CN204518207U - A kind of permanent magnetism line homogenizing six pole magnet - Google Patents

Abstract

The utility model belongs to the design technology of accelerators, in particular to a hexapole magnet for homogenizing permanent magnetic beam currents for accelerators. Based on the traditional design, the hexapole magnet cancels the magnetic field excitation of a pair of opposite magnetic poles, shortens the distance between the pair of magnetic poles, and changes the magnetic field excitation direction in a pair of adjacent magnetic poles. The magnetic field excitation assembly includes a permanent magnet as the main magnetic field excitation and an excitation wire package as the auxiliary magnetic field excitation. The utility model can generate a magnetic field on the X axis that is symmetrical about the origin of the coordinates, and the magnitude of the magnetic field is proportional to the square of the position, and can provide a good homogenization effect on beam spots with triangular density distribution.

Description

A six-pole magnet for homogenizing permanent magnetic beam current

technical field

The utility model belongs to the design technology of accelerators, in particular to a hexapole magnet for homogenizing permanent magnetic beam currents for accelerators.

Background technique

The particle distribution of the transverse section of the beam generated by the accelerator is generally Gaussian distribution, that is, the distribution of particles bombarded on the target is not uniform. In some industrial electron irradiation occasions, the requirements for beam irradiation uniformity are very high, such as the irradiation of semiconductor materials. In addition, when the high power density beam generated by the heavy ion accelerator bombards the target, in order to reduce the size of the target and realize the cooling of the target, it is necessary to shape the beam as uniformly as possible while expanding the beam spot. Therefore, the homogenization of the accelerator beam is a very important issue.

At present, the beam homogenization devices used at home and abroad are divided into two types: nonlinear multipole magnets and nonlinear step field dipole magnets. Non-linear multi-pole magnets include octopole magnets and twelve-pole magnets, etc. Non-linear step field dipole magnets are divided into single-step and multi-step.

Due to the very strong nonlinear effects introduced by nonlinear multipole irons in the process of beam homogenization, the results are not satisfactory. The goal of the homogenization of the non-linear step field dipole magnet is to translate the particles at the edge of the beam to the inner area with equal density, but the beam it translates is not uniform. When the translation is superimposed, it is high density and relatively high density. Superposition, the superposition of low density and lower density, the uniformity after superposition is still not very good.

Utility model content

The purpose of the utility model is to provide a hexapole magnet structure for homogenizing the permanent magnetic beam current in view of the defects of the prior art, so that the beam spot has a better homogenizing effect.

The technical scheme of the utility model is as follows: a permanent magnetic beam flow homogenization hexapole magnet, the six magnetic poles of the magnet are arranged in pairs along the ring, wherein, no magnetic field excitation assembly is arranged on the two opposite magnetic poles, and a magnetic field is arranged on the remaining magnetic poles Excitation components; the directions of the magnetic fields generated in the adjacent magnetic poles of the two magnetic field excitation components are opposite, and the directions of the magnetic fields generated in the opposite poles of the two magnetic field excitation components are the same, thereby forming a symmetrical magnetic field distribution relative to the center line of the magnet; The above-mentioned magnetic field excitation assembly includes a permanent magnet as the main magnetic field excitation and an excitation wire package as the auxiliary magnetic field excitation.

Further, in the beam homogenizing hexapole magnet for an accelerator as described above, the distance between the opposite magnetic poles without the magnetic field excitation assembly is smaller than the distance between the opposite magnetic poles with the magnetic field excitation assembly.

Further, the beam homogenizing sextupole magnet for the accelerator as described above, wherein, the excitation coil as the auxiliary magnetic field excitation is to adjust the magnetic field excited by the permanent magnet as the main magnetic field excitation in a small range; When the magnetic field excited by the permanent magnet does not need to be adjusted, the excitation wire package as the auxiliary magnetic field excitation can be cancelled.

Further, the beam homogenizing hexapole magnet for the accelerator as described above, wherein the direction of the magnetic field generated in the magnetic pole refers to a positive direction if the direction of the magnetic field points to the center of the magnet, and a negative direction if the direction of the magnetic field moves away from the center of the magnet.

Further, the beam homogenizing hexapole magnet for the accelerator as described above, wherein, the permanent magnet used as the main magnetic field excitation is arranged inside the pole core, and other parts of the pole core except the permanent magnet are made of soft magnetic materials ; The excitation wire package as the auxiliary magnetic field excitation is arranged on the outside of the pole core.

