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    • 专利摘要:
    variable angle collimator. The present invention relates to a system for producing a controllable radiation beam that is electronically controllable, and does not include any parts that must move relative to one another while in operation to form the beam. the direction and cross section of the beam can be electronically controlled by controlling an electron beam. various modalities provide an x-ray collimator that allows the formation of a scanning x-ray beam of the desired size and flux regardless of the thickness of the aperture material without requiring movement of the aperture or the physical components that create the aperture. some modalities provide an x-ray collimator that allows you to form a scanning x-ray beam of the desired size and flux regardless of the beam angle.
    公开号:BR112015000037B1
    申请号:R112015000037-1
    申请日:2013-07-02
    公开日:2021-06-29
    发明作者:Martin Rommel
    申请人:American Science and Engineering, Inc；
    IPC主号:
    专利说明:

    CROSS REFERENCE TO RELATED PATENT APPLICATIONS
    [001] The present patent application claims priority from U.S. provisional patent application no. 61/668268, filed July 5, 2012, entitled "Variable Angle Collimator", and naming Martin Rommel as the inventor [attorney file 1945/B62], the description of which is incorporated herein by reference in its entirety. . TECHNICAL FIELD
    [002] The present invention relates to X-ray sources, and more particularly, to collimators. BACKGROUND OF THE INVENTION
    [003] X-ray backscatter imaging is based on scanning an object with a well-collimated beam, often called "pencil beam". In the past, these beams were also widely used for X-ray transmission imaging, but today fans and cone beams together with pixelated detectors dominate transmission imaging.
    [004] There are two approaches commonly used to form the collimated scanning beam. Both are based on a stationary X-ray source and a movable aperture. This moving part consists of a rotating disk with radial slots, or a wheel with perimeter openings. The rotating disk covers the fan beam, and the scanning beam is formed by radiation emitted through slits that span the length of the fan beam opening. This approach is illustrated, for example, in U.S. Patent 3,780,291 of 1973 issued to Stein and Swift; see Fig. 1A. In the other approach, a wheel with radial holes that rotates around the X-ray source constitutes the moving part. If the source is placed at the center of the wheel, the sweep beam is emitted in the radial direction with the angular velocity of the wheel.
    [005] Other approaches to form a collimated beam from a stationary X-ray source have been proposed, based, for example, on a rotating cylinder with a spiral groove as described by Annis in U.S. Patent 5,493,596 of 1996.
    [006] System configurations with mobile X-ray sources were developed. The movement of the X-ray source is typically not formed by moving the X-ray tube, but by moving (sweeping) the electron beam along an extended anode. This produces a moving X-ray source spot (electron beam focal point) whose position can be electronically controlled. A moving X-ray source point allows the formation of the scanning X-ray beam with a single stationary aperture (tiny hole) at some distance from the point of origin. As the X-ray source point is moved from one end of the scanning path to the other, the scanning X-ray beam emerging from the aperture spans an angular range. One embodiment of this concept is, for example, part of the system described in U.S. Patent 4,045,672 of 1977 issued to Watanabe, see also Fig. 1B.
    [007] Since the X-ray beam covers the angular range, the cross-sectional area of the beam varies as the cosine of the angle between the beam and the normal of the aperture plane. If the angular range is small, beam variation is limited and can be neglected. If, however, a large angular range is required, the effect becomes significant. For example, for an angular range of 120°, an angle of 60° out of normal at the ends leads to a reduction of at least 50% in beam size and released flux, since the cosine of 60° is 0.5 .
    [008] In reality, the variation of the beam is even greater, because the material with the tiny hole has a finite thickness which leads to a further reduction in the cross-sectional area of the beam with increasing angle. This problem becomes more serious for higher energy X-rays that require a denser shielding material for the material with the tiny hole.
    [009] To allow for a thicker shielding material, and to avoid angular variation, it has been suggested to replace the tiny hole with a rotating cylinder containing a hole perpendicular through the shaft as described in US Patent 6,356,620 of 2002 issued to Rothschild and Grodzins, see also figure 1C. This cylinder must rotate in sync with the scanning electron beam so that the moving point of the X-ray source is always aligned with the hole. This approach solves both problems with the simple tiny hole design: it forms a beam of constant size regardless of the beam angle and does not limit the thickness of the material that forms the opening. However, this active solution introduces significant cost and complexity compared to the passive tiny hole. It also greatly eliminates the great flexibility offered by electronic control of the electron beam. SUMMARY OF MODALITIES
    [0010] A variable-angle collimator controllably produces a collimated radiation beam without physically manipulating any collimator member. The collimated beam angle can be fully electronically controlled via an electron beam that hits an anode.
    [0011] In a first embodiment, a system for producing a directable beam of radiation includes a radiation source configured to produce radiation at an angle, relative to a collimator, wherein the angle is electronically controllable; a collimator comprising a material opaque to radiation produced by the radiation source, the collimator comprising an aperture configured to receive radiation from the radiation source at a plurality of incidence angles, and configured to let a portion of the radiation pass through the collimator at each angle of the plurality of incidence angles, so as to form a collimated beam of radiation with a beam in cross section, and in which the collimator and the radiation source are configured to remain stationary with respect to each other when producing a beam of drivable radiation.
    [0012] The radiation source may include an electron source and an anode, configured in such a way that the electron source illuminates the anode with an electronically drivable beam of electrons, so as to produce a moving point of radiation source.
    [0013] The aperture, and therefore the cross-section of the resulting radiation beam, can have any of a variety of shapes, such as rhomboid, square, and rectangular. In some embodiments, the shape of the aperture (and therefore the cross-section of the resulting beam) is variable as a function of the angle of the incident radiation relative to the aperture.
    [0014] Several collimator modalities present a variety of structures. For example, in one embodiment, the collimator includes several surfaces, and the aperture is a composite aperture formed by cooperation between a first aperture in the surface of a first collimator and a second aperture in the surface of a second collimator. For example, the first surface can be a surface of a first plate, and the second surface can be a surface of a second plate arranged parallel to the first plate.
    [0015] Another embodiment of a collimator includes a first member having a first surface, which is a hyperbolic paraboloid surface, or a modified hyperbolic paraboloid surface; and a second member having a second surface, which is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; the first member disposed with respect to the second member such that the first surface opposes the second surface, with the first surface and second surface spaced apart to define an opening through the collimator. In some embodiments, the collimator is a helically cut cylinder.
