Sweep control circuit for a diagnostic imaging system

Abstract: A patient (12) is irradiated with x-rays (10) from an x-ray tube (A) . X-rays that have passed through a region of interest of the patient are converted to a light image by a phosphor screen (14) on the dome shaped input face (16) of an image intensifier (B) . The dome shaped input face causes the output optical image (20) of the image intensifier to be distorted with pin cushion distortion. The sweep pattern of the electron beam of a video pick up tube (24) of a video camera (C) is controlled by deflection plates (26a, 26b, 26c, 26d). A sweep control circuit (D) alters the sweep pattern such that image signals from the video camera are distorted so as to cancel the image intensifier tube distortion, so that a man-readable image (28) displayed on a video monitor (22) is substantially distortion-free. The sweep control circuit alters conventional vertical sweep control voltage ramps (V) and horizontal control voltage ramps (H) by adding third order, parabolic terms.

Description: This invention relates to image intensifiers. It finds particular application in conjunction with x-ray images that are monitored by a video camera and will be described with particular reference thereto. It is to be appreciated, however, that the invention may find utility in other applications. Traditionally, x-rays were projected through a patient onto a flat sheet of photographic film to produce film images. Now, the film is frequently replaced with an image intensifier and video camera to produce a video image. When the x-ray beam is projected on an image intensifier, rather thana flat sheet of film, there tends to be image distortion at the corners. More specifically, image intensifiers include a vacuum tube which has a spherical arc segment or dome on the receiving face. The dome deviates from the traditional film plane and presents a more glancing angle to the x-rays with increase in radial distance from the center of the dome. This produces "pin cushion" distortion in which the resultant image looks as if it were on a rubber sheet that was stretched outward at the corners. The image on the domed input face of the image intensifier is converted to a smaller higher intensity image which, of course, retains the pin cushion distortion. This distorted image is viewed by a video camera. A video signal from the video camera is conveyed to a video monitor on which a man-readable distorted image is displayed. Most commonly, video cameras include a magnetic sweep pattern control in order to maintain the accuracy of the high speed sweep pattern of a video tube. Although video cameras with electrostatic sweep controls are utilized for some applications, they have generally been considered undesirable for medical diagnostic imaging. First, controlling the ramp functions of the high voltages on the electrostatic plates required relatively slow, high voltage power transistors. The slow speed of the power transistors limits control of the video camera sweep pattern. Further, high capacitances involved in the sweep plates and the switching transistors limit the frequency response or switching timers still further. Finally, the capacitance of the plates tends to be so large that the initial charging time at the beginning of each sweep produced a noticeable degradation of the sweep pattern. In early image intensifiers, which were only about 15-20 cm across, this pin cushion distortion was not very pronounced. Although accurate measurements could not be scaled off the image, radiologists found it acceptable for diagnostic purposes. As technology has progressed, the size of image intensifiers has also increased such that today image itensifiers up to about 40 cm in diameter are available. The larger the diameter of the image intensifier, the larger the dome and the more pronounced the pin cushion distortion becomes around the edges of the picture. Another drawback of the prior art image intensifiers is that the intensity of the distorted image decreases with radial distance from the center. Thus, edge portions of the image are not only distorted but also of lower intensity. Another drawback of the prior art image intensifier and video camera systems is that a mechanical adjustment procedure is necessary in order to square the resultant image within the video monitor. That is, the orientation of the video monitor image is determined by the angular orientation of the video camera relative to the image intensifier. The video camera had to be physically moved relative to the image intensifier in order to eliminate an undesirable tilt or canting of the resultant video image relative to the video monitor. DE-A-3419043 discloses an imaging system that compensates for image distortion caused by an x-ray intensifier using a sweep control circuit generating appropriate deflection signals. DE-A-3419043 shows an x-ray source, an image intensifier having a domed input end, a video camera with a pick-up tube and deflection coils, means for generating horizontal and vertical sawtooth deflection currents, circuitry for adding correction signals to the deflection signals, and a display device. The device corrects distortion by storing correction signals in a memory and, upon display of the image, reading out these signals using the timing of counters, converting the correction signals from digital to analog and adding the correction signals to the signals from the sawtooth wave generators. The present invention