This application is based upon and claims the benefit of priority from Japanese Patent Application No. 2012-043816, filed Feb. 29, 2012, the entire contents of which are incorporated herein by reference.
Embodiments described herein relate generally to a laser ion source that generates ions by irradiation of a laser beam.
In recent years, a therapy method for cancer by high-energy carbon ion irradiation has been developed and a therapy using an ion source that generates an ion beam has been disclosed.
For advanced performance improvement of the ion source, a high-density C6+ needs to be generated. However, for example, since an ion source using μ-wave discharge plasma is lack of capability to generate the high-density C6+, development of a new ion source is required.
Therefore, a laser ion source having an ability to generate a high-density ion beam has been known. The laser ion source is a device that collects and irradiates a laser beam onto a solid target set in a space that satisfies a predetermined vacuum condition, ionizes the solid target by energy of the laser beam, and electrostatically extracts the ions to generate an ion beam.
A feature of the laser ion source is that the solid target is used as a generation source of the ion. By using the solid target as such, high-density ion current can be extracted in the laser ion source.
However, in the case where the laser ion source is continuously operated, the generation source of the ion (that is, the solid target) needs to be supplied in the laser ion source.
For example, in the ion source using the discharge plasma, gas may be just supplied as the generation source of the ion. In this regard, in the laser ion source, the solid target is generally supplied (exchanged) by releasing the laser ion source to the atmosphere whenever supplying the generation source of the ion (that is, the solid target).
When the laser ion source is applied to a medical service, since a long stabilizing operation is required for the corresponding laser ion source, the target is required to be supplied (exchanged) without damaging the vacuum condition in the space where the solid target (hereinafter, simply referred to as a target), which is the ion generation source is set.
In other words, it is important to establish a consecutive supply method of the target which does not significantly damage the vacuum condition in the laser ion source.
However, when the laser ion source is released to the atmosphere whenever supplying the target, the vacuum condition in the space, where the target is set, is damaged.
Therefore, in the laser ion source, a special device is required to supply the target.
Hereinafter, embodiments of the invention will be described with reference to the accompanying drawings. According to one embodiment, in general, there is provided a laser ion source, including: a vacuum chamber which is vacuum-exhausted and in which a target generating ions by irradiation of a laser beam is transported and set; a valve which is provided on a side of the vacuum chamber, and is opened when the target is transported into the vacuum chamber and is closed except for the transportation; a target supply chamber which is attached to the vacuum chamber via the valve, holds the target to be movable, and is vacuum-exhausted independently from the vacuum chamber; and a transportation unit which transports to the vacuum chamber the target held on the target supply chamber while opening the valve after the target supply chamber is vacuum-exhausted while closing the valve.
A laser ion source 100 illustrated in
A target shifting device 111 is provided in the ion generation vacuum chamber 110. A target 112 containing an element, which becomes an ion, is transported and set on the target shifting device 111. The target shifting device 111 serves to shift the target 112 so as to change an irradiation position of a laser beam to the target 112. Further, the target 112 is, for example, a carbon based plate-like member.
In addition, although not illustrated in
The target supply chamber 120 is attached to the ion generation vacuum chamber 110 via the valve 130. The target supply chamber 120 is able to be vacuum-exhausted by the exhaust system (not illustrated), independently from the ion generation vacuum chamber 110.
The valve 130 is provided in a part (a side) of the ion generation vacuum chamber 110 and serves to open/close a flow channel between the ion generation vacuum chamber 110 and the target supply chamber 120. The valve 130 is opened when the target is transported into the ion generation vacuum chamber 110 and closed except for the transportation, for example. Further, in the valve 130, for example, opening/closing is performed by a vacuum cut-off valve.
According to the laser ion source 100, the laser beam 200 is collected and irradiated onto the target 112, and as a result, an ion 300 is generated by energy of the laser beam and the ion 300 is electrostatically extracted, and as a result, an ion beam is generated.