    [009] A method for irradiating a target with a collimated beam of radiation includes providing a drivable radiation source configured to illuminate a collimator; the provision of a collimator comprising a hyperbolic paraboloid aperture having an inlet and an outlet, with the collimator disposed in a fixed position with respect to the drivable radiation source; the production of a collimated radiation beam at a plurality of exit angles by: illuminating the entrance of the hyperbolic paraboloid aperture with illuminating radiation from a first illuminating angle so that a portion of the illuminating radiation passes through the collimator and exiting the collimator at a first exit angle; and illumination of the entrance of the hyperbolic paraboloid aperture with illumination radiation of a second illumination angle, wherein the second illumination angle is different from the first illumination angle, so that a portion of the illumination radiation passes through the collimator and exits the collimator at a second exit angle, where the second exit angle is different from the first exit angle, so that radiation exiting the collimator at the first angle and at the second angle radiates the target.
    [0010] The step of providing a collimator may include providing a collimator having an input plate with a first face and a second face; and a fully elongated first opening through the inlet plate between the first face and the second face; and an outlet plate with a third face and a fourth face, and a second fully elongated opening through the outlet plate between the third face and the fourth face, the first face parallel to the fourth face, and separated from the fourth face by a distance. predetermined, such that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, such that the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which radiation can pass without contacting the input board and without contacting the output board.
    [0011] Alternatively, the step of providing a collimator may include providing a collimator having: a first member comprising a first surface, which is a hyperbolic paraboloid surface, or a modified hyperbolic paraboloid surface; and a second member comprising a second surface, wherein the second surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; the first member disposed with respect to the second member such that the first surface face opposes the second surface, wherein the first surface and second surface are spaced apart to define a hyperbolic paraboloid opening across the collimator.
    [0012] In some embodiments, producing a collimated beam at the first angle includes producing a collimated beam that has a first cross-sectional shape, producing a collimated beam at the second angle includes producing a collimated beam that has a second cross-sectional shape, where the second shape is different from the first shape.
    [0013] In another embodiment, a system for producing a directable beam of radiation includes a radiation source means for producing an electronically directable point of illumination radiation source; and a collimation means having an aperture configured to allow a portion of the illuminating radiation incident on said collimation means to pass; wherein the radiation source means is arranged, with respect to the collimation means, to remain stationary with respect to the collimation means, and so as to illuminate the aperture with incident radiation from the directable point of the radiation source, so that the aperture produce a directable beam of radiation.
    [0014] The collimation means may include a first member comprising a first hyperbolic paraboloid surface; and a second member comprising a second hyperbolic paraboloid surface; wherein the first member is disposed relative to the second member such that the first hyperbolic paraboloid surface is disposed opposite the second hyperbolic paraboloid surface such that the first hyperbolic paraboloid surface is separated from the second hyperbolic paraboloid surface through an opening span, and the first member and the second member form the opening through the opening span.
    [0015] Alternatively, the collimation means may include a first member comprising a first hyperbolic modified paraboloid surface; and a second member comprising a second hyperbolic modified paraboloid surface; in, that the first member is disposed relative to the second member such that the first modified hyperbolic paraboloid surface is disposed opposite the second modified hyperbolic paraboloid surface and that the first modified hyperbolic paraboloid surface is separated from the second surface of hyperbolic paraboloid modified by an opening span, where the opening span is not constant, so that the first member and the second member form the opening transverse to the opening span. BRIEF DESCRIPTION OF THE DRAWINGS
    [0016] The characteristics of the aforementioned modalities will be more readily understood by reference to the following detailed description, taken with reference to the attached drawings, in which:
    [0017] figures 1A - 1C schematically illustrate prior art collimators;
    [0018] figures 2A - 2I schematically illustrate an embodiment of a collimator;
    [0019] figures 2J - 2K schematically illustrate an embodiment of a collimator;
    [0020] Figure 2L schematically illustrates a cross section of a collimated beam that has the shape of a kite;
    [0021] figures 3A-C schematically illustrate a hyperbolic virtual paraboloid surface;
    [0022] figures 4A-C schematically illustrate an embodiment of a collimator;
    [0023] figures 5A - 5E schematically illustrate an embodiment of a cylindrical collimator of helical cut;
    [0024] figures 6A-C schematically illustrate an embodiment of a collimator;
    [0025] Figure 7 schematically illustrates an embodiment of a collimator block with a modified hyperbolic paraboloid surface and a secondary plate.
    [0026] Detailed Description of Specific Modalities
    [0027] Several modalities provide an X-ray collimator that allows to form a scanning X-ray beam of the desired size and flux, regardless of the thickness of the aperture material, without requiring movement of the aperture or the physical components that make up the aperture. Some modalities provide an X-ray collimator that allows you to form a scanning X-ray beam of the desired size and flux, regardless of the beam angle.
    [0028] In various embodiments, a still-part collimator creates a beam (eg, a pencil beam) from a point-shaped radiation source such that the cross-sectional area of the pencil beam varies. with the incident angle in a deliberate way. In particular, some modalities allow the creation of pencil beams with a cross-sectional area that is independent of the incident angle. In some embodiments, a variable-angle collimator includes attenuating materials rigidly arranged so that the point source radiation is effectively collimated into a beam (eg, a pencil beam) for a range of incident angles and such that the cross section beam is a function of the incident angle.
    [0029] For example, the beam angle can be determined by controlling the focal point of a beam from the electron source that impinges on an anode. Such an electron beam can be described as being “airship.” An electron beam source, together with an anode, can be described as a radiation source configured to produce radiation at an angle with respect to a collimator, in which the angle is electronically controllable.
    [0030] The focal point becomes an X-ray source. In this way, the movement of the electron beam in a controllable way provides the control of the focal point, and, thus, provides control of the position of the X-ray source Controlling the position of the X-ray source, in turn, provides control of the angle at which the X-rays collide with the collimator, and thus provides control of the direction of the collimator's X-ray beam. These features allow you to scan step by step the X-ray beam produced and/or vary the scan speed, and/or vary the angular range of the scan, for example. Such an X-ray source can be described as being "controllable" or "airshipable" because its position (eg, in an anode; and/or relative to an aperture in a collimator) can be electronically controlled.
