Method and magnetic resonance apparatus for acquiring magnetic resonance dataset with reduced susceptibility artifacts in the reconstruction image
US-2017248672-A1 · Aug 31, 2017 · US
US10401460B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10401460-B2 |
| Application number | US-201715442729-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 27, 2017 |
| Priority date | Feb 29, 2016 |
| Publication date | Sep 3, 2019 |
| Grant date | Sep 3, 2019 |
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In a method and apparatus for recording a magnetic resonance dataset of a volume of interest of an object, at least one gradient moment is calculated as a function of at least one jump in susceptibility that is present in the volume of interest, between two sections of the volume of interest. An excitation pulse is radiated and at least one compensation moment is activated in a part volume of the volume of interest, for the at least partial compensation of a gradient moment caused by the jump in susceptibility. The signal generated by the excitation pulse is read out.
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The invention claimed is: 1. A method for acquiring a magnetic resonance (MR) dataset of volume of interest of a subject, said method comprising: providing a processor with an electronic input that designates at least one jump in susceptibility that exists in said volume of interest between two sections of said volume of interest; in said processor, calculating at least one gradient moment dependent on said at least one jump in susceptibility; from said processor, operating an MR data acquisition scanner to execute an MR data acquisition sequence, consisting of gradients pulses and radio-frequency (RF) pulses, that includes radiation of an excitation pulse that excites nuclear spins in said volume of interest; for only a limited time during execution of said sequence, operating said MR data acquisition scanner to activate, as part of said sequence, a compensating field comprising at least one finite compensation moment that is effective in a portion of said volume of interest to at least partially compensate said gradient moment caused by said jump in susceptibility; from said processor, operating said MR data acquisition scanner, at a time in said sequence that does not encompass said limited time, to read out signals produced by said nuclear spins resulting from said excitation pulse; and from said processor, making the read out signal available from the processor in electronic form, as a data file. 2. A method as claimed in claim 1 comprising operating said MR data acquisition scanner to activate a gradient field, as said compensation field that generates said compensation moment. 3. A method as claimed in claim 1 comprising operating said MR data acquisition scanner to radiate a radio-frequency pulse, as said compensation field that generates said compensation moment. 4. A method as claimed in claim 1 comprising operating said MR data acquisition scanner to apply said compensation moment only in one sub-region of said region of interest. 5. A method as claimed in claim 4 wherein said one sub-region is selected as a sub-region of said region of interest in which said at least one jump in susceptibility occurs. 6. A method as claimed in claim 1 comprising using a gradient-echo sequence as said magnetic resonance data acquisition sequence. 7. A method as claimed in claim 6 comprising using a gradient echo imaging sequence as said gradient echo sequence. 8. A method as claimed in claim 1 wherein said subject is a patient, and comprising operating said MR data acquisition scanner to apply said gradient moment in a head region of the patient. 9. A method as claimed in claim 8 wherein said head region comprises at least one of the nose of the patient, the frontal sinus of the patient, or an auditory canal of the patient. 10. A method as claimed in claim 1 wherein the subject is a patient, and comprising operating said MR data acquisition scanner to apply said compensation moment in a region of the upper body of the patient. 11. A method as claimed in claim 10 comprising applying said compensation moment in a region containing the lungs of the patient. 12. A method as claimed in claim 1 comprising providing said computer with a further electronic input that describes a condition in said MR data acquisition scanner that has an effect on said at least one jump in susceptibility, and, in said processor, calculating said gradient moment using said electronic input and said at least one further electronic input. 13. A method as claimed in claim 12 wherein said MR data acquisition scanner comprises a basic field magnet that, during said sequence, generates a basic magnetic field (B 0 field), and wherein said further electronic input is an electronic designation of a B 0 map that depicts said B 0 field in at least a portion of said volume of interest. 14. A method as claimed in claim 12 wherein said excitation pulse produces a B 1 field in said MR data acquisition scanner, and wherein said further electronic input is an electronic designation of a B 1 map that depicts said B 1 field in at least a portion of said volume of interest. 15. A method as claimed in claim 12 wherein said further electronic input is a navigator echo. 16. A non-transitory, computer-readable data storage medium encoded with programming instructions, with said storage medium being loaded into a computer system of a magnetic resonance (MR) apparatus, that comprises an MR data acquisition scanner, said programming instructions causing a computer processor of said computer system, when the non-transitory, computer readable data storage medium is executed by the computer processor, to: receive an electronic input that designates at least one jump in susceptibility that exists in a volume of interest between two sections of said volume of interest; calculate at least one gradient moment dependent on said at least one jump in susceptibility; operate said MR data acquisition scanner to execute an MR data acquisition sequence, consisting of gradients pulses and radio-frequency (RF) pulses, that includes radiation of an excitation pulse that excites nuclear spins in said volume of interest; for only a limited time during execution of said sequence, operate said MR data acquisition scanner, as part of said sequence, to activate a compensating field comprising at least one finite compensation moment that is effective in a portion of said volume of interest to at least partially compensate said gradient moment caused by said jump in susceptibility; operate said MR data acquisition scanner, at a time in said sequence that does not encompass said limited time, to read out signals produced by said nuclear spins resulting from said excitation pulse; and make the read out signal available from the computer system in electronic form, as a data file. 17. A magnetic resonance (MR) apparatus comprising: an MR data acquisition scanner adapted to receive a subject therein, said subject comprising a volume of interest from which MR signals are to be acquired; a processor provided with an electronic input that designates at least one jump in susceptibility that exists in said volume of interest between two sections of said volume of interest; said processor being configured to calculate at least one gradient moment dependent on said at least one jump in susceptibility; said processor being configured to operate said MR data acquisition scanner to execute an MR data acquisition sequence consisting of gradients pulses and radio-frequency (RF) pulses, that includes radiation of an RF excitation pulse that excites nuclear spins in said volume of interest; said processor being configured to, for only a limited time during execution of said sequence, operate said MR data acquisition scanner as part of said sequence, to activate a compensating field comprising at least one finite compensation moment that is effective in a portion of said volume of interest to at least partially compensate said gradient moment caused by said jump in susceptibility; said processor being configured to operate said MR data acquisition scanner at a time in said sequence that does not encompass said limited time, to read out signals produced by said nuclear spins resulting from said excitation pulse; and said processor being configured to make the read out signal available from the processor in electronic form, as a data file.
using gradient refocusing, e.g. EPI · CPC title
due to magnetic susceptibility variations · CPC title
Assessment of an electric or a magnetic field, e.g. spatial mapping, determination of a B0 drift or dosimetry · CPC title
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