The present disclosure relates biomedical imaging and analysis. More specifically, the present disclosure relates to MRI image generation using a pre-learned spatial subspace.
Real-time magnetic resonance (MR) imaging is important in monitoring MR-based therapies and treatments. However, generating on-the-fly images with sufficient temporal resolution to track these therapies and treatments can be difficult. Due to the complexities involved, the generation of these on-the-fly images can be very slow. Thus, there is a need for new systems and methods that can more efficiently and rapidly construct on-the-fly MR images.
According to aspects of the present disclosure, a method for performing magnetic resonance (MR) imaging on a subject comprises applying a first pulse sequence to a region of interest of the subject; in response to applying the first pulse sequence to the object, obtaining initial k-space data D1; constructing a spatial factor Ux and a temporal factor Φ from the initial k-space data D1; determining a transformation T that maps the initial k-space data D1to the temporal factor Φ to the initial k-space data D1; applying a second pulse sequence to the object; obtaining real-time k-space data D2 at time t; and constructing a real-time image A, where A=UxTD2, real-time image A showing the region of interest of the subject at time t.
According to aspects of the present disclosure, a system for performing magnetic resonance (MR) imaging on a subject comprises a magnet operable to provide a magnetic field; a transmitter operable to transmit to a region within the magnetic field; a receiver operable to receive a magnetic resonance signal from the region with the magnetic field; and one or more processors operable to control the transmitter and the receiver, the one or more processors being configured to cause the following method to be performed: applying a first pulse sequence to a region of interest of the subject; in response to applying the first pulse sequence to the object, obtaining initial k-space data D1; constructing a spatial factor Ux and a temporal factor Φ from the initial k-space data D1; determining a transformation T that maps the initial k-space data D1 to the temporal factor Φ; applying a second pulse sequence to the object; obtaining real-time k-space data D2 at time t; and constructing a real-time image A, where A=UxTD2, real-time image A showing the region of interest of the subject at time t.
According to aspects of the present disclosure, a non-transitory machine-readable medium having stored thereon instructions for performing magnetic resonance (MR) imaging on a subject, which when executed by at least one processor, cause the following method to be performed: applying a first pulse sequence to a region of interest of the subject; in response to applying the first pulse sequence to the object, obtaining initial k-space data D1; constructing a spatial factor Ux and a temporal factor Φ from the initial k-space data D1; determining a transformation T that maps the initial k-space data D1 to the temporal factor Φ; applying a second pulse sequence to the object; obtaining real-time k-space data D2 at time t; and constructing a real-time image A, where A=UxTD2, real-time image A showing the region of interest of the subject at time t.
According to aspects of the present disclosure, a method for performing magnetic resonance (MR) imaging on a subject comprises obtaining a set of images of the subject; constructing a spatial factor Ux and a temporal factor Φ from the set of images of the subject; determining a transformation T that maps k-space data to the temporal factor Φ, the k-space data corresponding to the set of images; applying a pulse sequence to the object; obtaining real-time k-space data D at time t; and constructing a real-time image A, where A=UxTD, real-time image A showing the region of interest of the subject at time t.
According to aspects of the present disclosure, a system for performing magnetic resonance (MR) imaging on a subject comprises a magnet operable to provide a magnetic field; a transmitter operable to transmit to a region within the magnetic field; a receiver operable to receive a magnetic resonance signal from the region with the magnetic field; and one or more processors operable to control the transmitter and the receiver, the one or more processors being configured to cause the following method to be performed: obtaining a set of images of the subject; constructing a spatial factor Ux and a temporal factor Φ from the set of images of the subject; determining a transformation T that maps k-space data to the temporal factor Φ, the k-space data corresponding to the set of images; applying a pulse sequence to the object; obtaining real-time k-space data D at time t; and constructing a real-time image A, where A=UxTD, real-time image A showing the region of interest of the subject at time t.
According to aspects of the present disclosure, a non-transitory machine-readable medium having stored thereon instructions for performing magnetic resonance (MR) imaging on a subject, which when executed by at least one processor, cause the following method to be performed: obtaining a set of images of the subject; constructing a spatial factor Ux and a temporal factor Φ from the set of images of the subject; determining a transformation T that maps k-space data to the temporal factor Φ, the k-space data corresponding to the set of images; applying a pulse sequence to the object; obtaining real-time k-space data D at time t; and constructing a real-time image A, where A=UxTD, real-time image A showing the region of interest of the subject at time t.
