CN112704818B - Popular type light ion tumor treatment device - Google Patents

Popular type light ion tumor treatment device Download PDF

Info

Publication number
CN112704818B
CN112704818B CN202011479052.3A CN202011479052A CN112704818B CN 112704818 B CN112704818 B CN 112704818B CN 202011479052 A CN202011479052 A CN 202011479052A CN 112704818 B CN112704818 B CN 112704818B
Authority
CN
China
Prior art keywords
injection
synchrotron
light
light ion
leading
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN202011479052.3A
Other languages
Chinese (zh)
Other versions
CN112704818A (en
Inventor
詹文龙
杨建成
夏佳文
赵红卫
徐瑚珊
胡正国
马力祯
石健
杨磊
申国栋
吴巍
张红
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Guangdong Provincial Laboratory Of Advanced Energy Science And Technology
Institute of Modern Physics of CAS
Original Assignee
Guangdong Provincial Laboratory Of Advanced Energy Science And Technology
Institute of Modern Physics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Guangdong Provincial Laboratory Of Advanced Energy Science And Technology, Institute of Modern Physics of CAS filed Critical Guangdong Provincial Laboratory Of Advanced Energy Science And Technology
Priority to CN202011479052.3A priority Critical patent/CN112704818B/en
Publication of CN112704818A publication Critical patent/CN112704818A/en
Application granted granted Critical
Publication of CN112704818B publication Critical patent/CN112704818B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61NELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N5/00Radiation therapy
    • A61N5/10X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05HPLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H7/00Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
    • H05H7/001Arrangements for beam delivery or irradiation
    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05HPLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H7/00Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
    • H05H7/04Magnet systems, e.g. undulators, wigglers; Energisation thereof
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61NELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N5/00Radiation therapy
    • A61N5/10X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
    • A61N2005/1085X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy characterised by the type of particles applied to the patient
    • A61N2005/1087Ions; Protons

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Plasma & Fusion (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Biomedical Technology (AREA)
  • Radiology & Medical Imaging (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Pathology (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Animal Behavior & Ethology (AREA)
  • General Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Optics & Photonics (AREA)
  • Radiation-Therapy Devices (AREA)
  • Particle Accelerators (AREA)

Abstract

The invention relates to a general type light ion tumor treatment device, which comprises: ion source, ion source pack shell and air inlet pipe arranged in shellA tunnel, an evaporation furnace and a waveguide; the input end of the linear injector is connected with the output end of the ion source through a low-energy beam transport line, and the linear injector comprises an acceleration cavity and a magnetic focusing element sleeved outside the acceleration cavity; the input end of the synchrotron is connected with the output end of the linear injector through an intermediate energy beam transport line, and the beam input end of the synchrotron is provided with an injection cutting magnet, an injection convex rail magnet and an injection static deflection plate; and the treatment terminal is connected with the synchrotron through a high-energy beam transport line. The device of the invention can not only utilize protons for whole body treatment, but also can be used3He、4He、7And (3) carrying out superficial layer (less than or equal to 8cm) tumor treatment by using light ion beams such as Li and the like.

