|Numéro de publication||USRE32701 E|
|Type de publication||Octroi|
|Numéro de demande||US 07/036,103|
|Date de publication||21 juin 1988|
|Date de dépôt||8 avr. 1987|
|Date de priorité||4 janv. 1983|
|État de paiement des frais||Payé|
|Numéro de publication||036103, 07036103, US RE32701 E, US RE32701E, US-E-RE32701, USRE32701 E, USRE32701E|
|Inventeurs||Paul R. Moran|
|Cessionnaire d'origine||Wisconsin Alumni Research Foundation|
|Exporter la citation||BiBTeX, EndNote, RefMan|
|Citations de brevets (22), Citations hors brevets (61), Référencé par (26), Classifications (6), Événements juridiques (3)|
|Liens externes: USPTO, Cession USPTO, Espacenet|
S(t)=∫∫M.sub.1 (r,v)e.sup.2πiγ[G·rt+F·v(T).spsp.2.sup.] drdv
The field of the invention is gyromagnetic resonance spectroscopy, and particularly, nuclear magnetic resonance (NMR) techniques for measuring the properties of materials.
Gyromagnetic resonance spectroscopy is conducted to study nuclei that have magnetic moments and electrons which are in a paramagnetic state. The former is referred to in the art as nuclear magnetic resonance (NMR), and the latter is referred to as paramagnetic resonance (EPR) or electron spin resonance (ESR). There are other forms of gyromagnetic spectroscopy that are practiced less frequently, but are also included in the field of this invention.
Any nucleus which possesses a magnetic moment attempts to align itself with the direction of the magnetic field in which it is located. In doing so, however, the nucleus precesses around this direction at a characteristic angular frequency (.[.Larmour.]. .Iadd.Larmor .Iaddend.frequency) which is dependent on the strength of the magnetic field and on the properties of the specific nuclear species (the magnetogyric constant γ of the nucleus).
When a substance such as human tissue is subjected to a uniform magnetic field (polarizing field Bz) the individual magnetic moments of the paramagnetic nuclei in the tissue attempt to align with this field, but precess about it in random order at their characteristic .[.Larmour.]. .Iadd.Larmor .Iaddend.frequency. A net magnetic moment Mz is produced in the direction of the polarizing field but the randomly oriented components in the perpendicular plane (x-y plane) cancel one another. If, however, the substance, or tissue, is irradiated with a magnetic field (excitation field B1) which is in the x-y plane and which is near the .[.Larmour.]. .Iadd.Larmor .Iaddend.frequency, the net aligned moment, Mz, can be rotated into the x-y plane to produce a net transverse magnetic moment M1 which is rotating in the x-y plane at the .[.Lamour.]. .Iadd.Larmor .Iaddend.frequency. The degree to which the rotation of Mz into an M1 component is achieved, and hence, the magnitude and the direction of the net magnetic moment (M=M0 +M1) depends primarily on the length of time of the applied excitation field B1.
The practical value of this gyromagnetic phenomena resides in the radio signal which is emitted after the excitation signal B1 is terminated. When the excitation signal is removed, an oscillating sine wave is induced in a receiving coil by the rotating field produced by the transverse magnetic moment M1. The frequency of this signal is the .[.Larmour.]. .Iadd.Larmor .Iaddend.frequency, and its initial amplitude, A0, is determined by the magnitude of M1. The amplitude A of the emission signal (in simple systems) decays in an exponential fashion with time, t:
The decay constant 1/T2 is a characteristic of the process and it provides valuable information about the substance under study. The time constant T2 is referred to as the "spin-spin relaxation" constant, or the "transverse relaxation" constant, and it measures the rate at which the aligned precession of the nuclei dephase after removal of the excitation signal B1.
Other factors contribute to the amplitude of the free induction decay (FID) signal which is defined by the T2 spin-spin relaxation process. One of these is referred to as the spin-lattice relaxation process which is characterized by the time constant T1. This is also called the longitudinal relaxation process as it describes the recovery of the net magnetic moment M to its equilibrium value M0 along the axis of magnetic polarization (Z). The T1 time constant is longer than T2, much longer in most substances, and its independent measurement is the subject of many gyromagnetic procedures.
