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WO2001058352A1 - Magnetic resonance imaging device - Google Patents

Magnetic resonance imaging device Download PDF

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Publication number
WO2001058352A1
WO2001058352A1 PCT/JP2001/000832 JP0100832W WO0158352A1 WO 2001058352 A1 WO2001058352 A1 WO 2001058352A1 JP 0100832 W JP0100832 W JP 0100832W WO 0158352 A1 WO0158352 A1 WO 0158352A1
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WIPO (PCT)
Prior art keywords
measurement
space
magnetic field
origin
measured
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PCT/JP2001/000832
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French (fr)
Japanese (ja)
Inventor
Takayuki Abe
Shigeru Watanabe
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Hitachi Healthcare Manufacturing Ltd
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Hitachi Medical Corp
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Priority claimed from JP2000029817A external-priority patent/JP3847512B2/en
Priority claimed from JP2000097632A external-priority patent/JP3847519B2/en
Application filed by Hitachi Medical Corp filed Critical Hitachi Medical Corp
Priority to US10/203,260 priority Critical patent/US6611144B2/en
Publication of WO2001058352A1 publication Critical patent/WO2001058352A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • G01R33/56Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
    • G01R33/5601Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution involving use of a contrast agent for contrast manipulation, e.g. a paramagnetic, super-paramagnetic, ferromagnetic or hyperpolarised contrast agent