Description

Popular type light ion tumor treatment device
Technical Field
The invention relates to a general type light ion tumor treatment device, and belongs to the technical field of medical equipment.
Background
Because the irradiation of the ion beam to the organism has reversed depth dose distribution and higher relative biological effect, the damage to normal cells can be better avoided while tumor cells are killed, so that the ion cancer therapy becomes an international advanced and effective cancer radiotherapy method. The ions most commonly used in ion therapy of cancer at present are protons and carbon ions, which have advantages and disadvantages in terms of indication and cost.
The carbon ion linear energy density, the relative biological effect and the side scattering have more remarkable advantages, can generate DNA Double Strand Break (DSB) which is difficult to repair, and is usually used as the optimal choice for treating cancer, but because the energy of a carbon ion accelerator is required to be more than 430MeV/u, the magnetic rigidity is larger, the occupied area of the device is large, and the investment scale is higher; the proton treatment device needs low magnetic rigidity, generally adopts a fixed energy accelerator, has low cost, relatively mature technology, small occupied area and low market popularization difficulty, but has low proton beam energy transfer linear density (LET), can only break a DNA single chain and has slightly poor treatment effect on tumors.
If it is possible to simultaneously provide ions having biological effects close to those of carbon ions within the range of the size and acceleration capability of a proton accelerator, e.g.) "3He”、“4He "or"7Li' can be used for treating conventional proton-adaptive cancers, and can also effectively cover superficial tumors such as melanoma, head and neck tumors of five sense organs, prostate tumors, breast tumors and the like, thereby achieving the purpose of one machine with multiple purposes.
Disclosure of Invention
Aiming at the problems, the invention provides a general light-ion tumor treatment device, which adopts the combination of a miniature high-charge state full-permanent-magnet ECR ion source, a high-working-frequency linear injector with an external magnetic focusing structure, a variable-convex-track synchrotron and a treatment terminal, improves from the aspects of beam supply type, ion source structure, linear injector structure, injection method and the like, widens the treatment range of cancer types, and reduces the occupied area and the manufacturing cost of the system.
In order to achieve the purpose, the invention adopts the following technical scheme:
the invention provides a general type light ion tumor treatment device, which comprises the following components:
through the combination of a compact ECR ion source, a high-working-frequency linear injector, a variable-convex-track synchrotron and a treatment terminal, not only protons but also treatment can be accelerated3He、4He、7Li and light ions with atomic numbers of 4-20, so that the accelerator can not only realize the treatment of conventional protons adapting to cancer types, but also effectively cover shallow tumors;
the ion source comprises a shell, and an air inlet pipeline, an evaporation furnace and a waveguide tube which are arranged in the shell, wherein the air inlet pipeline is used for conveying gas into the shell, the evaporation furnace is used for evaporating solid molecules or atoms to generate gas, the waveguide tube is used for feeding microwave power into the shell, and electrons collide with gas molecules under the combined action of a magnetic field and microwaves to generate light ion beam current;
the linear injector is connected with the leading-out end of the ion source through a low-energy beam transport line and comprises an acceleration cavity and a magnetic focusing element sleeved outside the acceleration cavity, and the magnetic focusing element is used for generating a longitudinal magnetic field and providing extra focusing force for light ion beam current;
the input end of the synchrotron is connected with the output end of the linear injector through an intermediate energy beam transport line, the beam input end of the synchrotron is provided with an injection convex rail magnet and an injection static deflection plate, the injection convex rail magnet is used for raising a circulating beam balance track, so that the beam deflected by the injection static deflection plate enters the annular acceptance degree and gradually descends in the injection process, the loss caused by the fact that the returned beam hits the injection static deflection plate is avoided, meanwhile, the smearing and filling of the beam in a phase space are completed, after the injection is completed, the light ion beam is accelerated to reach the energy required by treatment, and the light ion beam is led out to the high energy beam transport line through an extraction system;
and the treatment terminal is connected with the synchrotron through the high-energy beam transport line and is used for enabling the light ion beam to accurately reach the position of the tumor cell.
The light ion tumor treatment device is characterized in that an injection end magnetic ring and a leading-out end magnetic ring are respectively arranged at an injection end and a leading-out end of the shell, a hexapole magnetic ring is arranged between the injection end magnetic ring and the leading-out end magnetic ring, an arc cavity is defined by the injection end magnetic ring, the hexapole magnetic ring and the leading-out end magnetic ring together, the air inlet pipeline, the evaporation furnace, the waveguide tube and the injection soft iron are arranged in the arc cavity close to the injection end of the shell, and a leading-out electrode is arranged in the arc cavity close to the leading-out end of the shell and used for leading light ion beams out of the ion source.
