JP4435059B2 - Particle beam cancer treatment system and irradiation method - Google Patents

Description

  The present invention relates to a particle beam cancer treatment system and an irradiation method.

The conventional particle beam cancer treatment system described in Patent Document 1 uses a ridge filter having a peak portion and a valley portion to form a predetermined distribution in the particle beam energy, and the depth of the particle beam reaching the irradiated body. The dose distribution in the depth direction is formed so as to have a predetermined width.
JP-A-11-285544

  The above particle beam cancer treatment system includes a ridge filter having a periodic thickness distribution for giving the particle beam a predetermined energy distribution. Depending on the position of the ridge filter, the kinetic energy of the particle beam that has passed through varies. Therefore, if the thickness distribution of the ridge filter and the size of the region having the thickness distribution are set to a predetermined value, the energy of the particle beam after passing through the ridge filter has a predetermined distribution as a whole. .

  After the particle beam passes through the ridge filter, if the particle beam is sufficiently mixed with each other due to the angular distribution in the traveling direction of the particle beam and reaches the irradiated region, a uniform irradiation dose at the end of the range of the irradiated region Distribution can be formed. Such a condition is usually satisfied when the particle beam is a proton beam. However, when the particle beam is a particle beam that hardly causes angular dispersion in the traveling direction (for example, a carbon beam), the particle beam cannot obtain a sufficient scattering angle after passing through the ridge filter. In that case, the particle beam that passes through the thinnest part of the ridge filter is concentrated near the projection position in the straight direction toward the irradiated region of the ridge filter. As a result, there arises a problem that, at the deepest position of the irradiation region, the lateral dose distribution remains non-uniformity corresponding to the periodic pattern of the thickness distribution of the ridge filter.

  An object of the present invention is to form a uniform dose distribution at the end of the range of an irradiation field in a cancer treatment system using a particle beam.

The present invention has been made to achieve the above object. The particle beam cancer treatment system according to the present invention comprises:
A particle beam cancer treatment system having particle beam irradiation means,
The particle beam irradiation means,
A ridge filter having a periodic thickness distribution in which the energy lost depending on the position through which the particle beam passes;
In-irradiation position changing means for changing the spatial position of the ridge filter on a plane substantially orthogonal to the traveling direction of the particle beam during particle beam irradiation is provided.

  In the particle beam cancer treatment system according to the present invention, a uniform dose distribution can be formed in the depth direction at the end of the range of the irradiation field. Moreover, since the position movement of the ridge filter during irradiation can be realized by a simple mechanism, both treatment accuracy and throughput can be improved.

Embodiment 1 FIG.
FIG. 1 is a longitudinal sectional view of particle beam irradiation means of the particle beam cancer treatment system according to Embodiment 1 of the present invention. FIG. 2 is a perspective view of the ridge filter 10 of the particle beam cancer treatment system according to Embodiment 1 of the present invention. FIG. 3 is an enlarged cross-sectional view of the ridge filter 10 of the particle beam cancer treatment system according to Embodiment 1 of the present invention.

  In FIG. 1, a particle beam 2 obtained from a particle beam generator (not shown) is irradiated from a transmission source point 4 to an irradiated object 24. The particle beam 2 is expanded by the first expansion unit 6 and further expanded by the second expansion unit 8. The expanded particle beam 2 passes through the ridge filter 10. The particle beam 2 that has passed through the ridge filter 10 is shaped into a predetermined shape by the collimator 22 and then irradiated onto the irradiated object 24.

  FIG. 2 is a perspective view of a bar ridge filter which is a typical configuration example of a ridge filter. FIG. 3 is an enlarged view of an example of the cross-sectional shape of a plurality of ridges in the bar ridge filter. 2 and 3, as will be described later, the ridge filter 10 is rotated by the rotating shaft 32 during particle beam irradiation on the installation plane of the ridge filter 10.

