Embodiments of the subject matter disclosed herein relate to magnetic resonance imaging (MRI), and more particularly, to MRI radio frequency (RF) coils.
Magnetic resonance imaging (MRI) is a medical imaging modality that can produce images of an interior of a patient without x-ray radiation or other types of ionizing radiation. MRI systems utilize a superconducting magnet to create a strong, uniform, static magnetic field within a designated region (e.g., within a passage shaped to receive a patient). When a body of a patient (or portion of the body of the patient) is positioned within the magnetic field, nuclear spins associated with the hydrogen nuclei that form water within tissues of the patient become polarized. The magnetic moments associated with these spins become aligned along the direction of the magnetic field and result in a small net tissue magnetization in the direction of the magnetic field. MRI systems additionally include magnetic gradient coils that produce spatially-varying magnetic fields of smaller magnitudes relative to a magnitude of the uniform magnetic field resulting from the superconducting magnet. The spatially-varying magnetic fields are configured to be orthogonal to each other in order to spatially encode the region by creating a signature resonance frequency of the hydrogen nuclei at different locations in the body of the patient. Radio frequency (RF) coil assemblies are then used to create pulses of RF energy at or near the resonance frequency of the hydrogen nuclei. The pulses of RF energy are absorbed by the hydrogen nuclei, thereby adding energy to the nuclear spin system and adjusting the hydrogen nuclei from a rest state to an excited state. As the hydrogen nuclei relax back to the rest state from the excited state, they release the absorbed energy in the form of an RF signal. This signal is detected by the MRI system and is transformed into an image by a computer using known reconstruction algorithms.
MRI may provide higher sensitivity relative to other imaging modalities (e.g., radiography) when utilized to scan patient breast tissues. However, current breast tissue MRI scanning configurations may not have widespread usage. For example, a scan time to image breast tissue via MRI may be longer than a scan time to image other parts of a patient's body via MRI due to the need to perform separate scans for multi-plan, bilateral, and single breast images in a breast tissue MRI examination. The increased scan times may not be suitable for certain clinical applications. Additionally, current RF coil assemblies may not be shaped to comfortably conform to the body of a patient, thereby lowering patient satisfaction and increasing a distance between breasts of the patient and RF coils included within the assemblies. The increased distance may result in degradation of images produced by the MRI system, such as a reduced signal-to-noise ratio (SNR) of images produced by the MRI system. Further still, some RF coil assemblies may include eight or less RF coils, thereby further reducing the SNR compared to assemblies which include a larger number of RF coils. It is therefore desirable to provide an RF coil assembly shaped to comfortably support breasts of a patient and configured to enable bilateral scanning of the patient with an increased number of coils.
In one embodiment, an RF coil for a medical imaging device includes a first coil array housed in a first cup-shaped support structure; a second coil array housed in a second cup-shaped support structure; a third coil array flanking the first coil array; and a fourth coil array flanking the second coil array.
It should be understood that the brief description above is provided to introduce in simplified form a selection of concepts that are further described in the detailed description. It is not meant to identify key or essential features of the claimed subject matter, the scope of which is defined uniquely by the claims that follow the detailed description. Furthermore, the claimed subject matter is not limited to implementations that solve any disadvantages noted above or in any part of this disclosure.
The present invention will be better understood from reading the following description of non-limiting embodiments, with reference to the attached drawings, wherein below:
The following description relates to various embodiments of a radio frequency (RF) coil assembly. In particular, an RF coil assembly is provided for a magnetic resonance imaging (MRI) system (such as the MRI system shown by
The RF coils within each of the first RF coil array and second RF coil array may be arranged in a semi-overlapping structure as shown by
In a first embodiment, the RF coil assembly includes additional coil arrays positioned at side regions of a patient's chest and adjacent to respective cups of the bra-like support structure. Specifically, the RF coil assembly includes a third RF coil array and a fourth RF coil array (as shown by
The MRI system 10 includes the patient table 26 for placing a subject 16 (e.g., a patient) thereon. The subject 16 may be moved inside and outside of an imaging space 18 by moving the patient table 26. The imaging space 18 may be positioned within a bore 19 of a gantry 17 formed by the MRI system 10. In some examples, controller unit 25 may transmit control signals (e.g., electrical signals) to operating console unit 32 and/or display unit 33 in order to indicate a position of the patient table 26 within the imaging space 18 to an operator (e.g., user, technician, etc.) of the MRI system 10.
