Mr imaging with b1 mapping
US-2015042335-A1 · Feb 12, 2015 · US
US9400319B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9400319-B2 |
| Application number | US-201113880634-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 13, 2011 |
| Priority date | Nov 5, 2010 |
| Publication date | Jul 26, 2016 |
| Grant date | Jul 26, 2016 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
There is provided an MRI apparatus capable of measuring the B1 distribution of an RF transmission coil in a short time with high accuracy. In order to realize this, imaging means of the MRI apparatus includes a B1 distribution measurement sequence that includes an application of a pre-pulse by RF radiation means and a plurality of signal acquisition sequences with different elapsed time (TI) from the pre-pulse. The signal acquisition sequence uses a pulse having a small flip angle as an RF pulse and is executed before the longitudinal relaxation after the pre-pulse ends. Calculation means calculates the B1 distribution of the RF radiation means using image data with different TI acquired in the respective signal acquisition sequences.
Opening claim text (preview).
The invention claimed is: 1. A magnetic resonance imaging apparatus comprising: an RF radiation unit that radiates a high-frequency magnetic field (B1) to cause nuclear magnetic resonance in an object; an imaging unit that images the object using a B1 distribution measurement sequence that includes a signal acquisition sequence to acquire a nuclear magnetic resonance signal with elapsed time (TI) between (a) application of a high-frequency magnetic field pre-pulse and (b) application of the signal acquisition sequence; and a calculation unit that reconstructs an image of the object using the nuclear magnetic resonance signal, wherein the calculation unit calculates an irradiation magnetic field distribution of the RF radiation unit using a plurality of images with the different elapsed time. 2. The magnetic resonance imaging apparatus according to claim 1 , wherein the imaging unit acquires images by executing a plurality of B1 distribution measurement sequences in which application conditions of the high-frequency magnetic field pre-pulse are different, and the calculation unit calculates the irradiation magnetic field distribution using images acquired in the plurality of B1 distribution measurement sequences in which the application conditions of the high-frequency magnetic field pre-pulse are different. 3. The magnetic resonance imaging apparatus according to claim 2 , wherein among the plurality of B1 distribution measurement sequences, a first B1 distribution measurement sequence is a signal acquisition sequence executed without using the high-frequency magnetic field pre-pulse, and a second B1 distribution measurement sequence includes an application of the high-frequency magnetic field pre-pulse and at least two signal acquisition sequences subsequent to the application of the high-frequency magnetic field pre-pulse. 4. The magnetic resonance imaging apparatus according to claim 3 , wherein the calculation unit calculates the irradiation magnetic field distribution by solving a determinant using a ratio between the signal intensity of an image, which is obtained by reconstructing a nuclear magnetic resonance signal acquired in a signal acquisition sequence of the first B1 distribution measurement sequence, and each signal intensity of a plurality of images, which are obtained by reconstructing nuclear magnetic resonance signals acquired in a plurality of signal acquisition sequences of the second B1 distribution measurement sequence. 5. The magnetic resonance imaging apparatus according to claim 1 , wherein the imaging unit executes the B1 distribution measurement sequence for each of a plurality of cross-sections, and the calculation unit calculates the irradiation magnetic field distribution for each of the plurality of cross-sections. 6. The magnetic resonance imaging apparatus according to claim 5 , wherein the signal acquisition sequence is a multi-slice imaging sequence or a three-dimensional imaging sequence. 7. The magnetic resonance imaging apparatus according to claim 1 , wherein the imaging unit includes a plurality of the B1 distribution measurement sequences in which application conditions of the high-frequency magnetic field pre-pulse are the same, and separately acquires all pieces of data required to reconstruct the images in the plurality of B1 distribution measurement sequences. 8. The magnetic resonance imaging apparatus according to claim 1 , wherein the imaging unit executes the B1 distribution measurement sequence multiple times while changing the elapsed time, and the calculation unit reconstructs the plurality of images with the different elapsed time using nuclear magnetic resonance signals acquired in the respective B1 distribution measurement sequences. 9. The magnetic resonance imaging apparatus according to claim 1 , wherein the high-frequency magnetic field pre-pulse is a high-frequency magnetic field pulse having a flip angle of 90° or more. 10. The magnetic resonance imaging apparatus according to claim 1 , wherein the signal acquisition sequence is a pulse sequence to acquire the nuclear magnetic resonance signal by scanning k-space radially. 11. The magnetic resonance imaging apparatus according to claim 1 , wherein the RF radiation unit has a plurality of channels, the imaging unit images the object by executing the B1 distribution measurement sequence for each of the channels, and the calculation unit calculates the irradiation magnetic field distribution for each of the channels. 12. A magnetic resonance imaging apparatus comprising: an RF radiation unit that radiates a high-frequency magnetic field (B1) to cause nuclear magnetic resonance in an object; an imaging unit that images the object using a B1 distribution measurement sequence includes a plurality of signal acquisition sequences, to acquire a nuclear magnetic resonance signal, with elapsed time (TI) between application of a high-frequency magnetic field pre-pulse and each of the plurality of signal acquisition sequences with the different elapsed time, and a calculation unit that reconstructs a plurality of images with the different elapsed time of the object using the nuclear magnetic resonance signals acquired in the plurality of signal acquisition sequences with the different elapsed time, wherein the calculation unit calculates an irradiation magnetic field distribution of the RF radiation unit using a plurality of images with the different elapsed time. 13. The magnetic resonance imaging apparatus according to claim 12 , wherein, in the signal acquisition sequence, a high-frequency magnetic field pulse having a flip angle of 10° or less is repeatedly applied to acquire the nuclear magnetic resonance signal. 14. The magnetic resonance imaging apparatus according to claim 13 , wherein, in the imaging unit, the plurality of signal acquisition sequences are continuous, and the high-frequency magnetic field pulse is applied at a fixed repetition time. 15. A method for measuring the irradiation magnetic field distribution of an RF radiation unit in a magnetic resonance imaging apparatus including an RF radiation unit, the irradiation magnetic field measuring method comprising: a measurement step of executing a signal acquisition sequence to acquire a nuclear magnetic resonance signal by setting elapsed time (TI) from application of a high-frequency magnetic field pre-pulse by the RF radiation unit; an image reconstruction step of reconstructing an image of the object using the nuclear magnetic resonance signal; and an irradiation magnetic field distribution calculation step of calculating the irradiation magnetic field distribution of the RF radiation unit using the image, wherein, in the irradiation magnetic field distribution calculation step, the irradiation magnetic field distribution is calculated using a plurality of images with the different elapsed time.
involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging · CPC title
Assessment of an electric or a magnetic field, e.g. spatial mapping, determination of a B0 drift or dosimetry · CPC title
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
Image enhancement or correction, e.g. subtraction or averaging techniques {, e.g. improvement of signal-to-noise ratio and resolution} · CPC title
Spatial mapping of the RF magnetic field B1 · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.