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
  • A61B6/02—Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
  • A61B6/03—Computed tomography [CT]
  • A61B6/032—Transmission computed tomography [CT]
• • H—ELECTRICITY
  • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
  • H05G—X-RAY TECHNIQUE
  • H05G1/00—X-ray apparatus involving X-ray tubes; Circuits therefor
  • H05G1/08—Electrical details
  • H05G1/26—Measuring, controlling or protecting
  • H05G1/30—Controlling
  • H05G1/46—Combined control of different quantities, e.g. exposure time as well as voltage or current
• • 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
  • A61B6/40—Arrangements for generating radiation specially adapted for radiation diagnosis
  • A61B6/4021—Arrangements for generating radiation specially adapted for radiation diagnosis involving movement of the focal spot
  • A61B6/4028—Arrangements for generating radiation specially adapted for radiation diagnosis involving movement of the focal spot resulting in acquisition of views from substantially different positions, e.g. EBCT

Definitions

• the invention relates to a computer tomography device, including an X-ray source, an X-ray detection system for picking up a number of density profiles of an object to be radiologically examined, - a reconstruction unit for deriving an image signal from the density profiles, and
• control system for adjusting the X-ray source on the basis of a density value of the object.
• a computer tomography device of this kind is known from United States patent US 5,400,378.
• the invention also relates to a method of computer tomography.
• the control system of the known computer tomography device adjusts the tube current of the X-ray source on the basis of relative X-ray absorption values derived from "scout data".
• the "scout data” represent the attenuation of X-rays in the object relative to a standard value. Such scout data comprises the minimum values of two density profiles picked up by exposing the object to be examined to X-rays from two mutually perpendicular directions.
• the tube current is adjusted on the basis of the relative X-ray absorption values.
• the adjustment of the X-ray source is adapted to the relative X-ray absorption in the part of the object to be examined, for example a patient to be radiologically examined.
• the control system does not suitably take into account the fact that the desired image quality differs for images of different parts of the object to be examined.
• the density profiles are picked up by irradiating the patient by means of X-rays from a number of directions. An image of, for example a cross-section of the object is reconstructed from the density profiles.
• the operation of the known computer tomography device is also known from the general article "X-ray computed tomography for medical imaging" by Harish P. Hiriyannaiah in IEEE Signal Processing Magazine, March 1997, pp. 42-59.
• control system is arranged to adjust the X-ray source on the basis of a kind of tissue of a part of the object to be examined.
• the intensity and/or energy of the X-rays can be accurately adapted to the part of the object to be examined.
• the intensity and/or energy of the X-rays can notably be adapted very well to the anatomy and the morphology of the patient to be examined, thus ensuring that an image of high diagnostic quality is formed whereas the X-ray dose whereto the patient is exposed remains comparatively low.
• An image of high diagnostic quality notably has a low noise level, so that small details of low contrast can still be reproduced in a suitably visible manner.
• the intensity and/or energy of the X-rays is adjusted to be as low as possible, but high enough to ensure that the noise level of the image is acceptably low.
• the intensity and/or energy of the x-rays is adjusted on the basis of the murphology of the part of the patient's anatomy to be examined.
• the X-ray source is adjusted so that it yields an image having the quality required for the part imaged.
• Image quality relates notably to the noise level of the image, the contrast of the image, and their mutual relationship which represents the contrast resolution.
• the contrast resolution is the smallest brightness difference in the image of a detail of given dimensions which can still be visibly reproduced.
• the noise level, or rather the contrast resolution is adapted to the part of the anatomy of the patient to be examined.
• the imaging of lung tissue requires only little contrast resolution, because small deviations can be readily noticed in the image against the background of low X-ray absorption.
• the contrast resolution is related to the noise level of the image.
• the contrast resolution is a function of the noise level.
• the noise level of the image can be readily predicted as a function of the adjustment of the X-ray source; this is because the noise in the image is caused mainly by shot noise of the X-rays, said shot noise having a Poisson distribution.
• the intensity of the X-rays can be readily adjusted by adjustment of the tube current of the X-ray source.