    [0031] A first mode of a collimator 200 is illustrated schematically by Figures 2A - 2H, and includes a first plate 210 and a second plate 220. The first plate 210 has a first face 210A and a second face 210B, and is opaque to the type of radiation for which the collimator 200 is designed. For example, if collimator 200 is designed to collimate X-rays, then the first plate 210 is opaque to X-rays.
    [0032] The first plate 210 includes an elongated opening 211 that extends completely between the first face 210A and the second face 210B for the purpose of passing radiation to which the first plate 210 is otherwise opaque. In this embodiment, the elongated opening 211 is rectangular in shape, but other shapes can be used in various embodiments.
    [0033] The collimator 200 also includes a second plate 220, which has a first face 220C and a second face 220D, and also has an elongated opening 221 that extends completely between the first face 220C and the second face 220D for the purpose of passing radiation to which the second plate 220 is otherwise opaque. In this embodiment, the elongated opening 221 is rectangular in shape, but other shapes can be used in various embodiments. When viewed as in Figures 2A and 2B, the openings 211 and 221 are at different angles.
    [0034] In the collimator 200, the first plate 210 and the second plate 220 are arranged parallel to each other, and separated by a gap "d" 240, as illustrated schematically in Figure 2C. The plates 210, 220 are arranged so that the elongated openings are arranged at an angle to each other, for example, so that a projection of the elongated opening 211 onto the elongated opening 221 forms an "X". In some embodiments, elongated opening 211 is arranged so that its projection in elongated opening 221 meets opening 221 at right angles (e.g., "+").
    [0035] In such configurations, the first plate 210 and the second plate 220 block all radiation 254 from anode 250, except that the first aperture 211 and the second aperture 221 cooperate to form a rhomboid aperture through which some radiation it can pass without contacting the first board 210 (which can be understood as an input board) and without contacting the second board 220 (which can be understood as an output board). More particularly, a projection of the first elongated opening 211 intersects the second elongated opening 221 at an angle other than zero, and so that the intersection of the projection of the first elongated opening 211 and the second elongated opening 221 forms a rhomboid opening through which the radiation can pass without contacting the input plate 210 and without contacting the output plate 220. In this way, all radiation incident on the input plate 210 is blocked, with the exception of the portion of incident radiation that passes through through the first elongated opening 211. All this radiation is blocked, in turn, by the second plate 220, with the exception of the portion of radiation that passes through the second elongated opening 221. In other words, all incident radiation is blocked by the collimator 200 , except for radiation approaching collimator 200 at an angle that aligns with both the first elongated opening 211 and the second elongated opening 221. Des If so, the first elongated opening 211 and the second elongated opening 221 can be described as forming a composite opening 270.
    [0036] The author of the present invention has found that the collimator 200 presents a useful feature, in that the composite aperture 270 formed by the cooperation of the first aperture 211 and the second aperture 221 exists at a variety of angles with respect to incident radiation. In other words, collimator 200 will present a composite aperture (ie, through collimator 200) to radiation approaching collimator 200 from various directions, all without having to move or manipulate the first plate 210 and/or the second plate 220. Consequently, a collimated beam of radiation 260 exits the collimator 200, and the direction of that collimated beam varies as a function of the position of the radiation source.
    [0037] More specifically, a source (which may be referred to as "a point of origin") of radiation 251 illuminates collimator 200 from any of a number of positions. For example, in Figure 2C, radiation source 250 is the focal point of an electron beam at anode 250. Radiation 254 comes from this point 251 at various angles, but only a part of that radiation, in this example, the radiation along vector 255A, approaches collimator 200 in a direction that goes allowing radiation to pass through both the first aperture 211 and the second aperture 221 to produce the collimated radiation beam 260A.
    [0038] The illustrative examples of the composite opening 270 formed by the cooperation of the openings 211 and 221 are illustrated schematically in figures 2D - 2H. In each figure, a collimated X-ray beam is formed from radiation falling through the projected rhomboid intersection of the two apertures 211; 221 (which can also be understood as grooves) as seen from the radiation origin 251. In Figure 2F, the beam angle is normal to the collimator plates 210, 220 (i.e., the angle α between the incident radiation vector (eg, 255B) and a vector normal to the surface 210A of plate 210 is equal to zero. ) and the composite aperture 270 (and hence the beam, for example, 260B) is square in shape. For reference purposes, a nonzero beam angle, α, between a vector 259 normal to the surface 210A of plate 210 and the beam vector 255A, is illustrated schematically in Figure 2C
    [0039] As the X-ray origin point 251 moves up or down, the beam angle α is modified and the height j (271; see, for example, figure 21) of the rhomboid aperture 270 is reduced as cos(α). At the same time, the aperture is displaced laterally by 0.5 d tg (α) where d 240 is the distance between the collimator plates.
    [0040] For example, as discussed above, when incident radiation is normal to the surface 210A of collimator 200, aperture 270 appears (from the point of radiation source) near the center of collimator 200. Alternatively, when incident radiation falls off approaches the surface 210A of the collimator 200 from another angle, the aperture appears (from the point of the radiation source) in a different position (eg, off-center), as in figures 2D, 2E, 2G, and 2H, for example. In this mode 200, if the beam angle varies between +45° and -45°, the lateral interval for the displacement of the opening must be equal to the distance between the plates d. In some embodiments, the path of the X-ray origin point can be adjusted to compensate for the lateral displacement of the aperture so as to maintain a straight scan line.
    [0041] Therefore, to control the collimated beam of radiation, the direction of the electron beam can be changed or manipulated, in ways known in the prior art, so that the focal point 251 of the electron beam can be moved to a position different at anode 250. Since focal point 251 is the source of the radiation that illuminates collimator 200, the radiation source is effectively manipulated in this way, and the radiation approaches collimator 200 from a different angle. For example, radiation focal point 251 can be moved to produce illuminating radiation along vector 255B or 255C. Of course, the position of the focal point can be moved step by step, or continuously, to produce radiation from various directions. Each position of focal point 241 therefore produces a collimated beam exiting collimator 200 at an angle that varies as a function of the position of focal point 251. For example, radiation along vector 255A produces collimated beam 260A; radiation along vector 255B produces collimated beam 260B; and radiation along vector 255C produces collimated beam 260C. In this way, the direction of a collimated beam of radiation can be electronically controlled, without physically moving or manipulating a structural element of the collimator, and without physically moving or manipulating a structural element of the radiation source.