The measurements described above are called "pulsed NMR measurements." They are divided into a period of excitation and a period of emission. As will be discussed in more detail below, this measurement cycle may be repeated many times to accumulate different data during each cycle or to make the same measurement at different locations in the subject. A variety of preparative excitation techniques are known which involve the application of one or more excitation pulses of varying duration. Such preparative excitation techniques are employed to "sensitize" the subsequently observed free induction decay signal (FID) to a particular phenomena. Some of these excitation techniques are disclosed in U.S. Pat. Nos. 4,339,716; 4,345,207; 4,021,726; 4,115,730 and 3,474,329.
Although NMR .[.meansurements.]. .Iadd.measurements .Iaddend.are useful in many scientific and engineering fields, their potential use in the field of medicine is enormous. NMR measurements provide a contrast mechanism which is quite different from x-rays, and this enables differences between soft tissues to be observed with NMR which are completely indiscernible with x-rays. In addition, physiological differences can be observed with NMR measurements, whereas x-rays are limited primarily to anatomical studies.
For most medical applications utilizing NMR, an imaging technique must be employed to obtain gyromagnetic information at specific locations in the subject. The foremost NMR imaging technique is referred to as "zeugmatography" and was first proposed by P. C. Lauterbur in a publication "Image Formation by Induced Local Interactions: Examples Employing Nuclear Magnetic Resonance", Nature, Vol. 242, Mar. 16, 1973, pp. 190-191. Zeugmatography employs one or more additional magnetic fields which have the same direction as the polarizing field B0, but which have a nonzero gradient. By varying the strength (G) of these gradients, the net strength of the polarizing field B0 =Bz +Gx X+Gy Y+Gz Z at any location can be varied. As a result, if the frequency response of the receiver is narrowed to respond to a single frequency, W0, then gyromagnetic phenomena, will be observed only at a location where the net polarizing field B0 is of the proper strength to satisfy the .[.Larmour.]. .Iadd.Larmor .Iaddend.equation; W0 =γB.sub. 0 : where W0 is the .[.Larmour.]. .Iadd.Larmor .Iaddend.frequency at that location.
By "linking" the resulting free induction signal FID with the strengths of the gradients (G=Gx, Gy, Gz) at the moment the signal is generated, the NMR signal is "tagged", or "sensitized", with position information. Such position sensitizing of the NMR signal enables an NMR image to be produced by a series of measurements.
The series of free induction decay signals produced during a scan of the subject are digitized and processed by a computer to extract their various frequency components for display on a screen. The most prevalent method involves the application of a discrete Fourier transform to the digitized NMR signals. Such transform may be in one or several variables as discussed in "The Fourier Transform and Its Applications", by R. N. Bracewall, published in 1978 by McGraw-Hill. Computer programs for performing such discrete Fourier transforms are well known, as discussed in "Fourier Analysis of Time Series: An Introduction", by P. Bloomfield, published in 1976 by Wiley. Two files of digital data are produced by the Fourier transformation of the time domain NMR signals. One file represents the "real" component and the second file represents the "imaginary" component. As discussed in U.S. Pat. No. 4,070,611 it can be demonstrated that the imaginary file is not required to reproduce an accurate image of the NMR phenomena of interest, and it is common practice to ignore this data.
The use of NMR to measure the flow of fluids in vessels is well known. A paper "The NMR Blood Flowmeter-Theory and History" by J. H. Battocletti et al, published in Medical Physics, Vol. 8, No. 4, July/August, 1981, describes the theory and history of this effort. The techniques heretofore employed to measure flow require special NMR apparatus with coils arranged to magnetize a sample of the fluid "upstream" of the coils which are employed to sense the FID signal. The physical distance between this "tagging" coil and the sensing coil is known, and the level of the FID signal provides velocity information in the direction of fluid flow. In an article "NMR Rheotomography: Feasibility and Clinical Potential", by J. P. Grant et al and published in Medical Physics, Vol. 9, No. 2, March/April 1982, imaging techniques are employed to provide a flow intensity distribution in a tube. Such techniques are limited to measuring flow in a known direction, and have been limited in practice to the measurement of flow in inanimate objects or to the measurement of blood flow in the arms and legs of animals.