Preferably, the light ion tumor treatment device is characterized in that a longitudinal electric field generated by the acceleration cavity provides an acceleration effect for the light ion beam, a generated transverse electric field provides a partial focusing effect for the light ion beam, and the magnetic focusing element sleeved outside the acceleration cavity provides another partial focusing effect for the light ion beam.
In the light ion tumor treatment device, preferably, a beam input end of the synchrotron is further provided with an injection cutting magnet, the injection cutting magnet is used for deflecting the beam to be close to an injection track, and the injection electrostatic deflection plate is used for further deflecting the beam transmitted by the injection cutting magnet into a beam acceptance.
In a second aspect, the present invention provides a method for operating the above-mentioned conventional light ion tumor therapy device, comprising the following steps:
a when light ions needing gas ionization are treated, gas is conveyed into the arc cavity through the gas inlet pipeline, microwave power is fed into the arc cavity through the waveguide tube, electrons generate cyclotron resonance under the combined action of a magnetic field and microwaves, the speed is increased continuously, after the electrons collide with gas molecules, outer layer electrons of the gas molecules are stripped, light ions are generated, the light ions are led out under the action of the leading-out electrode and conveyed into the linear injector through the low-energy beam transport line;
b, when the solid molecules or atoms are required to be ionized to light ions for treatment, evaporating the solid molecules or atoms through the evaporation furnace to generate steam and sending the steam into the arc cavity, feeding microwave power into the arc cavity by using the waveguide tube, generating cyclotron resonance by electrons under the combined action of a magnetic field and microwaves at an increasing speed, stripping outer-layer electrons of the steam molecules or atoms after colliding with the steam to generate charged light ions, leading the charged light ions out under the action of the leading-out electrode, and conveying the charged light ions into the linear injector through the low-energy beam transport line;
c, injecting the light ion beam transmitted by the low-energy beam transport line into the accelerating cavity in a radial matching manner, forming, bunching and accelerating the light ion beam by a longitudinal high-frequency electric field generated by the accelerating cavity, focusing the light ion beam by a transverse electric field and a focusing magnetic field generated by the magnetic focusing element, leading the light ion beam to gradually reach the energy required by the injection of the synchrotron, and leading the light ion beam out of the outlet of the linear injector and then conveying the light ion beam into the synchrotron through the medium-energy beam transport line;
d, after light ions are conveyed to the synchrotron, beam current is deflected by the injection cutting magnet and the injection electrostatic deflection plate, the beam current is gradually close to the synchrotron, the included angle between the beam current and a central track is gradually reduced, and an injection preparation state is achieved; in the injection process, the local convex rail magnet gradually descends, injected beam current is smeared from inside to outside in a horizontal phase space, and the beam current gradually fills the whole acceptance;
and e, after the injection is finished, accelerating the light ion beam to reach the energy required by treatment, transmitting the light ion beam to the high-energy beam line through the extraction system, and distributing the light ion beam to the treatment terminal through the high-energy beam line.
Due to the adoption of the technical scheme, the invention has the following advantages:
1. the treatment device of the present invention may be directed to protons and3He、4He、7various light ions such as Li and the like are accelerated, and not only can the proton be utilized for the whole body treatment, but also the proton can be used3He、4He、7The light ion beam current such as Li is used for treating superficial (less than or equal to 8cm) tumors to improve the curative effect, such as melanoma, head and neck tumors of five sense organs, prostate tumors, breast tumors and the like, and various ions supplement each other, thereby widening the range of tumor indications of the proton accelerator. Meanwhile, the treatment device has low manufacturing cost and is compatible with a pure proton treatment device in scale, thereby being a general precise external irradiation treatment device.
2. The ion source of the device is different from the traditional proton accelerator, is different from a special carbon beam heavy ion accelerator, and adopts a compact high-charge state full-permanent-magnet ECR ion source, and has the biggest characteristics of simple structure, no injection end vacuum chamber, compact structure, and the diameter of the ion source is only 0.1-0.2 meter, while the diameter of the conventional ECR ion source is 0.4-0.8 meter. And the ion source can generate H with high efficiency2 +And can generate He in a high charge state2+And metallic Li3+And the like.
3. Different from conventional H2 +Or H-The linear injector in the device is designed based on various light ion beam currents, adopts a high working frequency scheme with an external magnetic focusing structure, and can provide high-quality H2 +Bundle, and also has high-efficiency acceleration3He、4He、7The capability of light ion beams such as Li, and the like, and the injector adopts the working frequency of 500-900 MHz, so that the acceleration gradient is higher, the equipment size is more compact, and the occupied area of the device is further reduced.