The operating console unit 32 includes user input devices such as a keyboard and a mouse. The operating console unit 32 is utilized by an operator, for example, to input an imaging protocol (e.g., a parallel imaging protocol) and to set a region where an imaging sequence is to be executed. Data input by the operator into the operating console unit 32 about the imaging protocol and the imaging sequence execution region is output to the controller unit 25.
The display unit 33 includes a graphical display device (e.g., computer screen) and displays an image on the graphical display device based on control signals received from the controller unit 25. The display unit 33 displays, for example, an image regarding an input item about which the operator inputs operation data from the operating console unit 32. The display unit 33 also displays a slice image of the subject 16 generated by the data processing unit 31.
The data processing unit 31 includes a computer and a recording medium (e.g., hard drive) on which a program to be executed by the computer to perform predetermined data processing is recorded. The data processing unit 31 is electrically coupled with the controller unit 25 and performs data processing based on control signals received from the controller unit 25. The data processing unit 31 is also connected to the data acquisition unit 24 and generates spectrum data by applying various image processing operations to magnetic resonance (MR) signals output from the data acquisition unit 24 (described in further detail below).
The magnetostatic field magnet unit 12 includes an annular superconducting electromagnet coupled to a toroidal vacuum vessel (e.g., gantry 17) and positioned within an interior of the toroidal vacuum vessel. The electromagnet defines a cylindrical space (e.g., bore 19) surrounding the subject 16, and generates a magnetostatic field of approximately constant magnitude and direction within the cylinder space (e.g., in a direction of the y-axis within the cylinder space as shown by reference axes 199). The magnetostatic field generated by the electromagnet may be referred to herein as a uniform magnetic field.
The MRI system 10 also includes the magnetic gradient generator 13 that generates an additional magnetic field (which may be referred to herein as a gradient magnetic field) in the imaging space 18 so as to associate the MR signals received by the local RF coils 14 with three-dimensional positional information. For example, the gradient magnetic field produced by the magnetic gradient generator 13 may have a different magnitude (e.g., a different field strength) at different locations within the imaging space 18. The magnetic gradient generator 13 includes three gradient coil systems. Each gradient coil system adjusts the magnitude of the gradient magnetic field along one of three perpendicular directions. For example, a first gradient coil system adjusts the magnitude of the gradient magnetic field in a frequency encoding direction, a second gradient coil system adjusts the magnitude of the gradient magnetic field in a phase encoding direction, and a third gradient coil system adjusts the magnitude of the gradient magnetic field in a slice selection direction. The frequency encoding direction, phase encoding direction, and slice selection direction may be defined based on input from a user (e.g., operator) of the MRI system 10 (e.g., via the operating console unit 32). More specifically, the magnetic gradient generator 13 adjusts the magnitude of the gradient magnetic field in the slice selection direction of the subject 16 in response to input from the operator. The local RF coils 14 then transmits an RF pulse to a selected slice of the subject 16 and energizes the slice (e.g., excites a spin of hydrogen nuclei within the selected slice of the subject 16). The magnetic gradient generator 13 adjusts the magnitude of the gradient magnetic field in the phase encoding direction of the subject 16 to phase encode MR signals emitted by the slice energized by the RF pulse. The magnetic gradient generator 13 then adjusts the magnitude of the gradient magnetic field in the frequency encoding direction of the subject 16 to frequency encode MR signals emitted by the slice excited by the RF pulse.
The gradient driver 23 drives the magnetic gradient generator 13 based on a control signal received from the controller unit 25 and thereby generates the gradient magnetic field in the imaging space 18. The gradient driver 23 includes three systems of driver circuits (not shown) corresponding to the three gradient coil systems included in the magnetic gradient generator 13 (as described above).
The RF coils of the MRI system 10 (e.g., local RF coils 14 and/or volumetric RF coils 15) may transmit electromagnetic pulse signals to the subject 16 positioned within the imaging space 18, with the uniform magnetic field and the gradient magnetic field extending through the imaging space 18. The local RF coils 14 are shaped, for example, to enclose the region to be imaged of the subject 16. In some examples, the local RF coils 14 may be referred to as surface coils or receiver coils. The MRI system 10 receives MR signals from the subject 16 (e.g., via the data acquisition unit 24 coupled to the RF coils) and processes the MR signals (e.g., via the data processing unit 31) in order to construct an image of a slice of the subject 16 based on the received MR signals.