The present invention relates to an NMR imaging apparatus, and particularly, to a method and means for sensitizing the NMR signals to provide not only the conventional NMR image, but also to provide data from which a motion image can be constructed. In a gradient imaging NMR scanner the invention includes the application of a motion sensitizing magnetic field gradient (F) after the excitation portion of each measurement cycle and prior to the emission portion of each cycle. The resulting free induction decay signals which are produced by a series of such measurements are processed by performing an inverse Fourier transform to produce conventional image data mixed with motion image data in the real and imaginary data files. These data files may be processed to produce spin-density images modulated by conventional NMR phenomena, such as T1 and T2 relaxation, or the motion data may be processed to produce an image of the motion alone, or the data files may be processed to produce an image of conventional NMR phenomena modulated by motion.
A general object of the invention is to measure the motion of gyromagnetic material at any location within a subject. Conventional zeugmatrographic scanners may easily be modified to provide motion data along with image data. Such modifications include the application of a motion sensitizing magnetic field gradient F during the measurment cycle. The free induction decay signal FID which is produced is "linked" to a position and to the motion of the gyromagnetic material at that position. The same processing employed on the image data alone can be employed to construct a motion image.
Another object of the invention is to measure motion in any direction at any position within the subject. A conventional zeugmatographic scanner capable of exciting a gyromagnetic response from a location within the subject is used to produce a motion sensitized response. Motion sensitization is accomplished with a magnetic field gradient F of alternating polarity which is applied for a period 2T after the excitation portion of the measurement cycle is completed. The direction of the field (whose gradient is F) is the same as the polarizing field Bz, but its strength is graduated in the x, y and z directions to "tag" the flow data with a direction, as well as a magnitude and position.
Another object of the invention is to provide motion image data without significantly altering the NMR measurement cycle. The motion sensitizing field gradient F can either be added to each measurement cycle, or separate motion measurement cycles can be interlaced within standard NMR measurement cycles. In either case the numerous preparative excitation techniques and emission measurement techniques known to the art can be carried out with only minor modification. Independence of the motion measurements is maintained by providing that the integral of the field gradient F over the time period 2T is substantially zero. Although the motion sensitizing field F is thus separate and independent of the field gradient G used to position sensitize the NMR signals, the two fields may be generated using the same coils.
The foregoing and other objects and advantages of the invention will appear from the following description. In the description, reference is made to the accompanying drawings which form a part hereof, and in which there is shown by way of illustration a preferred embodiment of the invention. Such embodiment does not necessarily represent the full scope of the invention, however, and reference is made therefore to the claims herein for interpreting the scope of the invention.
FIG. 1 is a schematic elevation view of an NMR scanner which employs the present invention;
FIGS. 2A-2C are graphic illustrations of gradient magnetic fields produced in the scanner of FIG. 1;
FIGS. 3A-3C are perspective views of the gradient coils which form part of the scanner of FIG. 1;
FIG. 4 is an electrical block diagram of the control system which forms part of the scanner of FIG. 1;
FIG. 5 is a graphic illustration of a typical conventional measurement cycle performed by the scanner of FIG. 1;
FIG. 6 is a graphic illustration of a typical measurement cycle performed according to the present invention;
FIG. 7 is a graphic illustration of a portion of an alternative measurement cycle according to the present invention; and
FIGS. 8A-8C are graphic illustrations of alternative forms of the motion sensitizing field gradient F which may be employed in the measurement cycles of FIGS. 6 and 7.
Although the present invention may be easily implemented in a variety of gryromagnetic scanner .[.of.]. .Iadd.or .Iaddend.NMR spectrometer structures, the preferred embodiment of the invention employs a large electromagnet to generate the polarizing field. Referring particularly to FIG. 1, this polarizing magnet 1 is comprised of four circular cylindrical segments 2-5 of sufficient size to receive a table 6. A patient may be placed on the table 6 and any portion of his body may be scanned by suitably positioning him with respect to excitation coils 7. The polarizing magnet 1 produces a strong magnetic field Bz which is constant and homogeneous within the space defined by the excitation coils 7. The excitation coils 7 produce an excitation field B1 which is in the transverse plane, perpendicular to the polarizing field Bz. The excitation field B1 oscillates at a radio frequency W0 and it is applied as one or more pulses. The coils 7 are then switched to a passive mode in which they operate as receivers for the NMR signals produced in the patient's body.