4. Conventional proton synchrotron mostly injects H2 +Or H-Ions are implanted in a stripping mode, while the implantation accelerator adopts a variable convex track multi-circle implantation method which can simultaneously carry outAnd the high-efficiency injection of various light ion beams is realized. Space charge effects are the main reasons for using the variable-land-rail scheme, e.g. the mass-to-charge ratio of protons is 1, the injection flow is about 200euA strong,7Li3+the mass-to-charge ratio of the beam current was 7/3, the injection current was about 30euA stronger, and the space charge effect between the same number of injections was 15 times different. To reduce space charge effects of proton beams, increase7Li3+The invention relates to a device for injecting accumulated particle number by beam current, which adopts a multi-circle injection method of variable convex tracks: for the7Li3+When the beam with weak space charge effect is adopted, the slowly-descending convex rail is adopted, so that the acceptance of the synchrotron is filled as far as possible by a high-density core of the beam, and the cumulative beam intensity is improved; for beams with strong space charge effects such as protons, the fast-descending convex rail is adopted, so that the beams are distributed in a phase space as uniformly as possible, and the beam loss caused by the nonlinear space charge effect is reduced.
Drawings
FIG. 1 is a schematic diagram of a light ion tumor treatment device according to an embodiment of the present invention;
fig. 2 is a schematic diagram of the overall structure of the micro high-charge-state all-permanent-magnet ECR ion source according to the embodiment of the invention;
FIG. 3 is a schematic diagram of the overall structure of the linear injector with external magnetic focusing structure according to the embodiment of the present invention;
fig. 4 is a schematic diagram of multi-turn injection of beams in the synchrotron according to the embodiment of the present invention;
fig. 5 (a) to fig. 5 (f) show the phase space evolution during the beam multi-turn implantation process provided by the embodiment of the present invention;
FIG. 6 shows protons provided in this embodiment of the present invention7Li3+Injecting a convex rail magnet descending curve;
FIG. 7 (a) shows a proton-implanted phase space according to this embodiment of the present invention, and FIG. 7 (b) shows a proton-implanted phase space according to this embodiment of the present invention7Li3+Injecting a phase space;
the respective symbols in the figure are as follows:
1-an air inlet duct; 2-an evaporation furnace; 3-a waveguide; 4-injecting soft iron; 5-injection end magnetic ring; 6-a hexapole magnetic ring; 7-leading-out end magnetic ring; 8-leading out electrodes; 9-an acceleration chamber; 10-a magnetic focusing element; 11-a housing; 12-1 to 12-4 are injection convex rail magnets.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, the technical solutions of the present invention are described clearly and completely below, and it is obvious that the described embodiments are some, not all embodiments of the present invention. All other embodiments, which can be obtained by a person skilled in the art without any inventive step based on the embodiments of the present invention, are within the scope of the present invention.
Unless defined otherwise, technical or scientific terms used herein shall have the ordinary meaning as understood by one of ordinary skill in the art to which this invention belongs. The use of "first," "second," and similar terms in the present application do not denote any order, quantity, or importance, but rather the terms are used to distinguish one element from another. The word "comprising" or "comprises", and the like, means that the element or item listed before the word covers the element or item listed after the word and its equivalents, but does not exclude other elements or items. The terms "connected" or "coupled" and the like are not restricted to physical or mechanical connections, but may include electrical connections, whether direct or indirect.
The invention provides a general type light ion tumor treatment device, which adopts the combination of a miniature high-charge state full-permanent-magnet ECR ion source, a high-working-frequency linear injector with an external magnetic focusing structure, a variable-convex-track synchrotron and a treatment terminal, improves from the aspects of beam supply type, ion source structure, linear injector structure, injection method and the like, widens the treatment range of cancer types, and reduces the occupied area and the manufacturing cost of the system.
As shown in fig. 1-3, the present invention provides a general type of light ion tumor treatment device, comprising:
the ion source comprises a cylindrical shell 11, wherein an injection end magnetic ring 5 and a leading-out end magnetic ring 7 are respectively arranged at an injection end and a leading-out end of the shell 11, a hexapole magnetic ring 6 is arranged between the injection end magnetic ring 5 and the leading-out end magnetic ring 7, an arc cavity is jointly defined by the injection end magnetic ring 5, the hexapole magnetic ring 6 and the leading-out end magnetic ring 7, an air inlet pipeline 1, an evaporation furnace 2, a waveguide tube 3 and injection soft iron 4 are arranged in the arc cavity close to the injection end of the shell 11, the air inlet pipeline 1 is connected with a gas storage tank and used for conveying gas into the arc cavity, the evaporation furnace 2 is used for evaporating solid molecules or atoms to generate gas, the waveguide tube 3 is used for feeding microwave power into the arc cavity, electrons generate cyclotron resonance under the combined action of a magnetic field and microwaves, the speed is continuously increased, and after the electrons collide with the gas molecules, the outer layer electrons of the gas molecules are stripped to generate light ions; an extraction electrode 8 is arranged in an arc cavity close to the extraction end of the shell 11 and is used for extracting light ion beams out of an ion source;