  Next, the operation of the particle beam cancer treatment system according to Embodiment 1 will be described. First, a particle beam (for example, a carbon beam) is generated from a particle beam generator (not illustrated) (for example, from an ion source that generates carbon beam ions). It is composed of an electromagnet or the like after (for example) a carbon beam is accelerated to a kinetic energy corresponding to an underwater range of 20 cm to 30 cm by a particle beam acceleration means (not shown) composed of a charged particle accelerator or the like. The light beam is incident on the particle beam irradiation unit by a particle beam transport unit (not shown) including a beam optical system.

  As described above, the particle beam 2 incident on the particle beam irradiation means is, for example, a carbon beam having a kinetic energy of about several hundred MeV per nucleon. The particle beam 2 incident on the particle beam irradiation means usually has a cross-sectional size of less than 1 cm. In order to irradiate a tumor or the like with such a particle beam, it is necessary to scan by moving the position of the particle beam or to enlarge the beam size. In the particle beam irradiation apparatus according to the present invention, the beam size is enlarged.

  The particle beam 2 is incident on the first expanding means 6 composed of a scatterer such as lead or tungsten, and is scattered by electrons and atoms in the scatterer. After passing through the first enlargement means 6, the traveling direction, which is almost concentrated in the forward direction of the particle beam 2, is dispersed, and the particle beam 2 has a predetermined angular distribution. Therefore, when viewed from the position of the irradiated object 24, the cross-sectional size of the particle beam 2 is expanded to several centimeters or more.

  A sufficiently large beam size may not be obtained with only the first expansion means 6 composed of the above scatterers. Therefore, the particle beam is further expanded by the second expansion means 8 composed of a deflection electromagnet. The second expansion means 8 may be composed of two deflection electromagnets whose magnetic field directions are orthogonal to each other. The two deflecting electromagnets are excited from sin ωt and cos ωt AC power sources whose excitation current patterns are synchronized with each other. Therefore, the particle beam 2 passing through the second expansion means 8 is deflected to draw a circle. . Such an enlarging means is an existing prior art and is called a wobbling electromagnet, and the radius in the circle is called a wobbling radius.

  By adjusting the scattering radius of the particle beam cross section by the first magnifying means 6 and the wobbling radius by the second magnifying means 8 to a predetermined ratio, the irradiated body 24 is substantially flat in the lateral direction near the center of the irradiated area. Particle beam distribution can be formed. The non-uniform region of the particle beam distribution that is separated from the center of the irradiation region by a predetermined distance is removed by the collimator 22. The collimator 22 is composed of a plurality of leaf-like plates formed of copper having a thickness that does not allow the particle beam 2 to pass through. The arrangement of the leaf-like plates is controlled so that the opening of the collimator 22 exhibits an arbitrary two-dimensional shape. If this two-dimensional shape is matched to the shape of the tumor, an irradiation field is formed in accordance with the tumor existing range.

  By the way, in general, the depth (range) of the particle beam entering the human body is determined by the energy, and suddenly releases energy and stops near the end of the range. This phenomenon is called Bragg Peak. This phenomenon is used to kill tumor cells at a suitable depth from the body surface. By the way, the tumor has a thickness in the depth direction. Therefore, in order to uniformly irradiate the tumor (lesion) with the particle beam, an operation is required in which the Bragg peak is uniformly expanded in the thickness direction of the tumor. This uniformly expanded dose is referred to as SOBP (Speed-Out Bragg Peak).

  In order to form a distribution in the depth direction of the irradiation field as described above, it is necessary to adjust the energy distribution of the particle beam 2. For this purpose, the method conventionally used and also used in the present invention is to pass the particle beam 2 through the ridge filter 10 having a predetermined thickness distribution. The ridge filter 10 can broaden the energy distribution of the particle beam in a predetermined range according to a predetermined thickness distribution.