Definitions

  • the present invention relates to a magnetic resonance imaging apparatus (hereinafter, referred to as an MRI apparatus) for obtaining a tomographic image of a desired part of a subject using a nuclear magnetic resonance (hereinafter, abbreviated as “MRJ”) phenomenon, and particularly to a vascular system.
  • MRI apparatus magnetic resonance imaging apparatus
  • MRJ nuclear magnetic resonance
  • the present invention relates to an MRI apparatus capable of securing a desired rendering range and image quality in a minimum time required for rendering a travel.
  • An MRI device measures the density distribution, relaxation time distribution, etc. of nuclear spins (hereinafter simply referred to as spins) at a desired examination site in a subject using NMR phenomena, and uses the measured data to determine the Are displayed as images.
  • spins nuclear spins
  • MRA MR angiography
  • 'A common method of using a contrast agent is to combine a T1 shortened contrast agent such as M-DTPA with a short TR sequence in the gradient echo system.
  • This method includes a T1 shortened contrast agent Since the blood flow spin has a T1 shorter than that of the surrounding tissue, saturation is unlikely to occur when a high-frequency magnetic field excitation is applied for a short repetition time TR, and a relatively high signal is emitted from other tissues.
  • This method is used to visualize blood vessels filled with blood containing a contrast agent with high contrast to other tissues Measurement of Volume data including blood vessels while the contrast agent stays in the target blood vessel (Specifically, three-dimensional measurement) is performed, and the obtained three-dimensional images are superimposed to perform a projection process to draw a blood flow. Three-dimensional to get information Based on the three-dimensional Daladier cement echo method to get over data Is used.
  • (1) injection method of a contrast agent, and (2) imaging time and timing are important.
  • the contrast agent must be injected into the blood vessel to be imaged so as to maintain a stable and high concentration. For this reason, rapid injection using an automatic injector is generally used.
  • the imaging timing so that the concentration of the contrast agent in the artery becomes high during data collection.
  • the contrast agent concentration peaks in the center of k-space (low frequency region), which controls the contrast of the image, and the timing is set according to the data collection method used and the sequence of the sequence. I do.
  • the data collection method mainly consists of a sequential order in which measurement is performed from one high-frequency side of k-space to the other high-frequency side through a low-frequency region, and measurement is alternately performed from the low-frequency region of k-space toward both high-frequency ends.
  • There is a centric order and centric trick order is generally used.
  • Three-dimensional measurement ( ⁇ In the centric order, one of the phase-encoding-donorap and the slice-en code loop is the outer loop, the other is the inner loop, and either or both are controlled by centric, order.
  • the centric order in this case is not a true centric order because the distance from the origin in k-space to the measurement point (sampling point) fluctuates as shown in Fig. 1 (b), In some cases, and arteriovenous separation was insufficient. '.
  • the optimal imaging timing force is shifted by S ⁇
  • the image quality deteriorates due to the acquisition of low-frequency information when the agent is thin.
  • the measurement time is too early, the data in the low-frequency region will be sampled during the time when the signal from the blood vessel is extremely low, while the data in the high-frequency region will have a high signal from the blood vessel. Since the signal is sampled during the time zone, a ringing artifact without a DC component is generated.
  • the imaging time becomes longer because the measurement is performed in the high-frequency region in the vertical and horizontal directions of the k space with respect to the origin.
  • an object of the present invention is to provide an MRI apparatus capable of delineating the entire target blood vessel with high contrast in a short time while reducing the influence on the image quality due to the shift of the optimal imaging timing. It is another object of the present invention to provide an MRI apparatus which is hardly affected by body motion and can separate and depict arteries and veins with MRA. It is another object of the present invention to provide a data collection method suitable for MRA. Disclosure of the invention
  • the measurement points in the k space are divided into two groups, and in the first group to be measured first, the distance from the origin in the k space gradually approaches U In the other group of measurements, the measurement order of the measurement points is changed from the low-frequency component so that the distance gradually increases.
  • Adopt a data collection method that controls toward high frequency components.
  • the MRI apparatus of the present invention comprises: a static magnetic field generating means for generating a static magnetic field in a space where a subject is placed; and a gradient magnetic field generating means for applying a gradient magnetic field in the Rice, phase encoding, and reading directions to the space.
  • a transmission system for irradiating a high-frequency magnetic field to cause nuclear magnetic resonance to an atomic nucleus of the biological tissue of the subject; a receiving system for detecting an echo signal emitted by the nuclear magnetic resonance;
  • a gradient magnetic field generation means a control system for controlling the transmission system and the reception system, a signal processing system for performing an image rain synthesis operation using an echo signal detected by the reception system, and a means for displaying the obtained image.
  • the control system executes a three-dimensional sequence for giving a slice code and a phase encode, and at this time, a total of k space defined by the number of slice encodes and the number of vertical encodes is provided.
  • the points are divided into two groups.In the first group, the distance from the origin in k-space to the measurement point gradually decreases in the order of measurement.In the second group, the distance from the origin in k-space to the measurement point is measured.
  • the gradient magnetic field generating means is controlled in the slice direction and the phase encoder direction so that the values gradually increase in the order of measurement.
  • the method of dividing the measurement points in k-space into two groups is that at least one group contains the measurement points from the low-frequency region to the high-frequency region, and the measurement point of the other group contains at least the measurement points in the low-frequency region. I just need. Also, the number of measurement points actually measured among the measurement points belonging to the two groups may be the same or different. That is, one of the forces of the two groups may include a non-measurement point (a point that is not measured).
  • the measurement points are divided into two groups according to the k-space region.
  • the control system attaches the slice encode and the vertical encode.
  • the k-space defined by the number of slice encodes and the number of phase encodes is divided into two, and the distance from the origin in k-space to the measurement point in k-space is
  • the gradient magnetic field generating means in the slice direction and the phase encode direction is controlled so that the distance gradually decreases in the order of measurement, and in the other region, the distance from the origin on the k-space gradually increases in the order of measurement.
  • the measurement points in the k space are divided into two groups having a complex conjugate relationship with each other.
  • the control system executes the three-dimensional sequence for applying the slice encoding and the phase encoding, and at this time, sets the measurement point of the lc space defined by the slice encoding number and the phase encoding number to the origin.
  • the gradient magnetic field generating means in the slice direction and the cross-encode direction are controlled so as to gradually increase in the order of measurement.
  • the adjacent measurement points it is preferable to divide the adjacent measurement points so that they belong to different groups.
  • the measurement points that are partially adjacent to each other near the origin must belong to the same group. Therefore, in this specification, “division of adjacent measurement points so that they belong to different groups” means that the condition that the complex conjugate relationship is satisfied and the condition that adjacent measurement points belong to different groups is maximal. A state that is satisfied.
  • control system does not measure all of the measurement points in one of the two divided areas but measures a small number of measurement points compared to the other area.
  • the control for measuring is performed.
  • control is performed to measure a smaller number of measurement points than in the other group.
  • a predetermined region of a subject is selected and excited, and a gradient magnetic field that encodes at least two directions is applied.
  • the step of measuring one signal is repeated a plurality of times while changing the strength of the gradient magnetic field.
  • the measurement space defined by the two-direction encoder gradient magnetic field strength is divided into two, Measurement is performed sequentially on the two divided areas, and at that time, in the first measurement area, the measurement is performed so that the distance from the origin of the measurement space to the measurement point gradually decreases in the measurement order, and the area measured later In, measurement is performed such that the distance from the origin of the measurement space to the measurement point gradually increases in the order of measurement.
  • the point closest to the k-space from the previous measurement point is measured as the next measurement point.
  • the three-dimensional image data acquisition method of the present invention includes a step of selecting and exciting a predetermined region of the subject, applying a gradient magnetic field that encodes in at least two directions, and measuring an echo signal generated from the region.
  • the measurement points in the measurement space defined by the two-direction encode gradient magnetic field intensities are shared with the origin and are mutually complex. Adjacent measurement points in a conjugate relationship are divided into first and second groups so that they belong to different groups, and measurements are sequentially performed on the first and second groups.
  • the distance from the origin of the measurement space to the measurement ⁇ is measured so as to gradually decrease in the order of measurement
  • the distance from the origin of the measurement space to the measurement point is measured. So that it gradually increases in the order of measurement To measure.
  • Fig. 1 (a) measurement without distance fluctuation from the origin can be performed, and the time when the lowest frequency component is measured and the target blood By matching the point at which the signal intensity of the tube peaks with the contrast agent, the target blood vessel can be drawn with high contrast. In addition, even if there is a slight deviation between the point at which the low-frequency component is measured and the peak of the signal strength, the low-frequency component can be reliably measured, and there is no image deterioration.
  • Figures 1 (b) to 1 (d) show the conventional Centric orderer, elliptic force centric order, and sequential channel order. Indicates the change in distance from the k-space origin. -According to a preferred aspect of the data collection method of the present invention, in the first group, of all the measurement points, only the measurement points of the minus part are measured, and in the second group, all the measurement points are measured.
  • one group can collect the data that was not measured without measuring some of the measurement points.
  • the measurement of unnecessary data having a low signal intensity can be eliminated, and a good image can be obtained.
  • FIG. 1 is a schematic diagram illustrating a data collection method adopted by an MRI apparatus according to the present invention and a conventional data collection method.
  • FIG. 2 is a block diagram illustrating an overall configuration of the MRI apparatus to which the present invention is applied.
  • FIG. 4 is a diagram showing an embodiment of a pulse sequence of a contrast MRA measurement performed by the MRI apparatus of the present invention.
  • FIG. 4 is a diagram schematically showing an embodiment of a k-space data collection order according to the present invention.
  • FIG. 5 is a view for explaining MRA imaging by the MRI apparatus of the present invention
  • FIG. 6 is a view showing a result of simulation of MRA imaging by the MRI apparatus of the present invention and MRA imaging by the conventional method
  • FIG. 8 is a diagram schematically illustrating another embodiment of the k-space data collection order according to the present invention.
  • FIG. 8 is a diagram schematically illustrating another embodiment of the k-space data collection order according to the present invention.
  • FIG. 10 is a diagram for explaining MRA imaging by the MRI apparatus of the present invention
  • FIG. 11 is a diagram schematically showing another embodiment of the k-space data collection order according to the present invention
  • FIG. FIG. 10 illustrates an image reconstruction method to which the data acquisition method of FIG. 10 is applied
  • FIG. 13 is a diagram illustrating a simulation for evaluating MRA imaging by the MRI apparatus of the present invention
  • FIG. 15 is a figure which shows typically the other example of the data collection order of k space by this invention.
  • FIG. 2 is a block diagram showing the overall configuration of the MRI apparatus according to the present invention.
  • This MKI device obtains a tomographic image of the subject using the ⁇ R phenomenon, and includes a static magnetic field generating magnet 2, a magnetic field gradient generating system 3, a sequencer 4, a transmitting system 5 ', and a receiving system 6. , A signal processing system 7, and a central processing unit (CPU) 8.
  • CPU central processing unit
  • the static magnetic field generating magnet 2 generates a uniform static magnetic field around the subject 1 in the direction of its body axis or in a direction orthogonal to the body axis, and has a certain space around the subject 1.
  • a permanent magnet type, normal conduction type or superconducting type magnetic field generating means is provided.
  • the magnetic field gradient generating system 3 includes a gradient magnetic field coil 9 wound in three directions of X, ⁇ , and Z, a gradient magnetic field IT source 10 for driving each gradient magnetic field coil, and a force.
  • a gradient magnetic field power supplies 10 of the respective coils By driving the gradient magnetic field power supplies 10 of the respective coils in accordance with the instructions from 4, the gradient magnetic fields Gx, Gy, Gz in the three axial directions of X, ⁇ , and Z are applied to the subject 1.
  • this gradient magnetic field By applying this gradient magnetic field, a specific slice or slab of the subject 1 can be selectively excited, and the position of the measurement point (sampling point) in the measurement space (k space) and the measurement order must be specified. Can be.
  • the sequencer 4 operates under the control of the CPU 8 and sends various commands necessary for data collection of tomographic images of the subject 1 to the magnetic field gradient generating system 3, the transmitting system 5, and the receiving system 6.
  • the operation timing of the magnetic field gradient generation system 3, the transmission system 5, and the reception system 6 controlled by the sequencer 4 is called a pulse sequence.
  • a sequence for three-dimensional blood flow imaging is adopted as one of the pulse sequences. The control of the sequencer 4 will be described later in detail.
  • the transmission system 5 irradiates a high-frequency magnetic field to cause nuclear magnetic resonance in nuclei of atoms constituting the biological tissue of the subject 1 by high-frequency pulses sent from the sequencer 4, and modulates with the high-frequency oscillator 11. 12 and high-frequency amplifier 13 and high frequency on the transmitting side And a wave coil 14a.
  • the high-frequency pulse output from the high-frequency oscillator 11 is amplitude-modulated by the modulator 12 according to the instruction of the sequencer 4, and the high-frequency pulse subjected to the amplitude modulation is amplified by the high-frequency amplifier 13 and then placed close to the subject 1.
  • the electromagnetic wave is applied to the subject 1 by supplying it to the high-frequency coil 14a.
  • the receiving system 6 detects the echo signal (fan R signal) emitted by nuclear magnetic resonance of the nucleus of the living body a ⁇ of the subject 1, and includes a high-frequency coil 14b and an amplifier 15 on the receiving side and a quadrature phase detector. It consists of a container 16, A / D conversion ⁇ 3 ⁇ 4 17, and power.
  • the electromagnetic (response signal) of the response of the subject 1 due to the electromagnetic wave radiated from the high-frequency coil 14a on the transmitting side is detected by the high-frequency coil 14b arranged close to the subject 1.
  • the detected echo signal is input to the A / D converter 17 via the amplifier 15 and the quadrature detector 16 and is converted into a digital value. Further, the quadrature detector is output at a timing according to an instruction from the sequencer 4.
  • the collected data is sampled into two series and is sent to the signal processing system 7.
  • the signal processing system 7 includes a CPU 8, a recording device such as a magnetic disk 18 and a magnetic tape 19, and a display 20 such as a CRT.
  • the CPU 8 performs processing such as Fourier transform and correction coefficient calculation image reconstruction on the echo signal (digitized data) sent from the receiving system 6 and performs an appropriate operation on the signal intensity distribution of an arbitrary cross section or a plurality of signals. The obtained distribution is imaged and displayed on the display 20 as a tomographic image.
  • the high-frequency coils 14a and 14b on the transmitting side and the receiving side and the gradient magnetic field coil 9 are installed in the magnetic field space of the static magnetic field generating magnet 2 arranged in the space around the subject 1. .
  • the sequencer 4 operates according to a predetermined pulse sequence, here a three-dimensional MM sequence, according to the operation timing of the magnetic field gradient generation system 3, the transmission system 5, and the reception system 6. Control the ringing.
  • This pulse sequence is pre-installed as a program in the memo provided in the CPU 8), and can be executed by the user selecting as appropriate according to the purpose of photographing, similarly to other pulse sequences. That is, the sequence 4 in which the MRA using the contrast agent is selected via the input device of the CPU 8 is controlled by the CPU 8 to execute a three-dimensional MRA sequence.
  • This panless sequence is a sequence based on the gradient echo method, as shown in FIG. 3, for example, and is common to three-dimensional MRA sequences. That is, the high-frequency magnetic field panelless RF is simultaneously applied with the region selection gradient magnetic field Gs to excite the region (slab) including the target blood vessel, and then the gradient magnetic field pulse Gel in the slice direction and the gradient in the directional code direction. The magnetic field pulse Ge2 is applied, then the readout gradient magnetic field Gr is applied, and the polarity is inverted to measure the echo signal. From the high-frequency magnetic field pulse RF to the echo signal measurement, the magnetic field strength of the gradient magnetic field Gel in the slice direction and the gradient magnetic field Ge2 in the phase encode direction are changed at a predetermined repetition time TR to obtain three-dimensional data.
  • the number of encoders in the slice direction and the phase encoder direction determines the image resolution in the direction A, and is set in advance in consideration of the measurement time and the like. For example, the number of encodes in the phase encoding direction is set to 128, 256, and the slice direction is set to 10 to 30.
  • the k-space (ky-kz space, where the slice direction is the z direction and the phase encoding direction is the y direction) is defined by the number of encoders in the slice direction and the phase encode direction. That is, in the sequence of FIG. 3, the signals measured when the gradient magnetic field intensity in the slice direction is a certain value Gel (Gz) and the gradient magnetic field intensity in the phase encoder direction is a certain value Ge2 (Gy) are Gz and Gy. Is located at the grid point (ky, kz) in k-space corresponding to.
  • the three-dimensional MRA sequence itself shown in FIG. 3 is general in MRA, but in this sequence adopted in the present embodiment, the data collection method uses the conventional centric orderer or elliptic force sensor. This is different from trick ordering.
  • the ky-kz space is divided into two along the ky axis or the kz axis, and in one area where measurement is first started, the area is determined from the point at a large distance from the origin 0 in the k space. Start the measurement, and then perform sampling control from the high-frequency component to the low-frequency component so that the sampling point gradually approaches the origin 0.
  • the sampling point is controlled from the low frequency component to the high frequency component so that the distance from the origin 0 gradually increases from or near the origin 0.
  • this data collection method is as follows: 1) One of the two divided areas starts from the point farthest from the origin, and thereafter, determines the subsequent sampling points so that the distance from the origin gradually decreases. In the other area, start from the origin or the point closest to the origin, and then determine the subsequent sampling points so that the distance from the origin gradually increases. 2) Make the distance between sampling points adjacent in time the shortest. Is defined by the AND of the two conditions. .
  • the condition of 2) is not essential, but by making sampling points adjacent to each other as close as possible, it is possible to reduce the artifat.
  • the condition in 2) may be to select not the distance between the two sampling points but the force with the same ky value, for example.
  • the optimum sampling point may be determined in consideration of not only the relationship between two sampling points but also the relationship between a plurality of sampling points in the next measurement and further subsequent measurements.
  • Fig. 4 shows a simplified example of the data collection method described above, showing the data collection order in a 5 * 9 Matritus k-space where the number of slice codes is 5 and the number of phase codes is 9.
  • circled numbers indicate the data collection order. This divided into two k-space in kz axis, toward the origin (No. 25) a point in a high frequency region indicated with the lower region (E ⁇ C region) "S tart" from (No. 1) in numerical order Measure In the upper ⁇ area (C ⁇ E area), measurement is performed from the origin to the high frequency area in the numerical order up to number 45. Note that the distance ⁇ z between two adjacent points on the coordinates of the k space is 1 ZFOVz.
  • Timing imaging is performed by the test injection method.
  • a small amount of a contrast medium (about 1 to 2 ml) is first injected for test injection to obtain a time signal curve at the target site as shown in FIG.
  • the arrival time tl of the contrast agent is measured from this curve, and the timing for performing the main imaging is determined based on the result.
  • the timing imaging method sets R0I at a specific site in the monitor area for the arrival of the contrast agent, captures the signal change of the same site, and exceeds the set threshold.
  • a method of automatically starting imaging at a point in time or a method called fluoroscopy, in which a target blood vessel is observed in real time by repeating short-time imaging and display, and imaging is started when an appropriate signal rise is obtained. It is also possible to employ these methods. However, the test injection method is preferable because the timing can be accurately measured by using a contrast agent prior to the main imaging.
  • the main imaging is performed as shown in FIG. 5 (b).
  • the main imaging may be performed only after the injection of the contrast agent, but preferably, images before and after the injection of the contrast agent are taken.
  • the imaging before and after the imaging is performed continuously for the same slice or slab position under the same conditions.
  • the imaging sequence is a sequence based on the short TR 3D gradient echo method as shown in Fig. 3.
  • a gradient magnetic field for rephasing the dephasing due to the flow that is, Gradient Moment Nulling may be added, but this is not essential. Instead, it is preferable to use a rather simple gradient echo for shortening TR / TE.
  • the imaging time T is determined when the pulse sequence repetition time TR, matrix size (slice chain code number and phase end number), and addition number are determined, so that the target blood vessel obtained by the above timing imaging reaches the contrast agent of interest.
  • imaging start time t2 imaging is started after injection of contrast agent so that data measurement in the low-frequency region of the ky-kz space is performed when the contrast agent reaches the target blood vessel. Set the time up to).
  • the sequencer 4 uses the gradient magnetic field in the slice direction in the region to be measured first (for example, the E ⁇ C region). And the gradient magnetic field noise in the direction of the phase encoder are controlled so that high-frequency components and low-frequency components are measured in order, and in the subsequent measurement area (for example, C ⁇ E area), low-frequency components and high-frequency components are measured. Control to measure the thigh. In this case, as described above, control is performed so that the distance from the origin to the sampling point gradually decreases in the first region, and the distance from the origin gradually increases in the subsequent region.
  • Figure 6 shows the results of simulating the difference in arteriovenous separation due to the different data collection methods.
  • FOV 320
  • TR 10 ms
  • number of phase encodes 160
  • number of slice encodes 16
  • image matrix 256 *
  • slice 5
  • the arteriovenous separation is expressed as the ratio of the signal strength of the artery to the signal strength of the vein.
  • the data collection method of the present invention has an increased arteriovenous signal ratio as compared to sequential ordering and elliptical centric ordering. Therefore, even if there is a vein near the artery that is confusing, it is possible to draw only the artery with high contrast.
  • the three-dimensional data of only the blood vessel can be obtained.
  • the difference processing is performed, for example, by performing a complex difference between slices at the same slice position in three dimensions.
  • the difference may be a difference between absolute values.
  • the method of removing tissue other than blood vessels by performing differential processing between images before and after contrast in this manner is called 3D MR-DSA (Digital Subtraction Angiography) and is a known method, and is not essential in the present invention. In particular, it is suitable for delineating thin blood vessels in which it is difficult to obtain sufficient contrast with tissues other than blood vessels.
  • the three-dimensional data after the difference processing can be viewed three-dimensionally by projecting it in any direction, such as coronal section, sagittal section, and transverse axis.
  • a projection method a known maximum intensity projection method or the like can be employed.
  • a sequence based on the gradient echo method is exemplified as a three-dimensional MRA sequence, but an EPI (Echo Planer Imaging) method for measuring a plurality of echo signals with one excitation, a split-type EPI, and the like are also employed. can do.
  • EPI Echo Planer Imaging
  • the k space may be divided by the force ky axis which indicates the case where the k space is divided by the kz axis.
  • the areas may be asymmetric.
  • the imaging time as a whole can be reduced.
  • the number of measurement points in the area to be measured first is reduced, or the number of measurement points in the area to be measured later is reduced, so that the imaging time is shorter than in Fig. 5 (b).
  • the measurement method shown in Fig. 5 (d) is effective when the distance between the target blood vessel and the nearby vein is short, and the time when the contrast agent reaches the target blood vessel after reaching the target blood vessel is short.
  • the data in the area with a small number of measurement points may be estimated from the data in the area where the unmeasured data (the data in the shaded area in Fig. 7) is measured, or May be. Also in this embodiment, in addition to the above-described effects, it is possible to selectively obtain a high-contrast artery image while reducing the influence of the shift in the three-dimensional measurement timing.
  • data collection in k-space is not limited to rectangular matrices as shown in Figs. 4 and 7, and data within a circle (ellipse) centered on the origin (No. 15) as shown in Fig. 8 It is also possible.
  • the number of slice encodes is 5, and the number of phase encodes is 9.
  • both ky and kz are high-frequency components. The area (outside the circle) is collected, but data concentrically arranged around the origin (No. 15) is collected.
  • the order of data collection is as follows: in the lower half area, which is measured first, from the center to the center in order from the side farther from the center, and in the upper half area, the measurement is in the direction away from the center. I do.
  • the embodiment in which the region of the k space is divided and the measurement points are divided into two groups according to the region has been described. It is also possible to divide them into groups.
  • FIG. 9 shows a k-space of an 8 * 8 matrix in which the number of slice encodes is 8 and the number of phase encodes is 8, as an example of the data collection method according to the second embodiment, which is zero-purified.
  • Lattice points belonging to these two groups have a complex conjugate relationship with each other, and adjacent lattice points belong to different groups. However, in order to satisfy the complex conjugate relation, adjacent lattice points belong to one group near the origin. '
  • the first of these two groups which measures first, starts the measurement from the point in k-space where the distance from the origin 0 force is large, and then gradually increases the sampling point from the high-frequency component so as to approach the origin 0 gradually. Sampling control is performed toward low frequency components. Also the second In the group, on the contrary, the sampling point is controlled from the low-frequency component to the high-frequency component such that the distance from the origin 0 gradually increases from or near the origin 0.
  • circled numbers indicate the data collection order. No hierarchy is the measurement point of the same number, indicating that it may be measured from either of them ⁇
  • the measurement starts from the grid point (number 1) farthest from the origin (the grid point with number 33), that is, the highest frequency component, and then the grid point of number 2 Measurements are sequentially performed up to the origin, such as the grid point of number 3.
  • measurement of the second group is performed.
  • measurement is started from the lattice point (No. 34) closest to the origin, that is, the low-frequency component, and measurement is performed in order from the origin in order.
  • the subject is placed in the measurement space in the static magnetic field magnet, an imaging region including a target blood vessel is determined, and timing imaging is performed.
  • the timing imaging is performed by, for example, a test injection method. That is, a small amount of a contrast medium (about 1 to 2 ml) was test-injected, and as shown in Fig. 10, the time at the target site " ⁇ sign curve was obtained, from which the arrival time of the syrup (signal intensity) Measure the tl and determine the timing to perform the main imaging based on the result.
  • 'Timing imaging perform the main imaging as shown in Fig. 10 (b). May perform only imaging after the injection of the contrast medium, but preferably images before and after the injection of the contrast medium.Imaging before and after the imaging is performed under the same conditions under the same slice or slab position. Is performed continuously.
  • the imaging sequence is a sequence based on the short TR 3D gradient echo method as shown in Fig. 3.
  • a gradient magnetic field that is, Gradient Moment Nulling may be added for rephasing the phase due to the flow, but this is not essential. Instead, it is preferable to use a simple gradient echo for shortening TR / TE.
  • the imaging time T is determined. Based on tl, imaging start time t2 (from the injection of the contrast agent to the start of imaging, so that data measurement in the low-frequency region of the ky-kz space is performed when the contrast agent reaches the target blood vessel. Time).
  • imaging measurement of the first group is first started, and then measurement of the second group is performed.
  • the sequencer 4 controls both the gradient magnetic field pulse in the slice direction and the gradient magnetic field in the phase encode code in the first group to be measured first so that the high frequency component and the low frequency component are sequentially measured, and then the measurement is performed thereafter.
  • control is performed so that measurement is performed in order from low-frequency components to high-frequency components. In this way, three-dimensional image data after contrast is obtained.
  • the data collection method shows a case where all the measurement points belonging to both the first group and the second group are measured, as shown in Fig. 10 (c).
  • the first group may employ a data collection method in which measurement of a predetermined high-frequency component is omitted and low-frequency components are measured in a short time.
  • An example of such a data collection method is shown in FIG. ⁇ 11 also illustrates an 8 * 8 matrix k-space in which the number of slice switches is 8, and the number of phase switches is 8.
  • the k-space is divided into two groups under the same conditions as in the embodiment shown in Fig. 9, but here the measurement is performed first. Measure only the components.
  • grid points present in 4 * 4 madridas in the low frequency region are measured among grid points in the k space.
  • the grid point with the greatest distance of the origin is used as the starting point, and the grid point of number 2 and the grid point of number 3 are measured up to the origin.
  • the grid point (number 10) adjacent to the origin From the origin, and measure all grid points belonging to the second group up to the highest frequency component in the order away from the origin.
  • the data of the high frequency region that is not measured in the first group can be estimated based on the complex characteristics of the first group and the second group.
  • a method of estimating unmeasured data a method based on a known half Fourier reconstruction method can be employed.
  • FIG. 12 schematically shows these processes.
  • the measured data is subjected to one-dimensional Fourier transform in the frequency encoder direction (k x direction) to obtain the actual measured data in the three-dimensional hybrid space.
  • the three-dimensional estimated data is obtained from the actual measurement data, and the hybrid spatial data is obtained by combining the actual measurement data and the estimation data.
  • Three-dimensional image data is obtained by subjecting the hybrid space data to two-dimensional Fourier transform.
  • the spatial resolution is not degraded.
  • the low-frequency component in k-space is measured when the contrast agent reaches the target blood vessel and the signal intensity of the blood flowing through the target blood vessel becomes the highest. This means that artery images can be drawn with high contrast.
  • the concentration of the contrast agent rises sharply.
  • FIG. 13 and 14 show the results of simulating differences in arteriovenous separation due to differences in imaging methods (data collection methods).
  • a simulated artery and vein was used, and a contrast medium was flowed into it at a flow rate of 40 cm, an arterial venous return time of 7 seconds, and an injection speed of 2 cc / s.
  • FIG. 13 shows the signal strength under the above conditions.
  • the peak of the signal from the artery is seen first, and the peak of the signal from the vein appears later.
  • FIG. 14 (a) is an image obtained by the imaging method of the present invention
  • FIG. 14 (b) is an image obtained by elibutanore centric ordering.
  • veins as well as arteries are imaged, and arteriovenous separation is not complete, whereas the imaging method of the present invention allows only arteries to be drawn with bulk contrast.
  • data collection in k-space is not limited to the rectangular matrix shown in Fig. 9 and Fig. 11, and data in a circle (ellipse) centered on the origin as shown in Fig. 15 can also be collected. It is possible.
  • measurement starts at a point in k-space that is farther from the origin 0, and then gradually moves the sampling point from the high-frequency component to the low-frequency component so as to approach the origin 0 gradually. Sampling control.
  • the sampling point is controlled from the low-frequency component to the high-frequency component such that the distance from the origin 0 gradually increases from or near the origin 0.
  • the grid points (measurement points) in the ky-kz space are divided into two groups, and one of the groups measured first has a distance from the origin in the k space.
  • the sampling point is controlled from the high-frequency component to the low-frequency component so that the sampling point gradually approaches, and in the other group, the sampling point is shifted from the low-frequency component to the high-frequency component so that the distance gradually increases.
  • Sampling control is performed for each component, so that the effect of high contrast can be achieved while reducing the effect of the imaging timing shift.
  • a vein-separated surface image can be obtained.
  • the imaging time can be reduced by reducing the number of measurement points in one of the two divided areas.