the linear injector is characterized in that the input end of the linear injector is connected with the output end of the ion source through a low-energy beam transport line, the linear injector comprises an acceleration cavity 9 and a magnetic focusing element 10 sleeved outside the acceleration cavity 9, and the magnetic focusing element 10 is used for generating a longitudinal magnetic field and providing extra focusing force for light ion beam current;
the input end of the synchrotron is connected with the output end of the linear injector through an intermediate energy beam transport line, and the beam input end of the synchrotron is provided with an injection cutting magnet, injection convex rail magnets 12-1-12-4 and an injection static deflection plate;
and the treatment terminal is connected with the synchrotron through the high-energy beam transport line and is used for enabling the light ion beam to accurately reach the position of the tumor cell.
Fig. 4 is a schematic diagram of a multi-turn beam injection process, in which the beam is deflected by an injection cutting magnet and an injection electrostatic deflection plate, and is gradually positioned close to a synchrotron, and the included angle between the beam and a central track is gradually reduced, so as to achieve an injection preparation state. At the moment, the convex rail magnets 12-1-12-4 are started, the central track of the synchrotron is locally protruded, and beam current is injected into the acceptance of the synchrotron. In the injection process, the local convex rail magnets 12-1-12-4 gradually descend, injected beams are smeared from inside to outside in the horizontal phase space, and the beams gradually fill the whole acceptance. Fig. 5 (a) to 5 (f) show the phase space evolution during the multi-turn injection. The circle in the figure represents the acceptance of the synchrotron, the line in the vertical direction at the right side of the center of the circle represents the injection electrostatic deflection plate, the ellipse at the right side of the injection electrostatic deflection plate represents the injection beam group, the positions of the injection electrostatic deflection plate and the injection beam group are kept unchanged in the injection process, and different colors of the injection beam group represent different turns of injection. In the injection process, the convex rail magnet (namely the circle center) continuously descends, and the injected beam is smeared from the inner side to the outer side of the phase space to gradually fill the whole phase space.
The space charge effect is that the beam ions have charges, so that the ions or the ions and the wall of the vacuum tube have the effect of the charges, and the normal movement of the beam ions is interfered. The main factors influencing the space charge effect include energy, mass-to-charge ratio and strong injection flow, and the beam space charge effect is more remarkable when the energy is lower, the mass-to-charge ratio is lower and the injection flow is higher. The light ion tumor treatment device adopts the linear accelerator as the injector, the energy of different beams is basically consistent, but the difference between the mass-to-charge ratio and the injection flow is larger. For example, the proton mass to charge ratio is 1, the injection flow is about 200euA strong,7Li3+the mass-to-charge ratio of the beam current was 7/3, the injection current was about 30euA stronger, and the space charge effect between the same number of injections was 15 times different. To reduce space charge effects of proton beams, increase7Li3+The number of particles is accumulated by injecting the beam, and the light ion tumor treatment device adopts a multi-circle injection method of changing convex tracks. For the7Li3+When the beam with weak space charge effect is adopted, slowly-descending convex rail magnets 12-1-12-4 are adopted, so that the acceptance of the synchrotron is filled with high-density cores of the beam as much as possible, and the cumulative beam intensity is improved; for beams with strong space charge effects such as protons, fast-descending convex rail magnets 12-1-12-4 are adopted, so that the beams are distributed in a phase space as uniformly as possible, and the beam loss caused by the nonlinear space charge effect is reduced.
FIG. 6 shows protons and7Li3+the number of turns in the graph indicates the number of turns of beam injection and the height of the convex rail is usedThe percentage shows that the convex track magnets 12-1 to 12-4 are linearly decreased firstly and then exponentially decreased in the injection process. The proton has strong space charge effect, less injection turns, fast descending speed of the convex rail magnets 12-1 to 12-4,7Li3+more turns are required to be injected to increase the flow intensity, and the descending speed of the convex track magnets 12-1 to 12-4 is slow.