  That is, the energy of the particle beam after passing differs depending on the incident position of the particle beam 2 on the ridge filter 10 (see FIG. 2). For example, the first passing particle beam 26 shown in FIG. 1 is a particle beam that has passed through the thickest part of one ridge among (bar) ridges (mountains) provided in the ridge filter 10. The second passing particle beam 28 and the third passing particle beam 30 are particle beams that have passed through a portion corresponding to a valley between two ridges of a plurality of (bar) ridges provided in the ridge filter 10. Here, the particle beam energy of the first passing particle beam 26 is lower than that of the second and third passing particle beams 28 and 30, and the reaching depth in the irradiated body 24 is also shallow. On the other hand, the second and third passing particle beams 28 and 30 can reach the deepest position in the irradiated body 24. In this way, an irradiation field having a predetermined width in the depth direction of the irradiated object 24 is formed. This predetermined width is generally determined by the difference in thickness between the thickest part and the thinnest part of the ridge filter 10. That is, each ridge filter 10 generally forms a unique SOBP. In addition, the width (namely, the width of SOBP) in which the Bragg peak is expanded in the thickness direction (tumor) by the ridge filter is usually 1 to 20 cm.

  When a predetermined setting parameter is given to the first expansion unit 6 and the second expansion unit 8 and a ridge filter 10 having a predetermined SOBP is combined, a desired three-dimensional dose in the irradiated object 24 is obtained. Regions can be formed.

  However, for tumor irradiation, it is necessary to make the dose distribution uniform within the above three-dimensional dose region. In order to make the dose distribution uniform within the three-dimensional dose region, the energy of the particle beam that has passed through the ridge filter 10 must be mixed accordingly. For that purpose, for example, in the second passing particle beam 28 and the third passing particle beam 30, after passing through the ridge filter 10, until reaching the irradiation region and range of the irradiated object 24, It is preferable that the traveling direction is appropriately dispersed by the air between the ridge filter 10 and the surface of the irradiated body and by the multi-order scattering in the irradiated body.

  When the particle beam is a proton beam, the particle beam is relatively light, so that it is sufficiently scattered by the air and the irradiated object, and the particle beam can be sufficiently mixed spatially in the irradiation field. However, when the particle beam is a particle beam of a relatively heavy particle such as a carbon beam, it is difficult for scattering to occur. Therefore, a uniform irradiation dose distribution is not obtained at the end of the range of the particle beam, and the ridge peak of the ridge filter 10 is not obtained. A valley of dose is created at the corresponding position. That is, the striped periodic distribution as shown in FIG. 4B is formed in the dose distribution near the range end position.

  FIG. 4 (2) shows a case where a carbon beam having a kinetic energy per nucleon of about 400 MeV is irradiated through the ridge filter 10 having a fixed position in the Y direction at the end of the irradiation field range in water. The result of Monte Carlo simulation of dose distribution is shown. The Y direction shown in FIG. 4 is a direction perpendicular to the ridge direction (X direction) of the ridge filter 10. The period of the stripe pattern of the dose distribution in the Y direction seen in FIG. 4 (2) is the same as the period of the ridge of the projected image at the observation depth position of the ridge filter used in the simulation. For comparison, FIG. 4A shows a dose distribution in the X direction of the same simulation result.

  Therefore, in order to eliminate the non-uniform irradiation dose distribution at the end of the range of the particle beam, in the first embodiment of the present invention, as shown in FIGS. It is rotated in the plane during particle beam irradiation.

  In order to realize the above rotation operation, the following configuration is adopted. The ridge filter 10 is mounted on the ridge filter mounting base 12 by a knock pin (not shown) and a fixing jig (not shown). The ridge filter mounting base 12 is supported by a support base 14 and is rotated by a motor 18 provided outside the support base 14 and a belt 16 connecting the motor 18 and the ridge filter mounting base 12. A bearing 20 is sandwiched between the ridge filter mounting base 12 and the support base 14.