The beneficial effects of the utility model are as follows: the hexapole magnet provided by the utility model deletes the magnetic field excitation of a pair of relative magnetic poles on the basis of the traditional hexapole magnet, and shortens the distance between the pair of magnetic poles. Change the magnetic field excitation direction of a pair of adjacent poles. The magnetic field generated by this magnet on the X-axis is symmetrical about the origin of the coordinates, and the magnitude of the magnetic field is proportional to the square of the position, which can provide a good homogenization effect on the beam spot with a triangular density distribution.

Description of drawings

Fig. 1 is the structural representation of six pole magnets in the utility model embodiment;

Fig. 2 is the comparison schematic diagram of the magnetic field distribution of the six-pole magnet of the embodiment of the present invention and the prior art;

Fig. 3 is the schematic diagram of the initial density distribution of the beam formed by the hexapole magnet of the present invention;

Fig. 4 is a schematic diagram of the optical path of the beam;

Fig. 5 is a schematic diagram of the beam spot at the end of the optical path.

Detailed ways

Below in conjunction with accompanying drawing and embodiment the utility model is described in detail.

The utility model is an improvement made on the basis of the traditional hexapole magnet. The six magnetic poles of the traditional hexapole magnet are symmetrically arranged in pairs along the ring, and each magnetic pole is provided with an excitation wire package, and the two opposite magnetic poles The distance between them is equal, the direction of the magnetic field in the adjacent excited magnetic pole is opposite, and the direction of the magnetic field in the opposite magnetic pole is also opposite. The magnetic field distribution of this six-pole magnet is symmetrical about the plane passing through the center line of the magnet, as shown in the figure As shown in curve A in 2, the magnitude of the magnetic field is proportional to the square of the position.

As shown in Figure 1, the technical solution of the utility model is to remove the magnetic field excitation on a pair of opposite magnetic poles 1,2 of the hexapole magnet, and the excitation magnetic field of a pair of adjacent magnetic poles 3,4 is compared with the traditional The excitation magnetic field of the six-pole magnet is reversed, so that the direction of the magnetic field in the adjacent magnetic poles of the four magnetic poles set for magnetic field excitation is opposite, and the direction of the magnetic field in the opposite magnetic poles is the same, thus forming a symmetrical magnetic field distribution about the center line of the magnet. The centerline is perpendicular to the paper surface of Figure 1 and is located at the very center of the magnet. The magnetic field excitation assembly arranged on the magnetic pole of the utility model includes a permanent magnet as a main magnetic field excitation and an excitation wire package as an auxiliary magnetic field excitation. The main magnetic field excitation refers to the main bearer of the magnetic field excitation. Its material is permanent magnet, and its position can be placed in any appropriate position in the pole core, as long as it can excite the magnetic field shown in Figure 1; the auxiliary magnetic field excitation is the main The magnetic field excited by the magnetic field excitation is adjusted in a small range and controlled by the current passed into the excitation wire package. For example, the actual excitation intensity of the main magnetic field excitation deviates from the required excitation intensity or the change of the beam spot size requires a change in the magnetic field excitation intensity, etc. In some cases, if the magnetic field excited by the main magnetic field does not need to be adjusted, the auxiliary magnetic field excitation can be canceled.

The direction of the magnetic field generated in the magnetic pole refers to a positive direction if the direction of the magnetic field points to the center of the magnet, and a negative direction if the direction of the magnetic field is away from the center of the magnet. The magnetic field profile is a quadratic function with respect to the position coordinates. The magnetic field distribution of a traditional six-pole magnet is symmetrical about the plane passing through the center line of the magnet, as shown by the A curve in Figure 2, and the magnitude of the magnetic field is proportional to the square of the position. The magnetic field distribution of the present utility model is shown in the B curve in Fig. 2, and one side of the central point is the same as the A curve, and the other side is equal to the absolute value of the A curve, but the direction is opposite. The field distribution of the utility model can provide focusing effect on the edge particles on both sides, which is equivalent to a beam focusing element. The magnetic field distribution A curve formed by the traditional hexapole magnet focuses the particles on one side and defocuses the particles on the other side, which has an uneven deflection effect on the beam.

Compared with the traditional hexapole magnet, the distance between the two magnetic poles of the utility model that removes the magnetic field excitation needs to be correspondingly reduced in order to obtain the ideal curve B in FIG. 2 . That is to say, the distance between the two opposite magnetic poles 1, 2 is smaller than the distance between the two opposite magnetic poles 3, 6 and the two opposite magnetic poles 4, 5, the distance between the magnetic poles 3, 6 and the distance between the magnetic poles 4 , The distance between 5 remains equal.

The section curve of the magnetic pole head is the same as that of the traditional six-pole magnet, which is a binary cubic curve.

The magnet of the utility model can provide a good homogenization effect on the beam spot of the quasi-triangular density distribution, and the Gaussian distribution belongs to a kind of quasi-triangular distribution.