In FIG. 7, (a) and (b) are proton and7Li3+the horizontal phase space at the completion of the injection. The proton beam injection flow intensity is high, the mass-to-charge ratio is small, the space charge effect is strong, the injection turns are few (8 circles are injected in the figure), the descending speed of the convex rail magnet 12-1-12-4 is high, and a single circle of beam can be distinguished after the injection is finished;7Li3+the beam injection flow intensity is weak, the mass-to-charge ratio is large, the space charge effect is weak, the injection accumulated flow intensity is increased by increasing the number of injection turns, the convex rail magnets 12-1-12-4 descend slowly, and single-turn beams cannot be distinguished in a phase space after injection is completed.
In this embodiment, it is preferable that the atomic number of the gas or solid molecules or atoms transported by the gas inlet duct 1 is not more than 20.
In the present embodiment, preferably, the gas delivered by the gas inlet pipe 1 includes hydrogen, helium, methane, or a gas containing light ions; solid molecules or atoms include simple substances (e.g., lithium metal) or oxides.
In the present embodiment, the diameter of the housing 11 is preferably 0.1 to 0.2 m.
In this embodiment, the microwave power fed into the waveguide 3 is preferably 10 to 18 GHz.
In this embodiment, the linear injector preferably has an operating frequency of 500 to 900MHz, and the magnetic focusing element 10 is a solenoid. The acceleration chamber 9 in the linear injector provides the longitudinal electric field needed to accelerate the particles while providing a certain focusing effect. The linear injector adopts the working frequency of more than 500-900 MHz, has higher acceleration gradient, reduces the size of an acceleration cavity by about half compared with the conventional linear injector, and is favorable for further reducing the floor area of the device. However, the high operating frequency weakens the transverse electric field focusing ability, and after the external magnetic focusing element 10 (solenoid) is introduced, the transverse electric field focusing ability is weakenedThe injector has sufficient focusing power to ensure that it can provide high quality H2 +Bundle, and also has high-efficiency acceleration3He、4He、7Li, etc. light ion beam.
The invention also provides an operation method of the general type light ion tumor treatment device, which comprises the following steps:
a, when light ions needing gas ionization are treated, gas is conveyed into an arc cavity through a gas inlet pipeline 1, microwave power is fed into the arc cavity through a waveguide tube 3, electrons generate cyclotron resonance under the combined action of a magnetic field and microwaves, the speed is increased continuously, after the electrons collide with gas molecules, outer-layer electrons of the gas molecules are stripped, light ions are generated, the light ions are led out under the action of a leading-out electrode 8 and are conveyed into a linear injector through a low-energy beam transport line;
b, when the solid molecules or atoms are required to be ionized to light ions for treatment, evaporating the solid molecules or atoms through the evaporation furnace 2 to generate steam, sending the steam into the arc cavity, feeding microwave power into the arc cavity by using the waveguide tube 3, generating cyclotron resonance by electrons under the combined action of a magnetic field and microwaves at an increasing speed, stripping electrons on the outer layer of the steam molecules or atoms after colliding with the steam to generate charged light ions, leading the charged light ions out under the action of the leading-out electrode 8, and conveying the charged light ions into the linear injector through a low-energy beam transport line;
c, injecting light ion beams transmitted by a low-energy beam fortune line into an acceleration cavity 9 in a radial matching manner, forming, bunching and accelerating the light ion beams by a longitudinal high-frequency electric field generated by the acceleration cavity 9, focusing the light ion beams by a transverse electric field and a focusing magnetic field generated by a magnetic focusing element, leading the light ion beams to gradually reach the energy required by the injection of the synchrotron, and leading the light ion beams to the synchrotron through the medium-energy beam fortune line after being led out from an outlet of the linear injector;
d, after light ions are conveyed to the synchrotron, deflecting the beams through the injection cutting magnet and the injection static deflection plate, enabling the beams to be gradually close to the synchrotron, gradually reducing the included angle between the beams and the central track to achieve an injection preparation state, starting the injection convex track magnets 12-1-12-4 at the moment, locally protruding the central track of the synchrotron, and enabling the injected beams to enter the acceptance of the synchrotron; in the injection process, the local convex rail magnets 12-1-12-4 gradually descend, injected beams are smeared from inside to outside in a horizontal phase space, and the beams gradually fill the whole acceptance;
and e, after the injection is finished, the light ion beam current is accelerated to reach the energy required by the treatment, and is transmitted to a high-energy beam line through the extraction system, and then the light ion beam current is distributed to a treatment terminal through the high-energy beam line to carry out the cancer treatment.
Finally, it should be noted that: the above examples are only intended to illustrate the technical solution of the present invention, but not to limit it; although the present invention has been described in detail with reference to the foregoing embodiments, it will be understood by those of ordinary skill in the art that: the technical solutions described in the foregoing embodiments may still be modified, or some technical features may be equivalently replaced; and such modifications or substitutions do not depart from the spirit and scope of the corresponding technical solutions of the embodiments of the present invention.