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Abstract

While contrast MRA measurement is being carried out, the concentration of the contrast agent is made to reach its peak when the low-frequency component is measured by controlling the measurement order of the k-space, considering the distance from the origin. The measurement points in the k-space are divided into two groups. When the concentration of the contrast agent in a target vessel becomes high, the measurement of the first group is started. For the first group, the sample points are sampling-controlled from the high-frequency component toward the low-frequency component in such a way that the distance from the origin gradually decreases. For the other group to be measured consecutively, the sample points on the opposite side of the origin are sampling-controlled from the low-frequency component toward the high-frequency component in such a way that the distance from the origin gradually increases. The influence of the error of the imaging timing in the contrast MRA measurement is reduced, and the whole vessel is drawn in high contrast. The image of an artery can be selectively drawn.

Description

磁気共鳴ィメ一ジング装置 技術分野 , Magnetic resonance imaging equipment

本発明は、 核磁気共鳴 (以下、 「 MRJ と略記する)現象を利用じて被検体の所望 部位の断層画像を得る磁気共鳴イメージング装置 (以下、 MRI装置という) に関 し、 特に血管系の走行を描出する際に必要最小限の時間で、 所望の描出範囲と画 質を確保することの可能な MRI装置に関するものである。 背景技術  The present invention relates to a magnetic resonance imaging apparatus (hereinafter, referred to as an MRI apparatus) for obtaining a tomographic image of a desired part of a subject using a nuclear magnetic resonance (hereinafter, abbreviated as “MRJ”) phenomenon, and particularly to a vascular system. The present invention relates to an MRI apparatus capable of securing a desired rendering range and image quality in a minimum time required for rendering a travel.

MRI装置は、 NMR現象を利用して被検体中の所望の検査部位における原子核ス ピン (以下、 単にスピンと称す)の密度分布、 緩和時間分布等を計測して、 その計 測データから被検体の任意の断面を画像表示するものである。  An MRI device measures the density distribution, relaxation time distribution, etc. of nuclear spins (hereinafter simply referred to as spins) at a desired examination site in a subject using NMR phenomena, and uses the measured data to determine the Are displayed as images.

この MRI 装置の撮像機能に、 血流を描画する MR アンジォグラフィ(以下、 「MRA」 と略す)があり、 MMには造影剤を使用しない方法と造影剤を使用する方 法がある。  One of the imaging functions of this MRI apparatus is MR angiography (hereinafter abbreviated as “MRA”) that draws blood flow. MM has a method that does not use a contrast agent and a method that uses a contrast agent.

'造影剤を用いる方法としては (M - DTPAなどの T1短縮型の造影剤とグラジェン トエコー系の短い TRのシーケンスを組み合わせる方法が一般的である。 この方 法では、 T1短縮型の造影剤を含む血流スピンが周囲組織より短い T1を有してい るために、 高周波磁場による励起を短い繰り返し時間 TRで受けた場合に飽和が 起こりにくく相対的に他の組織より高信号を発することを利用し、 造影剤を含む 血液に満たされた血管を他組織に対し高コントラストで描出するものである。 造 影剤が目的とする血管内にとどまつている間に血管を含む Volume のデータの.計 測 (具体的には三次元計測)を行ない、 得られた三次元画像を重ね合わせて投影処 理を行うことにより、 血流を描画する。 ここで一 的には広範囲で高^^能の情 報を得るために、 三次元データを取得する三次元ダラディエントエコー法を基本 とするシーケンスが用いられる。 'A common method of using a contrast agent is to combine a T1 shortened contrast agent such as M-DTPA with a short TR sequence in the gradient echo system. This method includes a T1 shortened contrast agent Since the blood flow spin has a T1 shorter than that of the surrounding tissue, saturation is unlikely to occur when a high-frequency magnetic field excitation is applied for a short repetition time TR, and a relatively high signal is emitted from other tissues. This method is used to visualize blood vessels filled with blood containing a contrast agent with high contrast to other tissues Measurement of Volume data including blood vessels while the contrast agent stays in the target blood vessel (Specifically, three-dimensional measurement) is performed, and the obtained three-dimensional images are superimposed to perform a projection process to draw a blood flow. Three-dimensional to get information Based on the three-dimensional Daladier cement echo method to get over data Is used.

このような三次元造影 MRAにおいて良好な Ρί像を得るためには、 (1)造影剤の 注入法、 (2)撮像時聞およびタイミングが重要である。 (1)については、 造影剤を 撮像対象とする血管内に安定して高濃度を維持するように注入しなければならな い。 このため通常は自動注入器を使用した急速注入が一般的に用いられる。  In order to obtain a good X-ray image in such a three-dimensional contrast MRA, (1) injection method of a contrast agent, and (2) imaging time and timing are important. Regarding (1), the contrast agent must be injected into the blood vessel to be imaged so as to maintain a stable and high concentration. For this reason, rapid injection using an automatic injector is generally used.

(2)については、 例えば動脈のみを分離し選択的に撮像するためには、 データ 収集時に動脈における造影剤の濃度が高くなるように撮像タイミングを設定する 必要がある。 特に画像のコントラストを支配している k空間の中心部分 (低周波 領域)において造影剤濃度がピークに達するのが理想であり、 使用するノ、レスシ 一ケンスのデータ収集法に応じてタイミングを設定する。  Regarding (2), for example, in order to separate and selectively image the artery, it is necessary to set the imaging timing so that the concentration of the contrast agent in the artery becomes high during data collection. Ideally, the contrast agent concentration peaks in the center of k-space (low frequency region), which controls the contrast of the image, and the timing is set according to the data collection method used and the sequence of the sequence. I do.

データ収集法には、 主に k空間の高周波側一端から低周波領域を経て高周波側 他端まで計測するシーケンシャルオーダー (Sequential Order) と、 k空間の低 周波領域から交互に高周波両端に向かって計測するセントリックオーダー (Centric Order) があり、 一般的にはセン'トリックオーダーが用いられている。 三次元計測 (^セントリックオーダーでは、 位相ェンコ一ドノレープ、 スライスェン コードループの一方を外側のループ、 他方を内側のループとし、 そのどちらかあ るいは両方をセントリック,オーダーで制御している。  The data collection method mainly consists of a sequential order in which measurement is performed from one high-frequency side of k-space to the other high-frequency side through a low-frequency region, and measurement is alternately performed from the low-frequency region of k-space toward both high-frequency ends. There is a centric order, and centric trick order is generally used. Three-dimensional measurement (^ In the centric order, one of the phase-encoding-donorap and the slice-en code loop is the outer loop, the other is the inner loop, and either or both are controlled by centric, order.

しかしながら、 この場合のセントリックオーダーは、 図 1 ( b ) に示すように k空間上の原点から計測点 (サンプリング点) の距離が変動し真のセントリック オーダーではないため、 体動の影響を受けやすく、 また動静脈の分離が不十分の 場合があった。 ' .  However, the centric order in this case is not a true centric order because the distance from the origin in k-space to the measurement point (sampling point) fluctuates as shown in Fig. 1 (b), In some cases, and arteriovenous separation was insufficient. '.

このような問題を解決する方法として ky-kz空間において相対 F0Vをも考慮 し、 信号計測が進むに従い k空間上の原点からの距離が徐々に離れていくように 制御するエリプティ力ルセントリックオーダリング (Elliptical Centric Ordering) が提案されている (図 1 ( c ) ) ("Performance of an Elliptical As a method of solving such a problem, the relative F0V in the ky-kz space is also considered, and the elliptic force centric ordering is controlled so that the distance from the origin in the k space gradually increases as the signal measurement progresses ( Elliptical Centric Ordering) has been proposed (Fig. 1 (c)) ("Performance of an Elliptical

Centric View Oraer for Signal Enhancement and Motion Artifact Suppression in Breath-hold Three- Dimensional Gradient Echo Imaging. Alan, et al. agnetic Resonance in Medicine 38 : 793 - 802, 1997つ。 このデータ収集法では、 撮像時間の初めに画像のコントラス トを決定する俾周 波データを計測するので、 目的とする血管の造影剤濃度が増加したときに撮像を 開始することにより選択的に動脈像を得ることが可能となつた。 Centric View Oraer for Signal Enhancement and Motion Artifact Suppression in Breath-hold Three-Dimensional Gradient Echo Imaging. Alan, et al. Magnetic Resonance in Medicine 38: 793-802, 1997. In this data acquisition method, since the frequency data for determining the contrast of the image is measured at the beginning of the imaging time, the imaging is selectively started by starting the imaging when the concentration of the contrast agent in the target blood vessel increases. It became possible to obtain an image.

しかしながら上述したセントリックオーダーゃェリプティ力ルセントリックォ 一ダリングでは、 画像のコントラストを早期に決定でき選択的に動脈像を得るの に有効であるものの、 至適撮像タイミング力 Sずれた^^、 造影剤が薄い時間帯の ときに低周波情報を取得してしまうために画質が劣化しゃすいという P題がある。 特に計測時間が早すぎた場合、 低周波領域のデータは血管内からの信号が極めて 低信号である時間帯にサンプリングされることになり、一方、 高周波領域のデー タは血管からの信号が高信号である時間帯にサンプリングされ ため、 直流成分 のないリンギングアーチファタトを発生させることになる。 また原点を中心に k 空間の上下或いは左右高周波領域に計測を進める全計測であるため、 撮像時間が 長くなるという問題もあった。  However, although the above-mentioned centric order eccentricity bidding is effective for determining the contrast of the image at an early stage and effectively obtaining an arterial image, the optimal imaging timing force is shifted by S ^^ There is a problem that the image quality deteriorates due to the acquisition of low-frequency information when the agent is thin. In particular, if the measurement time is too early, the data in the low-frequency region will be sampled during the time when the signal from the blood vessel is extremely low, while the data in the high-frequency region will have a high signal from the blood vessel. Since the signal is sampled during the time zone, a ringing artifact without a DC component is generated. In addition, there is a problem that the imaging time becomes longer because the measurement is performed in the high-frequency region in the vertical and horizontal directions of the k space with respect to the origin.

一方、 シーケンシャルオーダーでは計測タイミングが少々ずれても画像に顕著 なアーチファタトが現われにくく安定した画像が取得できるが、 前述のセントリ クオーダーと同様に被検体の体動の影響を受けやすく、 動静脈分離も十分に行わ れないという問題があった。  On the other hand, in the sequential order, even if the measurement timing is slightly shifted, a remarkable artifact does not appear in the image, and a stable image can be acquired. Was not performed sufficiently.

そこで本発明は、 至適撮像タイミングのずれによる画質への影響を軽減しつつ、 短時間に目的とする血管全体を高コントラストで描出することができる MRI装置 を提供することを目的とする。 また体動の影響を受けにくく、 MRAにおいで動脈 と静脈を分離して描出することの可能な MRI装置を¾することを目的とする。 さらに本発明は MRAに好適なデータ収集法を »することを目的とする。 発明の開示 Therefore, an object of the present invention is to provide an MRI apparatus capable of delineating the entire target blood vessel with high contrast in a short time while reducing the influence on the image quality due to the shift of the optimal imaging timing. It is another object of the present invention to provide an MRI apparatus which is hardly affected by body motion and can separate and depict arteries and veins with MRA. It is another object of the present invention to provide a data collection method suitable for MRA. Disclosure of the invention

上記目的を 成するために、 本発明においては、 k空間の計測点を 2つの群に 分けて、 最初に計測する第 1の群では、 k空間上の原点からの距離が漸次的に近 づくように計測点の計測順序を高周波成分から低周波成分に向かって制御 U 他 方の群の計測では、 逆にその距離が漸次的に離れていくように計測点の計測順序 を低周波成分から高周波成分に向かって制御するデータ収集法を採用する。  In order to achieve the above object, in the present invention, the measurement points in the k space are divided into two groups, and in the first group to be measured first, the distance from the origin in the k space gradually approaches U In the other group of measurements, the measurement order of the measurement points is changed from the low-frequency component so that the distance gradually increases. Adopt a data collection method that controls toward high frequency components.

即ち、 本発明の MRI装置は、 被検体の置かれる空間に静磁場を発生する静磁場 発生手段と、 前記空間に^ライス方向、 位相エンコード方向及び読み出し方向の 各傾斜磁場を与える傾斜磁場発生手段と、 前記被検体の生体組麟の原子核に核磁' 気共鳴を起こさせるために高周波磁場を照射する送信系と、 前記核磁気共鳴によ り放出されるエコー信号を検出する受信系と、 前記傾斜磁場発生手段、 送信系お よび受信系を制御する制御系と、 受信系で検出したエコー信号を用いて画像雨冓 成演算を行う信号処理系と、 得られた画像を表示する手段とを備え、 前記制御系 は、 スライスェンコ一ド及ぴ位相エンコードを付与する三次元シーケンスを実行 し、 この際、 スライスエンコード数およ ϋ«ί立相エンコード数で規定される k空間 の計測点を 2つの群に分け、 第 1の群の計測は k空間上の原点から計測点までの 距離が計測順に漸減し、 第 2の群の計測は k空間上の原点から計測点までの距離 が計測順に漸増するように前記スライス方向および位相ェンコ一ド方向の頃斜磁 場発生手段を制御する。  That is, the MRI apparatus of the present invention comprises: a static magnetic field generating means for generating a static magnetic field in a space where a subject is placed; and a gradient magnetic field generating means for applying a gradient magnetic field in the Rice, phase encoding, and reading directions to the space. A transmission system for irradiating a high-frequency magnetic field to cause nuclear magnetic resonance to an atomic nucleus of the biological tissue of the subject; a receiving system for detecting an echo signal emitted by the nuclear magnetic resonance; A gradient magnetic field generation means, a control system for controlling the transmission system and the reception system, a signal processing system for performing an image rain synthesis operation using an echo signal detected by the reception system, and a means for displaying the obtained image. The control system executes a three-dimensional sequence for giving a slice code and a phase encode, and at this time, a total of k space defined by the number of slice encodes and the number of vertical encodes is provided. The points are divided into two groups.In the first group, the distance from the origin in k-space to the measurement point gradually decreases in the order of measurement.In the second group, the distance from the origin in k-space to the measurement point is measured. The gradient magnetic field generating means is controlled in the slice direction and the phase encoder direction so that the values gradually increase in the order of measurement.

k空間の計測点を 2つの群に分ける仕方は、 少なくとも一方の群が低周波領域 から高周波領域までの計測点を含み、 他方の群の計測点が少なくとも低周波領域 の計測点を含むものであればよい。 また 2つの群に属する計測点のうち実際に計 測される計測点の数は同一であっても異なっていてもよい。 即ち、 2つの群のい ずれ力一方は非計測点 (計測されない点) を含んでいてもよい。  The method of dividing the measurement points in k-space into two groups is that at least one group contains the measurement points from the low-frequency region to the high-frequency region, and the measurement point of the other group contains at least the measurement points in the low-frequency region. I just need. Also, the number of measurement points actually measured among the measurement points belonging to the two groups may be the same or different. That is, one of the forces of the two groups may include a non-measurement point (a point that is not measured).

