JP5339325B2 - X-ray generator and X-ray generation method - Google Patents

Description

  The present invention relates to an electron accelerator, and more particularly to an X-ray generator equipped with an electron accelerator used for an X-ray generator or the like.

  Conventionally, a nondestructive inspection apparatus using laser Compton scattering is known (see Patent Document 1). Laser Compton scattering is a highly directional electromagnetic wave generation process that occurs by irradiating a laser to electrons accelerated to high energy using an accelerator such as an electron linear accelerator or storage ring. Select the energy of the electron and the wavelength of the laser. By doing so, X-rays of various energies can be generated, and at the same time, the energy spread can be set to a so-called quasi-monochromatic state of about several percent (see Non-Patent Document 1).

  Laser Compton scattered X-rays using electron storage rings, linear accelerators, and high-intensity lasers are used for medical and industrial radiography, research on photonuclear reactions, and the like (see Non-Patent Documents 2 to 4). The X-ray mentioned here is defined as a broad term including photons in a high energy γ-ray region of several MeV or more.

  In research on medical and industrial radiography, low-exposure and high-quality imaging studies that take advantage of the monochromaticity of X-rays are being conducted. However, it is important to use high-energy monochromatic X-ray beams (Non-Patent Documents 5 to 5). 6). In order to increase the intensity and energy of generated X-rays, it is common to irradiate an electron beam with a laser beam at a position where the beam diameter is minimum, such as an electron converging point of an electron accelerator or a long straight line portion with small energy dispersion.

  The generated X-ray beam is passed through a lead block (collimator) provided with a through hole to make it a thin beam, and it is made quasi-monochromatic by limiting the scattering angle. As a result, a high-energy X-ray beam utilizing laser Compton scattering inevitably becomes a thin beam having a diameter of several mm to several cm.

  As shown in Equation 1 below, the laser Compton scattering determines the upper limit of the X-ray energy after the collision depending on the angle between the laser and the electron beam before the collision, and the X-ray with the highest energy in the traveling direction of the electron beam. Released.

  For this reason, usually, the collimator is placed on the extension of the electron beam trajectory to limit the solid angle, thereby extracting the portion including the X-ray beam with the highest energy and the highest X-ray flux intensity. For example, when an electron beam having an energy of 760 MeV is irradiated with a laser beam having a wavelength of 532 nm, it can be calculated from Equation 1 that X-rays having an energy of 20 MeV at the maximum are generated.

Here, E _γ , E ₀ , and E _e are the energy of laser Compton X-ray, laser, and electron, respectively, β is the ratio of electron velocity to light velocity, and θ ₁ and θ ₂ are the angles formed by the laser and the electron beam, respectively. , And the angle formed by the scattered X-rays and the electron beam. Usually, to obtain the highest energy and yield, θ ₁ is an angle close to 180 degrees, and θ ₂ is an angle close to 0 degrees.

FIG. 1 shows an energy spectrum measured by a NaI (Tl) scintillation detector. By arranging a lead collimator having an inner diameter of 2 mm and a length of 20 cm at the center of the beam axis, an X-ray having an energy width of about 5% was extracted from the maximum energy. The resolution of the detector is about 10%.
Spatial resolution and density using a laser Compton X-ray beam focused to about 1 mm and a CT stage that moves and scans the object to be inspected at high speed, using the high transmission and directivity of the Laser Compton X-ray beam An industrial non-destructive inspection apparatus using a first generation CT capable of performing high-precision inspection with a resolution of 1 mm or less and 3% respectively has been developed (see Non-Patent Document 7). The spatial resolution is 1 mm or less.

JP 2002-162371 A R. H. Milburn, Phys. Rev. Lett. 10 (3) 75-77 (1963). S. Goko et al, Phys. Rev. Lett., 96-192501, 1-4 (2006). H. Utsunomiya et al, Nuclear Physics A, 738 (28), 136-142 (2004). K. Y. Hara et al, Phys. Rev. D68, 072001-1-072001-6 (2003). H. Toyokawa, Nucl. Instrum. And Methods in Phys. Res. A545, 469-474 (2005). H. Toyokawa et al, Rev. Sci. Instrum., 73 (9), 3358-3362 (2002). H. Toyokawa et al, Proceedings of the 5th World Congress on Industrial Process Tomography, 2007, Bergen, Norway, in press.

  The biggest problem in the industrial nondestructive inspection method using laser Compton scattering is that the radiation field is small because the directivity of the X-ray beam is very high. When calculated from the above formula 1, approximately 80% of X-rays are emitted in the range of 1.5 mrad under the conditions of FIG. 1 (electron energy 760 MeV, laser wavelength). That is, even at a position of 5 m from the light source, it spreads only about 15 to 20 mm, and it is difficult to ensure wide irradiation.

  In such a high X-ray energy region, a one-dimensional or two-dimensional imaging detector that measures a transmission image of an irradiation field of several centimeters with sufficiently high resolution and detection efficiency has not been developed, and laser Compton scattering is used. In the conventional CT, a first-generation apparatus is inevitably employed in which an object to be inspected is placed on a stage that repeats parallel movement and rotation, and a transmission image is obtained by a finely focused X-ray beam.

  In order to achieve higher spatial resolution, it is common to collimate the beam finer. However, since the X-ray beam intensity decreases in proportion to the area of the collimator, there is a drawback that the time required for CT measurement is drastically increased.

  For example, in order to achieve a half spatial resolution for a measurement that yields the same statistics or image quality noise level as a measurement with a spatial resolution of 1 mm, it is necessary to halve the collimator diameter and halve the rotation angle pitch. .

  Furthermore, since the X-ray beam intensity is about 25%, the measurement time is simply estimated to be 16 times as a result. This was a major problem with the first generation CT apparatus.

  In order to solve this problem, it is conceivable to improve the CT apparatus to the second generation or the third generation. For this purpose, it is essential that the quasi-monochromatic, high-energy, and high-intensity X-ray beam of about 10 MeV is used as a fan beam so as to cover the object to be inspected widely. However, for this purpose, there has been no suitable quasi-monochromatic, high energy and high intensity X-ray beam.

  An X-ray generator using a small electron accelerator will be described for comparison with the present invention. Although X-ray energy generated from an X-ray generator using a small electron accelerator is low and the energy spread is large, it is widely used for non-destructive inspection because of its advantage of high intensity and spatial resolution.

  When an electron beam accelerated to about 10 MeV is irradiated onto a metal target such as tantalum, tungsten, or copper, high-energy bremsstrahlung X-rays having an average of several hundred keV to several MeV can be generated with an angular spread of several hundred mrad.

  However, since bremsstrahlung X-rays have a wide energy spread and a white spectrum, it is difficult to achieve high density resolution.

  In addition, characteristic X-rays with good monochromaticity are generated at the same time as bremsstrahlung X-rays, but even for extremely heavy elements such as lead with atomic number 82, the characteristic X-ray energy is 160 keV at the maximum, and the viewpoint of transmission power Therefore, it is difficult to use for high-precision nondestructive inspection requiring about 10 to 10 MeV.

  An object of the present invention is to solve the above-described conventional problems, and an object of the present invention is to realize an apparatus and an electron accelerator that generate a quasi-monochromatic and high-energy X-ray fan beam.

  In order to solve the above-described problems, the present invention provides an X-ray including an electron accelerator that performs orbital modulation by applying vertical or horizontal deflection to an electron trajectory using a deflecting magnet that can switch the direction of a magnetic field at high speed. In the generator, by applying the deflection, a node which is a spatially constant point is formed at an arbitrary position downstream of the point in the electron trajectory to which the deflection is applied, and the laser is focused on the position. X-ray beam can be generated by laser Compton scattering, and the direction of the X-ray beam can be switched or modulated by switching or modulating the magnetic field direction of the deflecting magnet and switching or modulating only the angle of the electron trajectory. An X-ray generator provided with an electron accelerator is provided.

  The electron trajectory may be a circular trajectory such as an electron storage ring.

  The electron trajectory may be an electron linear accelerator.

  By switching only the angle of the electron trajectory at the node, the laser Compton X-ray beam is modulated at high speed to generate a pseudo fan-type X-ray beam used in non-destructive inspection, medical radiography, or CT apparatus. Also good.

According to the present invention, the following effects are produced.
(1) Measurements that have been performed with the first generation high-energy X-ray CT apparatus can be performed in a very short time. Specifically, when performing CT measurement of an object to be inspected having a diameter of 100 mm with a resolution of 1 mm and sufficiently low image noise, the first generation requires 5 to 6 hours. The CT can be obtained in about 300 seconds, so that it can be sufficiently put into practical use and is expected to be an important means in industrial nondestructive inspection.
(2) It is possible to use a laser Compton X-ray beam that has been conventionally used as a thin beam having a diameter of several mm to several cm in a large irradiation field.
(3) In principle, any energy X-ray beam can be fan-shaped, which is very useful when examining radiation imaging and detector responses that require large-area X-ray and γ-ray irradiation. Useful.
(4) This is expected to contribute to fields such as nuclear and elementary particle experiments, nondestructive inspection, medical imaging, and radiation measurement.
(5) It is possible to obtain a perspective view or a cross-sectional view of a thick inspected object with high spatial resolution and high density resolution, which is impossible with conventional X-rays, γ-ray radiography, CT apparatus, etc. it can.

  The best mode for carrying out the X-ray generator according to the present invention will be described below with reference to the drawings based on the embodiments.

  First, the principle of the present invention will be described. The inventor has invented a method and apparatus for modulating only the emission angle while fixing the X-ray generation position in order to simultaneously realize the high directivity of the laser Compton X-ray beam and a wide irradiation field.

  This method and apparatus uses the fact that laser Compton X-rays are emitted mainly around the traveling direction of electrons due to the difference in the momentum of electrons and photons, and sweeps the electron beam angle at several Hz to several kHz at high speed. In this way, the angle of the laser Compton X-ray beam is changed to create a pseudo fan-shaped beam.

  In the X-ray generator according to the present invention, the electron linear accelerator and the electron storage ring have different embodiments. First, the case where an electron storage ring is used will be described. A conceptual diagram of the present invention is shown in FIG. The electrons are turning clockwise with respect to the page. A vertical magnetic field is applied at a certain point on the beam trajectory to kick the beam trajectory toward the outer circumference or the inner circumference.

  In FIG. 2, for the sake of simplification, a deflecting electromagnet, a converging quadrupole electromagnet, and the like are omitted, but the electrons meander around the design trajectory by these magnetic fields. Since the electron storage ring always returns to its original position after one round, this meandering is always a closed orbit. A state in which the track is closed while being deformed from the design track is called closed orbit distortion. In the following, it is called COD.

  At the position where the beam crosses the design trajectory, the beam position does not move even if the kick angle θ is changed. In this specification, this position is called a node. The laser Compton X-ray beam is swept into a pseudo fan-shaped beam when the collision point of the laser and the electron beam is aligned with the node and the kick angle is AC-modulated from the positive direction to the negative direction and further to the positive direction. . That is, since the momentum of electrons is much larger than that of photons, it is necessary to change the angle of the electron beam in order to change the direction of the laser Compton X-ray, and the laser Compton X-ray beam is deflected at high speed. Control the direction of release.

  The laser can irradiate the electron beam meandering surface at an arbitrary angle at the node. For example, when it is irradiated perpendicularly (90 degrees) to the electron meandering surface, it has a constant energy regardless of the deflection direction of the electron beam. Laser Compton X-rays are generated. In other cases, the energy is modulated by the deflection angle. The generated X-rays are quasi-monochromatic by a collimator arranged downstream, but since it is a fan beam, it is desirable to use a rectangular object that is long in the direction of the electron deflection surface.

  As a result, it is possible to generate a quasi-monochromatic high-energy fan beam that has been impossible until now with a stable intensity. Conventionally, it is a unique point of the present invention to actively excite and use COD that should be as small as possible.

The above description will be supplemented slightly. Take the coordinate system in the direction of the electron trajectory. Let S ₁ be the position where the kick is given, and let β (S ₁ ) and β (S), φ (S) and φ ( S ₁₎ to. The horizontal kick may be horizontal (x) or vertical (y), but here, a horizontal kick (x) represented by θ (mrad) is given.

The kick angle toward the outer circumference is the positive direction. The COD generated when a lateral kick of the kick angle θ is given at a certain point of the electron storage ring, where ν _x is the horizontal betatron frequency, is expressed by the following equation 2 with the variation from the central orbit as dx. It is.

  It is assumed that a deflection angle of θ = several mrad is given to the electron beam using a magnetic field of about 100 mT generated by a normal small electromagnet.

  As an example, consider a storage ring in which basic cells in which three quadrupole electromagnets (arranged in the order of focus, defocus, and focus) are arranged between two deflection electromagnets are symmetrically combined four times. FIG. 3 shows the result of calculating the COD observed when a kick of 1 mrad, 2 mrad, and −3 mrad was given immediately after a certain defocused quadrupole magnet. The betatron frequency was 2.75.

  It can be seen that the trajectory does not move at a specific point in the electron trajectory and that the node position can be fine tuned by appropriately adjusting the betatron frequency. The relationship between the kick position and the node position is shown in the figure. Although β (s) is also shown, it can be seen that nodes are formed where the β function is small.

  Originally, the node is formed at the point of the minimum value by the local kick where the node is formed at the point where β (S) is the minimum, and this is a long straight line portion between the two deflection magnets. Therefore, the beam diameter and the divergence angle are minimized. By condensing the laser at this point, laser Compton X-rays can be generated with high efficiency.

  The synchrotron radiation using an electron storage ring also has a problem that the irradiation is small. On the other hand, an electron wave ring which is a device similar to the present invention (Japanese Patent Laid-Open No. 1-95500, Japanese Patent Publication No. 6-101400). Have already been invented.

  In this conventional invention, in an N-fold symmetric electron storage ring, it is shown that the number of nodes is N when the betatron frequency ν of the electron beam satisfies the relationship of the following equation (3). It is not necessary to control the node position over the entire circumference of the ring, N = 4 and ν = 2.75, which does not apply to the condition of Equation 3.

  The electron wave ring is intended to expand the radiation field of the emitted light in a planar manner, whereas the present invention is a high energy quasi-monochromatic X-ray fan beam having a divergence only in the horizontal or vertical direction. The difference is that it is intended to generate.

  In the present invention, by changing only the angle of the electron trajectory at the node, the laser Compton X-ray beam trajectory is modulated at high speed, so that the pseudo-fan type X used in non-destructive inspection, medical radiography, or CT apparatus is used. It is preferable to adopt a configuration that generates a line beam.

  In the present invention, in an electron accelerator that performs orbital deformation by applying vertical or horizontal deflection to an electron trajectory, by applying the deflection, a node can be placed at an arbitrary position downstream of a point in the electron trajectory to which the deflection is applied. Forming and condensing the laser at the position to generate X-rays by laser Compton scattering, switching or modulating the direction of the magnetic field of the deflection magnet, and switching or modulating only the angle of the electron trajectory, Provided is an X-ray generator equipped with an electron accelerator, wherein the X-ray generation direction is switched or modulated.

  In addition, a quasi-monochromatic high-energy fan-shaped X-ray beam used for nondestructive inspection is thereby generated, and further, second-generation and third-generation CT apparatuses for nondestructive inspection using the same are provided.

  The electron trajectory is preferably a circular trajectory such as an electron storage ring with a local deflection magnet, or an electron linear accelerator with a wiggler or undulator of one period or more.

  An electron linear accelerator can also modulate only the angle of the electron beam at a certain position in the orbit by AC modulation of, for example, a quadrupole wiggler or undulator magnetic field, thereby generating a fan-shaped laser Compton X-ray beam. can do.

  In FIG. 4, the electron trajectory is meandered using the deflecting magnets A to D capable of AC modulation and the deflecting magnet E having a fixed magnetic field, and a node is formed between the electromagnets B and C. Laser Compton X-rays with angle modulation are generated by irradiating a laser here. The generated X-rays run in parallel with the electrons, but the X-rays are separated from the electrons by installing the deflection magnetic field E. In the drawing, the upper magnetic pole is not shown for simplification. Such a magnetic field can also be realized by a Halbach undulator or the like.

  When a laser is irradiated to a node perpendicular to the meandering surface of the electron beam, laser Compton X-rays having a constant energy are generated regardless of the deflection angle of the electrons. The generated X-rays are quasi-monochromatic by a collimator F disposed downstream of the deflecting magnet E. However, since it is a fan beam, it is desirable to use a rectangular object that is long in the direction of the deflecting surface.

  Further, the present invention will be described from the structural aspect. In order to solve the above conventional problems, the present inventor has conceived an electron accelerator that generates a quasi-monochromatic high-energy fan-shaped X-ray beam, a CT apparatus using the same, and the like.

  That is, in the present invention, in the electron accelerator, a deflecting magnet capable of switching or modulating the polarity is installed on the trajectory, thereby giving vertical or lateral deflection to the electronic trajectory to cause trajectory deformation. The switching or modulation of the orbital deformation is realized by arranging a deflecting magnet using an air core or a silicon steel plate or the like excited by a bipolar current source as a core at a predetermined position of the electron accelerator.

In order to switch the magnetic field or increase the modulation speed, a relatively small electromagnet is desirable. As an example, the specifications of a magnet necessary for high-speed modulation of a magnetic field necessary to deflect 760 MeV electrons by 10 mrad at 1 kHz are as follows.
Gap interval: 100mm
Maximum magnetic field strength in beam orbit: 70 mT
Magnetic pole length: 200mm
Magnetic field modulation frequency: 1 kHz or less

  By giving local deflection to the electron beam trajectory, a deflection effect by the focusing magnet or the deflecting magnet is generated, and as a result, the electron trajectory meanders around the design trajectory. The design trajectory mentioned here is a trajectory passing through the magnetic field center of all the focusing magnets.

  Orbital deformation forms nodes at various locations depending on the design of the electron accelerator. FIG. 2 shows a simple example using COD using an electron storage ring. Due to the locally applied deflection, the electrons meander around the design trajectory, but intersect the design trajectory in several places. Since the closed orbital deformation is reversed with respect to the design orbit when the deflection angle is reversed, the swing angle of the electron beam is changed at the node position in synchronization with the timing of switching the polarity of the deflection magnet.

  The present inventor has found that the node can be moved to an optimum position for laser Compton scattering by appropriately adjusting the magnetic field strength of the focusing magnet and deflecting magnet of the electron accelerator. This is a device that is more versatile than the electron wave ring because it does not need to impose conditions for adjusting the node position over the entire circumference unlike the electron wave ring, and the generated photons are 10 MeV or more. Since it is a high energy γ-ray region, it is suitable for high-precision industrial nondestructive inspection.

  FIG. 3 shows the orbital deformation that occurs when a 1 to 10 mrad deflection is applied locally to 760 MeV electrons that circulate in the electron storage ring. In this case, since the electrons circulate an infinite number of times, this orbital deformation is particularly called closed orbital deformation. In the case of FIG. 3, nodes are formed at six locations, but the fourth node from the point where the deflection is applied is formed by a long straight line portion.

  In drift spaces such as long straight sections, the electron beam has no angular dispersion and it is possible to have no energy dispersion. Therefore, laser Compton scattering can be most effectively performed by irradiating a laser here.

  Since the laser and electron scattering points are nodes, even if the magnetic field of the deflection magnet is switched or modulated, the position of the electron beam does not change and only the angle changes. In other words, X-rays are stably generated by irradiating a laser beam from a direction perpendicular to the meandering surface of electrons at the node, and the intensity of the X-ray beam does not change even when the direction of the magnetic field of the deflecting magnet is switched or modulated. However, since only the emission angle changes, a pseudo fan-shaped beam can be obtained.

  If laser Compton scattering is performed at a position other than the node, the laser irradiation position must be modulated in accordance with the modulation of the electron beam position, and a very complicated control mechanism is required.

  However, according to the present invention, a kick having an arbitrary deflection angle is locally applied to the electron beam, thereby creating a node on the beam trajectory using the trajectory deformation, and modulating the deflection angle at high speed. Thus, an X-ray beam equivalent to a fan beam can be produced effectively. CT is performed by irradiating the object to be inspected and measuring the transmission intensity with an X-ray detector. In the conventional first generation CT apparatus, it is necessary to measure while moving the object to be inspected. was there.

  However, this makes it difficult to move at a very high speed of several tens to several kHz. The present invention enables high-speed scanning, and the time required for measurement can be shortened by several orders of magnitude when using a one-dimensional array X-ray detector in the case of the second generation or third generation CT. The detector element can be a scintillator or a semiconductor detector of about 1 to several mm, and has a sufficiently high detection efficiency for high energy γ rays of several MeV or more. The resolution of CT is determined by the size of the detector element, but since a magnifying optical system using a fan beam can be used, a spatial resolution of 1 mm or less can be achieved, so there is no practical problem.

  Further, in the second generation or more CT using a fan-shaped beam, there is a problem that the spatial resolution of an image is remarkably deteriorated due to scattered rays from an object to be inspected. In the present invention, a pseudo fan beam using a thin beam that scans at high speed is used instead of a fan beam that is uniform in time and space.

  Since the position of the X-ray beam irradiated to the object to be inspected can be inferred from the intensity of the modulated magnetic field, the influence of scattered radiation can be significantly reduced by extracting only the response of the element in the vicinity of the position where the beam has passed. .

  In other words, the beam obtained with this device is thin in a short time, and only a very small area of the object to be inspected is irradiated. Therefore, by extracting the response of the detector element corresponding to that area, high spatial resolution can be obtained. Can be achieved.

  By constructing a second-generation and third-generation CT apparatus using this beam, a CT apparatus for nondestructive inspection having high spatial resolution and density resolution and performing high-accuracy inspection in a short time can be obtained.

  The embodiment of the present invention will be described after first explaining the conventional example so that the difference becomes clearer than the conventional example.

  In FIG. 5, a conventional apparatus for generating a laser Compton X-ray beam 1 includes an electron accelerator 2 and a laser 3, and generates an X-ray beam by laser Compton scattering. By passing this through a collimator 4 and reducing the diameter to several millimeters, a quasi-monochromatic and pencil beam is obtained.

  The quasi-monochromatic laser Compton X-ray beam 1 is irradiated onto an object to be inspected 5 mounted on a CT stage in a CT apparatus, and the intensity of transmitted light is measured by an X-ray detector 6 to inspect the inside. Transmission or tomographic images are obtained by sequentially moving and rotating the object to be inspected, or sequentially moving or rotating.

  FIG. 6 shows a schematic diagram of an embodiment of the present invention. In the electron accelerator 2, the electron trajectory is deflected horizontally or vertically by the deflecting magnet 7. By reversing the polarity of the deflecting magnet in an alternating manner, the angle of the electron beam at the interaction position of the laser and the electron beam. Can only shake. For example, the deflection magnet 7 can perform AC modulation of about 1 kHz.

  In the present invention, according to such an embodiment, an X-ray beam can be generated in exactly the same manner as normal laser Compton scattering without modulating the laser irradiation position and angle.

  However, the angle at which the laser Compton X-rays are emitted can be modulated to an arbitrary angle in an arbitrary direction by a deflecting magnet installed upstream of the point irradiated with the laser.

  In the electron storage ring, the laser Compton scattering can be performed with high efficiency at the position where the electron beam diameter and the divergence angle are minimum by adjusting the balance between the position where the deflecting magnet for giving a kick is inserted and the betatron frequency.

  In the electron linear accelerator, the angle at which the laser Compton X-ray is emitted can be modulated by using a four-pole AC deflecting magnet. By using a silicon steel electromagnet or the like, the modulation frequency can be modulated alternatingly to about 1 kHz.

  The modulation pattern may be a sine wave or a triangular wave. In order to irradiate laser Compton X-rays with spatially uniform intensity, modulation with a linear response like a triangular wave is desirable, but it is possible to correct the irradiation intensity distribution by the response of the detector, so it is fast. When modulating with sine wave, a sine wave may be used.

  The X-ray beam is quasi-monochromatic using a collimator to obtain a desired fan-type X-ray beam. As the collimator, a circular X-ray beam is usually used with a circular cross section, but in the case of this embodiment, a horizontally long rectangular shape can be used.

  The X-ray beam is irradiated onto the inspection object 5 placed on the CT stage, and the intensity of the transmitted light is measured by a plurality of X-ray detectors 6 to inspect the inside thereof.

  The best mode for carrying out the present invention has been described based on the embodiments. However, the present invention is not limited to such embodiments, and within the scope of the technical matters described in the claims. Needless to say, there are various embodiments.

  Since the X-ray generator according to the present invention is configured as described above, the present invention can be applied to non-destructive inspection, medical radiography, or CT using a high-energy quasi-monochromatic fan-type X-ray beam using laser Compton scattering. It can be applied to a device or the like.

It is a figure which shows the energy spectrum measured by the conventional NaI (Tl) scintillation detector. It is a schematic diagram which shows closed orbit deformation | transformation at the time of adding local deflection | deviation to a part of revolving electron orbit. It is a calculation example which shows a closed orbit deformation | transformation at the time of adding a local deflection | deviation to a part of a revolving electron orbit. It is a schematic diagram which shows an orbit deformation | transformation at the time of adding local deflection | deviation to a part of electron orbit of an electron linear accelerator. It is a figure explaining the 1st generation CT apparatus using the conventional laser Compton X-ray beam. It is a figure explaining the Example of this invention, and is a figure which shows the nondestructive inspection apparatus by CT using a fan-shaped X-ray beam.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Laser Compton X-ray beam 2 Electron accelerator 3 Laser 4 Collimator 5 Inspected object 6 X-ray detector

Claims (5)

In an X-ray generator equipped with an electron accelerator that performs orbital or angular modulation by applying vertical or horizontal deflection to an electron trajectory using a deflection magnet that can switch the direction of the magnetic field at high speed,
By applying the deflection and meandering, a node which is a spatially constant point is formed at a predetermined position downstream of the point in the electron trajectory to which the deflection is applied, and the laser is focused on the laser beam by condensing the laser at the position. The X-ray beam is generated by Compton scattering, the direction of the magnetic field of the deflection magnet is switched or modulated, and only the angle of the electron trajectory at the node is switched or modulated to switch the generation direction of the X-ray beam or An X-ray generator provided with an electron accelerator characterized by performing modulation.   2. The X-ray generator with electron accelerator according to claim 1, wherein the electron orbit is a circular orbit like an electron storage ring.   2. The X-ray generator with an electron accelerator according to claim 1, wherein the electron trajectory is an electron linear accelerator. By switching only the angle of the electron trajectory at the node, the laser Compton X-ray beam trajectory is modulated at high speed to generate a pseudo-fan X-ray beam used in non-destructive inspection, medical radiography or CT equipment. The X-ray generator provided with the electron accelerator according to claim 1, characterized in that:   A thin X-ray beam generated in a short time by the X-ray generator according to any one of claims 1 to 4 and an X-ray detector having a one-dimensional array or a two-dimensional matrix to be inspected. In radiography including X-ray CT in the form of high-speed scanning of the X-ray beam on the body, the transmission position is estimated by knowing the position irradiated with the beam, and only the corresponding X-ray detection element A method for generating X-rays for improving spatial resolution by removing scattered rays from an object to be inspected by making effective.