Referring to FIGS. 3A-3C, three sets of gradient field coils are also formed around the table 6. A set of Z gradient field coils 10a and 10b produce a magnetic field (Gz ·Z) which is directed along the z axis of the machine, but which has a strength that changes as a function of position along the z axis. As shown in FIG. 2A, this field is additive to the polarizing magnetic field Bz to provide a total field B0 which varies in strength substantially linearly (i.e., Gz ·Z) as a function of Z position on the table 6.
Referring to FIGS. 2B and 3B, a second set of gradient field coils 11a-11d produce a magnetic field (Gx ·X) which is directed along the z axis of the machine, but which has a strength that changes as a function of position along the x axis. This field is additive to the polarization magnetic field Bz to provide a total field B0 which varies in strength substantially linearly as a function of x position on the table 6.
Referring to FIGS. 2C and 3C, a third set of gradient field coils 12a-12d produce a magnetic field (Gy ·Y) which is directed along the z axis of the machine, but which has a strength that changes as a function of position along the y axis. This field is additive to the polarizing magnetic field Bz to provide a total field B0 which varies in strength substantially linearly as a function of y position on the table 6.
The generation and control of the polarizing magnetic field Bz and the field gradients Gx, Gy and Gz is well known in the art and is employed in existing NMR scanners.
Referring particularly to FIG. 4, the control system for the NMR scanner includes a set of four static power converters 15-18 which connect to an a.c. power source 19. The static power converters 15-18 produce d.c. currents for the respective coils 1, 10, 11 and 12 at levels determined by commands received from a processor 20. The polarity, or direction, of the d.c. currents produced for the gradient field coils 10-12 can also be controlled. Thus, both the magnitude and the direction of the gradient fields in the x, y and z direction can be switched on command from the processor 20.
The excitation winding 7 is driven by a radio frequency oscillator 21 when an electronic switch 22 is toggled to its active position. The switch 22 is controlled by the processor 20 and when the switch 22 is toggled to its passive position, the excitation winding 7 is coupled to the input of an amplifier and phase-coherent detector circuit 23. The NMR signals in the patient induce a voltage in the excitation winding 7 which is amplified and demodulated in the circuit 23. The oscillator 21 provides a reference signal to the circuit 23 that enables one phase-coherent detector therein to produce an in-phase, or sine, free induction decay (FID) signal to an analog-to-digital converter 24. A second phase-coherent detector produces an orthogonal, or cosine, FID signal to an analog-to-digital converter 25.
The free induction decay signals produced by the phase-coherent detector 23 are digitized by the A/D converters 24 and 25. The sample rate of this digitization is controlled by the processor 20, and the digital numbers which are produced by the A/D converters 24 and 25 are input to a processor 20 and stored in a memory 26. The processor 20 also stores values indicative of the gradient field strengths at the moment the FID signals are produced, and in this manner, the FID signals are linked to a specific position within the patient.
Referring particularly to FIG. 5, a typical measurement cycle for the NMR scanner in its imaging mode is illustrated. Such measurement cycles are repeated many times during a single scan, with the strengths of the field gradients Gx, Gy and Gz being changed for each measurement to obtain the desired NMR response from a series of points in the subject. In the example cycle of FIG. 5 a first transverse excitation pulse 30 at the desired Larmour frequency is applied and the field gradients Gx, Gy and Gz are switched on at their desired levels. The length of the excitation pulse 30 is selected to provide maximum transverse magnetization (90°) of the gyromagnetic nuclei, and the resulting free induction decay signal 31 has an amplitude A0. The rate at which the FID signal 31 decays (as indicated by dashed line 31') is a measure of the frequency distributions of the gyromagnetic nuclei excited in the subject by the field gradients (Gx, Gy, Gz).
To measure the T2 relaxation time within the same measurement cycle, a second excitation pulse 32 is applied. This pulse 32 is at the same .[.Larmour.]. .Iadd.Larmor .Iaddend.frequency, but it is twice as long as the pulse 30, and phase-shifted by 90°, with the result that the transverse magnetization is rotated 180°. This "echo" pulse stimulates the free induction decay signal 33 after the field gradients Gx, Gy and Gz are again applied. The peak value of this FID signal 33 is less than the value A0 of the first FID signal 31, and as indicated by dashed line 34, it provides an indication of the T2 relaxation time.