• the tube current is the electric current of an electron beam whereby X-rays are generated in an anode of the X-ray source.
• the energy of the X-rays can be readily adjusted by adjustment of the electric high voltage between the cathode and the anode of the X-ray tube.
• the period of time during which the X-ray source emits X-rays can also be adjusted.
• This period of t ' me is the pulse duration of the X-ray pulses produced by the X-ray source.
• the product of the tube current and the pulse duration is also referred to as the mAs value.
• This mAs value represents the X-ray dose whereto the patient is exposed.
• the energy of the X-rays can be adjusted by adaptation of the electric high voltage applied to the X-ray source.
• the control system preferably takes into account a density value of the object and a reference adjustment.
• the density value differs for each part of the anatomy to be examined; for example, lung tissue absorbs hardly any X-rays whereas the skull and the region of the hips absorb a comparatively large amount of X-rays.
• the reference adjustment concerns an adjustment which yields, in a rather large number of situations, an image of acceptable image quality while exposing the patient to an acceptable X-ray dose.
• the reference adjustment is an adjustment of the X-ray source which yields the desired result for a majority of patients undergoing the relevant radiological examination, a group of patients having a diameter in a predetermined range or the reference adjustment is an adjustment which is adequate for a radiological examination of a voluminous patient.
• the reference adjustment is preferably dependent on the part of the anatomy to be examined, on the expected pathology or on the diagnostic requirements.
• the reference adjustment is used, or the radiologist is at least offered the possibility of selecting the reference adjustment, when an adjustment derived by the control system does not lead to a substantial reduction of the required X-ray dose.
• the adjustment which is co-based on the reference adjustment and the density value can also be suitably used without taking into account the part of the patient to be examined for the adjustment.
• the reference adjustment preferably takes into account the fact that a different image quality is required for the imaging of different parts of the anatomy.
• the reference adjustment is chosen so that it yields the desired quality when a comparatively voluminous patient is examined.
• the adjustment of the X-ray source can be readily adapted to the patient to be examined.
• the reference adjustment can also be derived from a mean or representative volume of the relevant part of the anatomy to be examined, the density or the X-ray absorption of said part and the desired image quality also being taken into account.
• the control system takes into account a difference between the djustment derived by the control system and the reference adjustment.
• the adjustment of the X-ray source preferably is changed only if a patient is examined whose build deviates significantly from the build associated with the reference adjustment. It is thus achieved that most radiological examinations are performed on the basis of a standardized protocol. Moreover, the loss of a substantial amount of time for readjustment of the X-ray source is avoided. Furthermore, the adjustment of the X-ray source will not be influenced by inaccuracies occurring during extraction of the adjustment of the X-ray source.
• the adjustment of the X-ray source is adapted, so as to limit the X-ray dose whereto a patient is exposed, only in the case of particularly large or voluminous patients, particularly small or skinny patients or children.
• control system changes the adjustment of the X-ray source if the adjustment derived by the control system deviates from the reference adjustment by more than a threshold value.
• the threshold value can be adjusted in advance. In practice, preferably a threshold value is used which yields a reduction of the X-ray dose by approximately 1/3 relative to the X-ray dose associated with the relevant reference adjustment.
• the difference between the adjustment derived by the control system and the reference adjustment is displayed. This enables the radiologist to adjust the X-ray source by hand, on the basis of the adjustment advised by the control system, or to use the reference adjustment.
• the adjustment of the X-ray source concerns the intensity and/or the energy of the X-rays emitted by the X-ray source.
• the intensity of the X-ray source can be readily adjusted by controlling the tube current of the X-ray source.
• the energy of the X-ray source can be readily adjusted by controlling the electric high voltage of the X-ray source.
• the density value of the patient to be examined can be readily measured, notably locally, by irradiating the patient by means of X-rays and by locally detecting to what extent the X-rays are attenuated.
• the result of such a measurement is referred to as a "scanogram" or "scout data".
• the X-ray source irradiates the patient by means of X-rays while the X-ray source and the X-ray detector are maintained in a fixed orientation relative to the patient.
• the X-ray source thus forms an X-ray shadow image which is usually called a "scanogram".