The foregoing and additional aspects and implementations of the present disclosure will be apparent to those of ordinary skill in the art in view of the detailed description of various embodiments and/or implementations, which is made with reference to the drawings, a brief description of which is provided next.
The foregoing and other advantages of the present disclosure will become apparent upon reading the following detailed description and upon reference to the drawings.
While the present disclosure is susceptible to various modifications and alternative forms, specific implementations and embodiments have been shown by way of example in the drawings and will be described in detail herein. It should be understood, however, that the present disclosure is not intended to be limited to the particular forms disclosed. Rather, the present disclosure is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the present disclosure as defined by the appended claims.
While the present disclosure has been described with reference to one or more particular embodiments or implementations, those skilled in the art will recognize that many changes may be made thereto without departing from the spirit and scope of the present disclosure. Each of these embodiments or implementations and obvious variations thereof is contemplated as falling within the spirit and scope of the present disclosure. It is also contemplated that additional embodiments implementations according to aspects of the present disclosure may combine any number of features from any of the embodiments or implementations described herein.
Magnetic resonance-based imaging (MR imaging) is a technique most often used for imaging the human body that takes into account principles of nuclear magnetic resonance. For example, doctors and other medical professionals often use MR imaging to view tissue within the human body. Nuclear magnetic resonance is a phenomenon in which nuclei (such as protons in body tissue) localized in a magnetic field emit energy that can be detected. This energy that is detected can be used to create an image. MR imaging generally involves two principle steps. First, the magnetic moment of the nuclei (a vector property of a nucleus caused by the intrinsic spin property of elementary particles) are aligned (or polarized) by the presence of an external magnetic field. While in the presence of this external magnetic field, the magnetic moment of each nuclei will generally precess about an axis parallel to the magnetic field. The rate of this precession ω is generally proportional to γB0, where B0 is the magnitude of the external magnetic field, and γ is the gyromagnetic ratio of the nuclei, which is the ratio the nuclei's magnetic moment to its angular momentum. The rate of the precession ω is considered the nuclei's resonant frequency.
The second principle step in MR imaging is to apply an electromagnetic pulse sequence (usually a radiofrequency, or RF, pulse) to the nuclei. When the frequency of the RF pulses sequence is generally equal to the resonant frequency of the nuclei, the nuclei absorb the energy of the RF pulse and the magnetic moments are rotated out of alignment with the magnetic field. The magnetic moments of the excited nuclei eventually re-align within the presence of the external magnetic field in a process known as relaxation, which has two components, T1 and T2. T1 relaxation describes how the component of the magnetic moment parallel to the external magnetic field returns to its initial value. T2 relaxation describes how the components of the magnetic moment perpendicular to the external magnetic field return to their initial value. Because the magnetic moments of nuclei in the external magnetic field without the RF pulse sequence applied are generally parallel to the external magnetic field, T1 relaxation generally describes how parallel component of the magnetic moment returns to its maximum value, while T2 relaxation generally describes how the perpendicular components of the magnetic moment decay. The nuclei of different material relax at different rates and thus emit differing signals, which can be detected and used to form an image identifying the different materials.
Dynamic MR imaging can produce a spatiotemporal image sequence I(x, t), which is a function of (i) spatial location within the subject and (ii) one or more time-varying parameters related to the dynamic processes. The spatial location is denoted by vector x=[x1, x2, x3]T, which contains up to three spatially-varying parameters xi. The time-varying parameters are denoted by vector t=[t1, t2, . . . , tR]T containing R time-varying independent variables ti. The imaging data obtained from the MR imaging is generally from a specific region of interest of the subject. In an example, the region of interest could be the subject's abdomen or chest. In other examples, the region of interest of the subject is more specific. For example, the region of interest could be an organ, such as the subject's liver, lungs, heart, pancreas, brain, prostate, breast, or any other organ.