It should be apparent to those skilled in the art that the NMR measurement cycle illustrated in FIG. 5 is but one of many possible measurements that can be performed by the scanner system of FIG. 4. With this particular cycle, a number of images can be constructed which are of medical significance. Since the measurement variables such as gradient field strengths, and excitation pulse generation are under control of the processor 20, the NMR scanner system can be programmed to carry out any number of different measurement cycles.
Referring again to FIG. 4, the digitized representations of the FID signals generated during the complete scan are stored in the memory 26 as two files S1 (t) and S2 (t). S1 (t) is that portion of the FID signal S(t) which is phase-referenced to the "cosine" phase of the transverse excitation signal produced by oscillator 21, and S2 (t) is the "sine" phase. S1 (t) and S2 (t) may be combined to form the complex signal.
S(t)=S.sub.1 (t)+iS.sub.2 (t). (1)
This may be written as the spectral transform:
and K is a constant electronic conversion factor. This signal has been spacially modulated by the field gradient (G=Gx x+Gy y+Gz z) and is equivalent to the following:
.[.S(t)=∫M.sub.1 (r)e.sup.-2πiγG·rt.sbsp.dr.]. S(.Iadd.t)=∫M.sub.1 (r)e.sup.-2πiγG·rt dr .Iaddend.(3)
M1 =transverse magnetization
r=a position (x, y, z)
This can be expressed in "q" space as:
.[.S(q)=K∫M.sub.1 (r)e.sup.-2πiq·r.sbsp.dr.]. S(.Iadd.q)=K∫M.sub.1 (r)e.sup.-2πiq·.sbsp.rdr .Iaddend.(4)
where: "q" is a position in three-dimensional space which is determined by the field gradient G, q=γGt.
Each measurement cycle thus produces a line sampling in q-space, and the data files S1 (t) and S2 (t) represent a set of such line samplings. An image Im (r) can be reconstructed from this data by performing a numerical discrete Fourier inversion to the desired geometry:
.[.I.sub.m (r)=K∫H(q)S(q)e.sup.2πiq·r.sbsp.dq.]. I.sub.m (.Iadd.r)=K∫H(r)S(q)e.sup.2π q·rdq .Iaddend.(5)
Where: H(q) is the apodizing function associated with the digitizing process.
When the Fourier inversion is performed according to equation (5) by the processor 20, two data files are created, I(r) and iJ(r), where:
I.sub.m (r)=I(r)+iJ(r). (6)
It is well known in the art that the image data in the file I(r) may be output to a display device, such as the CRT 27 in FIG. 4, to produce an image. Such an image may represent primarily the density of the excited gyromagnetic nuclei ("spin-density") or the image may be modulated by T1 or T2 factors to provide improved contrast of the anatomical or .[.psysiological.]. .Iadd.physiological .Iaddend.phenomenon. The "imaginary" data file iJ(r) returns a null-value when the system is properly tuned, and it is usually discarded in prior NMR scanner systems.
Although spin-density, T1 and T2 images provide useful information of an anatomical nature, the present invention enables a motion image to be produced. The flow of fluids in a human subject is a most important phenomena, and its measure and imaging provides diagnostic medicine with invaluable information for functional assessment and physiological status. Although the "motion-zeugmatographic" imaging method and system of the present invention may be employed to image acceleration, jerk, etc., its primary value to medicine is believed to be in the production of velocity images.
Referring particularly to FIG. 6, the present invention may be implemented as part of a conventional NMR measurement cycle. After a first free induction decay signal 40 is received and digitized in the standard manner described above, a motion sensitizing field gradient,
F=F.sub.x x+F.sub.y y+F.sub.z z
is applied to the subject. This motion sensitizing field gradient may be generated with the gradient field coils 10-12 (FIG. 3), and it is characterized by the fact that it alternates in polarity such that its integral is equal to zero over its time period 2T.
The relative values of the coordinate components Fx, Fy, Fz determine the direction in which the subsequent NMR signal 41 is motion sensitized.
