Method and apparatus for acquiring B1 magnetic field information

Patent metadata

Field	Value
Publication number	US-9625553-B2
Application number	US-201314096317-A
Country	US
Kind code	B2
Filing date	Dec 4, 2013
Priority date	Dec 4, 2012
Publication date	Apr 18, 2017
Grant date	Apr 18, 2017

Abstract

A system acquires RF magnetic field information (B1 magnetic field information) in response to generated radio frequency (RF) pulses applied to a target object via at least one of a plurality of RF coil elements in a magnetic resonance imaging (MRI) system. The system acquires first information comprising B1 magnetic field phase information of a B1 magnetic field formed by the respective RF coil elements and acquires second information comprising B1 magnetic field phase information of a B1 magnetic field formed by a combination of two or more of a plurality of RF coil elements. The system acquires third information comprising B1 magnetic field phase information by combining the first information and the second information and processes the first, second and third information in providing a B1 map indicating spatial distribution of a B1 magnetic field.

First claim

What is claimed is:

1. A method of acquiring B1 magnetic field information from RF magnetic field information in response to generated radio frequency (RF) pulses applied to a target object via at least one of a plurality of RF coil elements in a magnetic resonance imaging (MRI) system, the method comprising:
acquiring first information comprising B1 magnetic field phase information of a B1 magnetic field formed by the respective RF coil elements;
acquiring second information comprising B1 magnetic field phase information of a B1 magnetic field formed by a combination of two or more of the plurality of RF coil elements;
acquiring phase information of transmission RF magnetic fields (B1+ magnetic fields) as third information comprising B1 magnetic field phase information by eliminating phase information of a reception RF magnetic field (B1− magnetic field) from the first information by using the second information;
applying RF pulses to the target object by activating the plurality of RF coil elements using signals having individual magnitudes and phases, respectively, based on the third information,
receiving responses corresponding to the RF pulses from the target object; and
generating an MR image regarding to the target object based on the response.

2. The method of claim 1 , wherein the B1+ magnetic fields comprise magnetic field elements which rotate in a same direction as a direction in which a magnetization vector of at least one atomic nucleus, which is magnetized by a main magnetic field of the MRI system and is included in a target object, rotates.

3. The method of claim 2 , further comprising acquiring the phase information of the B1− magnetic field by combining the first information and the second information, wherein the B1− magnetic field comprises a magnetic field element which rotates in a direction opposite to the direction in which the B1+ magnetic field rotates.

4. The method of claim 1 , wherein the acquiring of the first information formed by the respective RF coil elements comprises:
for individual coils of the plurality of RF coil elements,
selecting one of the plurality of RF coil elements;
applying the RF pulses to the target object via the selected RF coil element; and
acquiring the first information using echo response signals received from the target object.

5. The method of claim 1 , wherein the first information comprises phase information of a B1+ magnetic field formed by the respective RF coil elements and phase information of a B1− magnetic field.

6. The method of claim 1 , wherein the acquiring of the second information comprises:
applying the RF pulses to the target object concurrently via the combination of two or more of the plurality of RF coil elements; and
acquiring the second information based on echo response signals received from the target object.

7. The method of claim 1 , wherein the acquiring of the second information comprises acquiring the second information by concurrently driving the plurality of RF coil elements.

8. The method of claim 1 , wherein the second information comprises phase information of a B1+ magnetic field formed by the combination of two or more of the plurality of RF coil elements and phase information of a B1− magnetic field.

9. The method of claim 1 , wherein the MRI system is an MRI system using a high magnetic field equal to 3 Tesla (T) or higher.

10. A computer readable recording medium having recorded thereon a computer program for implementing the method of claim 1 .

11. An MRI system comprising at least one of a plurality of radio frequency (RF) coil elements for acquiring B1 magnetic field information in response to RF pulses applied to a target object and a control unit which controls the plurality of RF coil elements,
the control unit configured to:
acquire first information comprising B1 magnetic field phase information of a B1 magnetic field formed by the respective RF coil elements;
acquire second information comprising B1 magnetic field phase information of a B1 magnetic field formed by a combination of two or more of a plurality of RF coil elements; and
acquire phase information of transmission RF magnetic fields (B1+ magnetic fields) as third information by eliminating phase information of a reception RF magnetic field (B1− magnetic field) from the first information by using the second information,

the plurality of RF coil elements configured to:
apply RF pulses to the target object by activating the plurality of RF coil elements using signals having individual magnitudes and phases, respectively, based on the third information, and
receive responses corresponding to the RF pulses from the target object,

wherein the control unit generate an MR image regarding to the target object based on the responses.

12. The MRI system of claim 11 , wherein the B1+ magnetic fields comprise magnetic field elements which rotate in a same direction as a direction in which a magnetization vector of at least one atomic nucleus, which is magnetized by a main magnetic field of the MRI system and is included in a target object, rotates.

13. The MRI system of claim 12 , wherein the control unit is further configured to acquire the phase information of the B1− magnetic field by combining the first information and the second information, and
the B1− magnetic field comprises a magnetic field element rotating in a direction opposite to the direction in which the B1+ magnetic fields rotate.

14. The MRI system of claim 11 , wherein the control unit is configured to:
for individual coils of the plurality of RF coil elements,
select one of the plurality of RF coil elements;
apply the RF pulses to the target object via the selected RF coil element;
receive echo response signals from the target object; and
acquire the first information based on the echo response signals received from the target object.

15. The MRI system of claim 11 , wherein the first information comprises phase information of a B1+ magnetic field formed by the respective RF coil elements and phase information of a B1− magnetic field.

16. The MRI system of claim 11 , wherein the control unit is configured to:
apply the RF pulses to the target object concurrently using the combination of two or more of the plurality of RF coil elements and
receive echo response signals from the target object, and
acquire the second information using the echo response signals.

17. The MRI system of claim 11 , wherein the control unit acquires the second information by concurrently driving the plurality of RF coil elements.

18. The MRI system of claim 11 , wherein the second information comprises phase information of a B1+ magnetic field formed by the combination of two or more of the plurality of RF coil elements and phase information of a B1− magnetic field.

19. The MRI system of claim 11 , wherein the MRI system uses a high magnetic field equal to 3 Tesla (T) or higher.

Assignees

• Samsung Electronics Co Ltd
• Ind Acad Coop Found Kyunghee Univ

Inventors

• Lee Ju-Hyung
• Lee Soo-Yeol

Classifications

• G01R33/5659 Primary

  caused by a distortion of the RF magnetic field, e.g. spatial inhomogeneities of the RF magnetic field (G01R33/56509, G01R33/56518, G01R33/56536 take precedence) · CPC title

• G01R33/246

  Spatial mapping of the RF magnetic field B1 · CPC title