Dynamic adjustment of gradient rise times for MR HF pulse sequences
View Patent ↗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.
1. A method for image data acquisition using a magnetic resonance system, the method comprising:
irradiating, in order to excite nuclear spin signals, a sequence of high-frequency pulses into an examination subject while gradients are simultaneously switched for position encoding of the nuclear spin; and
adjusting rise times of the gradients used during the sequence dynamically with each high-frequency pulse irradiation of the sequence.
2. The method as claimed in claim 1 , wherein adjusting the rise times comprises adjusting, with each high-frequency pulse irradiation, the rise times such that the gradients exhibit a constant value only during a period of time from a start of pulse of the high-frequency pulse to an end of image data acquisition, and the remaining time is used as the rise time.
3. The method as claimed in claim 2 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.
4. The method as claimed in claim 2 , further comprising:
capturing, after the start of pulse of the high-frequency pulse, essentially only one raw data point in a k-space data set associated with the image data acquisition; and
filling the k-space data set line by line with raw data points captured from the sequence.
5. The method as claimed in claim 4 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.
6. The method as claimed in claim 1 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.
7. A magnetic resonance system comprising:
a basic field magnet;
a gradient field system;
a high-frequency antenna; and
a control unit configured to:
drive the gradient field system and the high-frequency antenna to irradiate, in order to excite nuclear spin signals, a sequence of high-frequency pulses into an examination subject while gradients are simultaneously switched for position encoding of the nuclear spin;
adjust rise times of gradients of the gradient field system dynamically with each high-frequency pulse irradiation of the sequence;
receive measurement signals captured by the high-frequency antenna;
evaluate the measurement signals; and produce magnetic resonance images.
8. A computer program product that is loadable directly into a non-transitory computer-readable storage medium of a programmable control unit of a magnetic resonance system, the computer program product including instructions for image data acquisition using the magnetic resonance system, the instructions being executable by the programmable control unit to:
irradiate, in order to excite nuclear spin signals, a sequence of high-frequency pulses into an examination subject while gradients are simultaneously switched for position encoding of the nuclear spin; and
adjust rise times of the gradients used during the sequence dynamically with each high-frequency pulse irradiation of the sequence.
9. In a non-transitory computer-readable storage medium that stores instructions executable by one or more processors to acquire image data using a magnetic resonance system, the instructions comprising:
irradiating, in order to excite nuclear spin signals, a sequence of high-frequency pulses into an examination subject while gradients are simultaneously switched for position encoding of the nuclear spin; and
adjusting rise times of the gradients used during the sequence dynamically with each high-frequency pulse irradiation of the sequence.
10. The non-transitory computer-readable storage medium as claimed in claim 9 , wherein adjusting the rise times comprises adjusting, with each high-frequency pulse irradiation, the rise times such that the gradients exhibit a constant value only during a period of time from a start of pulse of the high-frequency pulse to an end of image data acquisition, and the remaining time is used as the rise time.
11. The non-transitory computer-readable storage medium as claimed in claim 10 , wherein the instructions further comprise:
capturing, after the start of pulse of the high-frequency pulse, essentially only one raw data point in a k-space data set associated with the image data acquisition; and
filling the k-space data set line by line with raw data points captured from the sequence.
12. The non-transitory computer-readable storage medium as claimed in claim 10 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.
13. The non-transitory computer-readable storage medium as claimed in claim 11 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.
14. The non-transitory computer-readable storage medium as claimed in claim 9 , wherein a pointwise encoding time reduction with radial acquisition (PETRA) sequence is used as the sequence.