The measurement cycle illustrated in FIG. 6 may be repeated many times to motion sensitize a series of NMR signals 41 in many directions. The set of motion sensitized data which results from this series of "F cycles" is stored, and the gradient fields Gx, Gy and Gz are then changed to position sensitize the next series of F cycles to a different location in the subject. The process is continued with a series of motion sensitized measurements being made at each location in the scan.
It is a requirement of the present invention that the motion sensitizing field gradient F be applied after the application of an excitation field which produces a transverse magnetic moment M1. Furthermore, motion sensitization must occur prior to the emission of the FID signal which it is to sensitize. In the example measurement cycle of FIG. 6, excitation pulse 42 produces the required transverse magnetic moment M1. The flow sensitizing field gradient F is applied after the first free induction signal 40 is produced, and hence the data which is collected from the FID 40 is not motion sensitized. The FID signal 41 on the other hand, is produced by "echo" excitation pulse 43 after the motion sensitizing field gradient F has been applied. It contains motion information. In this example the echo excitation pulse 43 does not produce any additional transverse magnetic moment M1.
Another possible measurement cycle which produces motion sensitized data is illustrated in FIG. 7. In this cycle a 90° excitation pulse 45 is applied to produce maximum transverse magnetic moment and the position gradient field G is later switched on to produce the free induction decay signal 46. At time TA during the generation of the FID 46, a motion sensitizing field gradient F is applied until time TB. The FID signal 46' (generated after TB) is motion sensitized.
The direction of the motion which is measured is determined by the direction of the field gradient F. The measurement sensitivity is determined by a number of factors, including the strength (F0) of the field gradient F and its duration (2T). If the systematic phase errors produced by the system are denoted by "e", then the minimum velocity which can reliably be measured is as follows:
V.sub.min ≃e[2πγF.sub.0 T.sup.2 ].sup.-1 (7)
where e is in radians.
For example, if the motion of hydrogen nuclei is measured with a system having a phase resolution error of .Iadd.e.Iaddend.=0.1 radian, then the following conditions are typical:
y≃=4.6×10.sup.3 H.sub.z /gauss
F.sub.0 =0.5 gauss/cm.
V.sub.min ≃0.06 cm./second.
It should be apparent that the measurement process can be shortened and simplified considerably if fluid flow in only one direction is imaged. For example, if only the motion sensitizing field gradient Fz is employed, an average velocity image of fluid flow along the z axis is generated. In such case, only one flow sensitized measurement is required at each "G" position of the scan.
The flow sensitized FID signal .[.at.]. .Iadd.is .Iaddend.both position and motion sensitized. As indicated above in equation (3), the digitized FID signal S(t) which is stored in the memory 26 is linked to position by the gradient field G. Similarly the motion sensitized FID signal S(t) is linked to the velocity of the spin-density at this same position by the motion field gradient F:
S(t)=∫∫M.sub.1 (r,v)e.sup.2π γ[G·rt+F·v(T).spsp.2.sup.] drdv (8).
If a six-dimensional discrete Fourier inversion is performed on this stored data file, an image Δ(r,v) can be constructed on the CRT 27 which displays spin-density (p0) distributed according to the proportions of that density possessing particular velocities in the direction F of the gyromagnetic nuclei at that location.
Δ(r,v)=K∫∫H(q)H(f)S(q,f)e.sup.2πi(q·r+f.multidot.v) dqdf (9)
where: H(q) and H(f) are apodizing functions associated with digitizing the FID and "f" is a position in three-dimensional Fourier-velocity space which is determined by the velocity field gradient F, where f=γF(T2).
This six-dimensional image, Δ(r,v), is the most general and ambitious direct image of true flow velocities since it enables many points in "f" space to be measured by sensitizing a series of FID signals with velocity gradients F having different directions and different magnitudes. The technique can be considerably simplified if the image is modulated by a single velocity gradient F at each point. This considerably shortens the data collection portion of the process since it requires only one F cycle for each G cycle, but it returns only the average velocity of flow rather than a complete velocity distribution scale, or profile.
There is an endless variety of modifications and simplications by which the motion-zeugmatographic phase-modulation method of the present invention can be applied to studies of practical importance. Chemical shift distributions or T1 and T2 spectroscopy may be added and similarly "interlaced" in the data-collection cycle. The B1 excitation field may be modulated to suppress or isolate contributions to the T2 -process, and as will be described in more detail below, variations in the shape of the motion sensitizing field gradient F are possible.