  During the irradiation of the particle beam, the motor 18 which is a rotation driving means of the ridge filter 10 is rotated, and the ridge filter mounting base 12 is rotated via the belt 16. The ridge filter 10 mounted on the ridge filter mounting base 12 rotates during irradiation with the rotation of the motor 18, whereby the ridges of the ridge filter 10 face various directions. Here, when the particle beam 2 incident on the ridge filter 10 is divided into fine parts and considered, each particle beam at the fine part passes through various positions from the valley of the ridge to the mountain. At the end of the particle beam range, a more uniform dose distribution can be obtained. Therefore, for example, the striped distribution generated in the dose distribution simulation of FIG. 4B is averaged. In particular, the averaging becomes significant at a portion away from the rotation center of the ridge filter 10.

  The speed of the above-mentioned rotation is not particularly limited as long as it is performed at least 1 rotation to several tens of rotations during particle beam irradiation. The particle beam irradiation time is usually about 1 to 10 minutes.

  In the above description, the ridge filter 10 is rotated on its installation plane. However, even if the ridge filter 10 is translated so that the ridge peaks and valleys are interchanged, the dose near the end of the particle beam range. The non-uniform distribution is leveled out and a more uniform dose distribution is obtained. The translational motion in this case may be any one that reciprocates within one cycle of the thickness distribution periodic structure of the ridge filter 10. That is, in the irradiation process, the position of the ridge filter 10 with respect to the ridge peaks and valleys may be changed. The speed (cycle) of this translational movement may be such that there is at least one reciprocation between particle beam irradiations.

  The ridge filter in the present specification is intended to form a certain depth expansion irradiation range (SOBP). In cancer treatment, it is necessary to change the SOBP in accordance with the size of the tumor. At this time, it is sufficient that the SOBP is changed by changing the ridge filter 10 attached to the ridge filter attachment base 12. . A ridge filter changing mechanism for automatically replacing the ridge filter 10 may be provided.

  In the particle beam cancer treatment system according to Embodiment 1, a ridge filter having a bar ridge as shown in FIG. 2 or FIG. 3 is used as the ridge filter. However, the present invention is not limited to this, and an SOBP is formed. A ridge filter (for example, a cone ridge filter) having a periodic thickness distribution that can be used may be used. Moreover, the arrangement positions of the first enlargement means 6 and the second enlargement means 8 may be switched.

  In this specification, for the sake of simplicity, only the spatial spread due to scattering of particle beams passing through the ridge filter is considered. This is because, in practice, the particle beam already has an incident angle in a corresponding range due to the finite size and finite emittance of the particle beam itself (a quantity representing the direction distribution of the particle beam) upstream from the ridge filter 10. This is because this incident angle also contributes to expanding the spatial range of the second passing particle beam 28 and the third passing particle beam 30, for example. When discussing the effectiveness of the present invention, the effect of this finite emittance is included in the effect of scattering.

Embodiment 2. FIG.
FIG. 5 is a perspective view of a particle beam cancer treatment system according to Embodiment 2 of the present invention. The particle beam cancer treatment system according to Embodiment 2 of the present invention is substantially the same as the particle beam cancer treatment system according to Embodiment 1 of the present invention. Therefore, the same parts are denoted by the same reference numerals and description thereof is omitted.

  In the particle beam cancer treatment system according to the second embodiment, a storage mechanism for the ridge filter 10 is provided so that a plurality of ridge filters 10 forming irradiation fields each having a different SOBP can be easily replaced according to the irradiated object. Is provided. As shown in FIG. 5, the ridge filter storage device 34 has a disk shape, and stores a plurality of ridge filters 10 in the vicinity of the outer extension of the disk. These ridge filters 10 are stored such that the ridge direction of each ridge filter 10 is orthogonal to the radial direction of the disk of the ridge filter storage device 34. Each ridge filter 10 forms an irradiation field with an individual SOBP.

