link of a medical device. In an embodiment, the measurement data, as input data of a transformation method, is transformed to output values and, after transmission, back transformed again, the values of the input data lying between a maximum value and a minimum value and an assignment function being used for compression purposes, to allocate an output value to every value of the input data, a root function being used as the assignment function for at least some of the values.

Abstract: A method is disclosed for calibrating a CT system with at least one focus-detector combination with a quanta-counting detector including a plurality of detector elements, with the focus-detector combination being arranged to enable it to be rotated around a measurement region and a system axis arranged therein, and an X-ray bundle going out from the focus to the detector which possesses an X-ray energy spectrum over an energy range. In at least one embodiment of the method, actual attenuation values from CT scans obtained with an X-ray energy spectrum are compared with theoretical mono-energetic required attenuation values even in the paralysis range of the quanta-counting detector and a transfer function is determined between the required attenuation values and the actual attenuation values for each detector element and thereby a calibration of the measured attenuation values is carried out.

Abstract: A counting detector is disclosed. In at least one embodiment, the counting detector includes sensors for converting radiation quanta into electrical pulses and an evaluation unit with a number of energy thresholds, wherein the evaluation unit generates for each sensor a count value for each energy threshold from the pulses, which count value represents the number of radiation quanta with an energy above the respective energy threshold. In at least one embodiment, one of the energy thresholds is arranged directly above a characteristic energy of radiation quanta causing double counting in order to correct double counting; and a correction unit calculates a corrected count value from the count values of the energy thresholds, which corrected count value has reduced double counting for at least one of the energy thresholds. Images with an improved contrast-to-noise ratio and, at the same time, a reduced X-ray dose can be generated on the basis of the at least one corrected count value.

Abstract: A circuit arrangement of a quanta-counting detector with a multiplicity of detector elements is disclosed, wherein the X-ray quanta registered in each detector element generate a signal profile. In at least one embodiment, the circuit arrangement, in each detector element, includes: at least one first comparator with a first energy threshold lying in the energy range of the measured X-ray quanta and at least one second comparator with a second energy threshold lying above the energy range of the measured X-ray quanta, the at least one first and second comparators being connected to the detector element. Further, the at least two comparators have a logical interconnection, wherein at least a first comparator and a second comparator are connected to the inputs of an XOR gate, and each XOR gate connected to a first comparator is connected to precisely one edge-sensitive counter.

Abstract: A method and a CT system are disclosed for predicting specific cardiac cycle phases within the scope of a CT examination, wherein signal profiles of the heart are continuously recorded during the examination over a plurality of cardiac cycles, wherein times of successive cycle positions with the same characteristics are determined with the aid of the signal profiles and the successive cycle lengths of the cardiac cycles are determined with the aid of the determined times, wherein typical patterns in successive cycle lengths over a first number of past and successive cardiac cycles are sought after and a current or future cycle length is determined by recording cycle patterns in a second, smaller number of cycle lengths including their typical successive cycle length within the first number of current past cycle lengths, and predicting, using probabilistic methods, the cycle length that follows the last determined cycle pattern on the basis of the cycle patterns currently determined during the CT examination.

Abstract: An imaging system includes interleaved emission detectors and transmission detectors. Emission detectors and transmission detectors can be interleaved along the axis of relative patient motion. Emission detectors and transmission detectors can be interleaved orthogonal to the axis of relative patient motion. Emission detectors can be single photon emission computed tomography detectors and the transmission detectors can be x-ray computed tomography detectors.

Abstract: A method is disclosed for reconstruction of image data of an object under examination from measurement data, with the measurement data having been recorded during a rotating movement of a radiation source of a computed tomography system around the object under examination. The radiation source emits focal and extra-focal radiation. In at least one embodiment of the method, the image data is determined from the measurement data by use of an iterative algorithm. A variable is used in the iterative algorithm which contains a distribution of the extra-focal radiation.

Abstract: A method is disclosed for detecting X-ray radiation from an X-ray emitter. In at least one embodiment of the method, an electric pulse with a pulse amplitude characteristic of the energy of a quantum is generated when a quantum of the X-ray radiation impinges on a sensor, wherein a number of threshold energies are predetermined. When the pulse amplitude corresponding to the respective energy is exceeded, a signal is emitted each time the pulse amplitude corresponding to a respective threshold energy is exceeded. At least one embodiment of the method permits reliable and high-quality imaging, even in image regions with high X-ray quanta rates. To this end, at least one of the threshold energies is predetermined such that it is higher than the maximum energy of the X-ray spectrum emitted by the X-ray emitter.