具体的には、 一つの態様として k空間の領域によって計測点を 2つの群に分け る。 この態様によれば、 制御系は、 スライスエンコード及 立相エンコードを付 与する三次元シーケンスを実行し、 この際、 スライスエンコード数および位相ェ ンコード数で規定される k空間を 2分割し、 その二方の領域においては k空間上 の原点から計測点までの距離が計測順に漸減し、 他方の領域においては k空間上 の原点から計測点の距離が計測順に漸増するように前記スライス方向および位相 ェンコ一ド方向の傾斜磁場発生手段を制御する。 Specifically, as one aspect, the measurement points are divided into two groups according to the k-space region. According to this aspect, the control system attaches the slice encode and the vertical encode. The k-space defined by the number of slice encodes and the number of phase encodes is divided into two, and the distance from the origin in k-space to the measurement point in k-space is The gradient magnetic field generating means in the slice direction and the phase encode direction is controlled so that the distance gradually decreases in the order of measurement, and in the other region, the distance from the origin on the k-space gradually increases in the order of measurement.

また別の態様として k空間の計測点を互いに複素共役の関係にある 2つの群に 分ける。 この態様によれば、 制御系は、 スライスエンコード及び位相エンコード を付与する三次元シーケンスを実行し、 この際、 スライスエンコード数およ 立 相エンコード数で規定される lc空間の計測点を、 原点を共有し、 互いに複素 殳 の関係にある第 1および第 2の群に分割し、第 1の群では原点から計測点までの 距離が計測順に漸減し、 第 2の群では原点から計測点の距離が計測順に漸増する ように前記スラィス方向およ Ό¾相ェンコード方向の傾斜磁場発生手段を制御す .る。  As another mode, the measurement points in the k space are divided into two groups having a complex conjugate relationship with each other. According to this aspect, the control system executes the three-dimensional sequence for applying the slice encoding and the phase encoding, and at this time, sets the measurement point of the lc space defined by the slice encoding number and the phase encoding number to the origin. Divided into first and second groups that are shared and have a complex relationship with each other.In the first group, the distance from the origin to the measurement point gradually decreases in the order of measurement, and in the second group, the distance from the origin to the measurement point The gradient magnetic field generating means in the slice direction and the cross-encode direction are controlled so as to gradually increase in the order of measurement.

この場合、 隣り合う計測点は異なる群に属するように分割することが好ましい。 尚、 2つの群の計測点が互いに複素共役の関係にあるという条件を満たすために は、 原点の近傍において一部隣り合う計測点が同一の群に属する必要がある。 従 つて本明細書において 「隣り合う計測点は異なる群に属するように分割する」 と は、 複素共役の関係にあるという条件を満たし、且つ隣り合う計測点が異なる群 に属するという条件が最大限満たされている状態をいう。  In this case, it is preferable to divide the adjacent measurement points so that they belong to different groups. In order to satisfy the condition that the measurement points of the two groups have a complex conjugate relationship with each other, the measurement points that are partially adjacent to each other near the origin must belong to the same group. Therefore, in this specification, “division of adjacent measurement points so that they belong to different groups” means that the condition that the complex conjugate relationship is satisfied and the condition that adjacent measurement points belong to different groups is maximal. A state that is satisfied.

また本発明の ΜΚΙ装置の別な態様において、 前記制御系は、 2分割された領域 の一方の計測では、 計測点のすべてを計測するのではなく、 他方の領域に比べ少 なく数の計測点を計測する制御を行う。 或いは、 一方の群の計測では、 計測点の すべてを計測するのではなく、 他方の群に比べ少なく数の計測点を計測する制御 を行う。  In another aspect of the device of the present invention, the control system does not measure all of the measurement points in one of the two divided areas but measures a small number of measurement points compared to the other area. The control for measuring is performed. Or, in the measurement of one group, instead of measuring all of the measurement points, control is performed to measure a smaller number of measurement points than in the other group.

. 本発明の三次元画像データ収集法は、 被検体の所定の領域を選択して励起し、 少なくとも二方向にエンコードする傾斜磁場を印加し、 前記領域から生じるェコ 一信号を計測するステップを 記傾斜磁場の強度を変えながら複数回繰り返し、 三次元画像データを収集する際に、 前記二方向のェンコ一ド傾斜磁場強度で規定 される計測空間を 2分割し、 2分割された領域について順次計測を行い、 その際、 最初に計測される領域では、 前記計測空間の原点から計測点までの距離が計測順 に漸減するように計測し、 後で計測される領域においては前記計測空間の原点か ら計測点までの距離が計測順に漸増するように計測する。 ' In the three-dimensional image data acquisition method of the present invention, a predetermined region of a subject is selected and excited, and a gradient magnetic field that encodes at least two directions is applied. The step of measuring one signal is repeated a plurality of times while changing the strength of the gradient magnetic field.When three-dimensional image data is collected, the measurement space defined by the two-direction encoder gradient magnetic field strength is divided into two, Measurement is performed sequentially on the two divided areas, and at that time, in the first measurement area, the measurement is performed so that the distance from the origin of the measurement space to the measurement point gradually decreases in the measurement order, and the area measured later In, measurement is performed such that the distance from the origin of the measurement space to the measurement point gradually increases in the order of measurement. '

本発明のデータ収集方法において、 好適には、 原点からの距離が等しい点がい くつか存在する場合は、 前計測点からの k空間上の 離が最も近い点を次の計測 点として計測する。 '  In the data collection method of the present invention, preferably, when there are several points having the same distance from the origin, the point closest to the k-space from the previous measurement point is measured as the next measurement point. '

また本発明の三次元画像データ収集法は、 被検体の所定の領域を選択して励起 し、 少なくとも二方向にエンコードする傾斜磁場を印加し、 前記領域から生じる ェコ一信号を計測するステツプを前記傾斜磁場の強度を変えながら複数回繰り返 し、 三次元画像データを収集する際に、 前記二方向のエンコード傾斜磁場強度で 規定される計測空間の計測点を、 原点を共有し、 互いに複素共役の関係で且つ隣 り合う計測点は異なる群に属するように第 1および第 2の群に分割し、 第 1およ び第 2の群について順次計測を行い、 その際、 最初に計測される第 1の群では、 前記計測空間の原点から計測 ^までの距離が計測順に漸減するように計測し、 後 で計測される第 2の群では前記計測空間の原点から計測点までの距離が計測順に 漸増するように計測する。  Further, the three-dimensional image data acquisition method of the present invention includes a step of selecting and exciting a predetermined region of the subject, applying a gradient magnetic field that encodes in at least two directions, and measuring an echo signal generated from the region. When collecting the three-dimensional image data by repeating the gradient magnetic field intensity a plurality of times while changing the gradient magnetic field intensity, the measurement points in the measurement space defined by the two-direction encode gradient magnetic field intensities are shared with the origin and are mutually complex. Adjacent measurement points in a conjugate relationship are divided into first and second groups so that they belong to different groups, and measurements are sequentially performed on the first and second groups. In the first group, the distance from the origin of the measurement space to the measurement ^ is measured so as to gradually decrease in the order of measurement, and in the second group measured later, the distance from the origin of the measurement space to the measurement point is measured. So that it gradually increases in the order of measurement To measure.

. 本亮明のデータ収集方法によれば、'図 1 (a) に示すように原点からの距離変 動のない計測を行うことができ、 最も低周波成分を計測する時点と目的とする血 管の信号強度が造影剤によってピークとなる時点とを一致させることにより、 目 '的血管を高コントラストで描出することができる。 また低周波成分を計測する時 点と信号強度のピークに多少のずれがあっても、 確実に低周波成分を計測するこ とができ、 画像の劣化がない。 尚、 図 1 (b) 〜 (d) に従来のセントリツクオ一 ダー、 エリプティ力ルセントリックオーダー、 シーケンシヤノレオーダ一における k空間原点からの距離変化を示す。 - 本発明のデータ収集法の好適な態様によれば、 第 1の群では、 全計測点のうち、 —部の計測点のみを計測し、 第 2の群では全計測点を計測する。 According to Ryoaki Motoaki's data collection method, as shown in Fig. 1 (a), measurement without distance fluctuation from the origin can be performed, and the time when the lowest frequency component is measured and the target blood By matching the point at which the signal intensity of the tube peaks with the contrast agent, the target blood vessel can be drawn with high contrast. In addition, even if there is a slight deviation between the point at which the low-frequency component is measured and the peak of the signal strength, the low-frequency component can be reliably measured, and there is no image deterioration. Figures 1 (b) to 1 (d) show the conventional Centric orderer, elliptic force centric order, and sequential channel order. Indicates the change in distance from the k-space origin. -According to a preferred aspect of the data collection method of the present invention, in the first group, of all the measurement points, only the measurement points of the minus part are measured, and in the second group, all the measurement points are measured.

2つの群は複素共役の関係にあるので、 一方の群は一部の計測点を計測しなく ても、計測しなかったデータを他の群することができる。 特に造影剤濃度が増加 してピークまでの間に第 1群の計測を行う場合に、信号強度が低い不要なデータ の計測をなくすことができ、 良好な画像を得ることができる。 図面の簡単な説明  Since the two groups are in a complex conjugate relationship, one group can collect the data that was not measured without measuring some of the measurement points. In particular, when the first group is measured before the peak of the contrast medium increases, the measurement of unnecessary data having a low signal intensity can be eliminated, and a good image can be obtained. BRIEF DESCRIPTION OF THE FIGURES

図 1は、 本発明による MRI装置が採用するデータ収集法および従来のデータ収 集法を説明する概略図、 図 2は、 本発明が適用される MRI装置の全体構成を示す ブロック図、 図 3は、 本発明の MRI装置が実行する造影 MRA計測のパルスシーケ ンスの一実施例を示す図、 図 4は、 本発明による k空間のデータ収集順序の一実 施例を模式的に示す図、 図 5は、 本発明の MRI装置による MRA撮像を説明する図、 図 6は、 本発明の MRI装置による MRA撮像および従来法による MRA撮像をシ 、 レーションした結果を示す図、 図 7は、 本発明による k空間のデータ収集順序の 他の実施例を模式的に示す図、 図 8は、 本発明による k空間のデータ収集順序の 他の実施例を模式的に示す図、 図 9は、 本発明による k空間のデータ収集順序の 一実施例を模式的に示す図、 図 1 0は、 本発明の MRI装置による MRA撮像を説明 する図、 図 1 1は、 本発明による k空間のデータ収集順序の他の実施例を模式的 に示す図、 図 1 2は、 図 1 0のデータ収集法を適用した画像再構成法を説明する 図、 図 1 3は、 本発明の MRI装置による MRA撮像を評価するためのシミュレーシ ョンを示す図、 図 1 4は、 本発明の MRI装置による MRA撮像および従来法による MRA撮像をシミュレーションした結果を示す図、 図 1 5は、 本発明による k空間 のデータ収集順序の他の実施例を模式的に示す図である。 発明を実施するための最良の形態 FIG. 1 is a schematic diagram illustrating a data collection method adopted by an MRI apparatus according to the present invention and a conventional data collection method. FIG. 2 is a block diagram illustrating an overall configuration of the MRI apparatus to which the present invention is applied. FIG. 4 is a diagram showing an embodiment of a pulse sequence of a contrast MRA measurement performed by the MRI apparatus of the present invention. FIG. 4 is a diagram schematically showing an embodiment of a k-space data collection order according to the present invention. FIG. 5 is a view for explaining MRA imaging by the MRI apparatus of the present invention, FIG. 6 is a view showing a result of simulation of MRA imaging by the MRI apparatus of the present invention and MRA imaging by the conventional method, and FIG. FIG. 8 is a diagram schematically illustrating another embodiment of the k-space data collection order according to the present invention. FIG. 8 is a diagram schematically illustrating another embodiment of the k-space data collection order according to the present invention. Is a diagram schematically illustrating an example of an order of data collection in k-space according to the embodiment. FIG. 10 is a diagram for explaining MRA imaging by the MRI apparatus of the present invention, FIG. 11 is a diagram schematically showing another embodiment of the k-space data collection order according to the present invention, and FIG. FIG. 10 illustrates an image reconstruction method to which the data acquisition method of FIG. 10 is applied, FIG. 13 is a diagram illustrating a simulation for evaluating MRA imaging by the MRI apparatus of the present invention, and FIG. The figure which shows the result of having simulated the MRA imaging by the MRI apparatus of this invention, and the MRA imaging by the conventional method. FIG. 15 is a figure which shows typically the other example of the data collection order of k space by this invention. BEST MODE FOR CARRYING OUT THE INVENTION

以下、 本発明の実施例について添付図面を参照して説明する。  Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings.

図 2は本発明による MRI装置の全体構成を示すプロック図である。 この MKI装 置は、 丽 R現象を利用して被検体の断層像を得るもので、 静磁場発生磁石 2と、 磁場勾配発生系 3と、 シーケンサ 4と、 送信系 5'と、 受信系 6と、 信号処理系 7 と、 中央処¾¾置 (CPU) 8とを備えている。  FIG. 2 is a block diagram showing the overall configuration of the MRI apparatus according to the present invention. This MKI device obtains a tomographic image of the subject using the 丽 R phenomenon, and includes a static magnetic field generating magnet 2, a magnetic field gradient generating system 3, a sequencer 4, a transmitting system 5 ', and a receiving system 6. , A signal processing system 7, and a central processing unit (CPU) 8.