  The central portion of the ridge filter storage mechanism 34 is mounted on the ridge filter replacement motor unit 36. The ridge filter storage mechanism 34 is rotated by the ridge filter replacement motor unit 36 so as to move the corresponding ridge filter to the particle beam path. The ridge filter storage mechanism 34 and the ridge filter replacement motor unit 36 are horizontally moved by a ridge filter moving device 38. The ridge filter moving device 38 may be composed of, for example, a linear motor.

  Further, the ridge filter storage mechanism 34, the ridge filter replacement motor unit 36, and the ridge filter moving device 38 are supported by a fixed support device 40. The operations of the ridge filter replacement motor unit 36 and the ridge filter moving device 38 are controlled by an irradiation control device 46.

  During the irradiation with the particle beam, the ridge filter 10 is moved in a predetermined horizontal direction 44 as shown in FIG. The moving direction 44 is a direction in which the ridge filter moving device 38 moves. This direction 44 is preferably a direction orthogonal to the ridge direction of the ridge filter 10 on the installation plane of the ridge filter 10 installed in the path of the particle beam being irradiated.

  Similar to the first embodiment, the particle beam irradiation means is schematically configured as shown in FIG. However, the portion related to the replacement function of the ridge filter in the dotted line frame A in FIG. 1 is replaced by the ridge filter storage mechanism 34 shown in FIG.

  Next, the operation of the particle beam cancer treatment system according to Embodiment 2 will be described. Before starting the irradiation of the particle beam, the irradiation control device 46 performs irradiation with a predetermined SOBP from among the plurality of ridge filters 10 according to the SOBP in the depth direction of the irradiation field required by the irradiated object. Bring things that form the field into the path of the particle beam. At this time, the irradiation controller 46 moves the ridge filter storage mechanism 34 by rotating the ridge filter replacement motor 36.

  Each ridge filter 10 of the ridge filter storage device 34 is arranged such that the ridge direction is orthogonal to the movement direction 44 of the ridge filter movement device 38 on the particle beam path (that is, the disk of the ridge filter storage device 34). The installation direction is determined so as to be orthogonal to the radial direction. Note that the ridge filter replacement motor unit 36 is stopped after the start of irradiation.

  When particle beam irradiation starts, first, a particle beam (for example, a carbon beam) is generated from a particle beam generator (not shown) (for example, from an ion source that generates carbon beam ions). After the particle beam is accelerated to a predetermined kinetic energy by a particle beam accelerating unit (not shown), it is made incident on the particle beam irradiation unit by a particle beam transport unit (not shown).

  The particle beam guided to the particle beam irradiation means is expanded in cross-sectional size by a magnifying means (first magnifying means 6 and second magnifying means 8) such as a scatterer or a wobbling electromagnet, and then the ridge shown in FIG. The light enters the filter 10.

  The irradiation control device 46 operates the ridge filter moving device 38 so that the ridge filter 10 on the particle beam path crosses the particle beam in a reciprocating motion. The reciprocating motion may be any one that reciprocates within one cycle of the thickness distribution periodic structure of the ridge filter 10. Considering the particle beam 2 incident on the ridge filter 10 by dividing it into fine parts, each particle beam at the fine part passes through various positions from the valley of the ridge to the mountain. At the end of the range, a more uniform dose distribution can be obtained.

  That is, in the ridge filter 10 of the particle beam cancer treatment system according to the second embodiment, the mixing of particle beam energy occurs only in one direction, but the mixing direction is orthogonal to the ridge, that is, the ridge is periodic. Since the thickness distribution is a direction having a proper thickness distribution, mixing is eventually generated on the entire surface of the particle beam. Therefore, in the deepest region of the irradiation field, the non-uniformity in the ridge arrangement direction (direction orthogonal to the ridge direction) of the ridge filter 10 is leveled, and a more uniform dose distribution can be obtained.

  The reciprocating motion may be any movement that moves at least one half of the reciprocating motion during particle beam irradiation. Since the particle beam irradiation time is usually about 1 to 10 minutes, it is preferably several tens of times.