The imaging data is dependent on or related to the spatially-varying and time-varying parameters of the region of interest of the subject referred to above. The spatially-varying parameters include a voxel location, a contrast agent kinetic parameter, or a diffusion parameter (which includes changing strength, changing direction, or both). The spatially-varying parameters can additionally or alternatively be related to physical motion of the region of interest of the subject. The time-varying parameters can include, but is not limited to: the phase of the subject's heart within a cardiac cycle; the position of the subject's lungs, chest wall, or other organs within a respiratory cycle; a position of a dome of a liver during respiration; relaxation parameters such as T1, T1p (also known as T1-rho), T2, T2* (also known as T2-star), an inversion time (or other time since magnetization preparation); a diffusion weighting strength; a diffusion weighting direction; an echo time; a dynamic contrast enhancement phase; a flip angle; an elapsed time since the start of scanning; elastographic wave propagation, a phase offset of elastographic excitation waves; a frequency offset and duration of saturation preparation pulses (e.g., for chemical exchange saturation transfer); a duration of magnetization transfer preparation pulses; a chemical exchange saturation transfer, a spectral position (e.g., for spectroscopy); a flow encoding strength; a flow encoding direction; free induction decay, or the general passage of time.
Some of the spatially-varying parameters can also be time-varying, and some of the time-varying parameters can also be spatially-varying. For example, cardiac motion is generally a time-varying parameter, while the relaxation parameters, the contrast agent kinetic parameter, and the diffusion parameter are generally time-varying. Generally, the imaging data is indicative of the value or magnitude of the spatially-varying parameters and/or the time-varying parameters. In another example, the region of interest is the subject's abdomen containing their liver, and the spatially-varying parameter that is being measured is the T1 relaxation parameter. The T1 relaxation parameter can be spatially-varying, meaning that the value of the T1 relaxation parameter at a first physical location within the subject's liver can be different than the value of the T1 relaxation parameter at a second physical location within the subject's liver. In a resulting image showing the value measured T1 relaxation parameter, different locations in the image (corresponding to different physical locations within the subject's liver) will show different values. In some implementations, the spatially-varying parameters can also be time-varying. In other implementations, the spatially-varying parameters can additionally or alternatively be related to physical motion of the region of interest of the subject. In general, the techniques disclosed herein can be used to perform dynamic imaging that resolves parameters that can vary across space and time.
The image sequence I(x, t) can be represented as a matrix A:
Matrix A can be decomposed as:
In this formulation, J is the total number of voxels in the image, and Nt is the number of time points. Ux E CJ×L contains L spatial basis functions with J total voxels and is known as a spatial factor. Ux contains one or more spatial basis functions that describe the properties of the spatially-varying parameters. Ux is formed as a spatial factor matrix. (E CL×N
Referring now to
Φt
Referring now to
At step 202, initial k-space data D1 is obtained by applying a first pulse sequence to a region of interest of the subject. Generally, the first pulse sequence will be a “prep” pulse sequence, that is not actually used to create any images. The initial k-space data D1 includes both training data Dtr (sometimes referred to as navigator data) and imaging data Dim. The training data Dtr is data sampled frequently at a limited number of k-space locations, such as the central part of the k-space. The imaging data Dim is data acquired from the entire-space with appropriate sampling scheme, such as randomized Cartesian or golden-angle radial trajectories.
At step 204, spatial factor Ux and temporal factor Φ are obtained from the initial k-space data D1. In some implementations, the temporal factor Φ is constructed from only the training data Dtr. In other implementations, the temporal factor Φ is constructed from both the training data Dtr and the imaging data Dim. The spatial factor Ux can be reconstructed by solving the following problem:
Here, E is the signal encoding operator, Ω is the k-space undersampling operator, and R is the regularization function to explant compressed sensing.
At step 206, a transformation T is determined that maps the initial k-space data D1 to the temporal factor Φ. Because Φ are the temporal weights of Ux, any image can be generated according to A=UxTD, where D is k-space data obtained during the MR scan. Thus, with respect to the first pulse sequence, Φ=TDtr, where T is a linear transform given by T ∈L×M that maps the training data Dtr to the temporal factor Φ. For an individual time point t=ts, the training data dtr,t
In a long scan with periodic signal evolution, the spatial factor Ux and the transformation T should remain static during the acquisition process, unless abrupt body motion or unexpectedly-introduced contrast mechanisms force the new images outside the range of Ux. Thus, T can be determined using only the first pulse sequence (e.g., the prep pulse sequence), according to the following equation: T=Dtr+Φ. Here, Dtr+ is the pseudo-inverse of Dtr. By determining the spatial factor Ux, a pre-learned spatial subspace is obtained. By determining the transformation T, the pre-learned spatial subspace can then be used during real-time imaging. In some implementations, the pre-learned spatial subspace can have contributions from different image contrasts, such as T1-weighting, T2-weighting, or proton density-weighting.