静磁場発生磁石 2は、 被検体 1の周りにその体軸方向または体軸と直交する方 向に均一な静磁場を発生させるもので、 被検体 1の周りのある広がりをもった空 間に永久磁石方式または常電導方式あるいは超電導方式の磁場発生手段が配置さ れている。  The static magnetic field generating magnet 2 generates a uniform static magnetic field around the subject 1 in the direction of its body axis or in a direction orthogonal to the body axis, and has a certain space around the subject 1. A permanent magnet type, normal conduction type or superconducting type magnetic field generating means is provided.

磁場勾配発生系 3は、 X, Υ, Zの三軸方向に巻かれた傾斜磁場コイル 9と、 それ ぞれの傾斜磁場コイルを駆動する傾斜磁場 IT源 10 と力 ら成り、 後述のシーケン サ 4からの命令に従ってそれぞれのコィルの傾斜磁場電源 10 を駆動することに より、 X, Υ, Zの三軸方向の傾斜磁場 Gx, Gy, Gzを被検体 1に印加するようになつ ている。 この傾斜磁場の加え方により被検体 1の特定のスライス又スラブを選択 的に励起することができ、 また計測空間 (k空間) における計測点 (サンプリン グ点) の位置、 計測順序を規定することができる。  The magnetic field gradient generating system 3 includes a gradient magnetic field coil 9 wound in three directions of X, Υ, and Z, a gradient magnetic field IT source 10 for driving each gradient magnetic field coil, and a force. By driving the gradient magnetic field power supplies 10 of the respective coils in accordance with the instructions from 4, the gradient magnetic fields Gx, Gy, Gz in the three axial directions of X, Υ, and Z are applied to the subject 1. By applying this gradient magnetic field, a specific slice or slab of the subject 1 can be selectively excited, and the position of the measurement point (sampling point) in the measurement space (k space) and the measurement order must be specified. Can be.

シーケンサ 4は、 CPU8の制御で動作し、 被検体 1の断層像のデータ収集に必 要な種々の命令を、 磁場勾配発生系 3、 送信系 5及び受信系 6に送るようになつ ている。 シーケンサ 4が制御する磁場勾配発生系 3、 送信系 5及ぴ受信系 6の動 作タイミングはパルスシーケンスと呼ばれる。 ここでは'パルスシーケンスの一つ として三次元血流撮像のためのシーケンスが採用される。 シーケンサ 4の制御に ついては後に詳述する。  The sequencer 4 operates under the control of the CPU 8 and sends various commands necessary for data collection of tomographic images of the subject 1 to the magnetic field gradient generating system 3, the transmitting system 5, and the receiving system 6. The operation timing of the magnetic field gradient generation system 3, the transmission system 5, and the reception system 6 controlled by the sequencer 4 is called a pulse sequence. Here, a sequence for three-dimensional blood flow imaging is adopted as one of the pulse sequences. The control of the sequencer 4 will be described later in detail.

送信系 5は、 シーケンサ 4力ら送り出される高周波パルスにより被検体 1の生 体組織を構成する原子の原子核に核磁気共鳴を起こさせるために高周波磁場を照 射するもので、 高周波発振器 11と変調器 12と高周波増幅器 13と送信側の高周 波コイル 14aとから成る。 高周波発振器 11から出力された高周波パルスをシー ケンサ 4の命令にしたがって変調器 12で振幅変調し、 この振幅変調された高周 波パルスを高周波増幅器 13で増幅した後に被検体 1に近接して配置された高周 波コイル 14aに供給することにより、 電磁波が被検体 1に照射されるようになつ ている。 The transmission system 5 irradiates a high-frequency magnetic field to cause nuclear magnetic resonance in nuclei of atoms constituting the biological tissue of the subject 1 by high-frequency pulses sent from the sequencer 4, and modulates with the high-frequency oscillator 11. 12 and high-frequency amplifier 13 and high frequency on the transmitting side And a wave coil 14a. The high-frequency pulse output from the high-frequency oscillator 11 is amplitude-modulated by the modulator 12 according to the instruction of the sequencer 4, and the high-frequency pulse subjected to the amplitude modulation is amplified by the high-frequency amplifier 13 and then placed close to the subject 1. The electromagnetic wave is applied to the subject 1 by supplying it to the high-frequency coil 14a.

受信系 6は、 被検体 1の生体 a ^の原子核の核磁気共鳴により放出されるェコ 一信号 (扇 R信号)を検出するもので、 受信側の高周波コイル 14bと増幅器 15 と 直交位相検波器 16と A/D変 ^¾ 17と力 ら成る。 上記送信側の高周波コイル 14a 力 ら照射された電磁波による被検体 1の応答の電磁 (應 R信号)は被検体 1に近 接して配置された高周波コイル 14bで検出される。 検出さ たェコ一信号は、 增 幅器 15及び直交位相検波器 16を介して A/D変 « 17に入力されディジタル量 に変換され、 さらにシーケンサ 4からの命令によるタイミングで直交位相検波器 16 によりサンプリングされた二系列の収集データとされ、 信号処理系 7 に送ら れる。  The receiving system 6 detects the echo signal (fan R signal) emitted by nuclear magnetic resonance of the nucleus of the living body a ^ of the subject 1, and includes a high-frequency coil 14b and an amplifier 15 on the receiving side and a quadrature phase detector. It consists of a container 16, A / D conversion ^ ¾ 17, and power. The electromagnetic (response signal) of the response of the subject 1 due to the electromagnetic wave radiated from the high-frequency coil 14a on the transmitting side is detected by the high-frequency coil 14b arranged close to the subject 1. The detected echo signal is input to the A / D converter 17 via the amplifier 15 and the quadrature detector 16 and is converted into a digital value. Further, the quadrature detector is output at a timing according to an instruction from the sequencer 4. The collected data is sampled into two series and is sent to the signal processing system 7.

信号処理系 7は、 CPU8と、 磁気ディスク 18及び磁気テープ 19等の記録装置 と、 CRT等のディスプレイ 20とから成る。 CPU8は、受信系 6から送られたエコー 信号 (ディジタル化されたデータ) にフーリエ変換、 補正係数計算像再構成等の 処理を行い、 任意断面の信号強度分布あるいは複数の信号に適当な演算を行って 得られた分布を画像ィ匕してディスプレイ 20 に断層像として表示するようになつ ている。 なお、 図 2において、 送信側及び受信側の高周波コイル 14a、 14b と傾 斜磁場コイル 9は、 被検体 1の周りの空間に配置された静磁場発生磁石 2の磁場 空間内に設置されている。  The signal processing system 7 includes a CPU 8, a recording device such as a magnetic disk 18 and a magnetic tape 19, and a display 20 such as a CRT. The CPU 8 performs processing such as Fourier transform and correction coefficient calculation image reconstruction on the echo signal (digitized data) sent from the receiving system 6 and performs an appropriate operation on the signal intensity distribution of an arbitrary cross section or a plurality of signals. The obtained distribution is imaged and displayed on the display 20 as a tomographic image. In FIG. 2, the high-frequency coils 14a and 14b on the transmitting side and the receiving side and the gradient magnetic field coil 9 are installed in the magnetic field space of the static magnetic field generating magnet 2 arranged in the space around the subject 1. .

次に本発明の MRI装置における血流撮像機能の第 1の実施形態について説明す る。  Next, a first embodiment of the blood flow imaging function in the MRI apparatus of the present invention will be described.

既に述べたようにシーケンサ 4は、 所定のパルスシーケンス、 ここでは三次元 MMシーケンス、 に従い磁場勾配発生系 3、 送信系 5及び受信系 6の動作タイミ ングを制御する。 このパルスシーケンスは CPU8 に備えられたメモ])に予めプロ グラムとして組み込まれており、 他のパルスシーケンスと同様、 使用者が撮影の 目的に応じて適宜選択することにより実行することができる。 即ち、 CPU8 の入 力装置を介して造影剤を用いた MRAが選択される シーケンス 4は CPU8によ つて制御され、 三次元 MRAシーケンスを実行する。 As described above, the sequencer 4 operates according to a predetermined pulse sequence, here a three-dimensional MM sequence, according to the operation timing of the magnetic field gradient generation system 3, the transmission system 5, and the reception system 6. Control the ringing. This pulse sequence is pre-installed as a program in the memo provided in the CPU 8), and can be executed by the user selecting as appropriate according to the purpose of photographing, similarly to other pulse sequences. That is, the sequence 4 in which the MRA using the contrast agent is selected via the input device of the CPU 8 is controlled by the CPU 8 to execute a three-dimensional MRA sequence.

このパノレスシーケンスは、 例えば図 3に示すように、 グラディエントエコー法 を基本とするシーケンスで、 三次元 MRAシーケンスに一般的なものである。 即ち、 領域選択傾斜磁場 Gsと同時に高周波磁場パノレス RFを印カ卩して目的血管を含む領 域 (スラブ) を励起した後、 スライス方向の傾斜磁場パルス Gelおよ 立相ェン コード方向の傾斜磁場パルス Ge2を印加し、 次いで読み出し傾斜磁場 Gr印加す るとともにその極性を反転させてエコー信号を計測する。 高周波磁場パルス RF からエコー信号計測までをスライス方向の傾斜磁場 Gelおよび位相ェンコ一ド方 向の傾斜磁場 Ge2の磁場強度を変えながら、 所定の繰り返し時間 TRで繰り返し、 三次元データを得る。  This panless sequence is a sequence based on the gradient echo method, as shown in FIG. 3, for example, and is common to three-dimensional MRA sequences. That is, the high-frequency magnetic field panelless RF is simultaneously applied with the region selection gradient magnetic field Gs to excite the region (slab) including the target blood vessel, and then the gradient magnetic field pulse Gel in the slice direction and the gradient in the directional code direction. The magnetic field pulse Ge2 is applied, then the readout gradient magnetic field Gr is applied, and the polarity is inverted to measure the echo signal. From the high-frequency magnetic field pulse RF to the echo signal measurement, the magnetic field strength of the gradient magnetic field Gel in the slice direction and the gradient magnetic field Ge2 in the phase encode direction are changed at a predetermined repetition time TR to obtain three-dimensional data.

スライス方向および位相ェンコ一ド方向のェンコ一ド数は阿方向の画像分解能 を決めるもので、 計測時間等を考慮して予め設定されている。 例えば位相ェンコ ード方向のエンコード数は 128、 256など、 スライス方向は 10〜30などに設定さ れている。 またこのスライス方向および位相ェンコ一ド方向のェンコ一ド数によ つて k空間 (スライス方向を z方向、 位相エンコード方向を y方向とすると、 k y— k z空間) が規定される。 即ち、 図 3のシーケンスにおいて、 スライス方向 の傾斜磁場強度のある値 Gel (Gz)と位相ェンコ一ド方向の傾斜磁場強度のある値 Ge2 (Gy)のときに計測された信号は、 Gz、 Gy に対応する k空間の格子点 (ky, kz) に配置されることになる。  The number of encoders in the slice direction and the phase encoder direction determines the image resolution in the direction A, and is set in advance in consideration of the measurement time and the like. For example, the number of encodes in the phase encoding direction is set to 128, 256, and the slice direction is set to 10 to 30. The k-space (ky-kz space, where the slice direction is the z direction and the phase encoding direction is the y direction) is defined by the number of encoders in the slice direction and the phase encode direction. That is, in the sequence of FIG. 3, the signals measured when the gradient magnetic field intensity in the slice direction is a certain value Gel (Gz) and the gradient magnetic field intensity in the phase encoder direction is a certain value Ge2 (Gy) are Gz and Gy. Is located at the grid point (ky, kz) in k-space corresponding to.

例えば図 3に示す三次元 MRAシーケンス自体は MRAにおいて一般的なものであ るが、 本実施形態が採用するこのシーケンスでは、 データ収集法が従来のセント リックオ^ "ダー或レ、はェリプティ力ルセントリックオーダリングとは異なる。 こ - の方法では、 ky- kz空間を ky軸または kz軸に沿って 2分割し、 最初に計測が開 始される一方の領域においては、 k空間上の原点 0からの距離が大きい点から會十 測を開始し、 その後漸次原点 0に近づくようにサンプリング点を高周波成分から 低周波成分に向かってサンプリング制御する。 また他方の領域においては、 逆に 原点 0或いはその近傍から、.原点 0からの距離が漸次離れていくようにサンプリ ング点を低周波成分から高周波成分に向かってサンプリング制御する。 For example, the three-dimensional MRA sequence itself shown in FIG. 3 is general in MRA, but in this sequence adopted in the present embodiment, the data collection method uses the conventional centric orderer or elliptic force sensor. This is different from trick ordering. In the method of-, the ky-kz space is divided into two along the ky axis or the kz axis, and in one area where measurement is first started, the area is determined from the point at a large distance from the origin 0 in the k space. Start the measurement, and then perform sampling control from the high-frequency component to the low-frequency component so that the sampling point gradually approaches the origin 0. On the other hand, in the other area, the sampling point is controlled from the low frequency component to the high frequency component so that the distance from the origin 0 gradually increases from or near the origin 0.

この場合、 廐点からの距離が等しい点がいくつ力存在する場合は、 前サンプリ ング点からの k空間上の距離が最も近い点を次のサンプリング点として計測する。 即ち、 このデータ収集法は、 1 ) 2分割した領域の一方では、 原点から最も遠 い点から開始し、 以後、 原点からの距離が漸減するようにその後のサンプリング 点を決定する。 他方の領域では、 原点或いは原点に最も近い点から開始し、 以後、 原点からの距離が漸増するようにその後のサンプリング点を決定する。 2 ) 時間 的に隣接するサンプリング点間の距離が最短となるようにする。 という 2つの条 件の ANDによって定義される。 .  In this case, if there are several points at the same distance from the stool point, the point with the closest distance in k-space from the previous sampling point is measured as the next sampling point. That is, this data collection method is as follows: 1) One of the two divided areas starts from the point farthest from the origin, and thereafter, determines the subsequent sampling points so that the distance from the origin gradually decreases. In the other area, start from the origin or the point closest to the origin, and then determine the subsequent sampling points so that the distance from the origin gradually increases. 2) Make the distance between sampling points adjacent in time the shortest. Is defined by the AND of the two conditions. .

本発明のデータ収集法において、 2 ) の条件は必須ではないが、 互いに隣接す るサンプリング点をできるだけ近接したものにすることにより'、 アーチファタト を低減することができる。 この目的のためには、 2 ) の条件として、 2つのサン プリング点の距離ではなく、 例えば ky値が同じである力最も近いものを選択す るようにしてもよレ、。 また 2つのサンプリング点の関係のみならず、 次の計測や さらにその後の計測における複数のサンプリング点の関係を考慮して最適なサン 'プリング点を決めるようにしてもよい。  In the data collection method of the present invention, the condition of 2) is not essential, but by making sampling points adjacent to each other as close as possible, it is possible to reduce the artifat. For this purpose, the condition in 2) may be to select not the distance between the two sampling points but the force with the same ky value, for example. The optimum sampling point may be determined in consideration of not only the relationship between two sampling points but also the relationship between a plurality of sampling points in the next measurement and further subsequent measurements.

