WO2005050669A1 - Streustrahlenraster, insbesondere für medizinische röntgeneinrichtungen, sowie verfahren zur herstellung - Google Patents
Streustrahlenraster, insbesondere für medizinische röntgeneinrichtungen, sowie verfahren zur herstellung Download PDFInfo
- Publication number
- WO2005050669A1 WO2005050669A1 PCT/EP2004/052930 EP2004052930W WO2005050669A1 WO 2005050669 A1 WO2005050669 A1 WO 2005050669A1 EP 2004052930 W EP2004052930 W EP 2004052930W WO 2005050669 A1 WO2005050669 A1 WO 2005050669A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- scatter grid
- absorption elements
- fibers
- ray
- filler
- Prior art date
Links
Classifications
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/02—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/02—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators
- G21K1/025—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators using multiple collimators, e.g. Bucky screens; other devices for eliminating undesired or dispersed radiation
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/02—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators
- G21K1/04—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators using variable diaphragms, shutters, choppers
Definitions
- the present invention relates to an anti-scatter grid, in particular for medical X-ray devices, which is composed of numerous absorption elements for X-radiation separated from one another by a filler and carrier material, which are oriented approximately parallel to one another or towards a common focus.
- the invention further relates to a method for producing such an anti-scatter grid.
- the scattered radiation does not contribute to the image information and leads to a significant deterioration in the signal-to-noise ratio and the achievable resolution of the X-ray image if it hits the detector elements without weakening.
- suitable anti-scatter grids which usually depend on the geometric conditions of the respective X-ray system, in particular the arrangement of the X-ray tube and X-ray detector.
- the proportion of scattered radiation that reaches the detector elements can be significantly reduced, so that in many cases only usable x-ray images are obtained.
- Scattered radiation grids are composed of numerous absorption elements for X-ray radiation separated from one another by a filler and carrier material, which are either aligned approximately parallel to one another or towards a common focus, the focus of the X-ray tube.
- x-ray CT systems generally still use anti-scatter grids which have lead lamellae running approximately parallel to one another or oriented towards the x-ray focus, between which paper strips are introduced as filler and carrier material.
- the distance between the lead lamellae during the manufacture of the anti-scatter grid is set in such a way that the lead lamellae lie as precisely as possible above the separating septa of the detector-side fluorescent arrays when using the anti-scatter grid.
- the scattered grid must therefore be manufactured with very high mechanical precision.
- the realized part of the focus on the Fo ⁇ Kus the X-ray tube requires a complex production process. Due to these high demands on precision, the manufacture of the anti-scatter grids causes high costs. Even two-dimensional collimation of the X-rays, as is required when using two-dimensional detector arrays, cannot be achieved with such anti-scatter grids.
- a further anti-scatter grid is known from DE 199 20 301 C2, in which the absorption elements run essentially radially in spaced rows with respect to a center. The course and the arrangement of the absorption elements are specified in this anti-scatter grid according to a specific rule. Silicon is used as the carrier material in which holes are etched in accordance with the desired course of the rows of absorption elements. Pen-shaped absorption elements made of lead are inserted into these holes.
- This anti-scatter grid also requires compliance with a very high level of precision during production, which is achieved in particular through the proposed production technology with silicon as the carrier material.
- US Pat. No. 5,263,075 A describes an anti-scatter grid which allows two-dimensional collimation of the incident X-ray radiation.
- the anti-scatter grid is made up of one
- the object of the present invention is to provide a scattered radiation grid and a method for its production, which enable cost-effective production.
- the present anti-scatter grid is composed in a known manner from numerous absorption elements for X-rays separated from one another by a filler and carrier material, which are either aligned approximately parallel to one another or towards a common focal point.
- the anti-scatter grid is characterized in that the absorption elements are not arranged at exactly the same distance as in the prior art or according to a specific computational rule, but rather are statistically distributed.
- a statistical distribution is to be understood to mean randomly varying distances between the absorption elements, which result in an automatic distribution of the absorption elements over the width of the anti-scatter grid during manufacture.
- the Individual absorption elements must of course consist of an X-ray absorbing material, for example a heavy metal such as lead, tungsten, tantalum or molybdenum.
- Other materials that strongly absorb X-rays such as plastics filled with lead powder, can also be used as materials for the absorption elements.
- the filler and carrier material should absorb the X-rays as little as possible. Examples of such materials are plastics such as polyethylene, polystyrene or polypropylene.
- the absorption elements are preferably glued to the filler and carrier material, since this is a very simple and inexpensive technique for producing an anti-scatter grid.
- Collimation is achieved without having to accept a significant weakening of the X-radiation carrying the image information.
- the anti-scatter grid itself can be in this case a plate-shaped, in which case the absorption elements We ⁇ sentlichen are aligned in parallel.
- Such an anti-scatter grid produced in the form of a flat plate can also be mechanically deformed in such a way that it forms an approximately spherical cap-shaped plate, in which the absorption elements are then at least approximately aligned with the center of the sphere, which, when using the anti-scatter grid, focuses on X-ray tube should match ⁇ .