At step 208, real-time k-space data D2 is obtained by applying a second pulse sequence to the region of interest of the subject. Generally, the real-time k-space data D2 can be just real-time training data, e.g., a single k-space line or trajectory.
Finally, at step 210, a real time image A of the region of interest of the subject is constructed at time t, where A=UxTD2. Because Ux and T were determined from the first pulse sequence applied to the subject (e.g., the prep pulse sequence), and because Ux and T remain unchanged throughout data acquisition in the absence of abrupt movement and unexpectedly-introduce contrast mechanisms, real-time images can quickly be generated during a live scan simply by acquiring the real-time k-space data D2. In implementations where the real-time k-space data D2 is only training data obtained at time t=ts, the notation D:,t
When the above method is used for non-steady-state sequences with periodic signal evaluation, such as sequences with inversion recovery, saturation recovery, or T2 preparation modules, the temporal factor (contains the information not only about respiratory motion, but also contrast changes. In retrospective reconstruction, the raw data sampled at different motion states and different time points along the signal recovery curve can be grouped into different bins to generate images along one specific time dimension. Similarly, there is also a need during the second pulse sequence to separate the motion information and contrast information, so that real-time images can be displayed with a stable contrast, e.g., T1 weighted (T1w), T2 weighted (T2w), or proton density weighted (PDw), while maintaining the true motion state. This can be achieved by projecting real-time temporal factor Φ onto Bloch-simulated subspaces of different contrasts. First, an auxiliary temporal factor (Bloch is generated from the singular value decomposition of a Bloch simulated training dictionary, based on the sequence structure. It contains the information only about contrast change. Second, the temporal factor Φ learned from the first pulse sequence is projected onto ΦBloch. This gives Φcc, the “contrast change” part of Φ: Φcc=ΦΦBloch+ΦBloch, where ΦBloch+ is the pseudo-inverse of ΦBloch.
Last, the image contrast at any time t=tc can be synthesized in the second pulse sequence scan by replacing Φt
By using a sequence in which multiple image contrasts present along the signal evolution, multi-contrast real-time images can be generated using several different tc 's pointing at different image contrasts.
In some implementations, there is bulk motion during the scan. The bulk motion can be the result of the subject moving during the can, but can have other causes. In these implementations, differences between D1 and D2 can be detected, and Ux can be updated before applying transformation T. For example, a 1 millimeter bulk motion shift can be detected and corrected for.
In some implementations, the real-time k-space data D:,t
While
The images in
The images in
In some cases, abrupt motion can present difficulties when obtaining images using the techniques disclosed herein. However, abrupt motion can easily detected by setting an appropriate acceptable range for the principal contrast-transferred temporal weighting function (α1). Any images corresponding to times when α1 exceeds the appropriate acceptable range can be rejected for display.
Aspects of the present disclosure can be used during MR-guided radiation therapy, which generally includes a planning phase with the radiation beam off, and a treatment phase with the radiation beam on. The planning phase can simultaneously serve as the first pulse sequence to learn the spatial factor Ux and the linear transformation T, and the treatment phase can simultaneously be used to generate real-time multi-contrast 3D images with low latency.
While method 200 discusses obtaining the spatial factor Ux and the temporal factor Φ from the initial k-space data D1, in some implementations the spatial factor Ux and the temporal factor Φ can be obtained from a set of already-reconstructed images themselves. In some implementations, a set of images of the subject is obtained through any suitable technique. In some examples, the set of images is obtained from the first pulse sequence. In other examples, the set of images is obtained from pulse sequences other than the first pulse sequence. Then, Ux and Φ can be obtained from these images themselves, instead of directly from the obtained data. The transformation T can then be determined. In these implementations, the transformation T maps the k-space data corresponding to the set of images, to the temporal factor Φ. The second pulse sequence can then be applied to the subject as in method 200 to obtain the real-time k-space data, and the real-time image can be constructed using the spatial factor Ux, the temporal factor Φ, and the real-time k-space data obtained with the second pulse sequence. In implementations where the set of images is obtained from the first pulse sequence, the set of images is constructed from the training data D1, and then the spatial factor Ux and the temporal factor Φ are obtained from the set of images. In implementations where the set of images is obtained from a pulse sequence other than the pulse sequence, the set of images is constructed from data resulting from the pulse sequence, and then the spatial factor Ux and the temporal factor Φ are obtained from the set of images. Generally, the spatial factor Ux and the temporal factor Φ can be obtained from any set of images of the subject, so long as the set of images are from the same target location on the subject.