図 4に上述のデータ収集法の単純化した一例として、 スライスェンコ一ド数が 5、 位相ェンコ一ド数が 9である 5 * 9マトリッタスの k空間におけるデータ収 集順序を示す。 図中、 丸で囲まれた数字はデータ収集順序を示している。 ここで は k空間を kz軸で 2分割し、 下側の領域 (E→C領域) では 「Start」 と示され た高周波領域の一点 (番号 1) から番号順に原点 (番号 25) に向かって計測し、 上側の简域 (C→E領域) では原点から高周波領域に向かって番号順に番号 45ま で計測している。 尚、 k空間の座標上で隣接する 2点間の距離 Δ zが 1 ZF OV zである。 Fig. 4 shows a simplified example of the data collection method described above, showing the data collection order in a 5 * 9 Matritus k-space where the number of slice codes is 5 and the number of phase codes is 9. In the figure, circled numbers indicate the data collection order. This divided into two k-space in kz axis, toward the origin (No. 25) a point in a high frequency region indicated with the lower region (E → C region) "S tart" from (No. 1) in numerical order Measure In the upper 简 area (C → E area), measurement is performed from the origin to the high frequency area in the numerical order up to number 45. Note that the distance Δz between two adjacent points on the coordinates of the k space is 1 ZFOVz.

次にこのようなデータ収集法を採用した上記 MRI装置による造影 MRAの一実施 例を図 5を参照して説明する。  Next, an embodiment of a contrast-enhanced MRA using the above-described MRI apparatus employing such a data acquisition method will be described with reference to FIG.

まず被検体を静磁場磁石内の計測空間に配置し、 目的とする血管を含む撮像領 域を決定し、 タイミング撮像を行う。 タイミング撮像はテストインジェクション 法によって行う。 この方法では、 まず少量の造影剤(約 l〜2ml)をテスト注入し て、 図 5に示すように、 対象部位における時間 言号曲線を得る。 この曲線から 造影剤の到達時間 tl を計測し、 この結果を基にして本撮像を行うタイミングを 決定する。 タイミング撮像の方法としては、 このテストインジェクション法の他 に、 造影剤の到達に関してモニタ領域内で特定の部位に R0Iを設定し、 同部位の '信号変ィヒを捉え、 設定した閾値を超えた時点で自動的に撮像が始まる方法やフル オロスコピーと呼ばれる短時間撮像 ·表示の繰り返しによって目的とする血管を リアルタィムで観察し適切な信号上昇がえられた時点で撮像を開始する方法があ り、 これらの方法を採用することも可能である。 但し、 テストインジェクション 法は造影剤を本撮像に先行して使用することにより、 正確にタイミングを測定す ることができるので好適である。  First, the subject is placed in the measurement space inside the static magnetic field magnet, the imaging region including the target blood vessel is determined, and timing imaging is performed. Timing imaging is performed by the test injection method. In this method, a small amount of a contrast medium (about 1 to 2 ml) is first injected for test injection to obtain a time signal curve at the target site as shown in FIG. The arrival time tl of the contrast agent is measured from this curve, and the timing for performing the main imaging is determined based on the result. In addition to this test injection method, the timing imaging method sets R0I at a specific site in the monitor area for the arrival of the contrast agent, captures the signal change of the same site, and exceeds the set threshold. There is a method of automatically starting imaging at a point in time, or a method called fluoroscopy, in which a target blood vessel is observed in real time by repeating short-time imaging and display, and imaging is started when an appropriate signal rise is obtained. It is also possible to employ these methods. However, the test injection method is preferable because the timing can be accurately measured by using a contrast agent prior to the main imaging.

タイミング撮像の後、 図 5 ( b ) に示すように本撮像を行う。 本撮像は造影剤 注入後の撮像のみを行ってもよいが、好適には造影剤注入前と造影注入後の画像 を撮像する。 造影前と造影後の撮像は、 同一条件で同一スライスまたはスラブ位 置について連続的に行う。  After the timing imaging, the main imaging is performed as shown in FIG. 5 (b). The main imaging may be performed only after the injection of the contrast agent, but preferably, images before and after the injection of the contrast agent are taken. The imaging before and after the imaging is performed continuously for the same slice or slab position under the same conditions.

' 撮像シーケンスは図 3に示すような短 TR の三次元グラディエントエコー法を 基本とするシーケンスである。 この場合、 血流を撮像対象としているので、 流れ によるディフェイズをリフェイズするための傾斜磁場即ちダラディエントモーメ ントヌリング (Gradient Moment Nulling)を付カ卩してもよいが、 これは必須では なく、 TR/TE短縮のためにはむしろ単純なグラディエントエコーとするのが好ま しい。 ' · 'The imaging sequence is a sequence based on the short TR 3D gradient echo method as shown in Fig. 3. In this case, since the blood flow is to be imaged, a gradient magnetic field for rephasing the dephasing due to the flow, that is, Gradient Moment Nulling may be added, but this is not essential. Instead, it is preferable to use a rather simple gradient echo for shortening TR / TE. '·

パルスシーケンスの繰り返し時間 TRおよびマトリクスサイズ (スライスェン コード数及び位相ェン ード数) びに加算数が決まると撮像時間 Tが決まるの で、 上記タイミング撮像で得られた目的とする血管の造影剤到達時刻 tl を基に、 目的とする血管に造影剤が到達した時に ky-kz空間の低周波領域のデータ計測が 行われるように、 撮像開始時刻 t2 (造影剤を注入してから撮像を開始するまで の時間) を設定する。  The imaging time T is determined when the pulse sequence repetition time TR, matrix size (slice chain code number and phase end number), and addition number are determined, so that the target blood vessel obtained by the above timing imaging reaches the contrast agent of interest. Based on time tl, imaging start time t2 (imaging is started after injection of contrast agent so that data measurement in the low-frequency region of the ky-kz space is performed when the contrast agent reaches the target blood vessel. Set the time up to).

撮像はまず図 4に示す E→C領域の計測を開始し、 続いて C→E領域の計測を行 う。 この場合、 シーケンサ 4は先に計測する領域 (例えば E→C領域) ではスラ イス方向傾斜磁場ノヽ。ルスと位相ェンコ一ド方向の傾斜磁場ノヽレスをともに高周波 成分から低周波成分を順に計 するように制御し、 またその後の計測領域 (例え ば C→E領域) では低周波成分から高周波成分の腿こ計測するように制钿する。 この場合、 最初の領域ではサンプリング点は原点からの距離が漸次減少し、 後の 領域では原点からの距離が漸次増加するように制御することは前述のとおりであ る。  In the imaging, measurement of the E → C area shown in Fig. 4 is started first, and then measurement of the C → E area is performed. In this case, the sequencer 4 uses the gradient magnetic field in the slice direction in the region to be measured first (for example, the E → C region). And the gradient magnetic field noise in the direction of the phase encoder are controlled so that high-frequency components and low-frequency components are measured in order, and in the subsequent measurement area (for example, C → E area), low-frequency components and high-frequency components are measured. Control to measure the thigh. In this case, as described above, control is performed so that the distance from the origin to the sampling point gradually decreases in the first region, and the distance from the origin gradually increases in the subsequent region.

これによつて、 目的とする血管に造影剤が到達し目的血管を流れる血液の信号 '強度が最も高くなつた時点で k空間の低周波成分を計測することとなり、 動脈の 画像を高いコントラストで描 Ρίできる。 しかも図 5 ( b ) に示すように造影剤到 達時刻 tl を挟んで両側に低周波成分を計測する時間帯が存在するので、 タイミ ング撮像と本撮像との間のわずかな条件の違 、等によつて両者の造影剤到達時刻 tl にずれが生じた場合にも、 画質の劣化が殆どない高品質の画像を得ることが できる。  As a result, when the contrast agent reaches the target blood vessel and the signal of the blood flowing through the target blood vessel reaches the highest intensity, the low-frequency component in the k-space is measured, and the image of the artery is displayed with high contrast. I can draw. Moreover, as shown in Fig. 5 (b), there is a time zone for measuring low-frequency components on both sides of the contrast agent arrival time tl, so that the slight difference in the conditions between timing imaging and main imaging Even when the contrast agent arrival time tl is deviated due to the above, a high-quality image with almost no deterioration in image quality can be obtained.

データ収集法の違いによる動静脈分離の違いをシミュレーションした結果を図 6に示す。 尚、 このシミュレーションは、 FOV:320、 TR: 10ms、 位相エンコード 数: 160、 スライスエンコード数: 16、 画像マトリクス: 256*16、 スライス: 5瞧 の 条件で実行したものであり、 動静脈分離は、 動脈の信号強度と静脈の信号強度の 比で表している。 Figure 6 shows the results of simulating the difference in arteriovenous separation due to the different data collection methods. In this simulation, FOV: 320, TR: 10 ms, number of phase encodes: 160, number of slice encodes: 16, image matrix: 256 * 16, slice: 5 、 The arteriovenous separation is expressed as the ratio of the signal strength of the artery to the signal strength of the vein.

図からわかるように、 本発明のデータ収集法はシーケンシャルオーダリング、 エリプティカルセントリックオ一ダリングと比べ、 動静脈信号比が増加している。 従って動脈の近傍にそれと紛らわしい静脈がある場合でも、 動脈のみを高コント ラストで描画できる。  As can be seen, the data collection method of the present invention has an increased arteriovenous signal ratio as compared to sequential ordering and elliptical centric ordering. Therefore, even if there is a vein near the artery that is confusing, it is possible to draw only the artery with high contrast.

こうして造影前と造影後でそれぞれ三次元画像データを得た後、 これらの差分 を取ることにより、 血管のみの三次元データを得ることができる。 差分処理は、 例えば三次元内のスライス位置の一致するスライス間でそれぞれ複素差分するこ とにより行う。 差分は絶対値の差分でもよい。 このように造影前後の画像間で差 分処理を行なって血管以外の組織を除去する方法は 3D MR-DSA (Digital Subtraction Angiography)と呼ばれ公知の手法であり、 本発明において必須では ないが、 特に血管以外の組織とのコントラストを十分に得られにくい細い血管の 描出に好適である。  Thus, after obtaining the three-dimensional image data before and after the contrast, respectively, by taking the difference between the three-dimensional image data, the three-dimensional data of only the blood vessel can be obtained. The difference processing is performed, for example, by performing a complex difference between slices at the same slice position in three dimensions. The difference may be a difference between absolute values. The method of removing tissue other than blood vessels by performing differential processing between images before and after contrast in this manner is called 3D MR-DSA (Digital Subtraction Angiography) and is a known method, and is not essential in the present invention. In particular, it is suitable for delineating thin blood vessels in which it is difficult to obtain sufficient contrast with tissues other than blood vessels.

さらに差分処理後の三次元データを、 冠状断、 矢状断、 軸横断等、 任意の方向 に投影することにより立体的に観察できる。 投影の手法としては公知の最大ィ直投 影法 (Maximum Intensity Projection)等を採用することができる。  Furthermore, the three-dimensional data after the difference processing can be viewed three-dimensionally by projecting it in any direction, such as coronal section, sagittal section, and transverse axis. As a projection method, a known maximum intensity projection method or the like can be employed.

以上、 本発明の第 1の実施形態を図 4および図 5に示す実施例に基づき説明し たが、 種々の変更が可能である。 例えば、 上記実施例では三次元 MRAシーケンス としてグラディエントエコー法によるシーケンスを例示'したが、 1回の励起で複 数のエコー信号を計測する EPI (Echo Planer Imaging)法や分割型の EPI なども 採用することができる。  As described above, the first embodiment of the present invention has been described based on the examples shown in FIGS. 4 and 5, but various modifications are possible. For example, in the above embodiment, a sequence based on the gradient echo method is exemplified as a three-dimensional MRA sequence, but an EPI (Echo Planer Imaging) method for measuring a plurality of echo signals with one excitation, a split-type EPI, and the like are also employed. can do.

また上記実施例では k空間の分割を kz軸で分割した場合を示した力 ky軸で 分割してもよい。 さらに分割した領域について対称的にデータを収集する場合を 説明したが、 領域は非対称であってもよい。  Further, in the above embodiment, the k space may be divided by the force ky axis which indicates the case where the k space is divided by the kz axis. Although the case where data is collected symmetrically for the divided areas has been described, the areas may be asymmetric.

非対称の場合の実施例を図 7を参照して説明する。 ここでもマトリックスは 5 * 9とし、 k空間を kz軸で分割している場合を例に説明する。 この非対称のデ ータ収集では、 先に計測する領域、 例えば E→C領域では高周波領域からではな く、 中周波領域 (番号 1) 力 計測を開始し、 低周波領域 (番号 15) まで番号順 に計測する。 その後は図 4の場合と同様に低周波領域から高周波領域まで C→E 領域の全領域について計測を行う。 或いはその逆に先に計測する領域については 全領域について計測し、 後半の領域については低周波領域から中周波領域まで計 測を行うことも可能である。 例えば図 7で言えば、 番号 35から計測を開始し、 その後、 番号が小さくなる順序で番号 1まで計測を行ってもよい。 An embodiment in the case of asymmetry will be described with reference to FIG. Again the matrix is 5 * 9 and the case where the k space is divided by the kz axis will be described as an example. In this asymmetric data collection, force measurement is started not in the high-frequency region but in the medium-frequency region (No. 1) in the region to be measured first, for example, in the E → C region, and continues until the low-frequency region (No. 15). Measure in order. After that, measurement is performed for the entire C → E region from the low frequency region to the high frequency region as in the case of Fig. 4. Or, conversely, it is possible to measure the whole area for the area to be measured first, and to measure from the low frequency area to the medium frequency area for the latter area. For example, referring to FIG. 7, the measurement may be started from number 35, and thereafter, the measurement may be performed up to number 1 in the order of decreasing numbers.

このように 2分割された領域の一方の計測点数を他方よりも少なくすることに より、 全体としての撮像時間を短縮することができる。 即ち、 図 5 ( c ) ( d ) に示すように先に計測する領域の計測点数を減らしたり、 後に計測する領域の計 測点数を減らすことにより、 図 5 ( b ) に比べ撮像時 が短くなる。 さらに図 5 ( d ) に示す計測方法は、 目的血管とその近傍にある静脈との距離が短く、 造影 剤が目的血管に到達した後、 近傍の静脈に達する時間が短い場合に有効であり、 後半の領域を低周波成分から中周波成分まで計測することにより、 近傍の静脈か らの信号 (図中、 点線で示す信号強度曲線) が混入するのを防止することができ る。 ,  By making the number of measurement points of one of the two divided areas smaller than that of the other, the imaging time as a whole can be reduced. In other words, as shown in Figs. 5 (c) and (d), the number of measurement points in the area to be measured first is reduced, or the number of measurement points in the area to be measured later is reduced, so that the imaging time is shorter than in Fig. 5 (b). Become. Furthermore, the measurement method shown in Fig. 5 (d) is effective when the distance between the target blood vessel and the nearby vein is short, and the time when the contrast agent reaches the target blood vessel after reaching the target blood vessel is short. By measuring the low frequency component to the middle frequency component in the second half region, it is possible to prevent the signal from the nearby vein (the signal strength curve shown by the dotted line in the figure) from being mixed. ,

この場合、 計測点数が少ない領域のデータは、 計測されていないデータ (図 7 に斜線で示す領域のデータ) を計測されてレ、る領域のデータから推定してもよい し、 または 0づめをしてもよい。 この実施例でも上述した効果に加え、 三次元計 測タイミングのずれによる影響を低減しつつ、 選択的に高コントラストな動脈像 を得ることができる。  In this case, the data in the area with a small number of measurement points may be estimated from the data in the area where the unmeasured data (the data in the shaded area in Fig. 7) is measured, or May be. Also in this embodiment, in addition to the above-described effects, it is possible to selectively obtain a high-contrast artery image while reducing the influence of the shift in the three-dimensional measurement timing.