Claims (4)

1. A general type of light ion tumor treatment device, characterized in that:
through the combination of a compact ECR ion source, a high-working-frequency linear injector, a variable-convex-track synchrotron and a treatment terminal, not only protons but also treatment can be accelerated3He、4He、7Li and light ions with atomic numbers of 4-20, so that the accelerator can not only realize the treatment of conventional protons adapting to cancer types, but also effectively cover shallow tumors;
the ion source comprises a shell (11), and a gas inlet pipeline (1), an evaporation furnace (2) and a waveguide tube (3) which are arranged in the shell (11), wherein the gas inlet pipeline (1) is used for conveying gas into the shell (11), the evaporation furnace (2) is used for evaporating solid molecules or atoms to generate gas, the waveguide tube (3) is used for feeding microwave power into the shell (11), and electrons collide with the gas molecules under the combined action of a magnetic field and microwaves to generate light ion beam current; the diameter of the vacuum chamber without the injection end of the ion source is 0.1-0.2 m;
the linear implanter is characterized in that the input end of the linear implanter is connected with the leading-out end of the ion source through a low-energy beam transport line, the linear implanter comprises an accelerating cavity (9) and a magnetic focusing element (10) sleeved outside the accelerating cavity (9), and the magnetic focusing element (10) is used for generating a longitudinal magnetic field and providing an additional focusing force for light ion beam current; the working frequency of the linear injector is 500-900 MHz, and the magnetic focusing element (10) is a solenoid;
the input end of the synchrotron is connected with the output end of the linear injector through an intermediate energy beam transport line, the synchrotron adopts a variable convex rail multi-circle injection method, the beam input end of the synchrotron is provided with injection convex rail magnets (12-1-12-4) and injection static deflection plates, the injection convex rail magnets (12-1-12-4) are used for raising a circulating beam balance track, so that beams deflected by the injection static deflection plates enter a ring acceptance degree, and gradually descend in the injection process, thereby avoiding the loss of returning beams hitting the injection static deflection plates, completing the smearing and filling of the beams in a phase space, and after the injection is completed, light ion beams are accelerated to reach the energy required by treatment and are led out to the high energy beam transport line through an extraction system;
the treatment terminal is connected with the synchrotron through the high-energy beam transport line and is used for enabling the light ion beam to accurately reach the position of the tumor cell;
the ion source is characterized in that an injection end magnetic ring (5) is arranged at an injection end of the shell (11), a leading-out end magnetic ring (7) is arranged at a leading-out end of the shell (11), a hexapole magnetic ring (6) is arranged between the injection end magnetic ring (5) and the leading-out end magnetic ring (7), an arc cavity is defined by the injection end magnetic ring (5), the hexapole magnetic ring (6) and the leading-out end magnetic ring (7) together, the air inlet pipeline (1), the evaporation furnace (2), the waveguide tube (3) and the injection soft iron (4) are arranged in the arc cavity close to the injection end of the shell (11), and a leading-out electrode (8) is arranged in the arc cavity close to the leading-out end of the shell (11) and used for leading out light ion beams to the ion source.
2. The light ion tumor therapy device according to claim 1, wherein the longitudinal electric field generated by the acceleration chamber (9) provides an acceleration effect for the light ion beam, the generated transverse electric field provides a partial focusing effect for the light ion beam, and the magnetic focusing element (10) sleeved outside the acceleration chamber (9) provides another partial focusing effect for the light ion beam.
3. The light ion tumor treatment apparatus according to claim 1, wherein the beam input end of the synchrotron is further provided with an injection cutting magnet for deflecting the beam close to the injection track, and the injection electrostatic deflection plate is used for further deflecting the beam transmitted through the injection cutting magnet into the beam acceptance.
4. A method of operating the light ion tumor treatment apparatus of claim 3, comprising the steps of:
a, when light ions needing gas ionization are treated, gas is conveyed into the arc cavity through the gas inlet pipeline (1), microwave power is fed into the arc cavity through the waveguide tube (3), electrons generate cyclotron resonance under the combined action of a magnetic field and microwaves, the speed is increased continuously, after the electrons collide with gas molecules, outer-layer electrons of the gas molecules are stripped to generate light ions, and the light ions are led out under the action of the leading-out electrode (8) and conveyed into the linear injector through the low-energy beam transport line;
b, when the solid molecules or atoms are required to be ionized to light ions for treatment, the solid molecules or atoms are evaporated through the evaporation furnace (2) to generate steam and are sent into the arc cavity, microwave power is fed into the arc cavity through the waveguide tube (3), electrons generate cyclotron resonance under the combined action of a magnetic field and microwaves, the speed is increased continuously, after the electrons collide with the steam, the outer electrons of the steam molecules or atoms are stripped to generate charged light ions, and the charged light ions are led out under the action of the leading-out electrode (8) and are conveyed into the linear injector through the low-energy beam transport line;
c, light ion beams transmitted by the low-energy beam transport line are injected into the accelerating cavity (9) in a radial matching mode, a longitudinal high-frequency electric field generated by the accelerating cavity (9) shapes, bunches and accelerates the light ion beams, a transverse electric field and a focusing magnetic field generated by the magnetic focusing element (10) focus the light ion beams, the light ion beams gradually reach the energy required by the injection of the synchrotron, and are conveyed into the synchrotron through the medium-energy beam transport line after being led out from the outlet of the linear injector;
d, after light ions are conveyed to the synchrotron, beam current is deflected by the injection cutting magnet and the injection static deflection plate, the beam current is gradually close to the synchrotron, the included angle between the beam current and a central track is gradually reduced, and the beam current reaches an injection preparation state, at the moment, the injection convex track magnet (12-1-12-4) is started, the central track of the synchrotron is locally protruded, and the injected beam current enters the acceptance of the synchrotron; in the injection process, the local convex rail magnets (12-1-12-4) gradually descend, injected beam current is smeared from inside to outside in a horizontal phase space, and the beam current gradually fills the whole acceptance;
and e, after the injection is finished, accelerating the light ion beam to reach the energy required by treatment, transmitting the light ion beam to the high-energy beam line through the extraction system, and distributing the light ion beam to the treatment terminal through the high-energy beam line.
CN202011479052.3A 2020-12-15 2020-12-15 Popular type light ion tumor treatment device Active CN112704818B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011479052.3A CN112704818B (en) 2020-12-15 2020-12-15 Popular type light ion tumor treatment device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011479052.3A CN112704818B (en) 2020-12-15 2020-12-15 Popular type light ion tumor treatment device