For example, during conditions in which the subject 16 is positioned to be scanned by the MRI system 10 (e.g., during conditions in which the subject 16 is within the imaging space 18), spins of hydrogen nuclei within the tissues of the subject 16 may be aligned with initial magnetization vectors resulting from a combination of the uniform magnetic field and the gradient magnetic field. The local RF coils 14 transmit, based on a control signal from the controller unit 25, an RF pulse that is an electromagnetic wave to the subject 16. The RF pulses transmitted to the subject 16 generate a high-frequency magnetic field within the slice of the subject 16 to be imaged (e.g., as selected by the operator of the MRI system 10). The high-frequency magnetic field excites a spin of hydrogen nuclei in the slice of the subject 16 and aligns the spins with different magnetization vectors relative to the initial magnetization vectors. As the spins of the excited hydrogen nuclei in the slice of the subject 16 relax and return into alignment with the initial magnetization vectors, the local RF coils 14 receive electromagnetic waves generated from the tissues of the subject 16 as a MR signals.
In some examples, the volumetric RF coils 15 may alternately (or additionally) be utilized to generate a high-frequency magnetic field similar to that described above with reference to the local RF coils 14. For example, the volumetric RF coils 15 are positioned to enclose the imaging space 18 and may produce RF pulses in a direction orthogonal to the direction of the uniform magnetic field generated by the magnetostatic field magnet unit 12 within the imaging space 18 in order to excite the hydrogen nuclei of the subject 16. The volumetric RF coils 15 are fixedly attached and coupled to the MRI system 10, unlike the local RF coils 14 which may be disconnected from the MRI system 10 and replaced with different local RF coils. Furthermore, whereas local coils such as those comprising the local RF coils 14 may transmit to and/or receive signals (e.g., transmit RF signals and/or receive MR signals) from a localized region of the subject 16 (e.g., a particular anatomical structure or slice of the subject 16), the volumetric RF coils 15 may transmit to and/or receive signals from a larger portion of the subject 16 (e.g., an entire body of the subject 16).
In one example, utilizing local RF coils 14 to receive MR signals and volumetric RF coils 15 to transmit RF signals may increase a ratio of excited hydrogen nuclei relative to non-excited hydrogen nuclei and may result in increased image clarity. However, exciting the hydrogen nuclei via the volumetric RF coils 15 may result in a larger amount of power deposited into tissues of the subject 16 via the RF signals relative to a configuration in which RF signals are instead transmitted into the subject 16 via the local RF coils 14. During conditions in which the local RF coils 14 are instead utilized to both transmit RF signals into the tissues of the subject 16 and receive MR signals from the tissues, the local RF coils may reduce an amount of power deposited into the tissues of the subject 16 by directing the RF signals towards a particular anatomical structure or slice rather than the entire body of the patient. However, it should be appreciated that the particular configuration of the local RF coils 14 and/or the volumetric RF coils 15 (e.g., imaging the entire subject 16 via the volumetric RF coils 15, or imaging a smaller portion of the subject 16 via the local RF coils 14 as described above) depends on the clinical application for which the MRI system 10 is utilized.
The RF signal driver 22 electrically coupled to the coils (e.g., volumetric RF coils 15 and/or local RF coils 14) via the T/R switch 20 includes a gate modulator (not shown), an RF power amplifier (not shown), and an RF oscillator (not shown) that are used to drive the local RF coils 14 and/or volumetric RF coils 15 to form a high-frequency magnetic field in the imaging space 18 (as described above). The RF signal driver 22 modulates the RF signal received from the RF oscillator into a signal of predetermined timing and having a predetermined envelope via the gate modulator, with the RF signal based on a control signal from the controller unit 25. The RF signal modulated by the gate modulator is amplified by the RF power amplifier and then output to the local RF coils 14 and/or volumetric RF coils 15.