Example

The magnetic pole distance of the hexapole magnet provided by the present embodiment is as shown in Figure 1, wherein the distance between the magnetic poles 3,6 is the same as the distance between the magnetic poles 4,5, which is 5cm, and the distance between the magnetic poles 1,2 is 1.1 cm, no magnetic field excitation components are set on poles 1 and 2, and magnetic field excitation components are set on the remaining magnetic poles 3, 4, 5, and 6. The direction of the magnetic field generated in the opposite magnetic poles 3,6 of the two magnetic field excitation assemblies 7,10 is opposite to the direction of the magnetic field generated in the opposite magnetic poles 4,5 of the other two magnetic field excitation assemblies 8,9, and the opposite magnetic poles 3,6 (or 4, 5) the direction of the magnetic field generated in the same, so as to form a symmetrical magnetic field distribution with respect to the center line of the magnet. The magnetic field excitation assembly includes permanent magnets 11, 12, 13, 14 as the main magnetic field excitation and excitation wire packages 7, 8, 9, 10 as the auxiliary magnetic field excitation, the permanent magnets 11, 12, 13, 14 are respectively arranged on the magnetic poles 3, In the iron cores of 4, 5, and 6, the excitation wire packages 7, 8, 9, and 10 are respectively arranged outside the iron cores of the magnetic poles 3, 4, 5, and 6, and the permanent magnets 11, 12, 13, and 14 are the main magnets for magnetic field excitation. The undertaker forms the required magnetic field direction of the utility model, and the excitation wire packs 7, 8, 9, 10 play a role in adjusting the magnetic field. The initial density distribution of the beam is a Gaussian distribution, as shown in Figure 3. The beam flow path is shown in Figure 4, the upper part of the view is the beam envelope of the X-Z plane, and the lower part of the view is the beam envelope of the Y-Z plane, wherein S1 and S2 are the hexapole magnets of the present utility model, and a magnet is shown in Figure 1 Placed in the position, another magnet rotates the magnet in Figure 1 by 90 degrees and places it. The beam spot at the end of the optical path on the far right in Figure 4 is shown in Figure 5, and the beam spot size in the X and Y directions is a square beam spot of 200mm.

Obviously, those skilled in the art can make various changes and modifications to the utility model without departing from the spirit and scope of the utility model. In this way, if these modifications and variations of the present utility model fall within the scope of the claims of the utility model and equivalent technologies, the utility model is also intended to include these modifications and variations.

Claims (5)

1. a permanent magnetic beam current uniformization hexapole magnet, six magnetic poles of the magnet are set relative to each other along the ring, and it is characterized in that: no magnetic field excitation assembly is set on the two relative magnetic poles (1, 2), and all the other magnetic poles (3 , 4, 5, 6) to set the magnetic field excitation assembly; the direction of the magnetic field generated in the adjacent magnetic poles of the two magnetic field excitation assemblies is opposite, and the direction of the magnetic field generated in the opposite magnetic poles of the two magnetic field excitation assemblies is the same, thus forming a relative Magnetic field distribution symmetrical to the center line of the magnet; the magnetic field excitation assembly includes permanent magnets (11, 12, 13, 14) as the main magnetic field excitation and excitation coils (7, 8, 9, 10) as the auxiliary magnetic field excitation . 2. accelerator as claimed in claim 1 is characterized in that: the distance between the opposite magnetic poles (1,2) of not setting the magnetic field excitation assembly is less than the relative magnetic pole (3) of setting the magnetic field excitation assembly , 6) the distance between. 3. The beam homogenizing hexapole magnet for accelerator as claimed in claim 1 or 2, characterized in that: the described excitation coil (7, 8, 9, 10) as the auxiliary magnetic field excitation is for the main magnetic field The magnetic field excited by the permanent magnets (11, 12, 13, 14) of the excitation is adjusted in a small range; when the magnetic field excited by the permanent magnet does not need to be adjusted, the excitation wire package (7 , 8, 9, 10). 4. accelerator as claimed in claim 1 is used the homogenization sextupole magnet of beam current, it is characterized in that: the magnetic field direction that produces in described magnetic pole (3,4,5,6) refers to if magnetic field direction points to the magnet center as Positive direction, negative direction if the direction of the magnetic field is away from the center of the magnet. 5. beam current homogenization hexapole magnet for accelerator as claimed in claim 1, is characterized in that: described permanent magnet (11,12,13,14) as main magnetic field excitation is arranged on magnetic pole iron core inside, and magnetic pole Other parts of the iron core except the permanent magnets are made of soft magnetic materials; the excitation coils (7, 8, 9, 10) used as auxiliary magnetic field excitation are arranged on the outside of the magnetic pole iron core.