  In the particle beam cancer treatment system according to the second embodiment, a ridge filter having a bar ridge as shown in FIG. 2 or FIG. 3 is used as the ridge filter. However, the present invention is not limited to this, and an SOBP is formed. A ridge filter (for example, a cone ridge filter) having a periodic thickness distribution that can be used may be used.

Embodiment 3 FIG.
FIG. 6 is a perspective view of a particle beam cancer treatment system according to Embodiment 3 of the present invention. The particle beam cancer treatment system according to Embodiment 3 of the present invention is substantially the same as the particle beam cancer treatment system according to Embodiment 2 of the present invention. However, in the particle beam cancer treatment system according to the third embodiment, the mechanism in which the ridge filter storage mechanism 34 stores the ridge filter 10 and the mechanism in which the ridge filter storage mechanism 34 operates are different.

  The ridge filter storage mechanism 34 has a disk shape as in the second embodiment, and stores a plurality of ridge filters 10 that form irradiation fields each having a different SOBP in the outer extension of the disk. Here, the ridge filters 10 are installed so that the (bar) ridges of the ridge filter 10 generally face the center of the disk of the ridge filter storage mechanism 34.

  The central portion of the ridge filter storage mechanism 34 is mounted on the ridge filter replacement / movement motor unit 362. The ridge filter storage mechanism 34 is rotated by the ridge filter replacement / movement motor unit 362 so as to move the corresponding ridge filter to the path of the particle beam. This direction of rotation is indicated by arrow 42 in FIG.

  During irradiation with particle beams, the ridge filter 10 is rotated by the ridge filter replacement / movement motor unit 362 so as to move relatively small in a predetermined direction 44 as shown in FIG. This direction 44 is preferably a direction substantially orthogonal to the ridge direction of the ridge filter 10 on the installation plane of the ridge filter 10 installed in the path of the particle beam being irradiated. The rotation operation of the ridge filter replacement / movement motor unit 362 is controlled by the irradiation controller 46.

  Similar to the first embodiment, the particle beam irradiation means is schematically configured as shown in FIG. However, the portion related to the ridge filter replacement function in the dotted line frame A in FIG. 1 is replaced by the ridge filter storage mechanism 34 shown in FIG.

  Subsequently, the operation of the particle beam cancer treatment system according to Embodiment 3 will be described. Before starting the irradiation of the particle beam, the irradiation control device 46 performs irradiation with a predetermined SOBP from among the plurality of ridge filters 10 according to the SOBP in the depth direction of the irradiation field required by the irradiated object. Bring things that form the field into the path of the particle beam. At this time, the irradiation control device 46 rotates the ridge filter replacement / movement motor 362 to move the ridge filter storage mechanism 34.

  When particle beam irradiation starts, first, a particle beam (for example, a carbon beam) is generated from a particle beam generator (not shown) (for example, from an ion source that generates carbon beam ions). After the particle beam is accelerated to a predetermined kinetic energy by a particle beam accelerating unit (not shown), it is made incident on the particle beam irradiation unit by a particle beam transport unit (not shown).

  The particle beam guided to the particle beam irradiation unit is expanded in cross-sectional size by an enlarging unit (a first enlarging unit 6 and a second enlarging unit 8) such as a scatterer or a wobbling electromagnet, and then the ridge shown in FIG. The light enters the filter 10.

  The irradiation control device 46 operates the ridge filter replacement / movement motor unit 362 so that the ridge filter 10 on the particle beam path crosses the particle beam in a reciprocating motion (movement). In other words, the irradiation control device 46 adjusts the ridge so that the angular position of the ridge filter 10 (in the rotational angle of the disk of the ridge filter storage mechanism 34) fluctuates in the vicinity of the position where the ridge filter 10 is installed. The ridge filter storage mechanism 34 including the filter 10 is reciprocated. The reciprocating motion (movement) may be any one that reciprocates within one cycle of the thickness distribution periodic structure of the ridge filter 10. In this way, when the particle beam 2 incident on the ridge filter 10 is divided into fine parts and considered, each fine particle beam passes through various positions from the ridge valley to the mountain. Therefore, a more uniform dose distribution can be obtained at the end of the range of the particle beam. The above-described reciprocating movement may be a sweep movement that moves only half of one reciprocating movement.