- Such a deformation can be easily realized, especially when plastics are used as filler and carrier material.
- This anti-scatter grid can use applications for all to ⁇ where a collimation of the X-ray is required.
- the preferred field of application is in medical X-ray devices, in particular in computer tomography.
- rod-shaped or fibrous absorption elements which are aligned perpendicular to the surface of the anti-scatter grid, instead of lamellar or foil-like absorption elements, a two-dimensional statistical distribution and thus a two-dimensional collimation can also be achieved.
- the present anti-scatter grid is also suitable for two-dimensional detector arrays.
- the present anti-scatter grid can also be used for large-area X-ray detectors.
- the absorption elements are formed by individual fibers made of an X-ray radiation strongly absorbing material.
- fibers made of an X-ray material that is largely transparent are used as filler and carrier material.
- Can be a bundle of fibers is then obtained by simple mixing and bonding the two fiber types, the perpendicular to the fiber axis ⁇ into individual slices cut or sawed, which form the anti-scatter grid.
- the method for producing the anti-scatter grid according to the invention is characterized in particular by the fact that the absorption elements are connected to the filler and carrier material to form a anti-scatter grid so that there is a statistical distribution of the absorption elements over the width of the anti-scatter grid.
- the present anti-scatter grid is only placed on or attached to the detector array, without having to take into account an assignment to the individual detector elements or pixels of the detector array. This also eliminates the need for positioning.
- Figure 1 shows an example of the structure of the present anti-scatter grid from individual fibers.
- Fig. 3 shows an example of a scattered radiation grid, which is designed in the form of a spherical cap-shaped plate.
- the present anti-scatter grid 1 shows an example of the structure of the present anti-scatter grid 1, which corresponds to a section over a single approximately 1 mm 2 pixel, ie the detection area 6, of an exemplary detector element.
- the individual absorption elements are formed here from metal fibers 2 of a heavy metal which are aligned parallel to one another and which are embedded between plastic fibers 3 as filler and carrier material.
- the statistical distribution of the metal fibers 2 within the illustrated area of the anti-scatter grid 1 can be seen from the figure.
- the plastic fibers 3 are essentially transparent to the incoming X-rays, while the metal fibers 2 strongly absorb this X-rays.
- An X-ray quantum 4 which strikes the surface of the anti-scatter grid 1 and carries the desired image information, penetrates through the plastic fibers 3 and almost without weakening strikes the underlying detector or fluorescent pixel so that it is detected by the detector element.
- an obliquely incident quantum of scattered radiation 5 will encounter several highly absorbing metal fibers 2 on the way to the detector, so that it is absorbed.
- fibers 3 made of a material with lower X-ray absorption, for example polymer fibers made of polyethylene, polystyrene or polypropylene, as well as metal fibers 2 or fibers made of other materials with high X-ray absorption are provided.
- the fibers 2, 3 are mixed with one another in a predeterminable mixing ratio, in particular with a degree of filling of the highly absorbent fibers 2 of preferably between 5 and 30%, and provided as a fiber stack 7, as can be seen in FIG. 2a.
- the fiber stack 7 is impregnated with adhesive 11 in order to connect the fibers to form a fiber composite 8. Mixing the fibers 2, 3 results in a statistical distribution of the highly absorbent fibers 2 within the fiber stack 7.
- the fiber composite 8 After the fiber composite 8 has been produced, it is distributed into individual disks perpendicular to the fiber direction, which form the anti-scatter grid 1.
- 2b shows the saw cuts 9
- FIG. 2c shows the anti-scatter grid 1 formed by one of the sawn disks as a fiber composite.
- an anti-scatter grid for two-dimensional collision has been created, which has a statistical distribution of the has sorption elements 2 across the width of the anti-scatter grid, as can be seen in the detail in FIG. 1.
- anti-scatter screens can also be produced in the form of an approximately spherical cap-shaped plate, as is shown schematically in FIG. 3.
- Such an anti-scatter grid 1 is achieved by deforming the anti-scatter grid of FIG. 2 with the aid of mechanical means. Appropriate deformation allows collimation, i.e. achieve the alignment of the absorption elements on the x-ray focus 10 of the respective x-ray system.
