CA1101936A - Cardiac imaging with ct scanner - Google Patents
Cardiac imaging with ct scannerInfo
- Publication number
- CA1101936A CA1101936A CA298,633A CA298633A CA1101936A CA 1101936 A CA1101936 A CA 1101936A CA 298633 A CA298633 A CA 298633A CA 1101936 A CA1101936 A CA 1101936A
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- heart
- scanner
- cardiac
- image data
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- Prior art date
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- 230000000747 cardiac effect Effects 0.000 title claims abstract description 59
- 238000003384 imaging method Methods 0.000 title claims abstract description 13
- 230000005855 radiation Effects 0.000 claims description 21
- 238000012545 processing Methods 0.000 claims description 14
- 238000000034 method Methods 0.000 claims description 11
- 230000033001 locomotion Effects 0.000 claims description 6
- 230000002685 pulmonary effect Effects 0.000 claims description 6
- 230000001788 irregular Effects 0.000 claims description 5
- 230000002093 peripheral effect Effects 0.000 claims description 5
- 230000000903 blocking effect Effects 0.000 claims description 4
- 238000012544 monitoring process Methods 0.000 claims description 3
- 230000003111 delayed effect Effects 0.000 claims description 2
- 230000000593 degrading effect Effects 0.000 claims 1
- 238000000819 phase cycle Methods 0.000 claims 1
- 230000029058 respiratory gaseous exchange Effects 0.000 claims 1
- 230000000087 stabilizing effect Effects 0.000 claims 1
- 210000005240 left ventricle Anatomy 0.000 description 6
- 230000005540 biological transmission Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 238000012285 ultrasound imaging Methods 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 3
- 210000004369 blood Anatomy 0.000 description 3
- 239000008280 blood Substances 0.000 description 3
- 238000000718 qrs complex Methods 0.000 description 3
- 210000001519 tissue Anatomy 0.000 description 3
- 210000004556 brain Anatomy 0.000 description 2
- 238000002591 computed tomography Methods 0.000 description 2
- 230000004217 heart function Effects 0.000 description 2
- 210000004165 myocardium Anatomy 0.000 description 2
- 206010002329 Aneurysm Diseases 0.000 description 1
- OWNRRUFOJXFKCU-UHFFFAOYSA-N Bromadiolone Chemical compound C=1C=C(C=2C=CC(Br)=CC=2)C=CC=1C(O)CC(C=1C(OC2=CC=CC=C2C=1O)=O)C1=CC=CC=C1 OWNRRUFOJXFKCU-UHFFFAOYSA-N 0.000 description 1
- 206010027339 Menstruation irregular Diseases 0.000 description 1
- 208000020128 Mitral stenosis Diseases 0.000 description 1
- 210000001765 aortic valve Anatomy 0.000 description 1
- 238000009530 blood pressure measurement Methods 0.000 description 1
- 210000005242 cardiac chamber Anatomy 0.000 description 1
- 238000002592 echocardiography Methods 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 230000005251 gamma ray Effects 0.000 description 1
- 210000005003 heart tissue Anatomy 0.000 description 1
- 238000011835 investigation Methods 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 210000005246 left atrium Anatomy 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 210000004115 mitral valve Anatomy 0.000 description 1
- 208000006887 mitral valve stenosis Diseases 0.000 description 1
- 230000003387 muscular Effects 0.000 description 1
- 230000002107 myocardial effect Effects 0.000 description 1
- 230000035790 physiological processes and functions Effects 0.000 description 1
- 238000002604 ultrasonography Methods 0.000 description 1
- 230000002861 ventricular Effects 0.000 description 1
Classifications
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
- A61B6/54—Control of apparatus or devices for radiation diagnosis
- A61B6/541—Control of apparatus or devices for radiation diagnosis involving acquisition triggered by a physiological signal
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
- A61B6/02—Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
- A61B6/03—Computed tomography [CT]
- A61B6/032—Transmission computed tomography [CT]
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T11/00—2D [Two Dimensional] image generation
- G06T11/003—Reconstruction from projections, e.g. tomography
- G06T11/005—Specific pre-processing for tomographic reconstruction, e.g. calibration, source positioning, rebinning, scatter correction, retrospective gating
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2211/00—Image generation
- G06T2211/40—Computed tomography
- G06T2211/412—Dynamic
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- Engineering & Computer Science (AREA)
- Medical Informatics (AREA)
- Physics & Mathematics (AREA)
- Biomedical Technology (AREA)
- Animal Behavior & Ethology (AREA)
- Biophysics (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Optics & Photonics (AREA)
- Pathology (AREA)
- Radiology & Medical Imaging (AREA)
- Theoretical Computer Science (AREA)
- Heart & Thoracic Surgery (AREA)
- Molecular Biology (AREA)
- Surgery (AREA)
- High Energy & Nuclear Physics (AREA)
- General Health & Medical Sciences (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Pulmonology (AREA)
- Physiology (AREA)
- General Physics & Mathematics (AREA)
- Apparatus For Radiation Diagnosis (AREA)
- Ultra Sonic Daignosis Equipment (AREA)
- X-Ray Techniques (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Abstract
CARDIAC IMAGING WITH CT SCANNER
Abstract of the Disclosure The patient's ECG signal is employed in a traverse-and-rotate type CT scanner as a time base for triggering the beginning of a traverse such that the traveling beam reaches the heart at a desired phase of the cardiac cycle. For a purely-rotational-type CT scanner, continuously generated scan data is only stored for corresponding phases of successive cardiac cycles. Alternatively, gating of the beams themselves can be controlled by the ECG signal. The use of a pacemaker to stabilize the cardiac period is described along with a system for recognizing unacceptable variations in the cardiac period. In a traverse-and-rotate-type fan-beam CT scanner, the effective beam width is narrowed to hasten the traverse of the heart.
Abstract of the Disclosure The patient's ECG signal is employed in a traverse-and-rotate type CT scanner as a time base for triggering the beginning of a traverse such that the traveling beam reaches the heart at a desired phase of the cardiac cycle. For a purely-rotational-type CT scanner, continuously generated scan data is only stored for corresponding phases of successive cardiac cycles. Alternatively, gating of the beams themselves can be controlled by the ECG signal. The use of a pacemaker to stabilize the cardiac period is described along with a system for recognizing unacceptable variations in the cardiac period. In a traverse-and-rotate-type fan-beam CT scanner, the effective beam width is narrowed to hasten the traverse of the heart.
Description
3~
.. . . . . . ... . ..
Background of the Invention Computerized tomographic X-ray or gamma ray scanners (CT scanners) reconstruct an image representing a single tomo- '~
gram of the radiation absorptivity of tissues from data collected from numerous coplanar scan lines. The widest appli-cation of CT scanners thus far has been for brain studies.
Being stationary when supported in the CT scan circle, all parts of the brain generally remain in the same location during ; each of the numerous scans required for constructing~a single tomographic image. However, involuntary muscular activity makes accurate image reconstruction of other parts of the body difficult. This problem is presented with both basic types of CT scanners, namely, traverse-and-rotate type CT scanners and " :
~ ;~
3~
.
purely-rotational-type CT scanners.
Ileart structures, for example, are in constant motion. While the heart period is on the order of one second, distinct physiological phases of the cardiac cycle, for example, the periods referred to as end systole (ES) and end diastole (ED) last on the order of 1/20 and 1/5 of a second, respectively. That is, if all of the scan lines needed to reconstruct an image of the heart could be produced in less ~ -than 1/20 of a second, the motion of the heart would be effectively frozen during either of these periods. This speed, however, is difficult for conventional CT scanners which normally require from about 5 seconds to several minutes to Collect the scan data for a single image.
The objectives of cardiac imaging in general are visualizing the sizes of the cardiac chambers, estimating contractilities of the chambers, comparing chamber wall motions, locating aneurysms and areas of myocardial infraction and detecting mitral stenosis. Most of these objectives are, of course, difficult to attain using conventional exposed film X-ray techniques because the differences in absorption or density of heart tissues and blood is not sufficient to confidently distinguish these features at safe radiation dosages and because a tomogram or cross-sectional slice image is not generated.
An electrocardiogram (ECG) is produced by recording the amplitude of electrical activity associated with the heart muscle versus time. In ultrasound imaging, the ECG signal has been used before as a synchronizing device for producing a stop-action image of the heart. See, for example, U.S. Patent No. 3,954,098, issued May 4, 1976 to D. E. Dick et al. Some ultrasound imaging systems have used B
-3~;
computerized sorting and assembling multiple images per nominal heart cycle with recorded data from several heart cycles.
Ultrasound imaging differs fundamentally from X-ray imaging.
X-rays are not normally reflected detectably by tissue; that portion which is not absorbed is merely transmitted. All conventional X-ray imaging machines operate in the transmission mode. While ultrascund imaging can be carried out in the transmission mode in some instances, conventional ultrasound cardiac imaging, particularly ECG-gated imaging, is only done in the reflecting or echo mode.
Ultrasound imaging involves pinpointing each partially reflecting surface for a given pulse of sound energy by measuring the round trip transit time for reception of the echoes, just as in sonar. A
Single pulse of radiation, however, in the X-ray transmission moce results in a single datum describing the total absorption encountered over the entire path of the X-ray beam; that is, the location of structures is not identifiable from one pulse. ~
Summary of the Invention , The present invention relates to a method and radiographic apparatus for imaging a planar slice of a patient's heart. The apparatus comprises a CT scanner which has a source of radiation, scan means for scanning the beam of radiation from the source relative to the heart, data generating means for generating image data from radiation that has traversed the planar slice of the heart, processing means for processing the image data to reconstruct a tomographic image of the planar slice. The apparatus further comprises cardiac cycle monitoring means for producing a repeatirg pulse signal indicative of the same functional point in each successive cardiac cycle and control means responsive to the pulse signal for causing image data generated during the same selectable phase in successive cardiac cycles to be reconstructed. The control means includes a selectable delay means for delaying the pulse signal for a selectable duration thereby selecting the selectable phone in the cardiac cycle.
The method comprises sensing the same functional point in each su~essive cardiac cycle and producing a pulse signal, delaying the pulse signal for a selectable duration, generating and scanning at least one beam of radiation relative to the heart, generating image data indicative of the attenuation of radiation crossing through the planar slice, processing the image data to construct the tomographic image, and controlling the processing of image data with the delayed signal. In this manner the image data that is generated during the same selected plane in successive cardiac cycles is processed to construct the tomographic image of the planar slice of the heart in the selected phase. `~
Brief Description of the Drawings Fig. 1 is an ECG waveform;
Fig. 2 is a block diagram illustrating an ECG-controlled CT
scanner system according to the invention;
Fig. 3, appearing on the first sheet of drawings, is a schematic diagram indicating the CT scanner beam's traverse in relation to the patient's heart;
Fig. 4 is a schematic diagram of a traverse-and-rotate-type fan-beam CT scanner illustrating the beam pattern intersecting the patient's heart;
Fig. 5 is a schematic representation of the beam pattern of a purely-rotational-type CT scanner; and ~;
Figs. 6, 7 and 8 are detail block diagrams illustrating different systems of ECG-gating for a purely-rotational-type CT
scanner.
Description of the Preferred Embodiments The ECG waveform shown in Fig. 1 presents features designated by the letters P, Q, R, S and T. The group of features Q, R and S is referred to as the QRS complex, in which the R-feature or R-wave is the most prominent, highest amplitude feature of the entire ECG.
Moreover, the narrow pulse width of the QRS complex and in particular the R-wave, provides a digital clock pulse for timing the cardiac cycle.
The cardiac cycle is usually defined as beginning with ~ .
the R-wave and continuing until the occurrence of the next R-wave. Heart functions are characterized by two distinct periods called systole and diastole. In systole, the heart - muscle is contracting the volume of the left ventricle to pump the contents out through the aortic valve. During diastole, the left ventricle is filling through the mitral valve. At the end of systole (ES), the left ventricle has its smallest volume since it has contrac~ed to pump blood out. The end of ' diastole (ED) is the point at which the left ventricle has its largest volume since it is filled with blood ready to be pumped out. Thes~ two extremes of heart function, end of systole and end of diastole, are of interest, for example, in determining fractional ejection, i.e., the ratio of minimum-to-maximum ventricular volume. Each of these fea-tures, end of systole and end of diastole, lasts for an inter-val on the order of 1/10 second and occurs once every cardiac cycle.
Fig. 2 shows a conventional traverse-and-rotate-type CT scanner having a scan circle 12 defining a scan plane in which the patient 14 is positioned such that the scan plane preferably intersects the left ventricle, left atrium or aortic root of the heart. The mechanical operation of the traverse-and-rotate mechanism and the beam shutter is controlled by a scanner controller 16. An external pacemaker 18 may be employed to stabilize the cardiac period of a patient with irregular heart rate. The ECG signal from the patient is applied by an isolation amplifier 20 to a QRS complex detector 22 whose output is a digital timing pulse corresponding to each R-wave of the patient's live ECG signal. The items 20 and 22 are commercially available units, for example, Hewlett Packard Corporation, Model Nos. 7807C and 7330A. The output of the QRS detector 22 is fed to a delay timing circuit 24 which provides a trigger pulse to the CT scanner controller 16.
If the objective is to acquire an image of the heart at the end of diastole with the left ventricle fully expanded, the trigger pulse is timed to be applied to the scanner con-' troller 16 sufficiently in advance of the end of diastole so ; 10 that the scanner controller 16 can begin the traverse of ~he radiation beam, as shown in Fig. 3, from point xO so that by the time the beam travels distance Dl to position xl where it first begins to intersect the heart, the heart will be in the ;~ end of diastole stage. Of course, the beam must be traversing at a rate sufficient to traverse the width of the heart in thispresentation in approximately less than 1/10 of a second. Thus, the distance D2 from point xl to the point x2 would determine the minimally acceptable speed of traverse. The consequence , of traveling too slowly through the distance D2 in Fig. 3 would be a blurring of some of the moving heart structures.
The delay time pro~ided by the circuit 24 in Fig. 2 is determined ~y three parameters: (1) the speed of the traverse of the beam; (2) the position of the heart in the scan circle 12; and (3) a predication of when the particular phase of interest, for example end of diastole, will occur in the average or nominal cardiac cycle of the patient. The speed of traverse of the beam is normally a known constant value. However, the speed can be monitored during the scan to compensate in successive scans for any variations in the average scan speed.
Th ~osition of tl~e heart can be determined in two ways: the heart's position can be considered by adjusting the patient's positi~n in the scan circle or the patient can be prescanned and the location of the heart determined by the scanner operator from the reconstructed image. Prediction of the time that the heart will be in a particular phase, such as end diastole, requires a knowledge of the heart rate, as measured by the interval between R-waves, and the -average time elapsed from an R-wave up to the phase of interest~
This information is derived from the patient's electrocardiogram.
It could also be derived from a phonocardiogram or pressure measurements. The ultimate objective is to synchronize the CT
cardiac scanning with cardiac contractility. Use of the ECG signal is a means for inferring the phases of the cardiac contractility curve~ Contractility measurement devices may be employed to determine the contractile state of the heart directly and more accurately.
These parameters are taken into consideration in setting the delay implemented by the timing circuit 24. After the R-wave signal from the QRS detector 22, the delay timing circuit 4 pauses before issuing a trigger pulse for an interval of time which can be represented as follows:
Time Interval = TED - Dl/Ravg where TED is the predicted time from a given R-wave to the beginning of the end of the diastole phase; Dl is the position of the heart in terms of the distance the beam covers from the starting point xO until reaching the center wall of the heart (or some other point of interest); RaVg is the average speed of the traversing beam; and DlRaVg is the predicted elapsed time from the beginning of the traverse to the point where the center beam intersects the center of the heart.
For any patient the period of the cardiac cycle, as shown in Fig. 1, from one R-wave to the next R-wave always varies to some degree. Theitiming of the triggering of a traverse is based solely on the occurrence of the last R-wave . .
.
...
and the predicted time for beginning of the end of diastole or end of systole whichever phase is being imaged. It is entirely possible that the prediction may not be borne out.
- If the cardiac cycle, which the scanner is preparing to sample, is one of sufficiently increased or reduced period, the end of .
diastole or end of systole will occur at a significantly different time. Thus, it is advisable to place tolerance limits on the cardiac period in order to distinguish acceptable and unacceptable scan data.
The system of Fig. 2 merely illustrates one form of digital circuitry foL performing heart period dissemination.
In practice, it may be preferable to implement these functions with software using the CT scanner computer associated with image processing the machine control. The output of the QRS
detector 22 is passed to the reset input of a digital counter 26 clocked, for example, at one hundred or one thousand Hertz by a stable frequency oscillator 28. The parallel binary out-put of the counter 26 is passed via a latch circuit 30 to a subtractor circuit 32. The latch 30 operates as a digital sample-and-hold circuit which holds the count attained by the counter 26 immediately before being reset by the next R-wave.
The number contained in latch 30 is compared by the subtractor 32 to the number held in storage 34 representing the nominal period of the pàtient's cardiac cycle. The difference between the counts for the actual and nominal periods is passed to a comparator 36. A reference number indicating a tolerance limit on the difference between the actual and nominal periods is provided by the limit circuit 38. If the difference exceeds the limit provided by the circuit 38, the binary comparator output alerts the image processing unit 40 associated with the CT scanner 10 to discard the scan data corresponding to the irregular period.
The actual tolerance limits on cardiac period depend on the phase being imaged. For example, the tolerance for imaging end of diastole will be smaller than the tolerance for end of systole since the interval to end of diastole is generally regarded as proportional to the cardiac period and ;
comes at the very end of the cardiac cycle. Thus, in addition to setting the delay timing in accordance with the phase of interest, the tolerance limits for an acceptable cardiac period should also be adjusted accordingly.
Instead of employing a single beam as shown schematically in Fig. 3, several CT scanning devices currently on the market, such as the DELTA-SCAN~ model scanner marketed by Ohio-Nuclear, Inc., traverse with a fan-shaped pattern of beams as shown in Fig. 4. The fan-beam pattern covers a width Wl where it intersects the heart. The consequence of the width of the beam pattern is that it takes longer for the entire plurality of beams to traverse the heart from point x to point x2. As is the case in Fig. 4, if the width of the beam is approximately equal to D2, i.e. the width of the heart in the plane in the scan direction, the time relative to a narrow beam scan will be doubled for a full heart traverse of all of the beams in the fan pattern. To alleviate this problem, the effective beam width can be narrowed, for example to W2, by ignoring or "throwing out" data from several of the peripheral detectors. For example, the data from the two outermost detectors on either side can be ignored.
Alternatively, a shutter can be employed as shown in Fig. q to ,~
.
block certain peripheral rays thus narrowing the actual pattern. The effect of either of these remedies is to narrow the fan-beam width at the heart so that the distance D2 can be traversed more quickly. The faster the interval D2 is traversed, the less motion will be present to cause blurring in the image. Thus, the precision of the stop-action effect can be increased by omitting data from peripheral beams to achieve a shorter effective time window. Blocking the beams instead of ignoring the data from the detectors has the advantage of eliminating unnecessary X-ray dosage. However, removing several of the beams will cause a slight increase in the overall scan time for completing the image.
Cardiac imaging can also be accomplished with a purely rotatiOnal CT scanner as shown in Fig. 5 wherein ~ is the rotational axis. In this case, however, since rotation of the course and detectors is continuous, instead of triggering the mechanical traverse at the right point so that data is acquired in the phase of interest, scan data is generated continuously.
The patient's ECG signal can be used as in Fig. 6 to gate the storage of data by the image processing unit 40. The delay timing circuit is thus used to open a time window during the appropriate phase in each cardiac cycle in which data is collected. Several phases can be gated with the ECG signal or even a full set of images covering every distinct physiological point in the cardiac cycle can be generated. These images can be sequenced then to produce a movie or cine presentation of the subject's heart. This alternate also includes the possibility of a semi-circle of stationary detectors and a rotating source or stationary source(s) and rotating detectors.
In order to minimize X-ray dosage to the patient, the X-ray tube could be gated on and off as indicated by the gating of X-ray power supply 42 in Fig. 7, or dynamically shuttered as indicated in Fig. 8 by the gating of beam shutter control 44, which would open the shutter blocking the beams only during the physiological phase of interest during each cardiac cycle.
In addition to cardiac gating, chest motion from `breathing can be removed from the image by using pulmonary gating. Scan data would only be stored at times when the J phase of the cardiac cycle under investigation coincided with a particular phase of the pulmonary cycle.
The above-described embodiments are intended to be illustrative, not restrictive. For example, the use of the interval end of diastole or end of systole is intended to be illustrative of the use of any interval of interest. More-over, the same techniques disclosed herein may be applicable to other physiological functions besides the heart. The invention is applicable, of course, to any type of beam trans-mission sub;ect to differential tissue absorption such as X-rays, ~ rays, etc. The scope of the invention, however, is defined by the appended claims and all variations which fall within the range of equivalents thereto are intended to be embraced therein.
.. . . . . . ... . ..
Background of the Invention Computerized tomographic X-ray or gamma ray scanners (CT scanners) reconstruct an image representing a single tomo- '~
gram of the radiation absorptivity of tissues from data collected from numerous coplanar scan lines. The widest appli-cation of CT scanners thus far has been for brain studies.
Being stationary when supported in the CT scan circle, all parts of the brain generally remain in the same location during ; each of the numerous scans required for constructing~a single tomographic image. However, involuntary muscular activity makes accurate image reconstruction of other parts of the body difficult. This problem is presented with both basic types of CT scanners, namely, traverse-and-rotate type CT scanners and " :
~ ;~
3~
.
purely-rotational-type CT scanners.
Ileart structures, for example, are in constant motion. While the heart period is on the order of one second, distinct physiological phases of the cardiac cycle, for example, the periods referred to as end systole (ES) and end diastole (ED) last on the order of 1/20 and 1/5 of a second, respectively. That is, if all of the scan lines needed to reconstruct an image of the heart could be produced in less ~ -than 1/20 of a second, the motion of the heart would be effectively frozen during either of these periods. This speed, however, is difficult for conventional CT scanners which normally require from about 5 seconds to several minutes to Collect the scan data for a single image.
The objectives of cardiac imaging in general are visualizing the sizes of the cardiac chambers, estimating contractilities of the chambers, comparing chamber wall motions, locating aneurysms and areas of myocardial infraction and detecting mitral stenosis. Most of these objectives are, of course, difficult to attain using conventional exposed film X-ray techniques because the differences in absorption or density of heart tissues and blood is not sufficient to confidently distinguish these features at safe radiation dosages and because a tomogram or cross-sectional slice image is not generated.
An electrocardiogram (ECG) is produced by recording the amplitude of electrical activity associated with the heart muscle versus time. In ultrasound imaging, the ECG signal has been used before as a synchronizing device for producing a stop-action image of the heart. See, for example, U.S. Patent No. 3,954,098, issued May 4, 1976 to D. E. Dick et al. Some ultrasound imaging systems have used B
-3~;
computerized sorting and assembling multiple images per nominal heart cycle with recorded data from several heart cycles.
Ultrasound imaging differs fundamentally from X-ray imaging.
X-rays are not normally reflected detectably by tissue; that portion which is not absorbed is merely transmitted. All conventional X-ray imaging machines operate in the transmission mode. While ultrascund imaging can be carried out in the transmission mode in some instances, conventional ultrasound cardiac imaging, particularly ECG-gated imaging, is only done in the reflecting or echo mode.
Ultrasound imaging involves pinpointing each partially reflecting surface for a given pulse of sound energy by measuring the round trip transit time for reception of the echoes, just as in sonar. A
Single pulse of radiation, however, in the X-ray transmission moce results in a single datum describing the total absorption encountered over the entire path of the X-ray beam; that is, the location of structures is not identifiable from one pulse. ~
Summary of the Invention , The present invention relates to a method and radiographic apparatus for imaging a planar slice of a patient's heart. The apparatus comprises a CT scanner which has a source of radiation, scan means for scanning the beam of radiation from the source relative to the heart, data generating means for generating image data from radiation that has traversed the planar slice of the heart, processing means for processing the image data to reconstruct a tomographic image of the planar slice. The apparatus further comprises cardiac cycle monitoring means for producing a repeatirg pulse signal indicative of the same functional point in each successive cardiac cycle and control means responsive to the pulse signal for causing image data generated during the same selectable phase in successive cardiac cycles to be reconstructed. The control means includes a selectable delay means for delaying the pulse signal for a selectable duration thereby selecting the selectable phone in the cardiac cycle.
The method comprises sensing the same functional point in each su~essive cardiac cycle and producing a pulse signal, delaying the pulse signal for a selectable duration, generating and scanning at least one beam of radiation relative to the heart, generating image data indicative of the attenuation of radiation crossing through the planar slice, processing the image data to construct the tomographic image, and controlling the processing of image data with the delayed signal. In this manner the image data that is generated during the same selected plane in successive cardiac cycles is processed to construct the tomographic image of the planar slice of the heart in the selected phase. `~
Brief Description of the Drawings Fig. 1 is an ECG waveform;
Fig. 2 is a block diagram illustrating an ECG-controlled CT
scanner system according to the invention;
Fig. 3, appearing on the first sheet of drawings, is a schematic diagram indicating the CT scanner beam's traverse in relation to the patient's heart;
Fig. 4 is a schematic diagram of a traverse-and-rotate-type fan-beam CT scanner illustrating the beam pattern intersecting the patient's heart;
Fig. 5 is a schematic representation of the beam pattern of a purely-rotational-type CT scanner; and ~;
Figs. 6, 7 and 8 are detail block diagrams illustrating different systems of ECG-gating for a purely-rotational-type CT
scanner.
Description of the Preferred Embodiments The ECG waveform shown in Fig. 1 presents features designated by the letters P, Q, R, S and T. The group of features Q, R and S is referred to as the QRS complex, in which the R-feature or R-wave is the most prominent, highest amplitude feature of the entire ECG.
Moreover, the narrow pulse width of the QRS complex and in particular the R-wave, provides a digital clock pulse for timing the cardiac cycle.
The cardiac cycle is usually defined as beginning with ~ .
the R-wave and continuing until the occurrence of the next R-wave. Heart functions are characterized by two distinct periods called systole and diastole. In systole, the heart - muscle is contracting the volume of the left ventricle to pump the contents out through the aortic valve. During diastole, the left ventricle is filling through the mitral valve. At the end of systole (ES), the left ventricle has its smallest volume since it has contrac~ed to pump blood out. The end of ' diastole (ED) is the point at which the left ventricle has its largest volume since it is filled with blood ready to be pumped out. Thes~ two extremes of heart function, end of systole and end of diastole, are of interest, for example, in determining fractional ejection, i.e., the ratio of minimum-to-maximum ventricular volume. Each of these fea-tures, end of systole and end of diastole, lasts for an inter-val on the order of 1/10 second and occurs once every cardiac cycle.
Fig. 2 shows a conventional traverse-and-rotate-type CT scanner having a scan circle 12 defining a scan plane in which the patient 14 is positioned such that the scan plane preferably intersects the left ventricle, left atrium or aortic root of the heart. The mechanical operation of the traverse-and-rotate mechanism and the beam shutter is controlled by a scanner controller 16. An external pacemaker 18 may be employed to stabilize the cardiac period of a patient with irregular heart rate. The ECG signal from the patient is applied by an isolation amplifier 20 to a QRS complex detector 22 whose output is a digital timing pulse corresponding to each R-wave of the patient's live ECG signal. The items 20 and 22 are commercially available units, for example, Hewlett Packard Corporation, Model Nos. 7807C and 7330A. The output of the QRS detector 22 is fed to a delay timing circuit 24 which provides a trigger pulse to the CT scanner controller 16.
If the objective is to acquire an image of the heart at the end of diastole with the left ventricle fully expanded, the trigger pulse is timed to be applied to the scanner con-' troller 16 sufficiently in advance of the end of diastole so ; 10 that the scanner controller 16 can begin the traverse of ~he radiation beam, as shown in Fig. 3, from point xO so that by the time the beam travels distance Dl to position xl where it first begins to intersect the heart, the heart will be in the ;~ end of diastole stage. Of course, the beam must be traversing at a rate sufficient to traverse the width of the heart in thispresentation in approximately less than 1/10 of a second. Thus, the distance D2 from point xl to the point x2 would determine the minimally acceptable speed of traverse. The consequence , of traveling too slowly through the distance D2 in Fig. 3 would be a blurring of some of the moving heart structures.
The delay time pro~ided by the circuit 24 in Fig. 2 is determined ~y three parameters: (1) the speed of the traverse of the beam; (2) the position of the heart in the scan circle 12; and (3) a predication of when the particular phase of interest, for example end of diastole, will occur in the average or nominal cardiac cycle of the patient. The speed of traverse of the beam is normally a known constant value. However, the speed can be monitored during the scan to compensate in successive scans for any variations in the average scan speed.
Th ~osition of tl~e heart can be determined in two ways: the heart's position can be considered by adjusting the patient's positi~n in the scan circle or the patient can be prescanned and the location of the heart determined by the scanner operator from the reconstructed image. Prediction of the time that the heart will be in a particular phase, such as end diastole, requires a knowledge of the heart rate, as measured by the interval between R-waves, and the -average time elapsed from an R-wave up to the phase of interest~
This information is derived from the patient's electrocardiogram.
It could also be derived from a phonocardiogram or pressure measurements. The ultimate objective is to synchronize the CT
cardiac scanning with cardiac contractility. Use of the ECG signal is a means for inferring the phases of the cardiac contractility curve~ Contractility measurement devices may be employed to determine the contractile state of the heart directly and more accurately.
These parameters are taken into consideration in setting the delay implemented by the timing circuit 24. After the R-wave signal from the QRS detector 22, the delay timing circuit 4 pauses before issuing a trigger pulse for an interval of time which can be represented as follows:
Time Interval = TED - Dl/Ravg where TED is the predicted time from a given R-wave to the beginning of the end of the diastole phase; Dl is the position of the heart in terms of the distance the beam covers from the starting point xO until reaching the center wall of the heart (or some other point of interest); RaVg is the average speed of the traversing beam; and DlRaVg is the predicted elapsed time from the beginning of the traverse to the point where the center beam intersects the center of the heart.
For any patient the period of the cardiac cycle, as shown in Fig. 1, from one R-wave to the next R-wave always varies to some degree. Theitiming of the triggering of a traverse is based solely on the occurrence of the last R-wave . .
.
...
and the predicted time for beginning of the end of diastole or end of systole whichever phase is being imaged. It is entirely possible that the prediction may not be borne out.
- If the cardiac cycle, which the scanner is preparing to sample, is one of sufficiently increased or reduced period, the end of .
diastole or end of systole will occur at a significantly different time. Thus, it is advisable to place tolerance limits on the cardiac period in order to distinguish acceptable and unacceptable scan data.
The system of Fig. 2 merely illustrates one form of digital circuitry foL performing heart period dissemination.
In practice, it may be preferable to implement these functions with software using the CT scanner computer associated with image processing the machine control. The output of the QRS
detector 22 is passed to the reset input of a digital counter 26 clocked, for example, at one hundred or one thousand Hertz by a stable frequency oscillator 28. The parallel binary out-put of the counter 26 is passed via a latch circuit 30 to a subtractor circuit 32. The latch 30 operates as a digital sample-and-hold circuit which holds the count attained by the counter 26 immediately before being reset by the next R-wave.
The number contained in latch 30 is compared by the subtractor 32 to the number held in storage 34 representing the nominal period of the pàtient's cardiac cycle. The difference between the counts for the actual and nominal periods is passed to a comparator 36. A reference number indicating a tolerance limit on the difference between the actual and nominal periods is provided by the limit circuit 38. If the difference exceeds the limit provided by the circuit 38, the binary comparator output alerts the image processing unit 40 associated with the CT scanner 10 to discard the scan data corresponding to the irregular period.
The actual tolerance limits on cardiac period depend on the phase being imaged. For example, the tolerance for imaging end of diastole will be smaller than the tolerance for end of systole since the interval to end of diastole is generally regarded as proportional to the cardiac period and ;
comes at the very end of the cardiac cycle. Thus, in addition to setting the delay timing in accordance with the phase of interest, the tolerance limits for an acceptable cardiac period should also be adjusted accordingly.
Instead of employing a single beam as shown schematically in Fig. 3, several CT scanning devices currently on the market, such as the DELTA-SCAN~ model scanner marketed by Ohio-Nuclear, Inc., traverse with a fan-shaped pattern of beams as shown in Fig. 4. The fan-beam pattern covers a width Wl where it intersects the heart. The consequence of the width of the beam pattern is that it takes longer for the entire plurality of beams to traverse the heart from point x to point x2. As is the case in Fig. 4, if the width of the beam is approximately equal to D2, i.e. the width of the heart in the plane in the scan direction, the time relative to a narrow beam scan will be doubled for a full heart traverse of all of the beams in the fan pattern. To alleviate this problem, the effective beam width can be narrowed, for example to W2, by ignoring or "throwing out" data from several of the peripheral detectors. For example, the data from the two outermost detectors on either side can be ignored.
Alternatively, a shutter can be employed as shown in Fig. q to ,~
.
block certain peripheral rays thus narrowing the actual pattern. The effect of either of these remedies is to narrow the fan-beam width at the heart so that the distance D2 can be traversed more quickly. The faster the interval D2 is traversed, the less motion will be present to cause blurring in the image. Thus, the precision of the stop-action effect can be increased by omitting data from peripheral beams to achieve a shorter effective time window. Blocking the beams instead of ignoring the data from the detectors has the advantage of eliminating unnecessary X-ray dosage. However, removing several of the beams will cause a slight increase in the overall scan time for completing the image.
Cardiac imaging can also be accomplished with a purely rotatiOnal CT scanner as shown in Fig. 5 wherein ~ is the rotational axis. In this case, however, since rotation of the course and detectors is continuous, instead of triggering the mechanical traverse at the right point so that data is acquired in the phase of interest, scan data is generated continuously.
The patient's ECG signal can be used as in Fig. 6 to gate the storage of data by the image processing unit 40. The delay timing circuit is thus used to open a time window during the appropriate phase in each cardiac cycle in which data is collected. Several phases can be gated with the ECG signal or even a full set of images covering every distinct physiological point in the cardiac cycle can be generated. These images can be sequenced then to produce a movie or cine presentation of the subject's heart. This alternate also includes the possibility of a semi-circle of stationary detectors and a rotating source or stationary source(s) and rotating detectors.
In order to minimize X-ray dosage to the patient, the X-ray tube could be gated on and off as indicated by the gating of X-ray power supply 42 in Fig. 7, or dynamically shuttered as indicated in Fig. 8 by the gating of beam shutter control 44, which would open the shutter blocking the beams only during the physiological phase of interest during each cardiac cycle.
In addition to cardiac gating, chest motion from `breathing can be removed from the image by using pulmonary gating. Scan data would only be stored at times when the J phase of the cardiac cycle under investigation coincided with a particular phase of the pulmonary cycle.
The above-described embodiments are intended to be illustrative, not restrictive. For example, the use of the interval end of diastole or end of systole is intended to be illustrative of the use of any interval of interest. More-over, the same techniques disclosed herein may be applicable to other physiological functions besides the heart. The invention is applicable, of course, to any type of beam trans-mission sub;ect to differential tissue absorption such as X-rays, ~ rays, etc. The scope of the invention, however, is defined by the appended claims and all variations which fall within the range of equivalents thereto are intended to be embraced therein.
Claims (15)
1. A radiographic apparatus for imaging a planar slice of a patient's heart, the apparatus comprising:
a CT scanner comprising a source of at least one beam of radiation, scan means for scanning the beam of radiation relative to the heart substantially in the plane of the slice, data generating means for generating image data from detected radiation which has crossed through the planar slice of the heart, means for processing the image data from the data generating means to reconstruct a tomographic image of the planar slice;
cardiac cycle monitoring means for producing a repeating pulse signal indicative of the same functional point in each successive cardiac cycle of the patient; and control means responsive to said pulse signal for causing said processing means to process image data generated during the same selectable phase in successive cardiac cycles, said control means including selectable delay means for delaying said pulse signal for a selectable duration thereby selecting said selectable phase in the cardiac cycle.
a CT scanner comprising a source of at least one beam of radiation, scan means for scanning the beam of radiation relative to the heart substantially in the plane of the slice, data generating means for generating image data from detected radiation which has crossed through the planar slice of the heart, means for processing the image data from the data generating means to reconstruct a tomographic image of the planar slice;
cardiac cycle monitoring means for producing a repeating pulse signal indicative of the same functional point in each successive cardiac cycle of the patient; and control means responsive to said pulse signal for causing said processing means to process image data generated during the same selectable phase in successive cardiac cycles, said control means including selectable delay means for delaying said pulse signal for a selectable duration thereby selecting said selectable phase in the cardiac cycle.
2. The apparatus as set forth in claim 1 wherein said CT scanner comprises a traverse-and-rotate-type CT scanner system, wherein said scan means comprises means for laterally traversing the beam of radiation and means for rotating the beam of radiation, and wherein said control means further comprises means responsive to said pulse signal for generating a trigger pulse to initiate a lateral traverse such that the traveling beam will reach the heart substantially coincidental with said selected phase in the cardiac cycle.
3. The apparatus as set forth in claim 2 wherein said source of radiation generates a plurality of coplanar beams of radiation in a fan-shaped pattern, and wherein said traverse-and-rotate-type CT scanner further comprises means for omitting image data associated with at least one peripheral beam in said fan-shaped pattern in order to narrow the effective width of said pattern of beams.
4. The apparatus as set forth in claim 3, wherein said omitting means includes means for blocking at least one of said peripheral beams.
5. The apparatus as set forth in claim 1, further comprising irregular cardiac cycle sensing means comprising discriminator means responsive to said pulse signal for producing an output signal to command said processing means to discard image data when the corresponding cardiac period varies from the patient's nominal cardiac period beyond predetermined limits whereby data from irregular cardiac cycles is prevented from degrading the tomographic image.
6. The apparatus as set forth in claim 5 wherein said discriminating means further comprises means for adjusting said limits according to the selected phase in the cardiac cycle.
7. The apparatus as set forth in claim 1, further comprising external pacemaker means for stabilizing the patient's cardiac period.
8. The apparatus as set forth in claim 1, further comprising means for producing a pulmonary pulse signal indicative of the same functional point in each successive pulmonary cycle of the patient, said control means further being responsive to said pulmonary pulse signal for causing said processing means to process image data in a selected phase in corresponding cardiac cycles coinciding with a particular phase of the pulmonary cycle in order to eliminate errors from chest motion due to breathing.
9. The apparatus a set forth in claim 1, wherein said CT scanner is a purely-rotational-type CT scanner wherein said scan means rotates the beam of radiation relative to the heart, and wherein said control means further includes:
means responsive to said pulse signal for generating a gate signal having timing and duration corresponding to said selected phase cycle; and means responsive to said gate signal for enabling the processing means to process image data generated during said gate signal.
means responsive to said pulse signal for generating a gate signal having timing and duration corresponding to said selected phase cycle; and means responsive to said gate signal for enabling the processing means to process image data generated during said gate signal.
10. The apparatus as set forth in claim 1, wherein said CT scanner is a purely-rotational-type CT scanner wherein said scan means rotates the beam of radiation relative to the heart and wherein said control means further comprises means responsive to said pulse signal for generating a gate signal having timing and duration corresponding to said selected phase; and wherein said CT scanner further comprises:
means responsive to said gate signal for gating the beam on and off synchronously with said selected phase.
means responsive to said gate signal for gating the beam on and off synchronously with said selected phase.
11. The apparatus a set forth in claim 10, wherein said means for gating the beam includes controllable shutter means for blocking the beam.
12. The method of producing at least one tomographic image of at least one generally planar slice of a patient's heart in a selectable phase of the cardiac cycle with a CT
scanner comprising:
sensing the same functional point in each successive cardiac cycle of the patient and producing a pulse signal indicative of said same functional point;
delaying said pulse signal for a selectable duration for selecting the phase of the cardiac cycle to be imaged;
generating at least one beam of radiation;
scanning said beam relative to the patient's heart;
generating image data indicative of the attenuation of radiation crossing through the planar slice;
processing the image data to construct the tomographic image; and controlling the processing of image data with said delayed signal, whereby the image data generated during said same selected phase in successive cardiac cycles is processed to construct the tomograpic image of the planar slice of the heart in the selected phase.
scanner comprising:
sensing the same functional point in each successive cardiac cycle of the patient and producing a pulse signal indicative of said same functional point;
delaying said pulse signal for a selectable duration for selecting the phase of the cardiac cycle to be imaged;
generating at least one beam of radiation;
scanning said beam relative to the patient's heart;
generating image data indicative of the attenuation of radiation crossing through the planar slice;
processing the image data to construct the tomographic image; and controlling the processing of image data with said delayed signal, whereby the image data generated during said same selected phase in successive cardiac cycles is processed to construct the tomograpic image of the planar slice of the heart in the selected phase.
13. The method of cardiac imaging as set forth in claim 12 wherein said scanning step includes:
laterally traversing said beam relative to the heart, commencing said lateral traversing at said same functional point in each successive cardiac cycle whereby the traversing beam reaches the heart at the time of said selected phase in each cardiac cycle; and rotating said beam after each lateral traverse.
laterally traversing said beam relative to the heart, commencing said lateral traversing at said same functional point in each successive cardiac cycle whereby the traversing beam reaches the heart at the time of said selected phase in each cardiac cycle; and rotating said beam after each lateral traverse.
14. The method as set forth in claim 12 further including monitoring the heart for irregular cardiac cycles comprising the further steps of:
determining whether the period between successive pulse signals varies from the period of the patient's normal cardiac cycle beyond predetermined limits;
when said period between successive pulse signals varies from the normal period beyond the predetermined limits, discarding the image data generated during the irregular cardiac cycle.
determining whether the period between successive pulse signals varies from the period of the patient's normal cardiac cycle beyond predetermined limits;
when said period between successive pulse signals varies from the normal period beyond the predetermined limits, discarding the image data generated during the irregular cardiac cycle.
15. The method as set forth in claim 12 wherein the scanning step further includes continuously scanning said beam of radiation along a generally circular arc and wherein said image data generating step further includes generating image data generally continuously and wherein said controlling step further includes gating said image data with said delay signal.
Applications Claiming Priority (2)
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US78371777A | 1977-04-01 | 1977-04-01 | |
US783,717 | 1977-04-01 |
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CA298,633A Expired CA1101936A (en) | 1977-04-01 | 1978-03-10 | Cardiac imaging with ct scanner |
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AU (1) | AU512924B2 (en) |
CA (1) | CA1101936A (en) |
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FR (1) | FR2385375A1 (en) |
GB (1) | GB1576588A (en) |
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US4245646A (en) * | 1978-06-19 | 1981-01-20 | Picker Corporation | Nuclear cardiology apparatus and method |
FR2461485A1 (en) * | 1979-07-17 | 1981-02-06 | Radiologie Cie Gle | NOVEL METHOD OF USING AN X-RAY TOMODENSITOMETER FOR REALIZING CINENSENSORRAPHY, AND A TOMODENSITOMETER THUS USED |
DE2939975A1 (en) * | 1979-10-02 | 1981-04-16 | Siemens AG, 1000 Berlin und 8000 München | X-RAY LAYER FOR THE PRODUCTION OF TRANSVERSAL LAYER IMAGES |
JPS5917334A (en) * | 1982-07-21 | 1984-01-28 | 株式会社東芝 | Cardiac pulse cooperated radiation ct apparatus |
JPS6050900A (en) * | 1983-08-30 | 1985-03-20 | Toshiba Corp | X-ray diagnostic apparatus |
DE19622075C2 (en) * | 1996-05-31 | 1999-10-14 | Siemens Ag | Method and device for radiological examination of a patient's heart phases |
US6275560B1 (en) * | 1998-12-22 | 2001-08-14 | General Electric Company | Cardiac gated computed tomography system |
US6470208B1 (en) * | 1999-11-19 | 2002-10-22 | Ge Medical Systems Global Technology Company, Llc | Method and apparatus for controlling x-ray exposure during gated cardiac scanning |
US6510337B1 (en) * | 1999-11-26 | 2003-01-21 | Koninklijke Philips Electronics, N.V. | Multi-phase cardiac imager |
US6393091B1 (en) * | 1999-12-13 | 2002-05-21 | General Electric Company | Methods and apparatus for non-uniform temporal cardiac imaging |
AU2003281183A1 (en) * | 2002-07-12 | 2004-02-02 | Nihon University School Juridical Person | X-ray computed tomograph and its projection data collecting method |
EP1614070B1 (en) * | 2003-01-21 | 2006-12-06 | ELEKTA AB (publ.) | Imaging internal structures |
GB2397738B (en) * | 2003-01-21 | 2007-08-29 | Elekta Ab | Computed tomography scanning |
DE102005005916A1 (en) | 2005-02-09 | 2006-08-17 | Siemens Ag | Method and tomography apparatus for generating tomographic images of a beating heart |
DE102005012386B4 (en) * | 2005-03-17 | 2010-01-28 | Siemens Ag | A method of predicting the location of the diastolic resting phase in the cardiac cycle and using the method of displaying the coronary arteries |
JP2006340838A (en) * | 2005-06-08 | 2006-12-21 | Ge Medical Systems Global Technology Co Llc | Radiographing control method and x-ray ct apparatus |
DE102011076882B4 (en) * | 2011-06-01 | 2018-12-20 | Siemens Healthcare Gmbh | Method for controlling a medical device, device with a medical device and data carrier |
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FR2041477A5 (en) * | 1969-04-25 | 1971-01-29 | Thomson Medical Telco | |
GB1475308A (en) * | 1973-07-21 | 1977-06-01 | Emi Ltd | Radiography |
FR2403059A1 (en) * | 1976-05-18 | 1979-04-13 | Emi Ltd | Radiographic appts. avoiding image distortion from organ movements - detects heart beats so that scanning of radiation source and detector can be synchronised with them (NL 22.11.77) |
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- 1978-03-15 GB GB10298/78A patent/GB1576588A/en not_active Expired
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- 1978-03-31 FR FR7809624A patent/FR2385375A1/en active Granted
- 1978-03-31 DE DE19782813830 patent/DE2813830A1/en not_active Withdrawn
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FR2385375A1 (en) | 1978-10-27 |
GB1576588A (en) | 1980-10-08 |
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DE2813830A1 (en) | 1978-10-19 |
JPS53123693A (en) | 1978-10-28 |
AU512924B2 (en) | 1980-11-06 |
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