• the scanogram is usually employed to select a part of the patient of which density two are to be picked up.
• the local dimension of the patient notably the thickness, can be accurately derived from the scanogram.
• the X-ray source is adjusted while taking into account the dimensions of the patient.
• the intensity and/or the energy of the X-rays is chosen to be lower whereas in order to form a scanogram of a heavier or very heavy patient a higher intensity and/or energy of the X-rays is selected.
• a very low intensity and/or energy of the X-rays is used.
• the X-ray source in order to form the scanogram the X-ray source can be sufficiently accurately adjusted on the basis of a coarse judgement of the patient. Such a coarse judgement of the patient can be readily made in a glance. It also makes sense to form such a scanogram while taking into account a property of the patient to be examined, for example the stature thereof, independently of the use of the scanogram for adjusting the X-ray source.
• An embodiment of a computer tomography device is defined in Claim 8.
• the patient is exposed to a lower X-ray dose by reducing the intensity and/or energy of the X-ray source.
• the reference adjustment preferably concerns the adjustment which is adequate for a radiological examination of a voluminous patient, so that the X-ray dose whereto a patient is exposed in practice is practically always lower than the X-ray dose that would be applied according to the reference adjustment.
• the noise index represents the amount of noise to be expected in the image in dependence on the adjustment of the computer tomography device.
• the radiologist provides an indication as to which noise impression is desired for the image to be generated.
• the control system derives an adjustment of the X-ray source from the value selected for the noise index so as to achieve the desired image quality.
• the noise index is defined in such a manner that a strong correlation exists between a more or less subjective evaluation of noise by the radiologist and the objective value of the standard deviation of the brightness values of the image.
• the standard deviation represents variations of the brightness values in as far as they do not relate to image information.
• An embodiment of a computer tomography device is defined in Claim 10.
• the angle at which the patient is irradiated can thus be taken into account. As the angle of incidence of the X-rays is larger, the path traveled by the X-rays through the patient will be longer and the X-rays will be attenuated more. It is also an object of the invention to provide a method of computed tomography for forming an image of high diagnostic quality while limiting the x-ray dose whereto the patient is exposed. The object is achieved by the method defined in Claim 11.
• the Figure shows diagrammatically a computer device according to the invention.
• the Figure shows diagrammatically a computer tomography device according to the invention.
• An X-ray source 1 co-operates with a slit-shaped diaphragm 10 so as to emit a diverging flat (fan-shaped) X-ray beam 3 for irradiating the object 2, for example a patient to be examined.
• the X-ray detector 5 is arranged opposite the X-ray source 1.
• the X-ray detector of the present embodiment is a position-sensitive X-ray detector which comprises a row of separate detector cells 11.
• the detector cells 11 are, for example gas-filled (xenon) detectors or solid-state detectors.
• the thickness of the fan-shaped X-ray beam generally amounts to from 1 mm to 10 mm, measured halfway between the X-ray source and the X-ray detector.
• the intensity of the radiation having traversed the patient and incident on the X-ray detector is determined mainly by the absorption within the patient 2 who is arranged on a table 12 between the X-ray source and the X-ray detector.
• the absorption is measured along a large number of lines from a large number of directions by rotating the X-ray source 1 and the X-ray detector 5 together around the patient by means of a support 13.
• the combined rotation of the X-ray source and the X-ray detector may be continuous but also intermittent.
• the patient can be displaced along the axis of rotation during irradiation and rotation, so that the X-ray detector acquires data from a significant three-dimensional volume of the patient.
• the computer device may also include a detection system which is not rotatable but extends along (substantially) the entire circumference of the patient.
• the X-ray source and the X-ray detector are fully rotated together, i.e. through 360°, around the patient.
• annular anode arranged around the patient can also be used as the X-ray source, the point of incidence of an electron beam generating X-rays from the anode material then being displaced along the annular anode around the patient. It suffices in principle, however, to use a fan-shaped beam which rotates around the patient through an angle which amounts to the sum of 180° and the angle of aperture of the fan-shaped beam.
• the intensity of the X-rays received by the individual detector cells in any position or orientation of the X-ray source and the X-ray detector is digitized and applied to a reconstruction unit 4. In the reconstruction unit 4 this measured data is converted, after correction for known error sources and disturbances, into a density profile of the patient to be examined.
• high and low density values in the density profile correspond to parts of the patient in which the X-ray absorption is high and low, respectively.
• the intensity values of the X-rays received by the X-ray detector in individual orientations constitute a respective density profile.
• an image of a slice along a plane through the patient can be derived from these density profiles by means of the reconstruction unit.
• An image of this kind may represent, for example, a cross-section of the patient to be examined.
• Such an image can be displayed on a monitor 14 which is coupled to the reconstruction unit.
• the image may also be stored as a digital image matrix or be applied to an image processing unit 15 for further processing.
• the computer tomography device also includes a control unit 20 which serves to adjust the X-ray source.
• This adjustment concerns notably the adjustment of a high- voltage power supply 21 for the X-ray source, particularly the adjustment of the tube current and the high voltage whereby the intensity and the energy of the X-rays are adjusted.
• the control unit is connected to a memory unit 22 in which suitable reference adjustments of the X-ray source are stored for the examination of different parts of the anatomy of the patient to be examined. Such reference adjustments can be empirically determined by forming images of various parts of the anatomy of a large number of patients while using a number of adjustments of the X-ray source.
• the reference adjustments comprise the tube current and the high voltage of the X-ray source, and may also comprise other parameters of the computer tomography device, for example the slice thickness used, the speed of rotation of the X-ray source and the X-ray detector, and filter adjustments of the reconstruction unit.
• the reference adjustment preferably also comprises a reference thickness of the patient.
• the reference adjustments have been chosen in such a manner that in the circumstances represented by individual reference adjustments an image of the desired diagnostic quality is produced while using an acceptable X-ray dose.
• a so-called scanogram of the patient is formed by irradiating the patient by means of X-rays while the X-ray source and the X-ray detector are stationary and the patient table with the patient is displaced in the longitudinal direction of the patient.
• the reconstruction unit 4 derives from x-ray attenuation values density values of different parts of the patient from the local absorption of X-rays. These density values constitute the scanogram and are stored in the memory unit 22.
• the control unit 20 calculates the local thickness of the patient from the density values of the patient and compares the calculated thickness with the reference thickness. The control unit applies the calculated thickness of the patient and the reference thickness to a display 23.
• the control unit 20 also includes one or more selection members 24, such as preset keys, for adjusting the computer tomography device so as to form the scanogram. This adjustment is performed by adjusting the X-ray source on the basis of the thickness of the patient.
• preset keys are provided for forming a scanogram of a small child, a thin, a normal and a very voluminous patient.
• ⁇ is the mean X-ray absorption coefficient along the path traveled by the X-rays through the part of the patient to be examined and d is the path length of the X-rays through the part of the patient to be examined.
• the standard deviation is an accurate measure of the noise level in the image.
• p G( ⁇ d, ⁇ )
• ⁇ c y / exp( ⁇ tf) v sl ⁇
• V the electric high voltage
• s the slice thickness
• I the tube current
• ⁇ the pulse duration of the X-ray source
• c a proportionality constant.
• An acceptable noise level ⁇ ref can be empirically determined for adjustments p e.g.
• an effective patient thickness D eff is derived.
• I 0 /I is the ratio of the x-ray intensity incident on the part of the patient to be examined to the x-ray intensity passing through the part of the patient to be examined. This ratio is obtained from the scanogram.
• p G( ⁇ , D, ⁇ ref )
• the effective patient thickness D eff may be calculated even more accurately by taking into account the mean x-ray absorptivities of the part of the patient to be examined in respective directions. The values of this ratio for different parts of the patient to be examined are taken up in the scanogram.

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• 1998
  • 1998-05-25 DE DE69840290T patent/DE69840290D1/de not_active Expired - Lifetime
  • 1998-05-25 EP EP98919417A patent/EP0942682B1/en not_active Expired - Lifetime
  • 1998-05-25 JP JP10542107A patent/JP2000516834A/ja active Pending
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