Method and apparatus for acquiring high resolution spectral data or high definition images in inhomogeneous environments
A method and apparatus for treating a sample for acquiring high-definition magnetic resonance images (MRI images) or high resolution nuclear magnetic resonance (NMR) spectra even in the presence of magnetic field distortions within one or multiple scans. The spatial nature and temporal dependence of the field inhomogeneities are determined a priori using any of several literature procedures. A static or oscillating magnetic field gradient is applied on the sample so as to endow spins at different positions within the sample with different resonance frequencies. A phase- and amplitude-modulated radiofrequency (RF) pulse is applied in unison with the magnetic field gradient so as to endow spins at different positions within the sample with a homogeneous excitation/inversion profile. The nature of the spatially-selective RF irradiation is tailored in such a way that, when added on top of the effects of the inhomogeneities, the spins' evolution phases and their signal amplitudes at the time of the acquisition become independent of the inhomogeneities. The spin signals thus created are captured and decoded, so as to obtain the spins' response as if the inhomogeneity was not present. The collected data is processed to a suitable rearrangement and Fourier analysis procedure to retrieve a final undistorted image or spectrum. The magnetic field gradient can be oscillated to impose this kind of inhomogeneity corrections on multiple spatial dimensions sequentially, or simultaneously.
1. In a method for treating a sample to acquire one of high-definition magnetic resonance images (MRI images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises the steps of: (1) acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies while simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (2) correcting field inhomogeneities at the time of acquisition to be independent of the field inhomogeneities; (3) capturing and decoding the spin signals thus created to decode at least one of the spins' spatial locations and spectroscopic responses unaffected by field inhomogeneity; and (4) retrieving from decoded signals and storing a set of data indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising effecting the correction of field inhomageneities in step (3) by continuously sweeping chirped π/2 RF pulses twice during acquisition, over an initial time to effect progressive excitation of spins and over a final time to implement regressive storage of a transverse evolution resulting in encoding t 1 effects of the shifts and couplings as a spatial pattern of stored magnetizations.
2. In a method according to claim 1 the further improvement of applying a pair of consecutive frequency-chirped π−π RF pulses spanning the shortest possible times in-between signal acquisition of step (3) and after the spins have been excited to inversion to refocus the effects of inhomogeneities acting within a predetermined dwell time Δt 2 while preserving the effects of chemical shifts.
3. In a method according to claim 1 the further improvement of oscillating the field gradient.
4. In a method according to claim 2 including the further improvement of oscillating the field gradient.
5. In a method for treating a sample to acquire one of high-definition magnetic resonance images (MRI images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises the steps of: (1) quantifying a priori the spatial nature of the field inhomogeneities; (2) acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies; (3) simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (4) correcting the spins' evolution phases and their signal amplitudes at the time of the acquisition to be independent of the field inhomogeneities by temporal shaping of the encoding pulse; (5) capturing and decoding the spin signals thus created and decoding at least one of the spins' spatial locations and spectroscopic responses unaffected by inhomogeneity; and (6) subjecting the collected decoded spin signals to a suitable procedure to retrieve and store a set of data of the sample indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising eliminating the effects of field inhomogeneities by the steps of;
(a) in addition to temporal shaping of the encoding pulse in step (4), performing one of shaping the initial field gradient and predetermining dwell time Δt;
(b) maintaining a linearity between the coordinate direction of the pulse and the acquisition time; and
(c) maintaining a constant pixel size throughout acquisition.
6. In a method according to claim 5 the further improvement of oscillating the field gradient.
7. In a method for treating a sample to acquire one of high-definition magnetic resonance images (MRI images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises the steps of: (1) acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies while simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (2) correcting field inhomogeneities at the time of acquisition to be independent of the field inhomogeneities; (3) capturing and decoding the spin signals thus created to decode at least one of the spins spatial locations and spectroscopic responses unaffected by field inhomogeneity; and (4) retrieving from decoded signals and storing a set of data indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising effecting the correction of field inhomogeneities in step (2) by applying a pair of consecutive frequency-chirped π−π RF pulses spanning the shortest possible times in-between signal acquisition of step (3) and after the spins have been excited to inversion to refocus the effects of inhomogeneities acting within a predetermined dwell time Δt 2 while preserving the effects of chemical shifts.