さらに k空間におけるデータ収集は、 図 4や図 7に示すような矩形のマトリク ッスに限らず、 図 8に示すように原点 (番号 15) を中心とする円 (楕円) 内の データを収集することも可能である。 図 8に示す実施例でもスライスエンコード 数は 5、 位相エンコード数は 9であるが、 ここでは k y、 k zが共に高周波成分 となる領域 (円の外側) は計測せずに、 原点 (番号 15) を中心として同心円状 に配置されるデータを収集する。 データ収集の順序は、 図中丸で囲んだ番号で示 したように、 最初に計測される下半分の領域では、 中心から遠い方から順に中心 に向かい、 上半分の領域では中心から遠ざかる方向で計測する。 Furthermore, data collection in k-space is not limited to rectangular matrices as shown in Figs. 4 and 7, and data within a circle (ellipse) centered on the origin (No. 15) as shown in Fig. 8 It is also possible. In the embodiment shown in FIG. 8, the number of slice encodes is 5, and the number of phase encodes is 9. Here, both ky and kz are high-frequency components. The area (outside the circle) is collected, but data concentrically arranged around the origin (No. 15) is collected. As shown by the circled numbers in the figure, the order of data collection is as follows: in the lower half area, which is measured first, from the center to the center in order from the side farther from the center, and in the upper half area, the measurement is in the direction away from the center. I do.

この場合にも図 4に示す実施例と同様の効果を得ることができる。 またこの場 合にも必要に応じてデーダの補間を行うことができる。  In this case, the same effect as that of the embodiment shown in FIG. 4 can be obtained. Also in this case, data interpolation can be performed as needed.

以上、 本発明の第 1の実施形態として、 k空間の領域を分割して、 領域によつ て測定点を 2群に分けた実施形態を説明したが、 測定点を領域に関係なく、 2群 に分けることも可能である。  As described above, as the first embodiment of the present invention, the embodiment in which the region of the k space is divided and the measurement points are divided into two groups according to the region has been described. It is also possible to divide them into groups.

次に本発明の第 2の実施形態として、 k空間の測定点を、 互いに複素 殳関係 にあるものが異なる群に属するように分割する場合を説明する。  Next, as a second embodiment of the present invention, a case will be described in which measurement points in k-space are divided such that those having a complex relationship with each other belong to different groups.

この実施形態では、 k空間、 例えば ky-kz空間の格子点、 即ち計測点を 2つの 群に分割するに際し、 1 ) 2つの群は原点を共有し、 2つの群に属する計測点が 互いに複素 殳の関係にあること、 2 ) k空間において隣接する計測点が異なる 群に属することを満たすように、 分割する。 そして、 このように分割した 2つの 群を順次計測する。  In this embodiment, when dividing grid points in k space, for example, ky-kz space, that is, measurement points into two groups, 1) the two groups share the origin, and the measurement points belonging to the two groups are complex with each other. 2) Divide so that the adjacent measurement points in k-space belong to different groups. Then, the two groups thus divided are sequentially measured.

図 9に第 2の実施形態によるデータ収集法の零純化した一例として、 スライス エンコード数が 8、 位相エンコード数が 8である 8 * 8マトリックスの k空間を 示す。 こめマトリクスには 64 の格子点 (計測点) が存在し、 これら格子点は図 中、 左側に示す第 1群と右側に示す第 2群に分割されている。 これら 2つの群に 属する格子点 互いに複素共役の関係にあり、 隣接する格子点は異なる群に属す 'る。 但し、 複素共役の関係を満たすために、 原点の近傍においては、 隣接する格 子点は一つの群に属することになる。 '  FIG. 9 shows a k-space of an 8 * 8 matrix in which the number of slice encodes is 8 and the number of phase encodes is 8, as an example of the data collection method according to the second embodiment, which is zero-purified. There are 64 grid points (measurement points) in the rice matrix, and these grid points are divided into a first group on the left and a second group on the right. Lattice points belonging to these two groups have a complex conjugate relationship with each other, and adjacent lattice points belong to different groups. However, in order to satisfy the complex conjugate relation, adjacent lattice points belong to one group near the origin. '

これら 2つの群のうち最初に計測する第 1の群では、 k空間上の原点 0力 らの 距離が大きい点から計測を開始し、 その後漸次原点 0に近づくようにサンプリン グ点を高周波成分から低周波成分に向かってサンプリング制御する。 また第 2の 群では、 逆に原点 0或いはその近傍から、 原点 0からの距離が漸次離れていくよ うにサンプリング点を低周波成分から高周波成分に向かってサンプリング制御す る。 The first of these two groups, which measures first, starts the measurement from the point in k-space where the distance from the origin 0 force is large, and then gradually increases the sampling point from the high-frequency component so as to approach the origin 0 gradually. Sampling control is performed toward low frequency components. Also the second In the group, on the contrary, the sampling point is controlled from the low-frequency component to the high-frequency component such that the distance from the origin 0 gradually increases from or near the origin 0.

図中、 丸で囲まれた数字はデータ収集順序を示す。 同じ数字の計測点には序列 がなく、 それらのうちのいずれから計測してもよいことを示している ώ In the figure, circled numbers indicate the data collection order. No hierarchy is the measurement point of the same number, indicating that it may be measured from either of them ώ

最初に計測を開始する第 1群では原点 (番号 33 が付された格子点) から最も 遠い格子点 (番号 1)、 即ち最も高周波成分から計測を開始し、 次に番号 2 の格 子点、 番号 3の格子点というように順次原点まで計測を行う。 続いて第 2群の計 測を行い、 ここでは原点に最も近い格子点 (番号 34)、 即ち低周波成分から計測 を開始し、 順次原点から.離れる順序で計測を行う。  In the first group, which starts measurement first, the measurement starts from the grid point (number 1) farthest from the origin (the grid point with number 33), that is, the highest frequency component, and then the grid point of number 2 Measurements are sequentially performed up to the origin, such as the grid point of number 3. Next, measurement of the second group is performed. Here, measurement is started from the lattice point (No. 34) closest to the origin, that is, the low-frequency component, and measurement is performed in order from the origin in order.

次にこのようなデータ収集法を採用した上記 MRI装置による造影 MRAの一実施 例を図 1 0を参照して説明する。  Next, an embodiment of a contrast-enhanced MRA using the MRI apparatus adopting such a data collection method will be described with reference to FIG.

まず第 1の実施形態と同様に、 被検体を静磁場磁石内の計測空間に配置し、 目 的とする血管を含む撮像領域を決定し、 タイミング撮像を行う。 この場合にも、 タイミング撮像は、 例えばテストインジェクション法によって行う。 即ち、 少量 の造影剤(約 l〜2ml)をテスト注入して、 図 1 0に示すように、 対象部位におけ る時間 "^言号曲線を得、 そこから驟剤の到達時刻 (信号強度がピークとなる時 刻) tlを計測し、 この結果を基にして本撮像を行うタイミングを決定する。 ' タイミング撮像の锋、 図 1 0 ( b ) に示すように本撮像を行う。 本撮像は造影 剤注入後の撮像のみを行つてもよいが、 好適には造影剤注入前と造影注入後の画 像を撮像する。 造影前と造影後の撮像は、 同一条件で同一スライスまたはスラブ 位置について連続的に行う。  First, similarly to the first embodiment, the subject is placed in the measurement space in the static magnetic field magnet, an imaging region including a target blood vessel is determined, and timing imaging is performed. Also in this case, the timing imaging is performed by, for example, a test injection method. That is, a small amount of a contrast medium (about 1 to 2 ml) was test-injected, and as shown in Fig. 10, the time at the target site "^ sign curve was obtained, from which the arrival time of the syrup (signal intensity) Measure the tl and determine the timing to perform the main imaging based on the result. 'Timing imaging, perform the main imaging as shown in Fig. 10 (b). May perform only imaging after the injection of the contrast medium, but preferably images before and after the injection of the contrast medium.Imaging before and after the imaging is performed under the same conditions under the same slice or slab position. Is performed continuously.

撮像シーケンスは図 3に示すような短 TRの三次元グラディエントエコー法を 基本とするシーケンスである。 この場合、 血流を撮像対象としているので、 流れ によるディフェイズをリフェイズするための傾斜磁場即ちダラディエントモーメ ントヌリング(Gradient Moment Nulling)を付加してもよいが、 これは必須では なく、 TR/TE短縮のためにはむしろ単純なグラディエントエコーとするのが好ま しい。 The imaging sequence is a sequence based on the short TR 3D gradient echo method as shown in Fig. 3. In this case, since the blood flow is to be imaged, a gradient magnetic field, that is, Gradient Moment Nulling may be added for rephasing the phase due to the flow, but this is not essential. Instead, it is preferable to use a simple gradient echo for shortening TR / TE.

パルスシーケンスの繰り返し時間 TRおよびマトリクスサイズ (スライスェン コード数及び位相ェンコ一ド数) 並びに加算数が決まると撮像時間 Tが決まるの で、 上記タイミング撮像で得られた目的とする血管の造影剤到達時刻 tl を基に、 目的とする血管に造影剤が到達した時に ky- kz空間の低周波領域のデータ計測が 行われるように、 撮像開始時刻 t2 (造影剤を注入してから撮像を開始するまで の時間) を設定する。 撮像はまず第 1群の計測を開始し、 続いて第 2群の計測を 行う。 この場合、 シーケンサ 4は先に計測する第 1群ではスライス方向傾 磁場 パルスと位相ェンコード方向の傾斜磁場パノレスをともに高周波成分から低周波成 分を順に計測するように制御し、 またその後に計測する第 2群では低周波成分か ら高周波成分の順に計測するように制御する。 こうして造影後の三次元画像デー タを得る。  Once the pulse sequence repetition time TR and matrix size (number of slice codes and number of phase codes) and the number of additions are determined, the imaging time T is determined. Based on tl, imaging start time t2 (from the injection of the contrast agent to the start of imaging, so that data measurement in the low-frequency region of the ky-kz space is performed when the contrast agent reaches the target blood vessel. Time). In imaging, measurement of the first group is first started, and then measurement of the second group is performed. In this case, the sequencer 4 controls both the gradient magnetic field pulse in the slice direction and the gradient magnetic field in the phase encode code in the first group to be measured first so that the high frequency component and the low frequency component are sequentially measured, and then the measurement is performed thereafter. In the second group, control is performed so that measurement is performed in order from low-frequency components to high-frequency components. In this way, three-dimensional image data after contrast is obtained.

図 9および図 1 0 ( b ) では、 データ収集法としては第 1群と第 2群のいずれ' も群に属する全計測点を計測する場合を示したが、 図 1 0 ( c ) に示すように第 1群は所定の高周波成分の計測を省き、 短時間で低周波成分の計測を行うデータ 収集法を採用してもよい。 , このようなデータ収集法の一例を図 1 1に示す。 囪 1 1でも、 スライスェンコ 一ド数が 8、 位相ェンコ一ド数が 8である 8 * 8マトリックスの k空間を例示し た。 この実施例でも図 9に示す実施例と同様の条件で k空間を 2つの群に分割し ているが、 ここでは最初に計測する.第 群では所定の高周波成分の計測を行わず、 低周波成分のみを計測する。 図示する実施例では k空間の格子点のうち低周波領 域の 4 * 4マドリッタスに存在する格子点のみが計測される。 まずこれら低周波 領域の格子点のうち原点 (番号 9の格子点) 力 の距離が一番遠い格子点を始点 とし、 番号 2の格子点、 番号 3の格子点の順に、 原点まで計測する。  In Fig. 9 and Fig. 10 (b), the data collection method shows a case where all the measurement points belonging to both the first group and the second group are measured, as shown in Fig. 10 (c). As described above, the first group may employ a data collection method in which measurement of a predetermined high-frequency component is omitted and low-frequency components are measured in a short time. An example of such a data collection method is shown in FIG.囪 11 also illustrates an 8 * 8 matrix k-space in which the number of slice switches is 8, and the number of phase switches is 8. In this embodiment, the k-space is divided into two groups under the same conditions as in the embodiment shown in Fig. 9, but here the measurement is performed first. Measure only the components. In the illustrated embodiment, only grid points present in 4 * 4 madridas in the low frequency region are measured among grid points in the k space. First, among the grid points in these low-frequency regions, the grid point with the greatest distance of the origin (grid number 9) is used as the starting point, and the grid point of number 2 and the grid point of number 3 are measured up to the origin.

第 2群では、 図 9に示す実施例と同様に原点に隣接する格子点 (番号 10) か ら計測し、 原点から離れる順序で最高周波成分まで第 2群に属する格子点全体を 計測する。 In the second group, as in the embodiment shown in FIG. 9, the grid point (number 10) adjacent to the origin From the origin, and measure all grid points belonging to the second group up to the highest frequency component in the order away from the origin.

この場合、 第 1群のうち計測されなかった高周波領域のデータは、 第 1群と第 2群の複素^ f殳性に基づき推定することができる。 未計測データの推定方法は、 公知のハーフフーリエ再構成法に基.づく方法を採用することができる。 図 1 2は これらの処理を模式的に示したものである。 計測データをまず周波数ェンコ一ド 方向 (k x方向) に一次元フーリエ変換し、 三次元ハイブリッド空間の実計測デ ータを得る。 この実計測データから三次元推定データを得て、 実計測データと推 定データとを合成することによりハイプリッド空間データを得る。 このハイプリ ッド空間データを二次元フーリエ変換することにより三次元画像データを得る。 これ よりデータ点数を削減しても空間分解能を劣ィ匕させることがない。, この実施例でも、 図 9に示すデータ収集法と同様に目的とする血管に造影剤が 到達し目的血管を流れる血液の信号強度が最も高くなった時点で k空間の低周波 成分を計測することとなり、 動脈の画像を高いコントラストで描画できる。  In this case, the data of the high frequency region that is not measured in the first group can be estimated based on the complex characteristics of the first group and the second group. As a method of estimating unmeasured data, a method based on a known half Fourier reconstruction method can be employed. FIG. 12 schematically shows these processes. First, the measured data is subjected to one-dimensional Fourier transform in the frequency encoder direction (k x direction) to obtain the actual measured data in the three-dimensional hybrid space. The three-dimensional estimated data is obtained from the actual measurement data, and the hybrid spatial data is obtained by combining the actual measurement data and the estimation data. Three-dimensional image data is obtained by subjecting the hybrid space data to two-dimensional Fourier transform. Thus, even if the number of data points is reduced, the spatial resolution is not degraded. In this embodiment, as in the data collection method shown in FIG. 9, the low-frequency component in k-space is measured when the contrast agent reaches the target blood vessel and the signal intensity of the blood flowing through the target blood vessel becomes the highest. This means that artery images can be drawn with high contrast.