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Measurement Of Radiation (AREA)
- Apparatus For Radiation Diagnosis (AREA)
Abstract
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10/580,114 US7415098B2 (en) | 2003-11-21 | 2004-11-11 | Collimator for stray radiation, in particular for medical x-ray devices and method for producing said collimator |
JP2006540444A JP2007511307A (ja) | 2003-11-21 | 2004-11-11 | 特に医療x線装置用の散乱放射線グリッド及びその製造方法 |
CN2004800344973A CN1883010B (zh) | 2003-11-21 | 2004-11-11 | 散射束光栅及其制造方法 |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE10354811.4 | 2003-11-21 | ||
DE10354811A DE10354811B4 (de) | 2003-11-21 | 2003-11-21 | Streustrahlenraster, insbesondere für medizinische Röngteneinrichtungen, sowie Verfahren zu seiner Herstellung |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2005050669A1 true WO2005050669A1 (de) | 2005-06-02 |
Family
ID=34609246
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/EP2004/052930 WO2005050669A1 (de) | 2003-11-21 | 2004-11-11 | Streustrahlenraster, insbesondere für medizinische röntgeneinrichtungen, sowie verfahren zur herstellung |
Country Status (6)
Country | Link |
---|---|
US (1) | US7415098B2 (de) |
JP (1) | JP2007511307A (de) |
KR (1) | KR20060099537A (de) |
CN (1) | CN1883010B (de) |
DE (1) | DE10354811B4 (de) |
WO (1) | WO2005050669A1 (de) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101013613B (zh) * | 2006-02-01 | 2011-10-19 | 西门子公司 | X射线设备的焦点-检测器装置的x射线光学透射光栅 |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102011006421A1 (de) * | 2011-03-30 | 2012-10-04 | Siemens Aktiengesellschaft | Digitaler Röntgendetektor |
EP3574834B1 (de) | 2018-05-30 | 2020-05-13 | Siemens Healthcare GmbH | Streustrahlenraster für eine medizinische röntgeneinrichtung |
CN111522085A (zh) * | 2020-05-12 | 2020-08-11 | 深圳大学 | 二维x射线吸收光栅制作方法 |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5468970A (en) * | 1992-12-14 | 1995-11-21 | Institut Max Von Laue - Paul Langevin | Device for collimating beams of a radiation |
US6047044A (en) * | 1997-07-10 | 2000-04-04 | Siemens Aktiengesellschaft | Stray radiation grid |
US20010002699A1 (en) * | 1999-11-30 | 2001-06-07 | Olaf Such | X-ray detector |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE2031203A1 (de) * | 1970-06-24 | 1972-01-05 | Cawo Photochem Fab | Röntgen-Streustrahlenraster |
US5263075A (en) * | 1992-01-13 | 1993-11-16 | Ion Track Instruments, Inc. | High angular resolution x-ray collimator |
DE19726846C1 (de) * | 1997-06-24 | 1999-01-07 | Siemens Ag | Streustrahlenraster |
DE19730755A1 (de) * | 1997-07-17 | 1999-01-28 | Siemens Ag | Streustrahlenraster |
US6167110A (en) * | 1997-11-03 | 2000-12-26 | General Electric Company | High voltage x-ray and conventional radiography imaging apparatus and method |
JP2002509239A (ja) | 1997-12-17 | 2002-03-26 | シーメンス アクチエンゲゼルシヤフト | 散乱x線グリッド |
US6177237B1 (en) | 1998-06-26 | 2001-01-23 | General Electric Company | High resolution anti-scatter x-ray grid and laser fabrication method |
DE19920301C2 (de) * | 1999-05-03 | 2001-08-16 | Siemens Ag | Streustrahlenraster, insbesondere für eine medizinische Röntgeneinrichtung, sowie Verfahren zu dessen Herstellung |
US6408054B1 (en) * | 1999-11-24 | 2002-06-18 | Xerox Corporation | Micromachined x-ray image contrast grids |
DE10136946A1 (de) * | 2001-07-28 | 2003-02-06 | Philips Corp Intellectual Pty | Streustrahlenraster für eine Röntgeneinrichtung |
-
2003
- 2003-11-21 DE DE10354811A patent/DE10354811B4/de not_active Expired - Fee Related
-
2004
- 2004-11-11 CN CN2004800344973A patent/CN1883010B/zh not_active Expired - Fee Related
- 2004-11-11 JP JP2006540444A patent/JP2007511307A/ja not_active Abandoned
- 2004-11-11 KR KR1020067012305A patent/KR20060099537A/ko not_active Application Discontinuation
- 2004-11-11 US US10/580,114 patent/US7415098B2/en not_active Expired - Fee Related
- 2004-11-11 WO PCT/EP2004/052930 patent/WO2005050669A1/de active Application Filing
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5468970A (en) * | 1992-12-14 | 1995-11-21 | Institut Max Von Laue - Paul Langevin | Device for collimating beams of a radiation |
US6047044A (en) * | 1997-07-10 | 2000-04-04 | Siemens Aktiengesellschaft | Stray radiation grid |
US20010002699A1 (en) * | 1999-11-30 | 2001-06-07 | Olaf Such | X-ray detector |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101013613B (zh) * | 2006-02-01 | 2011-10-19 | 西门子公司 | X射线设备的焦点-检测器装置的x射线光学透射光栅 |
Also Published As
Publication number | Publication date |
---|---|
JP2007511307A (ja) | 2007-05-10 |
US7415098B2 (en) | 2008-08-19 |
CN1883010B (zh) | 2010-07-14 |
CN1883010A (zh) | 2006-12-20 |
US20070147587A1 (en) | 2007-06-28 |
DE10354811A1 (de) | 2005-06-30 |
DE10354811B4 (de) | 2012-09-27 |
KR20060099537A (ko) | 2006-09-19 |
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