    [0042] A virtual surface between the two slotted plates of the collimator, 210, 220, to which the X-ray beam is confined, has the shape of a hyperbolic paraboloid, as defined by the function z(x,y) = xy. Such virtual surface 300 is illustrated schematically in Figures 3A to 3C, where dark lines 301 indicate possible beam positions.
    [0043] An alternative embodiment 280 is illustrated schematically in Figures 2J and 2K, and includes a third plate, or intermediate plate, 230. Plate 230 has a first face 230E and a second face 230F, and is opaque to the type of radiation for to which the collimator 280 is designed. Intermediate plate 230 also has an opening 231, and is disposed between plates 210 and 220 so that virtual hyperbolic paraboloid surface 300 passes through opening 231, and thus forms a part of composite opening 270 and thereby , allow some radiation to pass through the collimator 280. Such a modality can increase the degree to which the collimator is opaque (ie, the opacity of the collimator), and can further refine the collimated beam. In some embodiments, for example a symmetrical design in which the angles of the slots for beam entry and exit are the same, a plate 230 in the center must have a horizontal slot 231.
    [0044] In another embodiment, a collimator 400 is formed not of multiple plates, but of two opposing blocks 401, 402, each with a hyperbolic paraboloid surface as illustrated schematically in figures 4A to 4C. In other words, such a modality includes two real, rather than virtual, surfaces between the entry and exit openings.
    [0045] Such a block 401 is illustrated schematically in Figure 4A, and shows the hyperbolic paraboloid surface 401A. Blocks 401, 402 cooperate to form an outlet opening 470, similar to composite opening 270 formed by plates 210 and 220 discussed above. In short, aperture 470 selectively lets radiation from a source through, depending on the angle at which the radiation impinges on collimator 400, so that the resulting collimated beam can be controlled by controlling the position of the radiation source. The apparent movement of such an opening 470 is schematically illustrated by the different positions of the opening 470 in Figure 4B and in Figure 4C.
    [0046] Figures 5A to 5E schematically illustrate an embodiment of helical-cut cylindrical collimator 500. In general, this embodiment 500 is a variable angle collimator consisting of a right circular cylinder 501 with a cylinder axis 503 and a groove 502. Groove 502 completely traverses cylinder 501 and spirals along axis 503.
    [0047] A cross-sectional view of an embodiment of the collimator 500 is illustrated schematically in Figure 5B, and shows the enclosing surface 501B. Enclosing surface 501B and cylinder surface 501C define the edges of groove 501D. In some embodiments, each edge of slot 501D defines a helix about the axis of cylinder 503. Thus, enclosing surface 501B, which is the surface between helical edges 501D, can be described as "a helical surface". Surface 501A is also a helical surface, and thus groove 502 can be described as "a helical groove". In other words, slot 502 has a helical shape, so that the boundary surfaces 501A, 501B of slot 502 form (or are transposed by) a double helix, as illustrated schematically in Figure 5A.
    [0048] In one embodiment, slot 502 at radius 504 of cylinder 501 (i.e., on surface 501C of cylinder 501) forms an angle 520 of 45° with the direction of axis 503 of cylinder 501, resulting in the square-shaped opening 510. See, for example, slot 502 in figure 5D.
    [0049] In some embodiments, slot 502 has a constant width 502A, which produces an angle-independent beam cross section. For example, opening 510 retains a square shape from a variety of angles, as illustrated schematically in Figures 5C to 5E.
    [0050] In another embodiment 600, schematically illustrated in figures 6A to 6C, the height h 605 of the span 604 between the two surfaces 601A, 602A of two opposing blocks 601A, 602A that form the spiral groove of the collimator 603 is not constant such as in mode 400 in Figures 4A to 4C, for example. Instead, the height h 605 of span 604 increases as the secant of beam angle α: h α sec(α) = 1/cos(α)
    [0051] In this way, an X-ray beam with constant cross-sectional area is independent of the beam angle that the hyperbolic paraboloid surface is maintained, because the square, or nearly square, cross section of the beam is maintained.
    [0052] Depending only on the angle-dependent height to modify the spiral groove of the collimator 603 leads to surfaces defined by:

    [0053] These surfaces maintain a constant height h of the beam cross section; however, the square shape obtained for α = 0 (where α = 0 is an angle normal to the collimator surface) is lost with increasing angle α. To maintain a square or nearly square cross section of the beam, the slope of the grooves on the collimator entry and exit surfaces will have to increase as the beam angle increases. Thus, the central surface of the groove will no longer be given by z(x, y) = x^y, but by: z(x, y)=x^sin h (y)
    [0054] or an approximation thereof. With the height given by 1 _ ya, the opening will maintain a square shape, but will be reduced in size with increasing angle. A height given by cos h(y) maintains a constant cross-sectional area.
    [0055] The central surface (h = 0) will remain linear at x because this is the direction of the straight beam. An example of the modified hyperbolic paraboloid surface is shown in Figures 6A to 6C. Figures 6B and 6C schematically illustrate a collimator 600 formed by two opposing blocks 601, 602, which form the outlet opening 670.
    [0056] The modification of the hyperbolic paraboloid surfaces of the collimator not only allows to obtain a beam cross-sectional area independent of the beam angle, but also allows the deliberate variation of the cross-sectional area as a function of the beam angle. Keeping the cross-sectional area of the beam constant is just a special case of area control. Controlling the cross-sectional area of the beam as a function of the beam angle allows designs with modulated beam shapes and the dose ratio (flow) delivered by the collimated beam. In various embodiments, the contours of an aperture in a collimator can be configured to produce a beam cross section in a variety of shapes, such as rhomboid (eg, rhomboid aperture 270 of Figure 2I), rectangular, or square (eg, square opening 10 of Fig. 5C), or even diamond-shaped (eg opening 299 of Fig. 2L), to mention just a few examples. In general, the aperture of a collimator can be configured to produce a beam in a size and shape (in cross section) in a way that a system designer finds beneficial to the application for which the system is designed.
