Method for examining a body with penetrating radiation

• US 4,380,817 A
• Filed: 09/10/1980
• Issued: 04/19/1983
• Est. Priority Date: 09/27/1979
• Status: Expired due to Term

• Current Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Harding, Geoffrey, Wagner, Wolfgang
• Primary Examiner(s): Church, Craig E.
• Application Number:
  US06/185,845
• Time in Patent Office: 951 Days
• Field of Search: 250/272, 250/273, 250/274, 250/277 R, 250/278, 250/279
• US Class Current: 378/87
• CPC Class Codes: A61B 6/02 Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
• CPC Class Codes: A61B 6/483 involving scattered radiation

Abstract

Devices that measure the electron density in a body by means of radiation scattered from a narrow pencil beam of penetrating radiation directed through the body, produce defective images on reconstruction of the density distribution because of multiple scattering of radiation. This can of course be reduced by scattered ray diaphragms, but cannot be eliminated entirely. The invention therefore provides a means for detecting the size of the multiple scattered radiation component be measurement. For this purpose, the detector array which measures radiation including the single scattered radiation, is screened, at least osscasionally, from the single scattered radiation and the detected intensity values measured by the detector elements when so screened, are used to correct the values generated by measuring the detected radiation including the single scattered radiation.

Claims

1. In a device for examining a body using penetrating radiation which comprises:

source means which generate a primary beam of said radiation, detector array means for measuring, and for generating output signals representing, scattered radiation generated in the body along the primary beam, diaphragm means disposed between the detector array means and the primary beam which define a slit shaped aperture having a longitudinal direction which is oriented at right angles to the primary beam; and

a large plurality of lamellae of radiation-absorbing material disposed between the aperture and the detector array means which lamellae are disposed at least approximately in planes which intersect colinearly in and along the primary beam whereby the detector array means measure radiation which is both singly and multiply scattered in the body;

the improvement which comprises;

means for generating a relative displacement between the primary beam and the diaphragm means, the detector array means, and the lamellae so that, during a portion of the examination, the planes of the lamellae intersect outside of the primary beam whereby the detector array means only measure radiation which is multiply scattered in the body; and

means which subtract output signals from the detectors which represent only said multiply scattered radiation from respective output signals which represent both singly and multiply scattered radiation to produce signals which represent only singly scattered radiation.

2. A device as claimed in claim 1 further comprising drive means which function to shift the detector array means, the diaphragm means, and the lamellae in a longitudinal direction with respect to the aperture.

3. A device as claimed in claim 1 further comprising:

a stationary diaphragm, disposed between the radiation source means and the body, which defines at least two apertures which function to form a plurality of spaced primary beams;

rotatable absorber disc means, disposed between the stationary diaphragm and the body, which defines a plurality of arc-shaped apertures which are concentric with a rotational axis of the disc and are arranged in staggered formation about said rotational axis so that no more than one of the primary beams can pass through the disc means at any time; and

means for rotating the disc means about the axis.

4. A device as claimed in claim 3 wherein a first of the arc-shaped apertures is positioned to pass a primary beam in which the planes the lamellae intersect and wherein the length of arc of said first aperture is greater than the length of arc of the other apertures defined by the disc means.