The T/R switch 20 can selectively electrically couple the local RF coils 14 and/or the volumetric RF coils 15 to the data acquisition unit 24 when operating in a receive mode, and to the RF signal driver 22 when operating in a transmit mode. During conditions in which the local RF coils 14 and the volumetric RF coils 15 are both used in a single scan (e.g., during conditions in which the local RF coils 14 are configured to receive MR signals and the volumetric RF coils 15 are configured to transmit RF signals), the T/R switch 20 may direct control signals from the RF signal driver 22 to the volumetric RF coils 15 while directing received MR signals from the local RF coils 14 to the data acquisition unit 24. As described above, the volumetric RF coils 15 may be configured to operate in a transmit-only mode, a receive-only mode, or a transmit-and-receive mode. The local RF coils 14 may be configured to operate in a transmit-and-receive mode or a receive-only mode.
The data acquisition unit 24 includes a preamplifier (not shown), a phase detector (not shown), and an analog/digital converter (not shown) used to acquire the magnetic resonance signals received by the local RF coils 14 and/or volumetric RF coils 15. In the data acquisition unit 24, the phase detector phase detects, using the output from the RF oscillator of the RF signal driver 22 as a reference signal, the MR signals received by the local RF coils 14 and/or volumetric RF coils 15 (with the MR signals being amplified by the preamplifier), and outputs the phase-detected analog MR signals to the analog/digital converter for conversion into digital signals. The digital signals thus obtained are output to the data processing unit 31 electrically coupled with the controller unit 25.
The controller unit 25 includes a computer and a recording medium on which a program to be executed by the computer is recorded. The program when executed by the computer causes various parts of the system to carry out operations corresponding to pre-determined scanning. The recording medium may comprise, for example, a read-only memory (ROM), flexible disk, hard disk, optical disk, magneto-optical disk, CD-ROM, or non-volatile memory card. The controller unit 25 is connected to the operating console unit 32 and processes the operation signals input to the operating console unit 32 (e.g., input by the operator of the MRI system 10) and furthermore controls the patient table 26, RF signal driver 22, gradient driver 23, and data acquisition unit 24 by outputting control signals to them. The controller unit 25 also controls, to obtain a desired image, the data processing unit 31 and the display unit 33 based on operation signals received from the operating console unit 32.
During a scan (e.g., imaging of the subject 16 according to the examples described above), coil-interfacing cables (not shown) may be used to transmit signals between the RF coils (e.g., local RF coils 14 and volumetric RF coils 15) and other aspects of the processing system (e.g., data acquisition unit 24, controller unit 25, and so on), for example to control the RF coils and/or to receive information from the RF coils. As explained previously, in one example the volumetric RF coils 15 may transmit RF signals and the local RF coils 14 may receive MR signals. The local RF coils 14 and/or volumetric RF coils 15 may include coils that are used to transmit RF excitation signals (“transmitter coil”) and coils that receive the MR signals emitted by an imaging subject (“receive coil”). In some examples, the transmitter coils and receive coils may be the same coils (e.g., configured to both transmit RF excitation signals and receive MR signals) such that the coils are a single mechanical structure or array of structures, with the transmit/receive modes of the coils switchable by auxiliary circuitry (e.g., T/R switch 20). In other examples, the volumetric RF coils 15 and local RF coils 14 may be independent structures that are physically coupled to each other via a data acquisition unit or other processing unit.
In some examples (e.g., examples in which the transmitter coils and receive coils are not the same coils), it may be desirable to configure the receive coils to be mechanically and electrically isolated from the transmitter coils in order to achieve an increased image quality. In one example, the receive coils (e.g., local RF coils 14) may be configured to receive MR signals for a duration following transmission of RF signals from the transmitter coils (e.g., volumetric RF coils 15). However, for the duration in which the transmitter coils are transmitting RF signals, it may be desirable to electromagnetically decouple the receive coils from the transmitter coils such that the receive coils are not resonant with the transmitter coils (e.g., such that the receive coils do not receive the RF signals from the transmitter coils). Electromechanically decoupling (e.g., deactivating) the receive coils during transmission of RF signals by the transmitter coils may reduce an amount of noise produced within auxiliary circuitry coupled to the receive coils and may result in increased image quality.