    [0057] Compared to a tiny hole collimator, various modalities can produce an increased dispersion which can be reduced by increasing the thickness of the collimator (eg 400 collimator) or, more effectively, by adding one or more additional secondary plates in the collimator output side. Such embodiment 700 is illustrated schematically in Figure 7, and includes a plate 701 adjacent to collimator 702. Collimator 702 can be any of the collimators described above in connection with Figures 2A to 6C, for example. The slot in plate 701 includes an opening 703 arranged to clear the path of primary beam 710 exiting collimator 702.
    [0058] A system for producing a collimated beam of radiation can be described as having a radiation source, and a collimator according to one of the modalities described above, and circuitry for controlling the radiation source so as to control the angle in which radiation from the source impinges on the collimator. A method of producing a controllable collimated radiation beam may include providing a collimator in accordance with one of the modalities described above, and then illuminating the collimator with radiation from the radiation source at a variety of angles to control the angle. of the collimated beam leaving the collimator.
    [0059] Some embodiments provide a variable angle collimator that includes an entry plate having a first face and a second face, and a first elongated opening that completely traverses the entry plate between the first face and the second face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, the first face parallel to the fourth face, and separated from the fourth face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero and so that the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which radiation can pass without contacting the input board and without contacting the output board.
    [0060] In some embodiments, the nonzero angle is a right angle.
    [0061] Some arrangements also include an intermediate plate that has a third opening that completely traverses the intermediate plate. The intermediate plate is disposed between the input plate and the output plate, so that the third opening lines up with the first elongated opening and the second elongated opening at a plurality of angles, so that the first elongated opening, the second The elongated opening and the third opening form a rhomboid-shaped opening (or an opening of other polygonal shape) through which radiation can pass without contacting any of the inlet plate, outlet plate or intermediate plate. In some embodiments, the third opening is an elongated opening, and in some embodiments, the third opening is a rectangular opening.
    [0062] Another embodiment of variable angle collimator includes a first member that has a first surface, which first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface, and a second member that also has a first, first surface which surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface. The first member is disposed relative to the second member such that the first surface opposes the second surface, and is separated from the second surface by a gap, so as to define a hyperbolic paraboloid opening across the collimator.
    [0063] In some embodiments, the first surface is a modified hyperbolic paraboloid surface and the second surface is a modified hyperbolic paraboloid surface, so the gap between the first surface and the second surface is not constant.
    [0064] In another embodiment, a radiation scanning system includes a radiation source configured to controllably provide a beam of radiation at a plurality of angles, and a collimator having a hyperbolic paraboloid aperture with an input and an output . In some embodiments, the collimator includes an entrance plate that has a first face and a second face, and a first elongated opening that completely traverses the entrance plate between the first face and the second face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, the first face parallel to the fourth face, and separated from the fourth face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, so that the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which radiation from the The radiation source can pass, at a plurality of angles, without contacting the input plate and without contacting the output plate.
    [0065] In some embodiments, the collimator includes a first member that has a first surface, wherein that first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface, and a second member that has a second surface, wherein the second surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface. The first member is disposed relative to the second member such that the first surface is opposed to the second surface, and is separated from the second surface by a gap so as to define a hyperbolic paraboloid opening across the collimator.
    [0066] A method for irradiating a target with a collimated beam of radiation includes providing a collimator having a hyperbolic paraboloid aperture with an input and an output; illuminating the entrance of the hyperbolic paraboloid aperture with illumination radiation from a first illumination angle such that a portion of the illumination radiation passes through the collimator and exits the collimator through the fourth surface at a first exit angle; illuminating the entrance of the hyperbolic paraboloid aperture with illumination radiation from a second illumination angle, so that a portion of the illumination radiation passes through the collimator and exits the collimator through the fourth surface at a second exit angle, the second exit angle being different from the first exit angle.
    [0067] In some embodiments, the provision of a collimator includes the provision of a collimator having an input plate with a first face and a second face, and a first elongated opening that completely traverses the input plate between the first face and the second face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, the first face parallel to the fourth face, and separated from the fourth face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, and the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which radiation can pass without contacting the input board and not contacting the output board.
    [0068] In some embodiments, providing a collimator includes providing a collimator that has a first member that has a first surface, wherein that first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; a second member having a second surface, second surface that is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; the first member being disposed relative to the second member such that the first surface opposes the second surface, and is separated from the second surface by a gap to define a hyperbolic paraboloid opening across the collimator.
    [0069] In another embodiment, a variable angle collimator is provided that has a cylindrical casing, which casing has a cylindrical surface and an axis, and comprises a helical groove that completely traverses the casing, wherein the helical groove defines a first enclosing surface and a second enclosing surface, with the first enclosing surface separated from the second enclosing surface by a gap. In some embodiments, the gap is at a constant distance between the first enclosing surface and the second enclosing surface on the cylindrical surface.
    [0077] Definitions. As used in this description and the appended claims, the following terms shall have the meanings indicated, unless the context otherwise requires:
    [0078] A hyperbolic paraboloid surface is a surface defined by the following formula, where z is the height of the gap between opposing surfaces that define an opening, and x and y are coordinates on orthogonal axes in a normal plane az:

    [0079] In some embodiments, a hyperbolic paraboloid surface is defined by the following form of the above formula:
    [0080] A modified hyperbolic paraboloid surface is a modified hyperbolic paraboloid surface as described in relation to Figure 7.
    [0081] A hyperbolic paraboloid opening is a passage through a collimator, which passage has at least one contour in the form of a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface.
    [0082] Various embodiments of the present invention can be characterized by the potential claims listed in the paragraphs that follow this paragraph (and before the actual claims provided at the end of this application). These potential claims form a part of the written description of this patent application. Accordingly, the subject matter of the following potential claims may be presented as actual claims in subsequent proceedings involving this patent application or any application claiming priority based on this application. The inclusion of these potential claims should not be interpreted to mean that the actual claims do not cover the subject matter of the potential claims. Thus, a decision not to present these potential claims in later proceedings should not be interpreted as a donation of the object to the public.
    [0070] Without limitation, the potential object that can be claimed (preceded by the letter "P" to avoid confusion with the actual claims presented below) includes:
    [0071] P1. A variable angle collimator comprising: an inlet plate having a first face and a second face, and a first elongated opening which completely traverses the inlet plate between the first face and the second face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, the first face parallel to the fourth face, and separated from the fourth face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, and thus the intersection of the projection of the first elongated opening with the second elongated opening forms a rhomboid opening through which radiation can pass. without contacting the input board and without contacting the output board.