Aspects of the present disclosure can be implemented using a variety of hardware. One such implementation is illustrated in
The RF transmission system 708 is used to apply the RF pulse sequence that provides energy to the protons in the sample to rotate their magnet moments out of alignment with the external magnetic field, and saturates the solute material protons. The RF transmission system 708 generally includes a frequency generator (such as an RF synthesizer), a power amplifier, and a transmitting coil. The RF receiving system 710 receives the signals emitted by the protons in the sample as they relax back to their standard alignment. The RF receiving system 710 can a receiving coil to receive the emitted signals, and a pre-amplifier for boosting the received signals and ensuring the signals are suitable for processing. In some implementations, the RF receiving system 710 can include a signal processing component that processes the received signals to provide data that is usable by the processing device 712. Each of the component of the imaging apparatus can be disposed within one or more housings. In some implementations, the imaging apparatus 702 is a 3.0 Tesla clinical scanner equipped with an 18-channel phase array body coil.
The processing device 712 can be communicatively coupled to the imaging apparatus 702, and can include a processor 714, processor-executable memory 716, a display 718, and a user input device 720. The processing device 712 is used to manage the operations of the imaging apparatus 702, and can thus be configured to cause the imaging apparatus 702 to perform dynamic imaging according to the principles disclosed herein. The memory 716 can contain instructions that when executed by processor 714, cause the imaging apparatus 702 to operate as desired. The memory 716 can also store the data obtained from the MRI sequence.
The reconstruction workstation 722 is generally a separate processing device or system that receives the training data and the imaging data from the processing device 712. The reconstruction workstation can be configured as necessary to perform any analysis of the data, include any or all of the steps in method 100 and method 200. In some implementations, the neural network is implemented on the reconstruction workstation 722. In other implementations, the neural network is implemented on separate hardware that can communicate with the reconstruction workstation 722.
In some implementations, a non-transitory, machine-readable medium has instructions stored thereon for implementing any of any of the methods or processes discussed herein. A machine processor is configured to executed the instructions in order to perform these methods or processes.
Aspects of the present disclosure can be implemented on a variety of types of processing devices, such as general purpose computer systems, microprocessors, digital signal processors, micro-controllers, application specific integrated circuits (ASICs), programmable logic devices (PLDs) field programmable logic devices (FPLDs), programmable gate arrays (PGAs), field programmable gate arrays (FPGAs), mobile devices such as mobile telephones, personal digital assistants (PDAs), or tablet computers, local servers, remote servers, wearable computers, or the like.
Memory storage devices of the one or more processing devices can include a machine-readable medium on which is stored one or more sets of instructions (e.g., software) embodying any one or more of the methodologies or functions described herein. The instructions can further be transmitted or received over a network via a network transmitter receiver. While the machine-readable medium can be a single medium, the term “machine-readable medium” should be taken to include a single medium or multiple media (e.g., a centralized or distributed database, and/or associated caches and servers) that store the one or more sets of instructions. The term “machine-readable medium” can also be taken to include any medium that is capable of storing, encoding, or carrying a set of instructions for execution by the machine and that cause the machine to perform any one or more of the methodologies of the various embodiments, or that is capable of storing, encoding, or carrying data structures utilized by or associated with such a set of instructions. The term “machine-readable medium” can accordingly be taken to include, but not be limited to, solid-state memories, optical media, and magnetic media. A variety of different types of memory storage devices, such as a random access memory (RAM) or a read only memory (ROM) in the system or a floppy disk, hard disk, CD ROM, DVD ROM, flash, or other computer readable medium that is read from and/or written to by a magnetic, optical, or other reading and/or writing system that is coupled to the processing device, can be used for the memory or memories.
While aspects of the present disclosure have been described with reference to one or more particular implementations, those skilled in the art will recognize that many changes may be made thereto without departing from the spirit and scope of the present disclosure. Each of these implementations and obvious variations thereof are contemplated as falling within the spirit and scope of the present disclosure. It is also contemplated that additional implementations according to aspects of the present disclosure may combine any number of features from any of the implementations described herein.
This application claims priority to and the benefit of U.S. Provisional Patent Application No. 63/019,791, filed May 4, 2020, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | |
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63019791 | May 2020 | US |
Number | Date | Country | |
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Parent | 17997639 | Oct 2022 | US |
Child | 18598544 | US |