Magnetic resonance imaging apparatus and method
View Patent ↗When imaging for sensitivity distribution measurement is performed, a whole-body coil for both transmission and reception and a specified coil used for the present imaging are used as a reception coil, while being switched. The switching of the reception coil is performed by switching between the whole-body coil and the specified coil for each echo in the same encode step. An image created from the echo obtained by the specified coil is divided by an image created from the echo obtained by the whole-body coil to calculate the sensitivity distribution of the specified coil. The sets of data used for the calculation are almost simultaneously obtained, thus providing accurate sensitivity distribution with no influence derived from the movement of a subject. The sensitivity distribution is used to correct the image obtained by the present imaging. Alternatively, the sensitivity distribution is used for the folding operation of parallel imaging.
1. A magnetic resonance imaging apparatus comprising:
magnet to generate a static magnetic field;
gradient magnetic field generator to generate a gradient magnetic field in the static magnetic field;
high-frequency magnetic field transmitter to apply a high-frequency magnetic field to an examination target placed in the static magnetic field;
receiver to receive a nuclear magnetic resonance signal generated from the examination target;
controller to control the gradient magnetic field generator, the high-frequency magnetic field transmitter and the receiver; and
signal processor to process the nuclear magnetic resonance signal,
wherein:
the receiver comprises a first reception coil and a second reception coil having a sensitivity region including a sensitivity region of the first reception coil and is wider than the sensitivity region of the first reception coil; and
the controller executes encode steps corresponding to k-space data while sequentially varying application amount of the gradient magnetic field, controls acquisition of data formed by a plurality of nuclear magnetic resonance signals, and alternately switches reception by the first reception coil and reception by the second reception coil for every one or more groups of nuclear magnetic resonance signals in at least a part of the encode step of a gradient echo sequence to measure one gradient echo after applying one high-frequency magnetic field.
2. The magnetic resonance imaging apparatus according to claim 1 , wherein the second reception coil is a whole-body coil which additionally operates as a transmission coil comprised in the high-frequency magnetic field transmitter.
3. The magnetic resonance imaging apparatus according to claim 1 , wherein the first reception coil is a local coil which receives signals from a region of interest in the examination target.
4. The magnetic resonance imaging apparatus according to claim 3 , wherein the first reception coil is a multiple coil formed by a plurality of small-sized reception coils, and sensitivity distribution regions of the respective small-sized coils are different from one another.
5. The magnetic resonance imaging apparatus according to claim 1 , wherein the controller switches the reception by the first reception coil and the reception by the second reception coil the to collect low-frequency region data in a k-space from among the encode steps corresponding to the k-space data.
6. The magnetic resonance imaging apparatus according to claim 1 , wherein the controller executes another multi-echo sequence for acquiring two or more nuclear magnetic resonance signals in one encode step, controls the receiver so that one of the two or more nuclear magnetic resonance signals is received by the first reception coil and the other signal is received by the second reception coil.
7. The magnetic resonance imaging apparatus according to claim 1 , wherein the signal processor calculates a sensitivity distribution of the first reception coil using the nuclear magnetic resonance signal received by the first reception coil and the nuclear magnetic resonance signal received by the second reception coil.
8. The magnetic resonance imaging apparatus according to claim 7 , wherein the signal processor calculates the sensitivity distribution of the first reception coil by dividing an image created using the nuclear magnetic resonance signal received by the first reception coil, by an image created using the nuclear magnetic resonance signal received by the second reception coil.
9. The magnetic resonance imaging apparatus according to claim 7 , wherein:
the controller acquires the nuclear magnetic resonance signal for imaging biological information of the examination target using the first reception coil; and
the signal processor generates an image of the biological information of the examination target using the acquired nuclear magnetic resonance signal and the sensitivity distribution of the first reception coil.
10. The magnetic resonance imaging apparatus according to claim 9 , wherein the controller executes switching of the reception by the first reception coil and the reception by the second reception coil in the imaging of the biological information of the examination target.
11. The magnetic resonance imaging apparatus according to claim 9 , wherein the controller executes measurement, which is separate from actual imaging, for acquiring the nuclear magnetic resonance signal for measuring the sensitivity distribution of the first reception signal, and executes switching of the reception by the first reception coil and the reception by the second reception coil in the measurement.
12. The magnetic resonance imaging apparatus according to claim 9 , wherein:
the first reception coil is a local coil configured to receive the signal from a region of interest in the examination target; and
the signal processor executes shading correction of the image generated from the nuclear magnetic resonance signal, using sensitivity distribution of a local coil.
13. The magnetic resonance imaging apparatus according to claim 9 , wherein:
the first reception coil is a multiple coil formed by a plurality of small-sized reception coils and the reception coils have respective different sensitivity distribution;
the controller collects the nuclear magnetic resonance signals that may cause folding in an image by executing a number of encode steps which is fewer than the number of encode steps corresponding to the k-space data; and
the signal processor generates an image without folding using sensitivity distribution of the respective small-sized reception coils at the time of generating the image using the nuclear magnetic resonance signal.
14. The magnetic resonance imaging apparatus according to claim 1 , wherein:
the reception means comprises gain measuring means configured to measure a reception gain of a reception coil; and
the controller sets reception gain of the reception means at the minimum reception gain from among the reception gains of the respective reception coils measured by the gain measuring means, at the time that the reception by the first reception coil and the reception by the second reception coil are switched.
15. The magnetic resonance imaging apparatus according to claim 1 , further comprising periodic-motion signal inputting means configured to input the signal from means to measure periodic motion of the examination target, wherein the controller, in the measurement of the nuclear magnetic resonance signal including switching of the reception by the first reception coil and the reception by the second reception coil, measures the nuclear magnetic resonance signal by synthesizing with the signal inputted by the periodic-motion signal inputting means.
16. A magnetic resonance imaging method performed by a magnetic resonance imaging apparatus including a first reception coil and a second reception coil including a sensitivity region of the first reception coil and has a sensitivity region wider than that of the first reception coil, the magnetic resonance imaging method comprising:
executing by the magnetic resonance imaging apparatus encode steps corresponding to k-space data while sequentially varying application amount of a gradient magnetic field;
controlling by the magnetic resonance imaging apparatus acquisition of data formed by a plurality of nuclear magnetic resonance signals; and
alternately switching by the magnetic resonance imaging apparatus reception by the first reception coil and reception by the second reception coil for each group of one or more nuclear magnetic resonance signals in at least a part of the encode step of a gradient echo sequence to measure one gradient echo after applying one high-frequency magnetic field.
17. The magnetic resonance imaging method according to claim 16 , wherein the second reception coil is a whole-body coil which additionally operates as a transmission coil.
18. The magnetic resonance imaging method according to claim 16 , wherein the first reception coil is a local coil configured to receive a signal from a region of interest in the examination target.
19. The magnetic resonance imaging method according to claim 18 , wherein the first reception coil is a multiple coil formed by a plurality of small-sized reception coils and each of the small-sized reception coils has a different sensitivity distribution region.
20. The magnetic resonance imaging method according to claim 16 , further comprising switching the reception by the first reception coil and the reception by the second reception coil while collecting low-frequency region data in a k-space from among the encode steps corresponding to the k-space data.