    [0072] P2. The variable-angle collimator of potential claim P1, where the nonzero angle is a right angle.
    [0073] P3. The variable angle collimator of potential claim P1, further comprising an intermediate plate having a third opening that completely traverses the intermediate plate, with the intermediate plate disposed between the input plate and the output plate so that the third opening aligns with the first elongated opening and the second elongated opening at a plurality of angles, and that the first elongated opening and the second elongated opening and the third opening form a rhomboid opening through which radiation can pass without contacting any between the input board, the output board or the intermediate board.
    [0074] P4. The variable angle collimator of potential claim P3, wherein the third opening is an elongated opening.
    [0075] P5. The variable-angle collimator of potential claim P3, wherein the third opening is a rectangular opening.
    [0076] P6. A variable angle collimator which comprises: a first member having a first surface, which first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; a second member comprising a second surface, which is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; wherein the first member is disposed relative to the second member such that the first face of the surface opposes the second surface, and the first surface and second surface are separated by a gap to define a hyperbolic paraboloid opening spanning the collimator.
    [0077] P7. The variable angle collimator according to potential claim P6, wherein the first surface is a modified hyperbolic paraboloid surface and the second surface is a modified hyperbolic paraboloid surface, so that the gap between the first surface and the second surface it is not constant.
    [0078] P11. A radiation scanning system comprising: a radiation source configured to controllably provide a beam of radiation at a plurality of angles; a collimator comprising a hyperbolic paraboloid aperture having an input and an output.
    [0079] P12. The radiation scanning system of potential claim P11, wherein the collimator comprises: an inlet plate having a first face and a second face, and a first elongated aperture that completely traverses the inlet plate between the first and second face face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, wherein the first face is parallel to the fourth face, and separate from the fourth face. face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, so that the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which radiation from the radiation source, at a plurality of angles, can pass without contacting the input plate and without contacting the output plate.
    [0080] P13. The radiation scanning system of potential claim P11, wherein the collimator comprises: a first member comprising a first surface, wherein the first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; a second member comprising a second surface, wherein the second surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; the first member is disposed with respect to the second member such that the first surface face opposes the second surface, the first surface and the second surface are separated by a gap to define a hyperbolic paraboloid opening passing through the collimator.
    [0081] P21. A method of irradiating a target with a collimated beam of radiation, the method comprising: providing a collimator comprising a hyperbolic paraboloid aperture having an input and an output; illuminating the entrance of the hyperbolic paraboloid aperture with illumination radiation from a first illumination angle so that a portion of the illumination radiation passes through the collimator and exits the collimator through the fourth surface at a first exit angle; the inlet illumination of the hyperbolic paraboloid aperture with illumination radiation from a second illumination angle, so that a portion of the illumination radiation passes through the collimator and exits the collimator through the fourth surface at a second exit angle, being that the second exit angle is different from the first exit angle.
    [0082] P22. The method for irradiating a target with a collimated radiation beam according to potential claim P21, wherein providing a collimator includes providing a collimator having: an input plate having a first face and a second face, and a first elongated opening which completely traverses the inlet plate between the first face and the second face; an outlet plate having a third face and a fourth face, and a second elongated opening which completely traverses the outlet plate between the third face and fourth face, with the first face parallel to the fourth face, and separated from the fourth face by a predetermined distance, so that a projection of the first elongated opening intersects the second elongated opening at an angle other than zero, and so that the intersection of the projection of the first elongated opening and the second elongated opening forms a rhomboid opening through which the radiation can pass without contacting the inlet plate and without contacting the output plate.
    [0083] P23. The method of irradiating a target with a collimated radiation beam according to potential claim P21, wherein providing a collimator includes providing a collimator having: a first member comprising a first surface, wherein the first surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; a second member comprising a second surface, wherein the second surface is a hyperbolic paraboloid surface or a modified hyperbolic paraboloid surface; the first member is disposed with respect to the second member such that the first surface face opposes the second surface, and the first surface and second surface are separated by a gap to define a hyperbolic paraboloid opening passing through the collimator.
    [0084] P31. A variable angle collimator comprising: a cylindrical shell, which shell has a cylindrical surface and an axis, and comprises a helical groove which completely traverses the shell, wherein the helical groove has a first boundary surface and a second boundary surface, where the first bounding surface is separated from the second bounding surface by a gap.
    [0085] P32. The potential variable angle collimator of claim P31, wherein the span is at a constant distance between the first boundary surface and the second boundary surface on the cylindrical surface.
    [0086] The embodiments of the invention described above should be merely examples; numerous variations and modifications will be apparent to those skilled in the art. All such variations and modifications are intended to be within the scope of the present invention as defined in any of the appended claims.
    权利要求:
    Claims (16)
    [0001]
    1. A system for producing a steerable radiation pencil beam characterized in that it comprises: a radiation source configured to produce radiation at an angle, with respect to a collimator, wherein the angle is electronically controllable; and a collimator (200, 400, 500) comprising material opaque to radiation produced by the radiation source, wherein the collimator (200, 400, 500) comprises a spiral collimator slot configured to receive radiation from the radiation source to a plurality of incident angles and configured to pass a portion of the radiation through the collimator (200, 400, 500) at each angle of the plurality of incident angles, so as to form a collimated pencil-beam of radiation having a cross-section of the beam, wherein the collimator (200, 400, 500) and the radiation source are configured to remain stationary with respect to each other when producing the steerable pencil beam of radiation.
    [0002]
    2. System according to claim 1, characterized in that the radiation source comprises an electron source and an anode, in which the electron source is configured to illuminate the anode with a drivable beam of electrons, so to produce a mobile radiation source point.
    [0003]
    3. System according to claim 1, characterized in that the opening has a rhomboid shape.
    [0004]
    4. System according to claim 1, characterized in that the opening has a square shape.
    [0005]
    5. System according to claim 1, characterized in that the shape of the opening is variable as a function of the incident angle of radiation in relation to the opening.
    [0006]
    6. System according to claim 1, characterized in that the collimator (200, 400, 500) comprises: a first member comprising a first delimiting surface; and a second member comprising a second bounding surface; the first member is disposed relative to the second member such that the first enclosing surface faces the second enclosing surface, the first enclosing surface and the second enclosing surface separated by a gap to define the spiral groove of the collimator through the collimator (200, 400, 500).
