EP0047780A1 - Tomographie transversale avec filtrage optique - Google Patents

Tomographie transversale avec filtrage optique

Info

Publication number
EP0047780A1
EP0047780A1 EP81900904A EP81900904A EP0047780A1 EP 0047780 A1 EP0047780 A1 EP 0047780A1 EP 81900904 A EP81900904 A EP 81900904A EP 81900904 A EP81900904 A EP 81900904A EP 0047780 A1 EP0047780 A1 EP 0047780A1
Authority
EP
European Patent Office
Prior art keywords
optical
filtering
light
beams
slice
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP81900904A
Other languages
German (de)
English (en)
Inventor
Harrison H. Barret
William Swindell
Scott Gordon
John E. Greivenkamp, Jr.
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
University Patents Inc
Original Assignee
University Patents Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from US06/132,562 external-priority patent/US4331877A/en
Priority claimed from US06/132,563 external-priority patent/US4329588A/en
Application filed by University Patents Inc filed Critical University Patents Inc
Publication of EP0047780A1 publication Critical patent/EP0047780A1/fr
Withdrawn legal-status Critical Current

Links

Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
    • A61B6/02Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
    • A61B6/03Computed tomography [CT]
    • A61B6/032Transmission computed tomography [CT]
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
    • A61B6/52Devices using data or image processing specially adapted for radiation diagnosis
    • A61B6/5205Devices using data or image processing specially adapted for radiation diagnosis involving processing of raw data to produce diagnostic data
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06TIMAGE DATA PROCESSING OR GENERATION, IN GENERAL
    • G06T11/002D [Two Dimensional] image generation
    • G06T11/003Reconstruction from projections, e.g. tomography
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06TIMAGE DATA PROCESSING OR GENERATION, IN GENERAL
    • G06T11/002D [Two Dimensional] image generation
    • G06T11/003Reconstruction from projections, e.g. tomography
    • G06T11/006Inverse problem, transformation from projection-space into object-space, e.g. transform methods, back-projection, algebraic methods
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/30Transforming light or analogous information into electric information
    • H04N5/32Transforming X-rays
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06TIMAGE DATA PROCESSING OR GENERATION, IN GENERAL
    • G06T2211/00Image generation
    • G06T2211/40Computed tomography
    • G06T2211/421Filtered back projection [FBP]

Definitions

  • the present invention is directed to an apparatus and method for generating a two-dimensional back- projected image of a slice of an object, and also to an optical filtering apparatus and method which, inter alia, is useful therein.
  • means are provided for generating successive beams of light, each having a narrow elongated cross-section with an optical intensity that is a function of the density characteris ⁇ tic of the slice of the object as measured at a particu ⁇ lar relative rotational angle.
  • the beams may be generated, for example, by successively illuminating individual one-dimensional optical projections, each having ai optical characteristic that is a function of the density characteristic of the slice of the object as measured at a' particular relative rotational angle.
  • Electro- optical sensing means which may be, for example, a television camera or a photo-detector (depending upon the type of system in which this form of the invention is employed) , are provided to receive the filtered beam. Further means are provided for combining suc- cessive electronic outputs of the electro-optical sensing means. Finally, means synchronized with the interposing means are provided for controlling the polarity of the combining means.
  • the first and second optical filtering means are electro-optically switch- able, and the interposing means includes means for controlling the electro-optical switching of the filtering means.
  • passing through a particular row of ele- ments is designated by I with two subscripts, the first subscript indicating the reference angle at which the X-ray energy is passed through the slice 90 (a 0° refer ⁇ ence angle is shown in FIG. 5, so the first subscript is 0) , and the second subscript indicating the relative position of the particular beam or beam portion along the one-dimensional data coordinate (e.g. the x axis in FIGS 1 and 2) .
  • the detected beams, or portions thereof, which have passed through the slice 90 are designated by primed versions of the input beams. Each output is equal to its corresponding input times a function of the elemental densities through which the beam or beam portion has passed.
  • filtering can be used in conjunction with back-projection.
  • the fil- tering can be visualized as a type of selective
  • h__ (x) is a sampled version of h_ (x) is not surprising since sampling a function in the space domain corresponds to replicating that function in the frequency domain.
  • the pupil function that led to h x) was a replicated version of the pupil function for _' (x) .
  • the corresponding optical transfer functions which are the autocorrelations of the pupil functions, bear a similar replicative relationship.
  • filter means 160 includes a polarizer 161 which polarizes the received beam of unpolarized light in a given direction, for example, to produce vertically polarized light.
  • the element 162 is an electro-optical polarization rotator that is operative, when activated by a given polarity of

Landscapes

  • Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Medical Informatics (AREA)
  • General Physics & Mathematics (AREA)
  • Molecular Biology (AREA)
  • Radiology & Medical Imaging (AREA)
  • Veterinary Medicine (AREA)
  • Public Health (AREA)
  • General Health & Medical Sciences (AREA)
  • Biophysics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Animal Behavior & Ethology (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Optics & Photonics (AREA)
  • Pathology (AREA)
  • Surgery (AREA)
  • Biomedical Technology (AREA)
  • Heart & Thoracic Surgery (AREA)
  • Algebra (AREA)
  • Pure & Applied Mathematics (AREA)
  • Mathematical Analysis (AREA)
  • Mathematical Optimization (AREA)
  • Mathematical Physics (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Pulmonology (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Image Processing (AREA)