8. In a method according to claim 7 the further improvement of oscillating the field gradient.
9. In an apparatus for treating a sample to acquire one of high-definition magnetic resonance images (MRI images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises: (1) means for acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies while simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (2) means for correcting field inhomogeneities at the time of acquisition to be independent of the field inhomogeneities; (3) means for capturing and decoding the spin signals thus created to decode at least one of the spins' spatial locations and spectroscopic responses unaffected by field inhomogeneity; and (4) means for retrieving from decoded signals and storing a set of data indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising the means for correcting field inhomogeneities including means for continuously sweeping chirped π/2 RF pulses twice during acquisition, over an initial time to effect progressive excitation of spins and over a final time to implement regressive storage of a transverse evolution resulting in encoding t 1 effects of the shifts and couplings as a spatial pattern of stored magnetizations.
10. in an apparatus according to claim 9 the further improvement of means for applying a pair of consecutive frequency-chirped π−π RF pulses spanning the shortest possible times in-between signal acquisition and after the spins have been excited to inversion to refocus the effects of inhomogeneities acting within a predetermined dwell time Δt 2 while preserving the effects of chemical shifts.
11. In an apparatus according to claim 9 the further improvement of means for controlling the field gradient to oscillate the field gradient.
12. In an apparatus according to claim 10 the further improvement of means for controlling the field gradient for oscillating the field gradient.
13. In an apparatus for treating a sample to acquire one of high-definition magnetic resonance images (MR images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises: (1) means for quantifying a priori the spatial nature of the field inhomogeneities; (2) means for acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies; (3) means for simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (4) means for correcting the spins' evolution phases and their signal amplitudes at the time of the acquisition to be independent of the field inhomogeneities by temporal shaping of the encoding pulse; (5) means for capturing and decoding the spin signals thus created and decoding at least one of the spins' spatial locations and spectroscopic responses unaffected by inhomogeneity; and (6) means for subjecting the collected decoded spin signals to a suitable procedure to retrieve and store a set of data of the sample indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising the means for eliminating the effects of field inhomogeneities, in addition to temporal shaping of the encoding pulse; including;
(a) means for performing one of shaping the initial field gradient and predetermining dwell time Δt;
(b) first means for controlling linearity between the coordinate direction of the pulse and the acquisition time; and
(c) second means for controlling pixel size throughout acquisition.
14. In an apparatus according to claim 13 the further improvement of third means for controlling the field gradient for oscillating the field gradient.
15. In an apparatus for treating a sample to acquire one of high-definition magnetic resonance images (MRI images) and nuclear magnetic resonance (NMR) spectra, even in the presence of magnetic field distortions, within one or multiple scans that comprises the steps of: (1) means for acquiring data of the sample by applying a magnetic field gradient on the sample to endow spins at different positions within the sample with different resonance frequencies while simultaneously applying a radiofrequency (RF) pulse in unison with the magnetic field gradient to encode spins at different positions within the sample with an excitation/inversion profile; (2) means for correcting field inhomogeneities; (3) means for capturing and decoding the spin signals thus created to decode at least one of the spins' spatial locations and spectroscopic responses unaffected by field inhomogeneity; and (4) means for retrieving from decoded signals and storing a set of data indicative of one of a final undistorted image and spectrum being sought;
the improvement comprising the means for effecting the correction of field inhomogeneities including means for applying a pair of consecutive frequency-chirped π−π RF pulses spanning the shortest possible times in-between signal acquisition and after the spins have been excited to inversion to refocus the effects of inhomogeneities acting within a predetermined dwell time Δt 2 while preserving the effects of chemical shifts.
16. In an apparatus according to claim 15 including the further improvement of controlling the field gradient for oscillating the field gradient.