    [0007]
    7. System according to claim 6, characterized in that the gap between the first boundary surface and the second boundary surface is not constant.
    [0008]
    8. System according to claim 6, characterized in that the collimator (200, 400, 500) is a helically cut cylinder.
    [0009]
    9. A method of irradiating a target with a collimated radiation pencil beam, characterized in that it comprises: providing a drivable radiation source configured to illuminate a collimator (200, 400, 500); providing a collimator (200, 400, 500) comprising a spiral collimator slot having an input and an output, the collimator (200, 400, 500) disposed in a fixed position relative to the drivable radiation source; produce a pencil beam of radiation collimated at a plurality of output angles by: illuminating the collimator spiral slot inlet with illuminating radiation from a first illuminating angle so that a portion of the illuminating radiation passes through the collimator (200, 400, 500) and exiting the collimator (200, 400, 500) at a first exit angle; and illuminating the collimator spiral slot inlet with illumination radiation from a second illumination angle, the second illumination angle different from the first illumination angle, so that a portion of the illumination radiation passes through the collimator (200, 400 , 500) and exit the collimator (200, 400, 500) at a second exit angle, with the second exit angle different from the first exit angle, so that the radiation exiting the collimator (200, 400, 500) at the first take-off angle and the second take-off angle radiate the target.
    [0010]
    10. Method of irradiating a target with a collimated radiation pencil beam, according to claim 9, characterized in that providing a collimator (200, 400, 500) includes providing a collimator (200, 400, 500) having: a first member comprising a first bounding surface; and a second member comprising a second bounding surface; the first member is arranged with respect to the second member such that the first enclosing surface faces the second enclosing surface, the first enclosing surface and the second enclosing surface separated by a gap to define a spiral collimator groove passing through the collimator (200, 400, 500).
    [0011]
    11. Method of irradiating a target with a collimated radiation pencil beam, according to claim 9, characterized in that the collimated pencil beam leaving the collimator (200, 400, 500) at the first exit angle it has a first cross-sectional shape, and the collimated pencil beam exiting the collimator (200, 400, 500) at the second exit angle has a second cross-sectional shape, with the second shape different from the first shape.
    [0012]
    12. A system for producing a steerable radiation pencil beam characterized in that it comprises: a radiation source means for producing a point source of electronically steerable illumination radiation; and a collimation means having a spiral collimator slot configured to pass a portion of the illuminating radiation incident on said collimation means; the radiation source means arranged, with respect to the collimation means, to remain stationary with respect to the collimation means, and to illuminate the spiral groove of the collimator with incident radiation from the steerable radiation point source, so that the spiral groove of the collimator produces a pencil beam of drivable radiation.
    [0013]
    13. System according to claim 12, characterized in that the collimation means comprises: a first member comprising a first delimiting surface; and a second member comprising a second bounding surface; wherein the first member is arranged, with respect to the second member, such that the first enclosing surface is disposed opposite the second enclosing surface such that the first enclosing surface is separated from the second enclosing surface by a gap, so that the first member and second member form the spiral groove of the collimator through the span.
    [0014]
    14. System according to claim 12, characterized in that the collimation means comprises: a first member comprising a first delimiting surface; and a second member comprising a second bounding surface; wherein the first member is arranged, with respect to the second member, such that the first enclosing surface is arranged opposite the second enclosing surface such that the first enclosing surface is separated from the second enclosing surface by a span, wherein the span it is not constant, so that the first member and the second member form the spiral groove of the collimator across the gap.
    [0015]
    15. System according to claim 14, characterized in that the collimation means comprises a helically cut cylinder.
    [0016]
    16. System according to claim 12, characterized in that the means of the radiation source comprises an electron source and an anode, in which the electron source is configured to illuminate the anode with a drivable electron beam.
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    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US3780291A|1971-07-07|1973-12-18|American Science & Eng Inc|Radiant energy imaging with scanning pencil beam|
    US4079259A|1973-07-18|1978-03-14|Blum Alvin S|Tomographic apparatus and method|
    US3894234A|1974-01-28|1975-07-08|Us Navy|Radial scanner|
    US4031401A|1975-03-14|1977-06-21|American Science & Engineering, Inc.|Radiant energy imaging scanning|
    US4045672A|1975-09-11|1977-08-30|Nihon Denshi Kabushiki Kaisha|Apparatus for tomography comprising a pin hole for forming a microbeam of x-rays|
    JPS5423237B2|1975-09-11|1979-08-11|
    US4419585A|1981-02-26|1983-12-06|Massachusetts General Hospital|Variable angle slant hole collimator|
    US4433427A|1982-01-26|1984-02-21|Elscint, Inc.|Method and apparatus for examining a body by means of penetrating radiation such as X-rays|
    GB2170980B|1985-02-07|1988-05-25|Steve Webb|Ct scanner and detector therefor|
    DE3829688A1|1988-09-01|1990-03-15|Philips Patentverwaltung|ARRANGEMENT FOR GENERATING A X-RAY OR GAMMA RAY WITH A SMALL SECTION AND CHANGING DIRECTION|
    DE3908966A1|1989-03-18|1990-09-20|Philips Patentverwaltung|ARRANGEMENT FOR GENERATING A X-RAY OR Gamma RAY WITH A SMALL SECTION AND CHANGEABLE LOCATION|
    JPH06237927A|1993-02-15|1994-08-30|Hitachi Medical Corp|Radiographic device|