As indicated above (equation (5)), the Fourier inversion performed on a conventional zeugmatographic NMR scanner returns data in a "real" file I(r) from which an image of spin-density p0 (r) can be produced on the CRT 27. As indicated above by equation (9), when the Fourier inversion is performed on motion sensitized NMR data, the real file I(r) is returned with data which enables an image of spin-density p0 (r) modulated by velocity V(r) to be produced on the CRT 27.
It is another aspect of the present invention that when the Fourier inversion of flow sensitized NMR data is performed, the "imaginary" data file iJ(r) returns information from which images of particular medical value can be produced. More specifically, if the NMR data is flow sensitized in a single direction (i.e., one F cycle per G cycle), and if the magnitude (F0) and duration (2T) of the flow sensitizing field gradient field are kept small such that:
e.sup.i2πγT.spsp.2.sup.F.sbsp.0.sup.·V ≃1+i2πγT.sup.2 F.sub.0 ·V (10)
the real file I(r) returns conventional image data p0 (r). However, the imaginary file iJ(r) now returns image data:
J(r)=(2πγT.sup.2 F.sub.0)·[p.sub.0 (r)(V)](11).
The values in parentheses are known measurement conditions and p0 (r) is precisely the set of values returned in the real life I(r). Consequently, a velocity image V(r) can be produced on the CRT 27 as follows:
V(r)=J(r)/[(2πγT.sup.2 F.sub.0)I(r)] (12).
Thus in a single scan of the subject, data files S1 (t) and S2 (t) can be created and stored in the memory 26. From the files I(r) and iJ(r) which are produced by the Fourier inversion of these data files, three separate images can be produced with .[.mineral.]. .Iadd.minimal .Iaddend.computation. The first image p0 (r) is the conventional spin-density NMR image as modulated by phenomena such as T1 and T2. The second image is the same spin-density image p0 (r) modulated by the magnitude of average spin velocity V(r) in the direction selected by the flow sensitizing field gradient F. The third image is the magnitude of spin velocity V(r) in the direction of F throughout the region of the NMR scan.
It should be apparent to those skilled in the art that other images of medical value can be constructed from this measured data with further computation. For example, the exchange flow of molecules into or out of a specified volume may be calculated by integrating the velocity modulated spin-density values Δ(r,v) over the surface area of the volume. The same flow rate through a specified plane may also be calculated by integrating across the surface of the plane. Such measurements may provide, for example, the quantity of blood flowing through a specific vessel. It is important to note that because an anatomical image may be produced from the same data, the location (r) of the particular volume or surface of interest in the patient can be prescisely located by the NMR scanner operator.
While the most important application of the invention is presently believed to be the measurement of velocity, the invention may be extended to measure "higher order" motion such as acceleration. For velocity sensitization, the flow sensitizing field gradient F must not only be of alternating polarity, but its wave form should be symmetrical. That is, the velocity sensitizing field gradient F should be a mirror image about horizontal and vertical axes of symmetry. Referring to FIG. 8A, for example, the field gradient wave form 50 alternates in polarity and is anti-symmetrically mirrored about an axis of symmetry 51. Needless to say, the integral of this wave form 50 over the interval TA to TB is zero and it therefore satisfies the basic requirement for motion sensitization. In contrast, the motion sensitization gradient field F produced by the wave form 52 in FIG. 8B is symmetrically mirrored about the vertical axis 51. This wave form will sensitize the subsequent NMR signal to acceleration. Note that the integral of the wave form 52 over the time period TA to TB is zero, thus satisfying the basic motion sensitization requirement.
It should also be understood that the alternating polarity requirement for the motion sensitizing field gradient F is referenced to the gyromagnetic nuclei--not the table 6. Thus, if a 180° echo pulse of excitation energy is applied to the gyromagnetic nuclei, their phase-polarity is effectively reversed and the second half-cycle of the motion sensitizing field gradient F need not be reversed in polarity. This is illustrated in FIG. 8C, where the wave form 53 of the field F is the equivalent of the wave form 50 in FIG. 8A, when an echo pulse 54 is generated at the axis of symmetry 55. This technique may be useful with systems which do not enable the gradient fields to be reversed in polarity.
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