  The reciprocating motion (movement) may be any movement that moves at least half of the reciprocation between particle beam irradiations. Since the particle beam irradiation time is usually about 1 to 10 minutes, it is desirable to perform several tens of reciprocations.

  In the ridge filter 10 of the particle beam cancer treatment system according to the third embodiment, as in the second embodiment, mixing of the energy of the particle beam occurs only in one direction, but the mixing direction is orthogonal to the ridge. That is, since the ridge is in a direction having a periodic thickness distribution, mixing is eventually generated on the entire surface of the particle beam.

  Compared to the second embodiment, the particle beam cancer treatment system according to the third embodiment includes a means for exchanging the ridge filter and a means for moving the ridge filter during the particle beam irradiation. 362 and an irradiation control device 46 that moves the motor unit 362. Therefore, the overall cost can be further suppressed.

  In the above description regarding the third embodiment, the ridge filter storage mechanism 34 is a rotary type. Here, the same effect can be obtained by installing the ridge filter in a straight line on a rail that is linearly driven by a linear motor or the like so that the ridge direction is orthogonal to the rail linear direction. In other words, if a means for exchanging the ridge filter and a means for moving the ridge filter during particle beam irradiation are configured by using an irradiation control device and a driving means such as a linear motor, the end of the particle beam range can be achieved. A uniform dose distribution can be expected.

  In the particle beam cancer treatment system according to the third embodiment, a ridge filter having a bar ridge as shown in FIGS. 2 and 3 is used as the ridge filter. However, the present invention is not limited to this, and an SOBP is formed. A ridge filter (for example, a cone ridge filter) having a periodic thickness distribution that can be used may be used.

Embodiment 4 FIG.
FIG. 7 is an example of a flowchart of a particle beam irradiation method performed using the particle beam cancer treatment system according to Embodiment 3 of the present invention. An example of the particle beam irradiation method according to the present invention will be described below with reference to FIGS.

  (Step 1) The energy and beam current of the particle beam emitted from the particle beam acceleration means are selected and set.

  (Step 2) Parameters such as an electromagnet in the particle beam transport means are set.

  (Step 3) Parameters of the beam expanding means provided in the particle beam irradiating means for irradiating the particle beam toward the patient are determined, and parameters of the corresponding expanding means (the first expanding means 6 and the second exceptional means 8) are determined. Set.

  (Step 4) The parameters of the SOBP forming means (ridge filter) that causes the range modulation of the particle beam are set according to the required SOBP width of the irradiation field, and the ridge filter that is the corresponding SOBP forming means is set. Select and set the particle beam path.

  (Step 5) The spatial position variation pattern of the ridge filter during particle beam irradiation is set in the irradiation control device.

  (Step 6) Parameters relating to a collimator for shaping the particle beam that has passed through the ridge filter into a predetermined shape are set.

  (Step 7) The position of the patient who is an irradiation object is confirmed.

  (Step 8) The preset value of the dose monitor is set based on the result of the treatment plan or the like.

  (Step 9) Particle beam irradiation is started. A particle beam beam is emitted from the particle beam accelerating unit and is incident on the particle beam irradiation unit.

  (Step 10) In the irradiation control device 46, the ridge filter is reciprocated or swept within a small range in a predetermined direction in accordance with the spatial position variation pattern during particle beam irradiation of the ridge filter selected and set in Step 5 above. Move. The movement is performed in the direction in which the thickness distribution variation of the ridge filter exists. As a result, during irradiation, each ridge of the ridge filter can move to the position of the adjacent ridge, and the non-uniform dose at the end of the range due to the thickness distribution of the ridge can be reduced.