    US5493596A|1993-11-03|1996-02-20|Annis; Martin|High-energy X-ray inspection system|
    GB2295266A|1994-11-21|1996-05-22|Secr Defence|X-ray generator|
    EP1206903A2|1999-07-30|2002-05-22|American Science & Engineering, Inc.|Method for raster scanning an x-ray tube focal spot|
    DE60035876T2|2000-09-27|2008-05-08|Euratom|Micro-beam collimator for high-resolution X-ray diffraction analysis using conventional diffractometers|
    US6735271B1|2000-11-28|2004-05-11|Ge Medical Systems Global Technology Company Llc|Electron beam computed tomographic scanner system with helical or tilted target, collimator, and detector components to eliminate cone beam error and to scan continuously moving objects|
    US6792077B2|2002-06-19|2004-09-14|Ge Medical Systems Global Technology Company, Llc|Collimation system for dual slice EBT scanner|
    CN1603946A|2003-09-29|2005-04-06|Ge医疗系统环球技术有限公司|X-ray orifice, X-ray irradiation machine and X-ray apparatus|
    JP2007534415A|2004-04-28|2007-11-29|コーニンクレッカフィリップスエレクトロニクスエヌヴィ|3D electron beam computed tomography|
    DE102005011467B4|2005-03-12|2008-02-28|Smiths Heimann Gmbh|Adjustable focal length collimator, directed method and X-ray inspection system|
    DE102005029674B4|2005-06-20|2008-08-21|BAM Bundesanstalt für Materialforschung und -prüfung|Diaphragm for an imaging device limits high-energy radiation from a radiation source so as to orientate it along an optical axis towards an imaging area based on a pin camera principle|
    WO2007023487A2|2005-08-26|2007-03-01|Camtek Ltd.|Device and method for controlling an angular coverage of a light beam|
    DE102006006840A1|2006-02-14|2007-08-23|Siemens Ag|X-ray computer tomograph with light beam-controlled X-ray source|
    CN101689466B|2007-06-21|2014-06-04|皇家飞利浦电子股份有限公司|Fast dose modulation using z-deflection in a rotaring anode or rotaring frame tube|
    JP5184251B2|2007-08-07|2013-04-17|富士フイルム株式会社|Spectroscopic element, spectroscopic device, and spectroscopic method|
    US7916300B2|2007-08-07|2011-03-29|Fujifilm Corporation|Spectroscopy device, spectroscopy apparatus and spectroscopy method|
    DE102008025109B4|2008-05-22|2010-06-17|BAM Bundesanstalt für Materialforschung und -prüfung|Aperture for an imaging device|
    CN201285377Y|2008-08-05|2009-08-05|同方威视技术股份有限公司|Radiation beam scanning apparatus for back scattering imaging|
    RU2405438C1|2009-07-27|2010-12-10|Общество с ограниченной ответственностью "С.П.ГЕЛПИК"|X-ray installation for medical diagnostics|
    US8315428B2|2009-10-22|2012-11-20|Siemens Medical Solutions Usa, Inc.|Automatic line identification and pairing for nuclear imaging collimator vector map characterization|
    DE102009052627B4|2009-11-10|2012-07-12|Siemens Aktiengesellschaft|A scattered radiation collimator and method of making a scattered radiation collimator|
    EP2333786B1|2009-12-08|2012-02-15|BAM Bundesanstalt für Materialforschung und -prüfung|Asymmetric slit diaphragm and device and method for producing same|
    CN102116747B|2009-12-30|2014-04-30|同方威视技术股份有限公司|Scanning device for ray bundle for backscatter imaging-used ray bundle and method|
    PL2548207T3|2010-03-14|2020-07-13|Rapiscan Systems, Inc.|Beam forming apparatus|
    US9117564B2|2012-07-05|2015-08-25|American Science And Engineering, Inc.|Variable angle collimator|US9958569B2|2002-07-23|2018-05-01|Rapiscan Systems, Inc.|Mobile imaging system and method for detection of contraband|
    US9117564B2|2012-07-05|2015-08-25|American Science And Engineering, Inc.|Variable angle collimator|
    EP3043864A4|2013-09-11|2017-07-26|The Board of Trustees of The Leland Stanford Junior University|Methods and systems for beam intensity-modulation to facilitate rapid radiation therapies|
    WO2015102681A2|2013-09-11|2015-07-09|The Board Of Trustees Of The Leland Stanford Junior University|Methods and systems for rf power generation and distribution to facilitate rapid radiation therapies|
    US11266006B2|2014-05-16|2022-03-01|American Science And Engineering, Inc.|Method and system for timing the injections of electron beams in a multi-energy x-ray cargo inspection system|
    WO2015175751A1|2014-05-16|2015-11-19|American Science And Engineering, Inc.|Source for intra-pulse multi-energy x-ray cargo inspection|
    US10228487B2|2014-06-30|2019-03-12|American Science And Engineering, Inc.|Rapidly relocatable modular cargo container scanner|
    EP3248207A4|2015-01-20|2018-09-26|American Science & Engineering, Inc.|Dynamically adjustable focal spot|
    DE102015008272A1|2015-06-18|2016-12-22|Kurt Osterloh|Slit diaphragm system for hard radiation imaging|
    GB201515666D0|2015-09-04|2015-10-21|Secr Defence|Scanning beam collinator|
    MX2018003016A|2015-09-10|2018-08-01|American Science & Eng Inc|Backscatter characterization using interlinearly adaptive electromagnetic x-ray scanning.|
    DE102016004624A1|2016-04-13|2017-10-19|Kurt Osterloh|The gamma eye: A device for imaging high-energy objects|
    KR101772324B1|2016-04-18|2017-08-28|고려대학교 산학협력단|Variable pin-hole collimator and radiation imaging device using the same|
    GB2572700A|2016-09-30|2019-10-09|American Science & Eng Inc|X-Ray source for 2D scanning beam imaging|
    CN110199373B|2017-01-31|2021-09-28|拉皮斯坎系统股份有限公司|High power X-ray source and method of operation|
    CN107966460A|2017-12-26|2018-04-27|清华大学|Radiation checking system and radiation testing method|
    GB2590561B|2018-06-20|2021-12-08|American Science & Eng Inc|Wavelength-shifting sheet-coupled scintillation detectors|
    CN109659061B|2018-12-27|2020-06-23|中国原子能科学研究院|Neutron collimator structure with continuously adjustable divergence angle and calibration method thereof|
    WO2021094591A1|2019-11-14|2021-05-20|Kurt Osterloh|Imaging ray-optical system|
    US11193898B1|2020-06-01|2021-12-07|American Science And Engineering, Inc.|Systems and methods for controlling image contrast in an X-ray system|
    US11175245B1|2020-06-15|2021-11-16|American Science And Engineering, Inc.|Scatter X-ray imaging with adaptive scanning beam intensity|
    法律状态:
    2018-12-04| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
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    优先权:
    申请号 | 申请日 | 专利标题
    US201261668268P| true| 2012-07-05|2012-07-05|
    US61/668,268|2012-07-05|
    PCT/US2013/049098|WO2014008275A1|2012-07-05|2013-07-02|Variable angle collimator|
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