In detail, in the laser ion source 100, the laser beam 200 is collected and irradiated onto the target 112 set in the ion generation vacuum chamber 110, and as a result, a minute fraction of the target 112 becomes hot as a high temperature, is made into plasma, and is emitted to a space, at a point (hereinafter, referred to as an irradiation point) onto which the laser beam is collected and irradiated. Ions in the plasma receive energy even from the laser beam 200, and as a result, multi-charged ions are generated. In the laser ion source 100, the generated ion 300 is accelerated in the acceleration electrode to be extracted as a high-energy ion beam.
Further, since the high-energy laser beam 200 is collected and irradiated onto the target 112, a crater is formed on the surface of the target 112 by one laser irradiation. For stabilization of ion generation in the laser ion source 100, the laser beam 200 may be irradiated onto a new surface of the target 112 whenever the laser beam 200 is collected and irradiated. To this end, in the laser ion source 100, the target 112 may be shifted little by little so as to avoid an irradiation point (the point onto which the laser beam 200 is collected and irradiated) which has been used, by the target shifting device 111.
Further, the center of ablation plume, which is ejected when the laser beam 200 is collected and irradiated onto the target 112, is a normal direction of the irradiation point (irradiation surface). That is, the surface of the target 112 at the irradiation point of the laser beam 200 is set such that a normal erected from the irradiation point matches an axial direction (a direction to generate the ion 300) which is mechanically determined in the laser ion source 100. Hereinafter, the axis, which is mechanically determined in the laser ion source 100, is referred to as an ion axis.
For example, in the case where the laser beam 200 is irradiated onto all surfaces of the target 112 by little by little shifting the target 112 with the target shifting device 111 as described above, the target 112 set in the ion generation vacuum chamber 110 (on the target shifting device 111) needs to be exchanged (that is, a new target 112 needs to be supplied).
Hereinafter, referring to
Herein, a case in which all surfaces of a target 112a set in the ion generation vacuum chamber 110 are collected and irradiated by the laser beam 200 (that is, a case in which the target 112a needs to be exchanged) is assumed. In this case, it is assumed that the ion generation vacuum chamber 110 is vacuum-exhausted by a vacuum exhausting device 140 provided in the ion generation vacuum chamber 110. Further, it is assumed that the valve 130 is in a closed state (hereinafter, referred to a closed state).
Hereinafter, the used target 112a, which is exchanged, is referred to as the used target 112a.
In this case, the target supply chamber 120 is vacuum-exhausted by a vacuum exhausting device 150 provided in the target supply chamber 120.
Subsequently, after the valve 130, which connects the ion generation vacuum chamber 110 and the target supply chamber 120, is in the opened state (hereinafter, referred to as the opened state), the used target 112a, which is set in the ion generation vacuum chamber 110, is drawn up to the target supply chamber 120 by, for example, a transportation rod inserted into the ion generation vacuum chamber 110 from the target supply chamber 120.
Thereafter, the valve 130 is in the closed state and the target supply chamber 120 is released to the atmosphere. The used target 112a, which is drawn up to the target supply chamber 120, is exchanged with a target 112b (hereinafter, referred to as a supplying target) which is newly supplied into the ion generation vacuum chamber 110. As a result, the supplying target 112b is held (set) in the target supply chamber 120 to be movable. A front end of a transportation rod 121 (a rod-shaped member) is attached to the supplying target 112b. Further, a target transporting device 160 for transporting the supplying target 112b to the ion generation vacuum chamber 110 is connected to the other end of the transportation rod 121.
In addition, since the valve 130 is in the closed state as described above, the ion generation vacuum chamber 110 is maintained in a vacuum-exhausted state even during an operation in which the supplying target 112b is set in the target supply chamber 120.
In the case where the supplying target 112b is set in the target supply chamber 120 as described above, the target supply chamber 120 is vacuum-exhausted by the vacuum exhausting device 150.
Subsequently, the valve 130 is in the opened state at the time when an internal pressure of the target supply chamber 120 is equal to or lower than an internal pressure of the ion generation vacuum chamber 110 by vacuum-exhaustion of the vacuum exhausting device 150, and the supplying target 112b is transported into the ion generation vacuum chamber 110 by the target transporting device 160 and the transportation rod 121.
Herein, the target shifting device 111 is provided in the ion generation vacuum chamber 110 as described and a target shifting stand 113 is installed in the target shifting device 111.
The supplying target 112b transported to the ion generation vacuum chamber 110 is fixed to the target shifting stand 113 and shifted with high precision by the target shifting device 111 such that the normal direction of the irradiation point (irradiation surface) matches the aforementioned ion axis direction.
That is, when the supplying target 112b is supplied in the laser ion source 100 according to the embodiment, the valve 130 is in the closed state while the ion generation vacuum chamber 110 and the target supply chamber 120 are in the vacuum exhaustion state and only the target supply chamber 120 is released to the atmosphere. When the supplying target 112b is set in the target supply chamber 120, the target supply chamber 120 is vacuum-exhausted again and thereafter, the valve 130 is in the opened state and the supplying target 112b is transported into the ion generation vacuum chamber 110. As a result, the supplying target 112b may be supplied to the ion generation vacuum chamber 110 without releasing the ion generation vacuum chamber 110 to the atmosphere.
Further, the target shifting device 111 provided in the ion generation vacuum chamber 110 includes, for example, an electric actuator. In the case where a motor of an electric actuator is installed in the ion generation vacuum chamber 110, power is supplied from the outside of the ion generation vacuum chamber 110 and rotation of the motor is controlled. In addition, (A surface of) the target 112 installed in the ion generation vacuum chamber 110 may be in a surface vertical to the ion axis which is mechanically determined in the laser ion source 100 and a shifting direction of the target 112 by the target shifting device 111 may be one direction or two directions.
In addition, the target 112 may be shifted by a linear introducer which is operable from the outside of the ion generation vacuum chamber 110 or shifted by a rotational introducer which is operable from the outside of the ion generation vacuum chamber 110 and a gear installed in the ion generation vacuum chamber 110.
As described above, in the embodiment, it is possible to supply the target 112 without damaging the vacuum condition by the configuration to include the ion generation vacuum chamber 110 vacuum-exhausted, in which a target generating ions by irradiation of the laser beam 200 is transported and set, the valve 130 provided on the side of the ion generation vacuum chamber 110, and opened when the target 112 is transported into the ion generation vacuum chamber 110 and closed except for the transportation, the target supply chamber 120 which is attached to the ion generation vacuum chamber 110 via the valve 130, holds the target 112 to be movable, and is vacuum-exhausted independently from the ion generation vacuum chamber 110, and the target transporting device 160 which transports to the ion generation vacuum chamber 110 the target 112 held on the target supply chamber 120 while opening the valve 130 after vacuum-exhausting the target supply chamber 120 while closing the valve 130.
Further, in the embodiment, the target 112 (112a and 112b) of a quadrangular prism (plate-like member) is used as illustrated in
Subsequently, a second embodiment of the invention will be described with reference to
Further,
As illustrated in
In the embodiment, the guide rail 410 is provided, and as a result, the supplying target 112b is transported to an ion generation vacuum chamber 110 along the guide rail 410. Therefore, the supplying target 112b is accurately mounted on a target shifting stand 113 installed in a target shifting device 111.
Further, the supplying target 112b and the guide rail 410 in the embodiment may be used by a combination of structures in which the supplying target 112b is certainly transportable in a stable state.
Herein,
As illustrated in
Further, since the embodiment is the same as the first embodiment except that the supplying target 112b is transported along the guide rail 410, a detailed description thereof will be omitted.