Publications (2)

Publication Number Publication Date
CN112704818A CN112704818A (en) 2021-04-27
CN112704818B true CN112704818B (en) 2022-02-11

Family

ID=75543258

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011479052.3A Active CN112704818B (en) 2020-12-15 2020-12-15 Popular type light ion tumor treatment device

Country Status (1)

Country Link
CN (1) CN112704818B (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113382529B (en) * 2021-06-08 2024-03-29 兰州科近泰基新技术有限责任公司 Superconducting ion annular synchrotron
CN113209501B (en) * 2021-06-08 2023-06-20 兰州科近泰基新技术有限责任公司 Miniaturized ion ray treatment device

Family Cites Families (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ATE392797T1 (en) * 2001-02-05 2008-05-15 Schwerionenforsch Gmbh DEVICE FOR PRE-ACCELERATION OF ION BEAMS FOR USE IN A HEAVY ION BEAM APPLICATION SYSTEM
KR100978618B1 (en) * 2007-12-12 2010-08-30 가부시키가이샤 나노빔 Magnetic field strength compensation method and device of Electron Cyclotron Resonance ion source
CN101631420B (en) * 2009-01-12 2010-10-13 中国科学院近代物理研究所 Accelerator used for cancer therapy with protons-heavy ion beams
KR101403662B1 (en) * 2011-12-29 2014-06-09 한국원자력연구원 Proton Therapy Facility
CN102623128B (en) * 2012-04-01 2014-06-11 中国科学院近代物理研究所 Superconducting hybrid magnet device for generating minimum B magnetic field
CN102793979B (en) * 2012-07-28 2015-05-20 中国科学院近代物理研究所 Proton or heavy ion beam cancer treatment device
CN202982960U (en) * 2012-07-28 2013-06-12 中国科学院近代物理研究所 Proton or heavy ion beam cancer therapy device
KR101618812B1 (en) * 2013-12-26 2016-05-10 기초과학연구원 arrangement method of magnet for Electron Cyclotron Resonance Ion Source
JP6624482B2 (en) * 2014-07-29 2019-12-25 俊 保坂 Micro accelerator and micro mass spectrometer
CN204906839U (en) * 2015-09-16 2015-12-23 中国工程物理研究院流体物理研究所 Direct injection type ion beam accelerating device
CN106879158B (en) * 2017-03-16 2019-05-28 东莞中子科学中心 Medical proton linear accelerator
CN108811297A (en) * 2017-05-03 2018-11-13 王云 A kind of medical proton heavy ion avcceleration
CN108257845A (en) * 2018-03-22 2018-07-06 大连交通大学 A kind of ion source for electron cyclotron resonance
CN208590144U (en) * 2018-06-29 2019-03-08 惠州离子科学研究中心 Linear accelerator and synchrotron
CN108566721B (en) * 2018-06-29 2024-01-05 惠州离子科学研究中心 Linear accelerator and synchrotron
CN109640508A (en) * 2019-01-28 2019-04-16 清华大学 A kind of vertical magnetic mode shift pipe linear accelerator of the focusing interdigital of separation
CN109786205B (en) * 2019-01-30 2021-02-05 中国科学院近代物理研究所 Electron cyclotron resonance ion source
CN110113859A (en) * 2019-06-12 2019-08-09 中广核中科海维科技发展有限公司 A kind of low energy irradiation linear accelerator

Also Published As

Publication number Publication date
CN112704818A (en) 2021-04-27

Similar Documents

Publication Publication Date Title
CN112704818B (en) Popular type light ion tumor treatment device
CN101631419B (en) Method and device for implanting heavy ion beams into synchrotron
JP2004525486A (en) A device that generates and selects ions for use in heavy ion cancer treatment facilities
GB936137A (en) Ion source with space charge neutralization
CN105810537A (en) X-waveband high-impedance relativity theory klystron amplifier adopting annular beam cold cathode
CN111408070A (en) Multi-ion treatment system based on isochronous cyclotron
CN112822830B (en) Proton and light ion synchrotron, treatment system containing same and application
CN116489864B (en) Compact strong current H 2+ Superconducting cyclotron
US20230199935A1 (en) Charged particle beam injector and charged particle beam injection method
CN115279008A (en) Medical ion linear accelerator
CN101631421A (en) Method and device for accumulating beams in synchrotron for cancer therapy with heavy ions
CN114540777A (en) Ion implantation method combined with magnetron sputtering
CN111370286A (en) Plasma source for therapeutic equipment and method of use thereof
CN212677437U (en) Synchronous acceleration system
Zhang et al. H− cusp source development for 100 MeV compact cyclotron at China Institute of Atomic Energy
Andreev et al. Reconstruction of light and polarized ion beam injection system of JINR Nuclotron-NICA accelerator complex
Degiovanni Future trends in linacs
Schlitt et al. Design of a carbon injector for a medical accelerator complex
Thieberger Possible use of synchrotrons as post-acceleration boosters for tandems
CN117042278A (en) Medical miniaturized ion accelerator
Saitoh et al. Development of 13 GHz compact electron cyclotron resonance ion source
Kester et al. The REX-ISOLDE LINAC
Papash et al. On Commercial Cyclotron of Intense Proton Beam of 30 MeV Energy Range
Alonso et al. New Opportunities for Medical Isotope Production using the IsoDAR Cyclotron
Efremov et al. Ion source DECRIS-3

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant