BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates, in general, to an apparatus used within a varying magnetic field and, in particular, to an apparatus used between magnetic poles of a magnet of a synchrotron.
2. Description of the Related Art
A synchrotron used in various fields including scientific researches, and medical and industrial applications, orbits and, at the same time, rapidly accelerates a charged particle beam injected from a pre-accelerator. The synchrotron typically includes an injection apparatus that injects the charged particle beam that have been preliminarily accelerated by the pre-accelerator, a dipole magnet that bends and moves the charged particle beam around a predetermined circular path, a quadrupole magnet that gives horizontal and vertical converging forces so as to prevent an orbiting beam from being widened, and an RF cavity that applies an RF acceleration voltage to the orbiting beam to thereby accelerate the orbiting beam to a predetermined level of energy.
In order to circulate the charged particle beam along a predetermined orbit at all times, the synchrotron intensifies the magnetic field generated by the dipole magnet in synchronism with the acceleration. Since the charged particle beam circulates in vacuum, the synchrotron includes a vacuum duct with an evacuated interior disposed between magnetic poles of the dipole magnet. If the vacuum duct is formed of a conductive substance, an induced electric field causes an eddy current to flow through the vacuum duct. The eddy current induced in the vacuum duct generates a new magnetic field in an area past which the charged particle beam moves. This magnetic field has varying intensities depending on the position at which the charged particle beam moves, which unsteadies circulation of the charged particle beam.
JP-08-78200-A discloses art in which a nonmagnetic correcting plate is disposed between magnetic poles of the dipole magnet to thereby flatten a magnetic field which an eddy current generates in an area past which the charged particle beam moves. JP-03-190099-A discloses art that prevents a distribution of a magnetic field generated in a vacuum duct from being disturbed by continuously increasing a thickness of a vacuum duct of a synchrotron from a central portion toward end faces.
SUMMARY OF THE INVENTION
With the dipole magnet described in JP-08-78200-A, because of the wide correcting plate, current density is large on end portions, so that a heat value may become high. The vacuum duct of the synchrotron described in JP-03-190099-A is made to be thick so as to flatten the magnetic field of the area past which the charged particle beam moves. This widens a spacing between the magnetic poles, which may increase load on a magnet power source.
To solve the foregoing problems, the present invention provides a plurality of conductive correcting plates disposed in each of four areas, the four areas being formed by dividing a cross section of a vacuum duct extending perpendicularly in a direction in which a charged particle beam travels with a symmetrical surface having each of both magnetic poles of a dipole magnet defined as a mirror image and a plane which extends perpendicularly to the symmetrical surface and through which a center of gravity of the charged particle beam passes.
In the present invention, the width of the correcting plate for flattening the magnetic field distribution can be reduced, which allows heat generated by the eddy current of the correcting plate to be reduced and a rate of increase in the spacing between the magnetic poles to be reduced.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a conceptual diagram showing general arrangements of a magnetic field control apparatus according to a first embodiment of the present invention.
FIG. 2 is a plan view showing the magnetic field control apparatus according to the first embodiment of the present invention, as viewed from above.
FIG. 3 is a cross-sectional view showing the magnetic field control apparatus according to the first embodiment of the present invention.
FIG. 4 is a conceptual diagram showing a magnetic field generated by an eddy current in the magnetic field control apparatus according to the first embodiment of the present invention.
FIG. 5 is a graph showing calculations of the magnetic field generated by the eddy current in the magnetic field control apparatus according to the first embodiment of the present invention.
FIG. 6 is a cross-sectional view showing a magnetic field control apparatus according to prior invention 1.
FIG. 7 is a conceptual diagram showing a magnetic field generated by the eddy current in the magnetic field control apparatus according to prior invention 1.
FIG. 8 is a graph showing calculations of the magnetic field generated by the eddy current in the magnetic field control apparatus according to prior invention 1.
FIG. 9 is a graph showing density of an eddy current induced in an end portion of a conductive thin plate disposed within a time-varying magnetic field.
FIG. 10 is a cross-sectional view showing a magnetic field control apparatus according to a second embodiment of the present invention.
FIG. 11 is a cross-sectional view showing a magnetic field control apparatus according to a third embodiment of the present invention.
FIG. 12 is a cross-sectional view showing a magnetic field control apparatus according to a fourth embodiment of the present invention.
FIG. 13 is a cross-sectional view showing a magnetic field control apparatus according to a fifth embodiment of the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
First Embodiment
As a first embodiment of the present invention, a synchrotron will be exemplified that flattens a magnetic field distribution generated by eddy currents induced in conductive substances disposed between magnetic poles of a dipole magnet. The synchrotron includes a conductive vacuum duct 1, a dipole magnet that bends a charged particle beam to a predetermined direction and moves the charged particle beam around an orbit, and an accelerating device that accelerates the charged particle beam. The magnetic field of the dipole magnet is intensified as the charged particle beam is accelerated, so that an eddy current is generated in the conductive vacuum duct 1 disposed between magnetic poles 3 of the dipole magnet.
A method for controlling a magnetic field generated by the eddy current and an apparatus thereof (hereinafter referred to as a magnetic field control apparatus) according to a first embodiment of the present invention will be described below with reference to FIGS. 1 through 8.
Arrangements of the magnetic field control apparatus according to the first embodiment of the present invention will be described with reference to FIG. 1. FIG. 1 is a conceptual diagram showing the arrangements of the magnetic field control apparatus according to the first embodiment of the present invention.
The magnetic field control apparatus according to the first embodiment of the present invention includes a plurality of conductive correcting plates 2 disposed on the conductive vacuum duct 1 placed between the dipole magnet magnetic poles 3. The conductive vacuum duct 1 as used herein means is a duct in which the eddy current is induced when the magnetic field generated by the dipole magnet changes with time, thereby disturbing the magnetic field in the area through which a beam passes. In the first embodiment of the present invention, the multiple correcting plates are disposed on an outer peripheral surface of the vacuum duct 1, which reduces a spatial change in the magnetic field arising from the eddy current induced in the vacuum duct 1, thereby flattening the magnetic field distribution. The correcting plates 2 are formed of a material having an electric resistivity lower than that of the vacuum duct 1. The correcting plates 2 are disposed such that a cross section of the vacuum duct 1 as viewed in a plane perpendicular to the charged particle beam is upper-lower and right-left symmetrical and multiple correcting plates 2 are disposed per quadrant. The term “right-left” as used herein means a direction extending in parallel with a magnetic pole surface and the term “upper-lower” as used herein means a direction extending perpendicularly to the magnetic pole surface. In the first embodiment of the present invention, two correcting plates 2 are disposed per quadrant. Nonetheless, the number of correcting plates 2 per quadrant may be more than two, or each quadrant may have a unique number of correcting plates 2. In addition, in the first embodiment of the present invention, an outer correcting plate 2b is thicker than an inner correcting plate 2a. A desired magnetic field distribution can be obtained by changing the width and the thickness of the correcting plate 2, and a position at which the correcting plate 2 is disposed. In this case, the correcting plates 2 may be disposed upper-lower and right-left asymmetrically. For a dipole magnet having magnetic pole surfaces that do not extend in parallel with each other, the correcting plates 2 are disposed symmetrically, in a vertical direction, relative to symmetrical surfaces having each of the magnetic poles defined as a mirror image.
FIG. 2 is a plan view showing the magnetic field control apparatus according to the first embodiment of the present invention. The correcting plates 2 are disposed on the outer peripheral surface of the vacuum duct 1 so as to follow along the shape of the vacuum duct 1, specifically, so as to have a constant cross-sectional shape.
FIG. 3 is a cross-sectional view showing the magnetic field control apparatus according to the first embodiment of the present invention. In FIG. 3, the charged particle beam travels in a direction perpendicular to a sheet surface. A point of intersection between dash-single-dot lines A and B is here defined as the center of the vacuum duct 1. The dash-single-dot line A is a straight line along which the symmetrical surface having each of the magnetic poles of the dipole magnet defined as a mirror image intersects the sheet surface. Similarly, the dash-single-dot line B is a straight line along which a plane which extends perpendicularly to the symmetrical surface and through which a center of gravity of the charged particle beam passes intersects the sheet surface. The correcting plates 2 are disposed symmetrically with respect to the dash-single-dot lines A and B.
An axis which is parallel to the dash-single-dot line A is denoted as X and the right direction in FIG. 3 is defined as positive. Similarly, an axis which is parallel to the dash-single-dot line B is denoted as Y and the upper direction in FIG. 3 is defined as positive. The dipole magnet generates a magnetic field for bending the charged particle beam in a direction in which Y is positive. When the magnetic field for bending the charged particle beam intensifies with the accelerating charged particle beam, an electric field according to a change with time in the magnetic field is induced, so that an eddy current is induced in the vacuum duct 1 and the correcting plates 2. For the vacuum duct 1, the direction in which the eddy current flows is, as shown in FIG. 3, forward from the sheet surface in a direction in which X is positive as viewed from the center of the vacuum duct 1, while the direction in which the eddy current flows is backward from the sheet surface in a direction in which X is negative as viewed from the center of the vacuum duct 1. Similarly, for the correcting plates 2, the direction in which the eddy current flows is forward from the sheet surface in a direction in which X is positive as viewed from the center in the X direction of the correcting plates 2, while the direction in which the eddy current flows is backward from the sheet surface in a direction in which X is negative as viewed from the center in the X direction of the correcting plates 2.
The magnetic field generated by the eddy current in the area through which the charged particle beam passes will be described below with reference to FIG. 4. In FIG. 4, the positive direction of the magnetic field is the direction of the magnetic field for bending the charged particle beam, so that the eddy current generates a magnetic field in the negative direction. The eddy current induced in the vacuum duct 1 generates a magnetic field that is intense in an area near the duct center and weak toward the outside as indicated by a broken line. If such a magnetic field exists in the area through which the charged particle beam passes, a bending force varies according to the position at which the charged particle beam passes, so that a converging state of the charged particle beam changes and a loss of the charged particle beam may result. The eddy current induced in the correcting plates 2 generates a magnetic field as indicated by dotted lines. In the first embodiment of the present invention, the outer correcting plates 2b are thicker than the inner correcting plates 2a, so that the magnetic field generated by the eddy current induced in the outer correcting plates 2b is more intense than the magnetic field generated by the eddy current induced in the inner correcting plates 2a. By combining the magnetic field generated by the eddy current induced in the vacuum duct 1 with the magnetic field generated by the eddy current induced in the correcting plates 2, the magnetic field in the area through which the charged particle beam passes is flattened as indicated by a solid line in FIG. 4.
FIG. 5 shows calculations of a distribution of the magnetic field generated by the eddy current. As shown in FIG. 5, the magnetic field in the area through which the charged particle beam passes is flattened. It is noted that, in this calculation system, the inner correcting plates 2a have a width of 24 mm and the outer correcting plates 2b have a width of 30 mm.
FIG. 6 shows locations where correcting plates 4 in prior invention 1 (JP-A-08-78200) are disposed. As shown in FIG. 6, one correcting plate 4 having a wide width in the X direction is disposed per quadrant such that a cross section of the vacuum duct 1 as viewed on a plane perpendicular to the charged particle beam is upper-lower and right-left symmetrical. The direction of the magnetic field for bending the charged particle beam and the direction in which the eddy current flows are the same as those of the first embodiment of the present invention shown in FIG. 3.
The magnetic field generated by the eddy current according to prior invention 1 will be described with reference to FIG. 7. In prior invention 1, the magnetic field in the area through which the charged particle beam passes is flattened by adding the wide magnetic fields (indicated by dotted lines) generated by the eddy current induced in the correcting plates 4 to both sides of the magnetic field (indicated by a broken line) generated by the eddy current induced in the vacuum duct 1.
FIG. 8 shows calculations of a distribution of the magnetic field generated by the eddy current according to prior invention 1. The correcting plates 4 are required to have a wide width in order to generate a wide magnetic field and, in this calculation system, the correcting plates 4 have a width of 160 mm.
Generally speaking, density of the eddy current induced in a conductive thin plate disposed within a time-varying magnetic field is high in proportion to a distance from the center of the plate. As a result, the density of the eddy current induced in end portions of the correcting plate is high in proportion to the width of the correcting plate as shown in FIG. 9. The wider the width, the higher the current density at the end portions and the greater the heat value. If, for example, a copper having an extremely low electric resistivity is used for the correcting plate 4, the heat value involved is particularly large and, in prior invention 1, the correcting plate 4 is not applicable to a synchrotron having a high excitation speed. By reducing the width of the correcting plate according to the first embodiment of the present invention, the heat value produced by the eddy current can be reduced to thereby expand ranges of the excitation speed and of types of materials to be selected for the correcting plate, while maintaining an effect of magnetic field correction.
In prior invention 2 (JP-A-03-190099), on the other hand, the vacuum duct is made to be thick in order to achieve flattening. This results in a wider spacing between magnetic poles, which may increase load on a magnet power source (not shown). By using a material having an electric resistivity lower than that of the vacuum duct 1 for the correcting plate 2 according to the first embodiment of the present invention, a rate of increase in the spacing between the magnetic poles as a result of flattening can be reduced.
Second Embodiment
FIG. 10 is a cross-sectional view showing a magnetic field control apparatus according to a second embodiment of the present invention. Outer correcting plates 5 are formed of a material having an electric resistivity lower than inner correcting plates 2a. While an eddy current amount generated is controlled by forming the outer correcting plates 2b thicker than the inner correcting plates 2a in the first embodiment of the present invention, the eddy current amount to be generated can be controlled by using materials having different electric resistivity values as in the second embodiment.
Third Embodiment
FIG. 11 is a cross-sectional view showing a magnetic field control apparatus according to a third embodiment of the present invention. In the first embodiment of the present invention, the correcting plates 2 are disposed on the outside (atmospheric side) of the vacuum duct 1. As in the third embodiment of the present invention, however, the magnetic field generated by the eddy current can also be controlled by disposing correcting plates 2 inside (vacuum side) a vacuum duct 1. It is noted that correcting plates 2b disposed on the outside may be replaced with the outer correcting plates 5 formed of a material having an electric resistivity lower than correcting plates 2a disposed on the inside.
Fourth Embodiment
FIG. 12 is a cross-sectional view showing a magnetic field control apparatus according to a fourth embodiment of the present invention. In the first, second, and third embodiments, the correcting plates 2 are disposed without overlapping each other. However, by overlapping correcting plates 2 as in the fourth embodiment, the magnetic field generated by the eddy current can be controlled.
Fifth Embodiment
FIG. 13 is a cross-sectional view showing a magnetic field control apparatus according to a fifth embodiment of the present invention. In the first, second, third, and fourth embodiments, the correcting plates 2 are disposed right-left symmetrically. In the fifth embodiment, however, magnetic poles 3 are right-left asymmetrical as shown in FIG. 13. If the eddy current induced to correcting plates 2 varies according to the positions at which the correcting plates 2 are disposed in the X direction, the magnetic field generated by the eddy current can be controlled by disposing the correcting plates 2 right-left asymmetrically. In FIG. 13, the number and positions of the correcting plates 2 are asymmetrical, it is nonetheless effective to use correcting plates, each having a unique thickness or electric resistivity value.
Even if the magnetic poles 3 are not right-left asymmetrical, if the dipole magnet has a small bending radius and the eddy current induced to the correcting plates 2 varies according to the positions at which the correcting plate 2 are disposed in the X direction, the magnetic field generated by the eddy current can be controlled by disposing the correcting plates 2 right-left asymmetrically.
Patent Application
20120133305