RF coil assembly 200 includes a first coil array 202, second coil array 204, third coil array 206, and a fourth coil array 216 coupled to a support structure 220. The coil arrays described herein may also be referred to as coil sets. In the example shown by
The first coil array 202 is coupled to the first cup 222 and the second coil array 204 is coupled to the second cup 224 such that the first coil array 202 and second coil array 204 are each positioned at a front end of the patient during conditions in which the support structure 220 is coupled to the patient (e.g., as shown by
First coil array 202 and second coil array 204 each include a plurality of RF coils (described in further detail below with reference to
As shown, first cup 222 coupled to first coil array 202 includes a substantially circular frame 230 supporting the cup-shaped exterior surface 226. Second cup 224 coupled to second coil array 204 includes a similar circular frame 232 supporting the cup-shaped exterior surface 228. The coils of the first coil array 202 and second coil array 204 may be sewn or otherwise secured to the respective exterior surface of the support structure 220 (e.g., exterior surface 226 of first cup 222 and exterior surface 228 of second cup 224, respectively). In some examples, the coils of one or more of the coil arrays may be exposed along an interior surface of the first cup 222 and/or second cup 224. In other examples, one or more layers of fabric or other material may be fastened to the interior surface of the first cup 222 and/or second cup 224 in order to contain the coils within their respective cups.
The third coil array 206 and fourth coil array 216 each include pluralities of RF coils similar to those included by the first coil array 202 and second coil array 204, with the pluralities of RF coils secured to panels of fabric or other material forming the support structure 220. For example, the third coil array 206 may be secured to a first panel of fabric at the first side 250 of the support structure 220, and the fourth coil array 216 may be secured to a second panel of fabric at the second side 252 of the support structure 220. In the example shown by
Turning now to
The RF coils included by the first coil array 202 may be mounted (e.g., coupled) to a flexible substrate (e.g., stretchable fabric, polymer, etc.). The flexible substrate may be fabricated from a material that is substantially transparent to RF and MR signals (e.g., a material that does not absorb, reflect, or otherwise interact with RF and MR signals). For example, the substrate may be fabricated from a cloth material or any other suitable material that is flexible to enable the RF coils to be repositioned relative to each other as described below with reference to
As described above, first coil array 202 includes a plurality of individual RF coils positioned in a symmetrical, circular arrangement, similar to an arrangement of petals of a lotus flower. The RF coils are local RF coils (e.g., similar to the local RF coils 14 described above with reference to
Various axes are shown by first view 490 in order to illustrate the relative positions of the RF coils described above. Specifically, a first axis 452 intersects a midpoint of the first RF coil 400 and a midpoint of the fifth RF coil 408, a second axis 454 intersects a midpoint of the second RF coil 402 and a midpoint of the sixth RF coil 410, a third axis 456 intersects a midpoint of the third RF coil 404 and a midpoint of the seventh RF coil 412, and a fourth axis 457 intersects a midpoint of the fourth RF coil 406 and a midpoint of the eighth RF coil 414. The RF coils are arranged symmetrically such that an amount of angle between midpoints of adjacent RF coils is a same amount of angle for each pair of adjacent RF coils. For example, a first angle 458 between the midpoint of the third RF coil 404 and the midpoint of the fourth RF coil 406 (e.g., an angle between the third axis 456 and the fourth axis 457) is a same amount of angle as a second angle 460 between the midpoint of the third RF coil 404 and the midpoint of the second RF coil 402. In one example, an angle (e.g., first angle 458, second angle 460, etc.) between adjacent coils within the first coil array 202 may be 45 degrees. In other examples including a different number of coils, the amount of angle between adjacent coils may be a different amount (e.g., 36 degrees with 10 RF coils, 30 degrees with 12 RF coils, etc.).
The third coil array 206 shown by the second view 492 of
The RF coils included by the third coil array 206 are local RF coils (e.g., similar to the coils of the local RF coils 14 shown by
The flank coil arrays (e.g., third coil array 206 and fourth coil array 216) may enable imaging of a subject (e.g., subject 16 described above with reference to
The RF coil assembly 300 includes a support structure 320 similar to the support structure 220 shown by
The RF coil assembly 300 includes a first coil array 302 and a second coil array 304. The first coil array 302 and second coil array 304 each include a plurality of RF coils. In one example, the RF coils are similar to the RF coils described above with reference to
The second coil array 304 is further illustrated by
The first section 470 includes eight RF coils positioned in a symmetrical arrangement similar to the arrangement of the RF coils included by the first coil array 202 of the RF coil assembly 200, and the second section 472 includes four RF coils positioned in a symmetrical arrangement similar to the arrangement of the RF coils included by the third coil array 206 of the RF coil assembly 200. The first section 470 and second section 472 are coupled together via a third section 474. In the example shown by
During conditions in which the RF coil assembly 200 is worn by a patient, the first cup 222 supports a breast of the patient. In order to conform a shape of the first cup 222 to a shape of the body of the patient, a distance between opposing coils of the first coil array 202 may expand from a first diameter 500 shown by
The RF coil array 701 includes a plurality of RF coils 702. In some examples, each of the RF coils 702 of the RF coil array 701 may be a loop and/or butterfly coil formed of a flexible, flat, and electrically-conductive material (e.g., tin-plated copper). The RF coils 702 are configured to detect MR signals. In some examples, two or more of the RF coils 702 may overlap with each other (e.g., may be positioned in a partially or fully overlapping arrangement relative to each other). Signals transmitted by the RF coils 702 to the MRI system are electrically isolated from each other via preamplifiers 710. The preamplifiers 710 additionally amplify the MR signals transmitted by the RF coils 702 (e.g., increase an amplitude of the MR signals). In some examples, the RF coil array 701 may configured to operate in a receive-only mode in which the RF coils 702 receive MR signals (e.g., from a body of a patient) and transmit the MR signals to the MRI system (e.g., to data acquisition unit 24 shown by
The RF coil array 701 forms part of the multi-channel signal-receiver section 700 coupled to an MRI system. The signal-receiver section 700 includes a plurality of data channels (e.g., RCVR 1, RCVR 2, etc.). In some examples, the signal-receiver section 700 may include eight data channels. In other examples, the signal-receiver section 700 may include a larger or smaller number of data channels (e.g., six, ten, twelve, etc.), with the number of channels corresponding to the number of RF coils 702 utilized to form the RF coil array 701. In one example, the signal-receiver section 700 includes a multi-channel system interface 720 (e.g., a 1.5T System Interface). The multi-channel system interface 720 may be configured to include a relatively larger number of separate data channels 722 (e.g., RCVR 1, RCVR 2, etc.), with each of the data channels 722 coupled to separate RF coils (e.g., RF coils 702) of one or more RF coil arrays (e.g., RF coil array 701). For example, the multi-channel system interface may be configured to include 24 data channels, with each data channel coupled to separate RF coils of an RF coil assembly (e.g., RF coils included by the first coil array 202, second coil array 204, third coil array 206, and fourth coil array 216 of the RF coil assembly 200 shown by
The system interface 720 may include a plurality of bias control lines 724 (e.g., BIAS 1 and BIAS 2) in order to control the switching of decoupling circuits (not shown), which may be controlled, for example, using a coil configuration file stored in computer memory of the MRI system and/or based on a user input. For example, based on a user input, a particular coil configuration file may be selected to control the RF coil array 701 in a particular imaging mode (e.g., a user-selected mode of operation via controls input on a control console, such as operating console unit 32 shown by
The RF coil 702 include an RLC resonant circuit formed from a resistor 850, an inductor 852, and a capacitor 854. The RF coil 702 is connected in series to an impedance transformer 856. More specifically, the impedance transformer 856 is electrically connected between the RF coil 702 and the preamplifier 710. The impedance transformer 856 forms an impedance matching network between the RF coil 702 and the preamplifier 710. The impedance transformer 856 is configured to transform a coil impedance of the RF coil 702 into a source impedance of the preamplifier 710. The source impedance of the preamplifier 710 is represented in
In one example, the impedance transformer 856 includes a lattice-type balun. More specifically, the impedance transformer 856 includes two inductors 860 and 862 and two capacitors 864 and 866. The inductor 860 is connected in series to the capacitor 864, while the inductor 862 is connected in series with the capacitor 866. The inductor 860 and the capacitor 864 are connected in parallel to the inductor 862 and the capacitor 866. The arrangement of the lattice-type balun impedance transformer 856 produces a +/−90° phase shift. Each of the inductors 860 and 862 may be referred to herein as a “first” and/or a “second” inductor. The capacitors 864 and 866 may be referred to herein as a “first” and/or a “second” capacitor.
The impedance transformer 856 is configured to transform the coil impedance of the RF coil 702 into a relatively high source impedance ZOUT. In some examples, a “relatively high” source impedance ZOUT is at least approximately 100 ohms. Accordingly, the impedance transformer 856 is configured to transform the coil impedance of the RF coil 702 into a source impedance ZOUT of at least approximately 100 ohms. In some examples, the impedance transformer 856 is configured to transform the coil impedance of the RF coil 702 into a source impedance ZOUT of at least approximately 300 ohms, at least approximately 400 ohms, or at least approximately 500 ohms. Exemplary values for the inductors 860 and 862 include, but are not limited to, approximately 123.5 nH. Exemplary values for the capacitors 864 and 866 include, but are not limited to, approximately 51 pF.
The impedance transformer 856 also provides a blocking impedance to the RF coil 702. Transformation of the coil impedance of the RF coil 702 to a relative high source impedance ZOUT may enable the impedance transformer 856 to provide a higher blocking impedance to the RF coil 702. Because the relatively high source impedance ZOUT of the preamplifier 710 is greater than, for example, the conventional value of approximately 50 ohms, the reactance X of the inductors 860 and 862 and the capacitors 864 and 866 of the impedance transformer 856 are increased. For example, the reactance XC of each of the capacitors 864 and 866 and the reactance XL of each of the inductors 860 and 862 can be defined by the equation: XC=XL=√(R1×R2); where R1 is the coil impedance and R2 is the source impedance ZOUT. Because the input impedance ZIN of the preamplifier 710 is relatively low, the impedance transformer 856 forms a parallel resonance circuit that results in a higher impedance at an output 870 of the RF coil 702. As the reactances XC and XL increase, the blocking impedance increases because the blocking impedance is directly proportional to the values of XC and XL. The higher blocking impedance suppresses an increased amount of RF current along the RF coil 702, which may ultimately result in a higher SNR ratio because of fewer interactions between the RF coils of the RF coil array 701 and/or less correlated noise. Exemplary values for such higher blocking impedances include, for example, a blocking impedance of at least 500 ohms, and at least 1000 ohms.
The impedance transformer 856 is not limited to a lattice-type balun structure for transforming the coil impedance of the RF coil 702 into a relatively higher source impedance. Rather, any components and arrangement of the connections therebetween may be used to transform the coil impedance of the RF coil 702 into a relatively high source impedance, such as, but not limited to, other types of equivalent phase shift baluns, and/or the like.
The input circuit 982 includes an impedance transformer 984, which includes a capacitor 986 and the inductor 930. The input circuit 982 also includes a field effect transistor (FET) 988 that is electrically connected between the impedance transformer 984 and the amplifier 980, for example as shown in
The FET 988 has a relatively larger noise circle, which may be centered in the Smith Chart, for the FET 988 to yield a relatively lower noise figure. In other words, the FET 988 is capable of providing a relatively lower noise figure over a relatively broader range of source impedance ZOUT. In some examples, a “relatively larger” size of the noise circle of the FET 988 is at least approximately 0.3 decibels. In other examples, the noise circle of the FET 988 has a size of at least approximately 0.6 decibels. The size of the noise circle of the FET 988 is dependent on the noise resistance RN of the FET 988. The FET 988 may have any value of noise resistance RN that provides a noise circle having a size of at least 0.3 decibels, such as, but not limited to, less than approximately 0.03 ohms, equal to or less than approximately 0.02 ohms, and/or the like. The location of the noise circle of the FET 988 within the Smith Chart is dependent on the optimum reflection coefficient of the FET 988. For example, the noise circle of the FET 988 may be located closer to the center of the Smith Chart (e.g., closer to being concentric) when the optimum reflection coefficient of the FET 988 is less than approximately 100 ohms. In some examples, the noise circle of the FET 988 is centered within the Smith Chart (e.g., concentric with the Smith Chart), and the FET 988 may have an optimum reflection coefficient of less than approximately 100 ohms. In other examples, the FET 988 has an optimum reflection coefficient of between approximately 40 ohms and approximately 60 ohms, for example approximately 50 ohms.
The electronics (e.g., preamplifiers 710, inductors 930, 852, 860, and 862, capacitors 854, 864, and 866, impedance transformer 856, etc.) described above with reference to the signal-receiver section 700 and
In order to make RF coils in an array sufficiently spatially distinct, and thus improve their signal-to-noise ratio (SNR) for accelerated imaging, it is common to leave gaps between neighboring (e.g., adjacent) coils within the array. This, however, has the drawback of increasing the coupling between the RF coils, which can in turn degrade performance. To overcome this, the RF coils in the array may be overlapped by an amount that minimizes the mutual inductance between neighboring coils. When such an array is employed for parallel imaging, the SNR decreases, because the geometry factor of the array has increased.
The RF coil assemblies described herein are bra-like coil assemblies that may increase patient comfort while increasing spatial resolution and reducing scan time during a breast MRI examination. Standard breast coil assemblies that include a middle divider may be particularly uncomfortable as the material of the coil is too hard and it is difficult for patients to keep a prone position and/or hold still for thirty minutes or more. Further, SNR performance of standard breast coils is relatively lower and may not meet clinical high spatial resolution requirements because of only eight receive channels and/or an increased distance between the breast and the coil surface. Further still, the scan time of breast MRI is relative longer than an MRI scan time of other parts of the body because of the multi-plan, bilateral breasts and single breast scans needed by a whole breast MRI examination. In standard breast MRI coil configurations, right to left direction acceleration is not an option because of a lack of available elements in this direction. Long scan times may not be suitable for some clinical applications. Additionally, standard coil assemblies may have reduced performance during chemical fat-sat (fat saturation) scans. B0 and B1 maps all show the obvious asymmetry. Standard breast coil assemblies additionally have reduced coverage of the axillary area. This may increase a difficultly of scanning axillary lymph nodes for breast cancer examination.
The technical benefits of the RF coil assemblies disclosed herein include providing comfortable, high performance breast coil assemblies that may be comprised of flexible and wireless “all” digital coils. Additionally, the coil assemblies disclosed herein may eliminate the skin-air interface, increase the regional B0 and B1 uniformity, and to increase clinical bad chemical fat saturation scan performance and right to left shading. The coil assemblies described herein may increase scan coverage of the axillary areas due to the additional elements in the right and left flanks of the patient. This may increase the detectable rate of the axillary lymph nodes for breast cancer MRI.
Increasing the number of RF coils per each breast (e.g., from 4 channels to 8 channels) enables the RF coils to be positioned more closely to each other and to anatomical structures that are to be imaged. The RF coil assemblies include adjustable straps in order to adapt to different body sizes. Additionally, the RF coils of each RF coil array may move relative to each other during conditions in which the material forming the cups is expanded or contracted, thereby enabling the RF coil assemblies to be utilized with an increased amount of body sizes. The RF coils coupled to the cups of the RF coil assemblies and the flanking RF coils positioned to surround the sides of the patient may enable parallel imaging of the patient in all directions, including right to left. As a result, a signal-to-noise ratio of signals transmitted by the coils may be increased. Additionally, parallel imaging via the RF coil assemblies increases an amount of the patient's body that may be scanned without repositioning the coils and/or the patient. In this way, scan time may be reduced and an imaging quality of axillary lymph nodes of the patient may be increased.
As used herein, an element or step recited in the singular and proceeded with the word “a” or “an” should be understood as not excluding plural of said elements or steps, unless such exclusion is explicitly stated. Furthermore, references to “one embodiment” of the present invention are not intended to be interpreted as excluding the existence of additional embodiments that also incorporate the recited features. Moreover, unless explicitly stated to the contrary, embodiments “comprising,” “including,” or “having” an element or a plurality of elements having a particular property may include additional such elements not having that property. The terms “including” and “in which” are used as the plain-language equivalents of the respective terms “comprising” and “wherein.” Moreover, the terms “first,” “second,” and “third,” etc. are used merely as labels, and are not intended to impose numerical requirements or a particular positional order on their objects.
This written description uses examples to disclose the invention, including the best mode, and also to enable a person of ordinary skill in the relevant art to practice the invention, including making and using any devices or systems and performing any incorporated methods. The patentable scope of the invention is defined by the claims, and may include other examples that occur to those of ordinary skill in the art. Such other examples are intended to be within the scope of the claims if they have structural elements that do not differ from the literal language of the claims, or if they include equivalent structural elements with insubstantial differences from the literal languages of the claims.
The present application claims priority to U.S. Provisional Application No. 62/433,718, entitled “SYSTEMS FOR AN MRI BREAST RF COIL ARRAY,” and filed on Dec. 13, 2016, the entire contents of which are hereby incorporated by reference for all purposes.
Filing Document | Filing Date | Country | Kind |
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PCT/US2017/030654 | 5/2/2017 | WO | 00 |
Number | Date | Country | |
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62433718 | Dec 2016 | US |