Abstract

Dispositif et procede pour generer une image bidimensionnelle retroprojetee d'une tranche d'un objet, et dispositif et procede de filtrage optique utiles entre autres dans le procede de tomographie decrit. Des rayons de lumiere successifs sont generes, chacun possedant une section transversale etroite et allongee avec une intensite optique qui est fonction de la caracteristique de densite de la tranche de l'objet mesuree selon un angle de rotation relatif particulier. Les rayons sont filtres optiquement et diffuses dans une direction transversale par rapport a leur longueur. Un filtrage optique avec une fonction de filtre possedant des composants positifs et negatifs est executee de preference en utilisant une technique modulee dans le temps a canal simple. Une camera de television (280) recoit les rayons filtres diffuses. Une rotation relative est effectuee entre les rayons et la camera, la rotation etant fonction des angles de rotation relatifs de l'objet associe a la generation des rayons de lumiere successifs. Une memoire de sequence digitale (287) accumule les intensites detectees dans des zones elementaires des moyens de detection de l'image. Les intensites accumulees comprennent une image retroprojetee bidimensionnelle de la tranche de l'objet pouvant etre ensuite affichee sur un ecran de television (290). Dans une autre forme de la realisation, les images retroprojetees sont obtenues a l'aide d'un processeur de "boucles" optiques (140) utilisant une technique de filtrage modulee dans le temps a canal simple.
EP81900904A 1980-03-21 1981-03-16 Tomographie transversale avec filtrage optique Withdrawn EP0047780A1 (fr)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
US06/132,562 US4331877A (en) 1980-03-21 1980-03-21 Transverse tomography with optical filtering
US132562 1980-03-21
US06/132,563 US4329588A (en) 1980-03-21 1980-03-21 Polarization switched optical filtering for transverse tomography
US132563 1998-08-11

Publications (1)

Publication Number Publication Date
EP0047780A1 true EP0047780A1 (fr) 1982-03-24

Family

ID=26830496

Family Applications (1)

Application Number Title Priority Date Filing Date
EP81900904A Withdrawn EP0047780A1 (fr) 1980-03-21 1981-03-16 Tomographie transversale avec filtrage optique

Country Status (2)

Country Link
EP (1) EP0047780A1 (fr)
WO (1) WO1981002800A1 (fr)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA2024475A1 (fr) * 1989-11-27 1991-05-28 Leopold Neumann Systeme et methode de saisie et de transmission de donnees d'imagerie
EP0614645A4 (fr) * 1992-08-31 1996-04-03 Hitachi Ltd Appareil de tomographie optique informatisee.

Family Cites Families (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE693374C (de) * 1938-06-27 1940-07-12 C H F Mueller Akt Ges Verfahren zur Herstellung von Koerperschnittbildern mittels Roentgenstrahlen
US3027806A (en) * 1957-03-14 1962-04-03 Ibm Electro-optical devices
US4081673A (en) * 1976-04-12 1978-03-28 University Patents, Inc. Transverse tomography apparatus and method
US4023036A (en) * 1975-06-16 1977-05-10 University Patents, Inc. Apparatus and method for transverse tomography
NL7605254A (nl) * 1976-05-17 1977-11-21 Optische Ind De Oude Delft Nv Beeldconstructie.
NL7609963A (nl) * 1976-09-08 1978-03-10 Optische Ind De Oude Delft Nv Signaalverwerkend stelsel.
US4135096A (en) * 1977-11-23 1979-01-16 Giordano Ames F Electronic-optical system for X-ray object cross section image reconstruction
NL7804881A (nl) * 1978-05-05 1979-11-07 Optische Ind De Oude Delft Nv Werkwijze en inrichting voor het elektro-optisch convo- lueren van een eendimensionaal signaal.

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO8102800A1 *

Also Published As

Publication number Publication date
WO1981002800A1 (fr) 1981-10-01

Similar Documents

Publication Publication Date Title
Raven Numerical removal of ring artifacts in microtomography
KR100929357B1 (ko) 치과용 구강외 엑스레이 영상 시스템 및 방법
JP3481631B2 (ja) 能動型照明及びデフォーカスに起因する画像中の相対的なぼけを用いる物体の3次元形状を決定する装置及び方法
US3936639A (en) Radiographic imaging system for high energy radiation
US5319550A (en) High resolution digital image registration
Lanman et al. Shield fields: Modeling and capturing 3D occluders
US4017730A (en) Radiographic imaging system for high energy radiation
US10559393B2 (en) X-ray detector for phase contrast and/or dark-field imaging
US5712685A (en) Device to enhance imaging resolution
US4598369A (en) Tomography apparatus and method
US4331877A (en) Transverse tomography with optical filtering
US3840747A (en) Gamma ray imaging system
FR2630903A1 (fr) Dispositif de tomographie a grande cadence d'acquisition
Edholm et al. Ectomography: a new radiographic method for reproducing a selected slice of varying thickness
US4329588A (en) Polarization switched optical filtering for transverse tomography
US4081673A (en) Transverse tomography apparatus and method
JP2978238B2 (ja) Ct装置
US4023036A (en) Apparatus and method for transverse tomography
EP0047780A1 (fr) Tomographie transversale avec filtrage optique
Petersson et al. Ectomography-a new radiographic reconstruction method-II. Computer simulated experiments
US3560740A (en) Depth-perception radiography
Budinger et al. Reconstruction of the Fresnel-coded gamma camera images by digital computer
Chang et al. Coded aperture imaging of gamma-rays using multiple pinhole arrays and multiwire proportional chamber detector
Honda et al. Image processing by multiple aperture scanning
JPH04288147A (ja) X線ct装置

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

AK Designated contracting states

Designated state(s): CH DE FR GB LU NL SE

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN

18D Application deemed to be withdrawn

Effective date: 19820524

RIN1 Information on inventor provided before grant (corrected)

Inventor name: BARRET, HARRISON H.

Inventor name: GORDON, SCOTT

Inventor name: GREIVENKAMP, JOHN E., JR.

Inventor name: SWINDELL, WILLIAM