また一般に図 1 2に示すように造影剤注入後、 造影剤濃度 (信号強度) は急激 に上昇するので、 最も低周波成分を計測する時点を信号強度のピークに合わせ、 ピーク前の計測が短レ、本実施例の撮像方法を実施することにより、 造影剤到達前 の不要な信号の計測を避けることができる。  In general, as shown in Fig. 12, after the injection of the contrast agent, the concentration of the contrast agent (signal intensity) rises sharply. By implementing the imaging method of the present embodiment, it is possible to avoid measurement of an unnecessary signal before reaching the contrast agent.

撮像法 (データ収集法) の違いによる動静脈分離の違いをシミュレーションし た結果を図 1 3及び図 1 4に示す。 このシミュレーションは、 動脈および静脈の 模擬血管を用い、 これに流速 40cm 、 動脈静脈還流時間 7秒、 注入速度 2cc/s で造影剤を流入レ、 これを異なる撮像法で撮像したものである。 図 1 3は、 上記 条件における信号強度を示す。 図示するように、 最初に動脈からの信号のピーク が見られ、 遅れて静脈からの信号のピークが現れる。 また図 1 4 (a) は本発明 の撮像法による画像、 同図 (b)はェリブティカノレセントリックオーダリングによ る画像である。 図からわかるように、 エリプティカルセントリックオーダリングでは動脈の他 に静脈も画像化してしまい、 動静脈分離が完全でないのに対し、 本発明の撮像法 では動脈のみを嵩コントラストで描画できる。 Figures 13 and 14 show the results of simulating differences in arteriovenous separation due to differences in imaging methods (data collection methods). In this simulation, a simulated artery and vein was used, and a contrast medium was flowed into it at a flow rate of 40 cm, an arterial venous return time of 7 seconds, and an injection speed of 2 cc / s. FIG. 13 shows the signal strength under the above conditions. As shown in the figure, the peak of the signal from the artery is seen first, and the peak of the signal from the vein appears later. FIG. 14 (a) is an image obtained by the imaging method of the present invention, and FIG. 14 (b) is an image obtained by elibutanore centric ordering. As can be seen from the figure, in the elliptical centric ordering, veins as well as arteries are imaged, and arteriovenous separation is not complete, whereas the imaging method of the present invention allows only arteries to be drawn with bulk contrast.

尚、 以上説明した第 2の実施形態でも、 三次元 MMシーケンスとしてダラディ ェントエコー法によるシーケンスを例示したが、 1回の励起で複数のエコー信号 を計測する EPI (Echo Planer Imaging)法や分割型の EPI なども採用することが できる。  Note that, in the second embodiment described above, a sequence using the Daradent echo method has been exemplified as the three-dimensional MM sequence, but an EPI (Echo Planer Imaging) method in which a plurality of echo signals are measured by one excitation or a split type EPI can also be adopted.

さらに k空間におけるデータ収集は、 図 9や図 1 1に示すような矩形のマトリ クッスに限らず、 図 1 5に示すように原点を中心とする円 (楕円) 内のデータを 収集することも可能である。 図中、 実線で示す第 1の群では、 k空間上の原点 0 からの距離が大きい点から計測を開始し、 その後漸次原点 0に近づくようにサン プリング点を高周波成分から低周波成分に向かってサンプリング制御する。 また 第 2の群では、 逆に原点 0或いはその近傍から、 原点 0からの距離が漸次離れて いくようにサンプリング点を低周波成分から高周波成分に向かってサンプリング 制御する。  Furthermore, data collection in k-space is not limited to the rectangular matrix shown in Fig. 9 and Fig. 11, and data in a circle (ellipse) centered on the origin as shown in Fig. 15 can also be collected. It is possible. In the first group shown by the solid line in the figure, measurement starts at a point in k-space that is farther from the origin 0, and then gradually moves the sampling point from the high-frequency component to the low-frequency component so as to approach the origin 0 gradually. Sampling control. On the other hand, in the second group, the sampling point is controlled from the low-frequency component to the high-frequency component such that the distance from the origin 0 gradually increases from or near the origin 0.

この場合にも図 9および図 1 1に示す実施例と同様の効果を得ることができる。 またこの場合にも必要に応じて第 1群の高周波成分の計測を省略することができ る。 産業上の利用性  In this case, the same effects as those of the embodiment shown in FIGS. 9 and 11 can be obtained. Also in this case, the measurement of the first group of high-frequency components can be omitted as necessary. Industrial applicability

以上説明したように本発明の MRI装置によれば、 ky- kz 空間の格子点 (測定 点) を 2つの群に分割し、 先に計測する 1方の群では k空間上の原点からの距離 が漸次的に近づくようにサンプル点を高周波成分から低周波成分に向かってサン プリング制御し、 他方の群においては逆にその距離が漸次的に離れていくように サンプル点を低周波成分から高周波成分に向かってサンプリング制御するように したので、 撮像タイミングのずれによる影響を低減しつつ、 高コントラストで動 静脈分離された面像を得ることが可能となる。 また、 2分割した一方の領域にお ける計測点数を少なくすることにより撮像時間の短縮を図ることができる。 As described above, according to the MRI apparatus of the present invention, the grid points (measurement points) in the ky-kz space are divided into two groups, and one of the groups measured first has a distance from the origin in the k space. The sampling point is controlled from the high-frequency component to the low-frequency component so that the sampling point gradually approaches, and in the other group, the sampling point is shifted from the low-frequency component to the high-frequency component so that the distance gradually increases. Sampling control is performed for each component, so that the effect of high contrast can be achieved while reducing the effect of the imaging timing shift. A vein-separated surface image can be obtained. Also, the imaging time can be reduced by reducing the number of measurement points in one of the two divided areas.

Claims

請求の範囲 The scope of the claims 1. 被検体の置かれる空間に静磁場を発生する静磁場発生手段と、 前記空間にス ライス方向、 位相ェンコ一ド方向及び読み出し方向の各傾斜磁場を与える傾斜磁 場発生手段と、 前記被検体の生体 の原子核に核磁気共鳴を起こさせるために 高周波磁場を照射する送信系と、 前記核磁気共鳴により放出されるエコー信号を 検出する受信系と、 前記傾斜磁場発生手段、 送信系および受信系を制御する制御 系と、 受信系で検出したェコ一信号を用いて画像再構成演算を行う信号処理系と、 得られた画像を表示する手段とを備えた磁気共鳴イメージング装置において、 前記制御系は、 スライスエンコード及 立相エンコードを付与する三次元シー ケンスを実行し、 この際、 スライスエンコード数および位相エンコード数で規定 きれる k空間の計測点を 2つの群に分け、 第 1の群の計測は k空間上の原点から 計測点までの距離が計測順に漸減し、 第 2の群の計測は k空間上の原点から計測 点までの距離が計測順に漸増するように前記スラィス方向および位相ェンコ一ド 方向の傾斜磁場発生手段を制御することを特徴とする磁気共鳴イメージング装置。1. a static magnetic field generating means for generating a static magnetic field in a space where a subject is placed; a gradient magnetic field generating means for applying a gradient magnetic field in each of a slice direction, a phase encoding direction, and a readout direction to the space; A transmitting system that irradiates a high-frequency magnetic field to cause nuclear magnetic resonance in an atomic nucleus of a living body of a specimen; a receiving system that detects an echo signal emitted by the nuclear magnetic resonance; a gradient magnetic field generating unit; a transmitting system; A magnetic resonance imaging apparatus comprising: a control system that controls the system; a signal processing system that performs an image reconstruction operation using the echo signal detected by the reception system; and a unit that displays an obtained image. The control system executes a three-dimensional sequence that provides slice encoding and erroneous phase encoding. At this time, the k-space defined by the number of slice encodings and the number of phase encodings is used. The measurement points are divided into two groups.The measurement of the first group gradually reduces the distance from the origin in k-space to the measurement point in the order of measurement.The measurement of the second group measures the distance from the origin in k-space to the measurement point. A magnetic resonance imaging apparatus characterized in that the gradient magnetic field generation means in the slice direction and the phase encode direction is controlled so that the distance gradually increases in the order of measurement. 2. 前記 2つの群は、'前記 k空間を 2分割してなる 2つの領域にそれぞれ属す る:!とを特徴とする請求項 1記載の磁気共鳴ィメ一ジング装置。 2. The two groups belong to two regions that are obtained by dividing the k-space into two:! 2. The magnetic resonance imaging apparatus according to claim 1, wherein: 3 . 前記 2つの群は、.原点を共有し、 互いに複素共役の関係にあることを特徴 とする請求項 1記載の磁気共鳴ィメ一ジング装置。  3. The magnetic resonance imaging apparatus according to claim 1, wherein the two groups share an origin and are in a complex conjugate relationship with each other. 4. 前記 k空間の計測点は、 隣り合う計測点が異なる群に属するように分割さ れることを特徴とする請求項 3記載の磁気共鳴ィメ一ジング装置。 4. The magnetic resonance imaging apparatus according to claim 3, wherein the measurement points in the k-space are divided so that adjacent measurement points belong to different groups. 5. 前記 2.つの群の少なくとも一方は、 非計測点を含むことを特徴とする請求 項 1記載の磁気共鳴ィメ一ジング装置。  5. The magnetic resonance imaging apparatus according to claim 1, wherein at least one of the two groups includes a non-measurement point. 6 . 前記 2つの群の和集合は、 前記 k空間に内接する円領域内であることを特 徴とする請求項 1記載の磁気共鳴イメージング装置。  6. The magnetic resonance imaging apparatus according to claim 1, wherein the union of the two groups is within a circular region inscribed in the k-space. 7. 被検体の所定の領域を選択して励起し、 少なくとも二方向にェンコ一ドす る傾斜磁場を印加し、 前記領域から生じるェコ一信号を計測するステツプを前記 傾斜磁場の強度を変えながら複数回繰り返し、 三次元画像データを収集するデー タ収集方法において、 7. Select and excite a given area of the subject and encode in at least two directions A data acquisition method for acquiring three-dimensional image data by repeating a step of applying a gradient magnetic field and measuring an echo signal generated from the region a plurality of times while changing the intensity of the gradient magnetic field. 前記二方向のェンコ一ド傾斜磁場強度で規定される計測空間の計測点を第.1及 ぴ第 2の群に分割し、  Dividing the measurement points of the measurement space defined by the two-way encoder gradient magnetic field strength into the first and second groups, 第 1及び第 2の群について順次計測を行い、  The first and second groups were measured sequentially, その際、 最初に計測される第 1の群では、 前記計測空間の原点から計測点まで の距離が計測順に漸減するように計測し、 後で計測される第 2の群では前記計測 空間の原点から計測点までの距離が計測順に漸増するように計測することを特徴 とするデータ収集方法。  At that time, in the first group that is measured first, the distance from the origin of the measurement space to the measurement point is measured so as to gradually decrease in the order of measurement, and in the second group that is measured later, the origin of the measurement space is measured. A data collection method characterized in that the distance from a measurement point to a measurement point gradually increases in the order of measurement. 8 . 被検体の所定の領域を選択して励起し、 少なくとも二方向にェンコ一ドす る傾斜磁場を印加し、 前記領域から生じるエコー信号を計測するステップを前記 傾斜磁場の強度を変えながら複数回繰り返し、 三次元画像データを収集するデー タ収集方法において、  8. A plurality of steps of selecting and exciting a predetermined region of the subject, applying a gradient magnetic field that encodes in at least two directions, and measuring an echo signal generated from the region while changing the intensity of the gradient magnetic field. Data collection method to collect 3D image data 前記二方向のェンコ一ド傾斜磁場強度で規定される計測空間を 2分割し、 2分割された領域について順次計測を行い、 .  The measurement space defined by the two-direction encoder gradient magnetic field strength is divided into two, and measurements are sequentially performed on the two divided regions. その際、 最初に計測される領域では、 前記計測空間の原点から計測点までの距 離が計測順に漸減するように計測し、 後で計測される領域においては前記計測空 間の原点から計測点までの距離が計測順に漸増するように計測することを特徴と するデータ収集方法。  At that time, in the area to be measured first, measurement is performed so that the distance from the origin of the measurement space to the measurement point gradually decreases in the order of measurement, and in the area to be measured later, the measurement point is measured from the origin of the measurement space to the measurement point. A data collection method characterized in that measurements are taken so that the distance to the target gradually increases in the order of measurement. 9 . 被検体の所定の領域を選択して励起レ、 少なくとも二方向にェンコ一ドす る傾斜磁場を印カ卩し、 .前記領域から生じるエコー信号を計測するステップを前記 傾斜磁場の強度を変えながら複数回繰り返し、 三次元画像デ タを収集するデー タ収集方法において、  9. Select a predetermined region of the subject, excite it, apply a gradient magnetic field that encodes in at least two directions, and measure the echo signal generated from the region. In a data collection method that collects 3D image data by repeating multiple times while changing 前記二方向のエンコード傾斜磁場強度で規定される計測空間の計測点を、 原点 を共有し、 互いに複素共役の関係で且つ隣り合う格子点は異なる群に属するよう に第 1及び第 2の群に分割し、 The measurement points in the measurement space defined by the two-direction encoding gradient magnetic field intensities share the origin, and the lattice points adjacent to each other have a complex conjugate relationship and belong to different groups. Divided into the first and second groups, 第 1及び第 2の群について順次計測を行い、  The first and second groups were measured sequentially, その際、 最初に計測される第 1の群では、 前記計測空間の原点から計測点まで の距離が計測順に漸減するように計測し、 後で計測される第 2の群では前記計測 空間の原点がら計測点までの距離が計測順に漸増するように計測することを特徴 とするデータ収集方法。  At that time, in the first group that is measured first, the distance from the origin of the measurement space to the measurement point is measured so as to gradually decrease in the order of measurement, and in the second group that is measured later, the origin of the measurement space is measured. A data collection method characterized in that the distance to a measurement point is gradually increased in the order of measurement. 1 0; 前記 2つの群のいずれ力一方の群では、 全計測点のうち、 一部の計測点 のみを計測し、 他方の群では全計測点を計測することを特徴とする請求項 7記載 のデータ収集方法。  10. The method according to claim 7, wherein one of the two groups measures only a part of the measurement points in one of the two groups and measures all the measurement points in the other group. Data collection method. 1 1 . 造影剤を用いた三次元血流描画方法であって、 1 1. A three-dimensional blood flow drawing method using a contrast agent, 造影剤投与後、目的とする血管に造影剤が到達するまでの時間を計測するステ ップと、  Measuring the time it takes for the contrast agent to reach the target blood vessel after administration of the contrast agent, 前記請求項 7ないし 9のいずれか 1項記載のデータ収集法を実施するステップ とを有し、  Carrying out the data collection method according to any one of claims 7 to 9, 前記第 1の群の計測の終了が、 造影剤到達時間に一致するように前記第 1の群 の計測開始時間を制御することを特徴とする三次元血流描画方法。  A three-dimensional blood flow drawing method, wherein the measurement start time of the first group is controlled so that the end of the measurement of the first group coincides with the arrival time of a contrast agent.
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JPH0523314A (en) * 1991-07-19 1993-02-02 Hitachi Medical Corp Mri apparatus
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