  (Step 11) During irradiation, it is checked whether or not the dose set by the dose monitor has been irradiated. If the dose has expired, the process proceeds to Step 12, and if not, the process proceeds to Step 10.

  (Step 12) The irradiation is terminated and stopped.

  In the fourth embodiment, the spatial position of the SOBP forming means (ridge filter) that forms an irradiation field having a predetermined SOBP is set in the thickness distribution cycle in the direction in which the ridge thickness distribution periodically changes. It is important to move more than half of the space length. Moreover, you may replace said step other than step 9, step 10, and step 11 as needed.

It is a longitudinal cross-sectional view of the particle beam irradiation means of the particle beam cancer treatment system which concerns on Embodiment 1 of this invention. 1 is a perspective view of a ridge filter of a particle beam cancer treatment system according to Embodiment 1 of the present invention. It is an expanded sectional view of the ridge filter of the particle beam cancer treatment system concerning Embodiment 1 of the present invention. Monte Carlo simulation results of dose distribution in the Y direction at the end of the irradiation field range in water when a carbon beam with a kinetic energy per nucleon of about 400 MeV is irradiated through a ridge filter with a fixed position (Fig. 4 (2)) and the dose distribution in the X direction of the same simulation result (FIG. 4 (1)). It is a perspective view of the particle beam cancer treatment system which concerns on Embodiment 2 of this invention. It is a perspective view of the particle beam cancer treatment system which concerns on Embodiment 3 of this invention. It is an example of the flowchart of the particle beam irradiation method in the particle beam cancer treatment system which concerns on this invention.

Explanation of symbols

2 particle beam, 4 transmission source point, 6 first expansion means, 8 second expansion means, 10 ridge filter, 12 ridge filter mounting base, 14 support base, 16 belt, 18 motor, 20 bearing, 22 collimator, 24 Object to be irradiated, 26 First passing particle beam, 28 Second passing particle beam, 30 Third passing particle beam, 32 Rotating shaft, 34 Ridge filter storage mechanism, 36 Ridge filter replacement motor unit, 362 Ridge filter replacement・ Moving motor part, 38 ridge filter moving device, 40 fixed support device, 46 irradiation control device.

Claims (5)

A particle beam cancer treatment system having particle beam irradiation means,
The particle beam irradiation means,
A plurality of ridge filters having a cross-section with a periodic thickness distribution in which the energy lost depending on the position through which the particle beam passes;
Storage means for storing the plurality of ridge filters;
Exchanging means for moving the storage means so that the predetermined ridge filter is arranged in the path of the particle beam before irradiating the particle beam to the predetermined ridge filter among the plurality of ridge filters;
While irradiating the predetermined ridge filter with the particle beam, an irradiation position for moving the storage means so that the position of the predetermined ridge filter changes in a plane orthogonal to the axis of the particle beam in the traveling direction Change means,
The particle beam cancer treatment system, wherein the exchanging means and the irradiation position changing means share one driving means . The storage means has a disk shape, and stores and stores the plurality of ridge filters on concentric circles of the disk,
2. The particle beam cancer treatment system according to claim 1, wherein the irradiation-time position changing unit rotates and moves the storage unit about the center of the disk as a rotation axis . The storage means stores the plurality of ridge filters arranged linearly in a first direction,
The particle beam cancer treatment system according to claim 1, wherein the irradiation position changing means linearly moves the storage means in the first direction . The plurality of ridge filters are formed such that the cross section is linearly connected in the second direction,
The storage means arranges the plurality of ridge filters so that the second direction faces the center of the disk.
The particle beam cancer treatment system according to claim 2 . The plurality of ridge filters are formed such that the cross section is linearly connected in the second direction,
The storage means arranges the plurality of ridge filters so that the second direction is orthogonal to the first direction.
The particle beam cancer treatment system according to claim 3 .

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