provides a new and improved image intensifier system which substantially eliminates pin cushion distortion. According to the invention there is provided an x-ray diagnostic imaging system comprising: an x-ray source (A) for radiating a region of interest with penetrating radiation; a phosphor screen for converting penetrating radiation that has passed through the region of interest into an optical image, an image intensifier (B) having a domed input end operatively connected with the phosphor screen for intensifying the image to produce an intensified image, which intensified image is optically distorted by the image intensifier domed input end, a video camera (C) which has a pick up tube that sweeps an electron beam across a received image, the video camera (C) being connected with the image intensifier (B) such that the pick up tube receives the distorted intensifier output image and converts it to an image representation, means for generating vertical V and horizontal H sweep control ramp signals, means for generating a third order parabolic correction in said V and H signal, said third degree parabolic correction in said V and H signals being made by (a) combining the V and H signals to produce V and H dependant correction signal and (b) combining a function of the V and H dependant correction signal use in each of the V signal and the H signal, the third order corrected vertical and horizontal sweep control signals being connected with the video camera to control the electron beam sweep pattern; a video monitor which converts the electronic image representation from the video camera into a man-readable image and means for adjusting the third order correction in said V and H signals to enable the operator to adjust the degree of curvature of the parabolas in real time while the system is in operation. One advantage of the present invention is that it corrects for image intensifier distortion. Another advantage of the present invention is that it accurately and precisely controls the sweep pattern of electrostatic video cameras. Another advantage of the present invention is that the distortion corrected image can be rotated electronically without reintroducing distortion. Yet another advantage of the present invention is that it corrects for intensity inconsistency in the output of image intensifiers. Still further advantages of the present invention will become apparent to those of ordinary skill in the art upon reading and understanding the following detailed description. One method and apparatus in accordance with the invention will now be described by way of example with reference to the accompanying drawings in which:- Figure 1 is a diagrammatic illustration of an x-ray diagnostic system, image intensifier, electrostatic video camera, and sweep control circuit in accordance with the present invention; Figure 2 is an illustration to assist in visualising derivation of the distortion correction algorithm; Figure 3 is an illustration to assist in visualising the application of the distortion correction algorithm. A source of penetrating radiation A , such as an x-ray tube directs a swatch of radiation 10 through a region of interest of a subject 12 . The intensity of radiation that traverses the region of interest varies as a shadowgraphic projection of the x-ray absorptive properties of the materials in the region of interest. An image intensifier B converts this x-ray shadowgraph into a pin cushion distorted optical image. That is, x-rays impinge upon a phosphor screen 14 mounted to a dome shaped input face 16 of the image intensifier. The phosphor screen converts the x-rays into light of the visible spectrum that is projected onto a target 18 as an optically distorted image 20 . A video camera C converts the output optical image into a video signal or other electronic image representation. The electronic image representation can be stored on tape or disk, subject to various types of processing, displayed on a video monitor 22 , or the like. The video camera includes a video pick-up tube 24 whose sweep pattern is controlled by electrostatic deflection plates 26a , 26b , 26c , 26d . A sweep control circuit D modifies a conventional, linear beam sweep pattern to introduce a second distortion in the video camera image representation, which second distortion is equal and opposite to the image intensifier optical distortion. In particular, the modified sweep pattern generally follows the arcuate lines of a pin cushion distorted grid image 20 rather than conventional straight, parallel lines. Moreover, this arcuate sweep pattern becomes slower at points more radially outward from the center of the video pick-up tube. The lighter intensity peripheral portions of the intensifier image 20 become balanced with the intensity of central portions of the image in a resultant video image 28 . In the preferred embodiment, the sweep control circuit D adds a parabolic correction to the normal vertical and horizontal saw tooth sweep voltages. That is: Vt = V + kV (V 2 + H 2 ) Ht = H + kH (V 2 + H 2 ) where V is the normal or uncorrected vertical sweep voltage and H is the normal or uncorrected horizontal sweep voltage, and k controls or determines the amount of correction. When k is equal to zero, conventional saw tooth vertical and horizontal sweep voltages are applied and an uncorrected image is produced. The value of k is increased, such as by adjusting a variable potentiometer or resistor until the resultant man-readable image 28 meets preselected criteria of accuracy and linearity. Of course, a third order parabolic correction of this form might also be provided in a magnetically controlled sweep tube type video camera or by shifting and averaging pixel values of a CCD type video camera. In the preferred embodiment, the sweep control circuit D includes a vertical deflection ramp generator 30 and a horizontal deflection ramp generator 32 . A mixed parabola generator includes circuit means 34 which calculates the sum of the squares of the vertical and horizontal ramp voltages. A multiplying or other magnitude adjusting means 36 multiplies the function by a selectable constant k. A first multiplying means 38 multiplies the vertical ramp voltage by the sum of the squares and a second multiplying means 40 multiplies the horizontal ramp by the sum of the squares function. A first adding means 42 adds the vertical voltage ramp to the parabolic product of multiplying means 38 and a second adding means 44 adds the horizontal ramp voltage to the parabolic product of multiplying means 40 . In this manner, a vertical deflection voltage as described by Equation (1a) and a horizontal deflection voltage as described by Equation (1b) are defined. The parabolically adjusted sweep control signals are split and inverted by inverters 46 and 48 . The inverted and uninverted parabolically adjusted sweep control signals are amplified by four substantially identical amplifiers 50a , 50b , 50c , 50d . The amplified inverted and uninverted vertical sweep signals are applied to the vertical sweep plates 26a , 26b and the amplified horizontal sweep signals are applied to the horizontal sweep plates 26a , 26b . Because all four amplifier circuits are substantially the same, only one is described herein in detail, which detailed explanation applies analogously to all four circuits. The amplifiers increase the sweep voltages to provide a sweep voltage of ± 200 volts on a 600 volt pedestal. A transistor 52 , which can handle 400 volts, is interconnected with a pair of zener diodes 54, 56 . These zener diodes each shift the voltage by 200 volts such that the transistor 52 only sees a 400 volt voltage swing, even although the plate voltages are swinging between 400 and 800 volts. The transistor 52 is connected with a common base configuration to eliminate a substantial portion of the capacitance. Because the frequency response of an amplifier is proportional to 1/2πRC, minimizing the capacitance maximizes the frequency response of the amplifier. In order to reduce the effects of the capacitance of the deflector plates, denoted electrically as C 26 , an isolation transistor 58 disconnects the plate capacitance C 26 from the system capacitance C sys . When transistor 52 is open, there is approximately 800 volts on the plates, hence on capacitor C 26 . When the transistor 52 closes to ground, the voltage on C 26 drops to about 400 volts. When the transistor 52 closes, the current flows through transistor 52 and when it is open, the current charges capacitor C sys . The output potential E out is related to a charging current I in flowing into C sys . I in is established by the constant current source 60 . Then E out may be expressed by the equation: E out = 1 c ∫ I in dt Some of this current also flows to the deflection plates or capacitor C 26 . In order to bring the plates quickly to the applied potential, the isolation transistor 58 has a high current gain, e.g. 100:1, so that the output current is very high and capacitor C 26 charges quickly. A diode 62 and resistor 64 hold the voltage on the base of a transistor 66 constant such that a constant, high current flows through resistor 68 and transistor 58 . Amplifier means 50b produces a complementary signal to that produced by 50a for application to the other vertical deflection plate. Analogously, amplifiers 50c and 50d produce complementary voltage signals for application to the horizontal deflection plates. An x,y interchanging means 70 interchanges the horizontal and vertical deflection signals and deflection plates 26a, 26b, 26c , and 26d to produce a 90° image rotation. A vernier rotation control 72a and 72b are provided for continuous rotation from 0 to ± 45°. Alternately, the rotation control 72a and 72b may be interconnected with the image intensifier B or a support for the patient such that in diagnostic procedures in which the subject and image intensifier are moved relative to each other, the sweep pattern is not rotated but the image 28 on the video monitory 22 remains constant. Although a parabolic correction is utilized in the preferred embodiment, the exact shape of the correction is determined by the shape of the dome of the image intensifier. In the preferred embodiment, the dome is a spherical segment as illustrated by curve 80 of FIGURE 2. The x and y distance from an arbitrary point on the curve to the point where a radial line through the curve point intersects the flat picture plan can be described by the coordinates Δ r y , Δ r x where: Δr y = R - R 2 - r 2 Stated in terms of the tangent of the angle of the radius: tan = r R 2 - r 2 = Δr y Δr x By similar triangles, Δr y can be stated as Δr y = Δr x r R 2 -r 2 To simplify the mathematics, one can define the radius of the dome as unity: Δr y = Δr x r 1-r 2 Δr x = 1 1-r 2 Substituting the value of Δr x in Equation (6b) into Equation (6a) expresses the value of Δr y in terms only of r. Δr y = (1 - 1-r 2 ) r 1-r 2 Δr y = r-r (1-r 2 ) 1/2 (1-r 2 ) 1/2 Δr y = r(1-r 2 ) -1/2 - r Using a Taylor series expansion of the form (1 ± x) -n = 1 ∓ nx + . . . , Δr y becomes: Δr y = r (1 + r 2 2 ) - r Δr y = r + r 3 2 - r Δr y = r 3 2 Δr y = kr 3 Thus, the displacement Δr y along the flat picture plane is proportional by a constant k times the cube of r. With reference to FIGURE 3, a corresponding correction ΔV deflection voltage V and correction ΔH to the horizontal deflection voltage H can be readily determined by conventional trigonometry: r 2 = V 2 + H 2 r = V 2 + H 2 ΔV = Δr y V r ΔH = Δr y H r Substituting Equation (8d) into Equations (11a) and (11b): ΔV = kr 3 V r = kr 2 V ΔH = kr 3 H r = kr 2 H Substituting Equation (10) into Equations (12a, 12b), the corrections ΔV and ΔH can be expressed solely in terms of V and H: ΔV = k(V 2 + H 2 )V ΔH = k(V 2 + H 2 )H The corrected sweep values V T , H T are the sum of the original sweep value and these corrections: V T = V + ΔV H T = H + ΔH V T = V + kV(V 2 + H 2 ) H T = H + kH(V 2 + H 2 ) If an input lens or dome of a different contour is utilized, the appropriate corrections are calculated analogously. It is to be further appreciated that additional refinement is obtainable through the use of the vernier rotational control 72a and 72b as shown in FIGURE 1. Specifically through the use of the vernier rotation control Equations (15a) and (15b) are further refined to: V r = V + kV (V 2 + H 2 ) ± KH H T = H + kH (V 2 + H 2 ) ± KV The invention has been described with reference to the preferred embodiment. Obviously, modifications and alterations will occur to others upon reading and understanding the preceding detailed description. It is intended that the invention be construed as including all such alterations and modifications insofar as they come within the scope of the appended claims or the equivalents thereof.

Claims: An x-ray diagnostic imaging system comprising: an x-ray source (A) for radiating a region of interest with penetrating radiation; a phosphor screen (16) for converting penetrating radiation that has passed through the region of interest into an optical image, an image intensifier (B) having a domed input end (16) operatively connected with the phosphor screen (14) for intensifying the image to produce an intensified image, which intensified image is optically distorted by the image intensifier domed input end (16), a video camera (C) which has a pick up tube (24) that sweeps an electron beam across a received image, the video camera (C) being connected with the image intensifier (B) such that the pick up tube (24) receives the distorted intensifier output image and converts it to an image representation, means (30, 32) for generating vertical V and horizontal H sweep control ramp signals, means for generating a third order parabolic correction in said V and H signals, said third degree parabolic correction in said V and H signals being made by (a) combining the V and H signals to produce V and H dependant correction signal and (b) combining a function of the V and H dependant correction signal with each of the V signal and the H signal, the third order corrected vertical and horizontal sweep control signals being connected with the video camera to control the electron beam sweep pattern; a video monitor (22) which converts the electronic image representation from the video camera into a man-readable image and means for adjusting the third order correction in said V and H signals to enable the operator to adjust the degree of curvature of the parabolas in real time while the system is in operation. A system as claimed in Claim 1, comprising a sweep control circuit (D) including said means (30, 32) for generating vertical and horizontal sweep control ramp signals; a first inverting means (46) for inverting the vertical control voltage ramp; a second inverting means (48) for inverting the horizontal control voltage ramp; first, second, third, and fourth amplifier means (50a, 50b, 50c, 50d) for amplifying the vertical control voltage ramp, inverted vertical control voltage ramp, horizontal control voltage ramp, and inverted horizontal control voltage ramp respectively; the first and second amplifiers (50a, 50b) being operatively connected with a first pair of oppositely disposed deflection plates (26a, 26b) to provide voltage ramps thereacross in a push-pull relationship; the third and fourth amplifiers (50c, 50d) being connected with a second pair of oppositely disposed deflection plates (26c, 26d) for applying the voltage ramps thereacross in a push-pull relationship; each amplifier means including: a relatively low voltage, first transistor (52) connected in a common based configuration for switching the control voltage ramp; a zener diode (54, 56) for shifting the controlled voltage ramp to a higher voltage; an isolation transistor (58) for isolating capacitance (Csys) of the first transistor (52) from the deflection plate (26a, 26b, 26c, 26d) to which the amplified ramp voltage is applied; a current source (60) for providing a recharging current to the deflection plate (26a, 26b, 26c, 26d). A system as claimed in claim 2 further including an electronic interchanging means (70) for altering the sweep signals of the sweep control circuit (D) to rotate the resultant image.

Inventors: LEONG DAVID L, PLUT LEONARD F, VAGI ROBERT J, LEONG, DAVID L., PLUT, LEONARD F., VAGI, ROBERT J.
Applicants: PICKER INT INC, PICKER INTERNATIONAL, INC.
Application year: 1990
Main classification: H04N5
IPC codes: H04N3, H04N5, A61B6, H04N7