In the embodiment as described, the supplying target 112b may be accurately mounted (transported) onto the target shifting stand 113 in the stable state by the configuration in which the supplying target 112b is transported along the guide rail 410 installed from the target supply chamber 120 to the ion generation vacuum chamber 110.
Further, in the embodiment, by the configuration in which the guide rail 410 is divided at the position of the valve 130, the guide rail 410 may be avoided from interrupting opening/closing of the valve 130 even in the case where the guide rail 410 is provided.
Subsequently, a third embodiment of the invention will be described with reference to
The embodiment is different from the first embodiment in that a supplying target 112b is held on a target holder 510 as illustrated in
A junction portion 511 of the target holder 510 with a transportation rod 520, which is illustrated in
By using the transportation rod 520, the target holder 510 holding the supplying target 112b may be magnetically captured (suctioned) to be transported.
Further, the target holder 510 is transported to the ion generation vacuum chamber 110 as described above, and as a result, the supplying target 112b is mounted on a target shifting stand 113 provided in the ion generation vacuum chamber 110.
In addition, since the embodiment is the same as the first embodiment except that the target holder 510 holding the supplying target 112b is transported by using the transportation rod 520, as illustrated in
In the embodiment as described above, it is possible to improve stability of a supply operation of the supplying target 112b by the configuration in which the target holder 510 holding the supplying target 112b is provided and the target holder 510 is transported to the ion generation vacuum chamber 110.
Further, in the embodiment, the junction portion 511 of the target holder 510 is made of the magnetic material, but the entirety of the target holder 510 may be made of the magnetic material.
Further, in the embodiment, the junction portion 511 of the target holder 510 is made of the magnetic material and the magnetic field generating device is mounted on the junction portion 521 of the transportation rod 520, but a dielectric is used in the junction portion 511 of the target holder 510 instead of the magnetic material and an electrostatic system may be generated in the junction portion 521 of the transportation rod 520. In this case, the target holder 510 holding the supplying target 112b may be electrostatically captured (suctioned) to be transported.
In addition, in the embodiment, the junction portion 511 of the target holder 510 is made of the magnetic material and the magnetic field generating device is mounted on the junction portion 521 of the transportation rod 520, and as a result, the target holder 510 is magnetically captured, but for example, the transportation rod 520 is used when the target holder 510 is transported into the ion generation vacuum chamber 110, while the target holder 510 may be mechanically captured by using, for example, a hook, and the like when the target holder 510 is drawn from the ion generation vacuum chamber 110.
Further, when the target holder 510 is transported in the embodiment, the guide rail in the second embodiment may be used.
Subsequently, a fourth embodiment of the invention will be described with reference to
The embodiment is different from the first embodiment in that (a target shifting stand 113 provided in) a target shifting device 111 includes a fixation mechanism that fixes a supplying target 112b.
The supplying target 112b transported to an ion generation vacuum chamber 110 from the target supply chamber 120 as described above is mounted on the target shifting stand 113. In this case, the supplying target 112b needs to be fixed on the target shifting stand 113 such that the normal direction of the irradiation point (irradiation surface) of the supplying target 112b onto which a laser beam 200 is collected and irradiated matches the ion axis direction (the axial direction which is mechanically determined in a laser ion source 100).
Therefore, in the embodiment, a surface 610 (hereinafter, referred to as a reference surface), which is orthogonal to the ion axis, is provided on the target shifting stand 113, as described in
In the embodiment as described above, it is possible to improve the stability of the generation of the ion beam by the configuration in which the point (irradiation point) of the transported supplying target 112b is fixed onto the target shifting stand 113 to be orthogonal to the ion axis direction to generate the ions.
Further, in the embodiment, the supplying target 112b is fixed to the target shifting stand 113, but the target holder holding the supplying target 112b as described in the third embodiment is brought into close contact with the reference surface 610 to fix the supplying target 112b.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Date | Country | Kind |
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2012-043816 | Feb 2012 | JP | national |