Background field removal method for MRI using projection onto dipole fields
US-9448289-B2 · Sep 20, 2016 · US
US9733318B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9733318-B2 |
| Application number | US-201214112674-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 23, 2012 |
| Priority date | Apr 22, 2011 |
| Publication date | Aug 15, 2017 |
| Grant date | Aug 15, 2017 |
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A method of observing axial magnetization (Mz) in an object (O) located in a main magnetic field (B 0 ) comprises the step of determining magnetic field intensity (B p ) in at least one magnetic field probe (P) arranged in the neighborhood of the object. The magnetic field probe comprises a magnetic resonance (MR) active substance, means for pulsed MR excitation of the substance and means for receiving an MR signal generated by said substance.
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The invention claimed is: 1. A method of observing axial magnetization (Mz) in an object (O) located in a main magnetic field (B 0 ), determining magnetic field intensity (B P ) in at least one magnetic field probe (P) arranged in the neighborhood of the object, said magnetic field probe comprising a magnetic resonance (MR) active substance, means for pulsed MR excitation of said substance and means for receiving an MR signal generated by said substance, said step of determining magnetic field intensity (B P ) comprising pulsed excitation of said substance with said means for pulsed MR excitation, said step of determining magnetic field intensity being carried out in a plurality of at least two magnetic field probes (P i , with i=1 to n, n≧2), thereby providing respective magnetic field intensities (B Pi , with i=1 to n, n≧2), said method further comprising the step of subtracting a background magnetic field (B B ) from each one of said respective magnetic field intensities Bpi, said step of determining magnetic field intensity being repeated at a predetermined sampling rate, said sampling rate being up to 100 Hz. 2. The method according to claim 1 , wherein said background magnetic field (B B ) is modeled as a linear combination of preselected basis functions ƒ 1 (r). 3. The method according to claim 2 , wherein said pulsed excitation induces nuclear magnetic resonance of said substance. 4. The method according to claim 2 , further comprising the step of obtaining from said magnetic field intensity (B P ) an observable (Az) that is proportional to said axial magnetization (Mz). 5. The method according to claim 2 , further comprising the step of manipulating nuclear magnetization of an MR active nuclear species in said object by applying at least one radiofrequency field and optionally at least one gradient field before or concomitantly with said observing of axial magnetization (Mz). 6. The method according to claim 1 , wherein said pulsed excitation induces nuclear magnetic resonance of said substance. 7. The method according to claim 6 , further comprising the step of obtaining from said magnetic field intensity (B P ) an observable (Az) that is proportional to said axial magnetization (Mz). 8. The method according to claim 6 , further comprising the step of manipulating nuclear magnetization of an MR active nuclear species in said object by applying at least one radiofrequency field and optionally at least one gradient field before or concomitantly with said observing of axial magnetization (Mz). 9. The method according to claim 6 , further comprising the step of manipulating nuclear magnetization of an MR active nuclear species in said object by applying at least one radiofrequency field and optionally at least one gradient field before or concomitantly with said observing of axial magnetization (Mz). 10. The method according to claim 1 , further comprising the step of obtaining from said magnetic field intensity (B P ) an observable (Az) that is proportional to said axial magnetization (Mz). 11. The method according to claim 10 , further comprising the step of manipulating nuclear magnetization of an MR active nuclear species in said object by applying at least one radiofrequency field and optionally at least one gradient field before or concomitantly with said observing of axial magnetization (Mz). 12. The method according to claim 1 , further comprising the step of manipulating nuclear magnetization of an MR active nuclear species in said object by applying at least one radiofrequency field and optionally at least one gradient field before or concomitantly with said observing of axial magnetization (Mz). 13. The method according to claim 12 , further comprising the step of determining a nuclear relaxation property of said MR active nuclear species from the temporal behavior of said observed axial magnetization (Mz). 14. The method according to claim 1 , wherein the object of interest is a material sample, a water sample, a sample of body liquid, a cell culture, or a plant or part thereof. 15. The method according to claim 1 , wherein the object of interest is a live human or animal, wherein said at least one magnetic field probe is mounted on a chest region, for observing field fluctuations caused by the beating heart. 16. The method according to claim 1 , wherein the object of interest is a live human or animal, wherein said observing of axial magnetization (Mz) is used to control an MRI procedure carried out in said main magnetic field. 17. The method according to claim 1 , wherein the object of interest is a live human or animal, wherein said observing of axial magnetization (Mz) is used to monitor status and/or compliance of said human or animal. 18. The method according to claim 1 wherein the object of interest is a live human or animal, wherein said observing of axial magnetization (Mz) is used to to support signal processing anellor image reconstruction. 19. The method according to claim 1 , wherein the object of interest is a live human or animal, wherein said at least one magnetic field probe is mounted on a head region, wherein said observing of axial magnetization (Mz) is used to observe field fluctuations caused by physiological processes in the brain.
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